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Controlled Modification of Metal-Organic<br />
Frameworks at Metal Sites:<br />
Local Environment Study and Properties<br />
Dissertation<br />
Wenhua Zhang
Controlled Modification of Metal-Organic<br />
Frameworks at Metal Sites:<br />
Local Environment Study and Properties<br />
Dissertation<br />
to obtain the doctorate Dr. rer. nat.<br />
of the Faculty of Chemistry and Biochemistry<br />
Ruhr‐University Bochum<br />
Submitted by Wenhua Zhang, M. Sc.<br />
July 2016
This thesis is based on the work performed during the time of October<br />
2012 and July 2016 under the supervision of Prof. Dr. Roland A. Fischer<br />
at the Chair of Inorganic Chemistry II, Organometallic & Materials, of the<br />
Ruhr‐University Bochum.<br />
1 st referee: Prof. Dr. Roland A. Fischer<br />
2 nd referee: Prof. Dr. Nils Metzler‐Nolte<br />
Herein I declare that I have written this thesis independently and<br />
without unauthorized help. Further, I assure that I have used no other<br />
sources, auxiliary means or quotes than those stated. I further declare<br />
that I have not submitted this thesis in this or in a similar form to any<br />
other university or college. Besides, I declare that I have not already<br />
undertaken an unsuccessful attempt to obtain a doctorate from another<br />
college or university.<br />
Wenhua Zhang<br />
July 2016
Acknowledgements<br />
First of all, I sincerely appreciate my supervisor<br />
Prof. Dr. Roland A. Fischer<br />
for giving me the opportunity to study in the group of Inorganic Chemistry II at Ruhr-<br />
University Bochum. I am grateful to him for affording me guidance and motivation on the<br />
scientific research. Besides, I thank his support for allowing me to attend the international<br />
conferences and visit the world-class research group, which open my mind and give me<br />
much inspiration in scientific field as well.<br />
I also thank Prof. Dr. Nils Metzler-Nolte for accepting to be the co‐referee of this<br />
dissertation.<br />
Further I would like to thank Dr. Zhenlan Fang for bringing me to the topic of Cu-based<br />
DEMOFs and her help on this topic.<br />
I address very special thanks to Dr. Olesia Halbherr for introducing me to the world of the<br />
challenging project on Ru-based (DE)MOFs and for having been advising me during my<br />
study on this topic. Thanks very much for your patience, your assistance and your<br />
knowledge on the topic as well as your invaluable guidance on writing reports. I cannot<br />
make so much progress without you.<br />
Furthermore, I would like to thank the following persons without whom this work is not<br />
able to be accomplished:<br />
Dr. Kira Khaletskaya, Dr. Min Tu, Dr. Harish Paralla, Suttipong Wannapaiboon,<br />
Christoph Rösler, and Inke Schwedler for collecting powder X-ray diffraction<br />
patterns.<br />
Dr. Arik Puls, Dr. Kerstin Freitag, Dr. Sebastian Henke and Manuela Winter for<br />
conducting single‐crystal X‐ray experiments and helping me solve the singlecrystal<br />
structure.<br />
Andreas Schneemann for teaching me to perform the TG measurements.<br />
Dr. Yuemin Wang (Karlsruhe Institute of Technology), Max Kauer, and Penghu Guo<br />
(Laboratory of Industrial Chemistry, Prof. Dr. Martin Muhler, Ruhr‐University
Bochum) for the study of XPS and UHV-FTIR and providing the corresponding<br />
figures.<br />
Dr. Bauke Albada and Martin strack for carrying out the HPLC measurements<br />
(Chair of Inorganic Chemistry I - Bioinorganic Chemistry, Prof. Dr. Nils Metzler‐<br />
Nolte, Ruhr‐University Bochum).<br />
Noushin Arshadi (group of Prof. Dr. Martin Muhler, Ruhr‐University Bochum) for<br />
collecting the N2 sorption isotherms.<br />
Dr. Rolf Neuser (Faculty of Geosciences, Institute of Geology, Mineralogy and<br />
Geophysics, Ruhr‐University Bochum) for the gold coating on the non-conducting<br />
SEM samples.<br />
Dr. Kira Khaletskaya and Stefan Cwik for conducting SEM-EDX measurements.<br />
Dr. Christian Wiktor for collecting TEM-EDX spectra.<br />
Dr. Christian Sternemann (and Andreas Schneemann, Suttipong Wannapaiboon)<br />
for helping me to gather X‐ray diffraction patterns at the DELTA facility. Ralph<br />
Wagner (and Andreas Schneemann) for assistance of performing XAS on the Ru-<br />
(DE)MOF samples and for introducing me to the study of XANES.<br />
Karin Bartholomäus for elemental analysis.<br />
Prof. Dr. Jeffrey R. Long for the chance to have a research stay in his group, at the<br />
Department of Chemistry, University of California, Berkeley (USA). The whole<br />
group for an inspiring communication and very nice time during my stay. I address<br />
many thanks to Miguel Gonzalez for guiding me on conducting the catalytic<br />
reaction in Chapter 4 and assistance on evaluating the data. Last but not the least,<br />
Dianne Xiao, Douglas Reed, Julia Oktawiec for their great assistance with sorption<br />
studies and help on collecting sorption isotherms.<br />
Dr. Francesc X. Llabrés i Xamena (Institute of Chemical Technologies, Polytechnical<br />
University of Valencia, Spain) for the collaboration and Konstantin Epp (group of<br />
the Prof. Dr. Roland A. Fischer in Technical University of Munich) for performing<br />
the catalytic reaction in Chapter 4.<br />
Zhihao Chen and Majd Al-Naji (group of Prof. Dr. Roger Gläser, University of<br />
Leipzig) for carrying out the catalytic reaction in Chapter 5 and the assistance on<br />
study the catalytic activity.<br />
I also want to acknowledge the financial support from China Scholarship Council to my<br />
whole Ph.D study and Research School Plus at Ruhr-University Bochum for the funding of
attending conferences, my research stay at UC Berkeley and my invitation of Dianne Xiao<br />
(from UC Berkeley) for the short visit in ACII group.<br />
I am thankful to the master students who work with me during my Ph.D study: Marco<br />
Rehosek, Sebastian Kunze, and Konstantin Epp.<br />
I am grateful to all ACII members for a nice working atmosphere, the great team spirit and<br />
inspiring communications, especially the former and present MOF family. The memorable<br />
and wonderful time we spend together in the MOF 2014 conference and the trip in Japan<br />
with our MOF guest Takashi Toyao. I express my many thanks to Dr. Christian Wiktor on<br />
teaching me skills for my first poster. Also further thanks to Dr. Chuanqiang Li, Suttipong<br />
Wannapaiboon, Andreas Schneemann, and Konstantin Epp for the kind accompany<br />
during XAS data collecting in DELTA facility.<br />
Besides, I address many thanks to my lab neighbor Dr. Raghavender Medishetty and Dr.<br />
Arik Puls for the abundant and fruitful discussions.<br />
I would like to express my thanks to Dr. Mariusz Molon for affording technical help on my<br />
computer, and OM group members for sharing the experience on air-free synthesis.<br />
I am grateful to Uschi Hermann for her kindness and great help in the lab.<br />
Furthermore, I would like to express my thanks to Jana Weiing, Andreas Schneemann,<br />
Jiyeon Kim, Inke Schwedler and Dr. Christian Wiktor for the great time during ACS fall<br />
meeting and the nice trip in Boston.<br />
I would like to express my warm thanks to Sabine Pankau and Jacinta Essling for their<br />
great help with administrative issues.<br />
Many thanks to my office colleagues for nice working atmosphere, giving me suggestions<br />
and help on the daily life and as translators: Sarah Karle, Mathies Evers, Stefan Cwik,<br />
Maximilian Gebhard, Inke Schwedler, Richard O'Donoghue, Jiyeon Kim, Andreas<br />
Schneemann, Dr. Christian Wiktor, Dr. Arik Puls, and Dr. Sun Ja Kim.<br />
I am also thankful to Dr. Ke Xu for helping me go through a bunch of documents to settle<br />
down in Germany.<br />
Last but the most important, I would like to deeply thank my parents Denggao Zhang and<br />
Chunying Wu, for giving me the freedom and support to study abroad and their endless<br />
love and motivation during my studies. Also thank my siblings, Wenjing and Wenbo
Zhang, for their continuous support and care. My love and deep appreciation to Zhihao<br />
Chen for always being at my side. His motivation and continuous care help me recover<br />
from the sadness of homesick and overcome the challenging in my life and study. All these<br />
would not happen without them.
Table of Contents<br />
Table of Contents ................................................................................................................................................. I<br />
Abbreviations ....................................................................................................................................................... V<br />
1 Motivation .................................................................................................................................................... 1<br />
2 General introduction ............................................................................................................................... 3<br />
2.1 Origin of MOFs - Coordination polymers ............................................................................... 3<br />
2.2 Definition, Chemistry and features of MOFs ........................................................................ 7<br />
2.2.1 Definition and nomenclature of MOFs ................................................................ 7<br />
2.2.2 MOF features .................................................................................................................. 8<br />
2.3 Synthetic approaches, modification and applications of MOFs ................................ 14<br />
2.3.1 Traditional synthesis approaches ...................................................................... 14<br />
2.3.2 Reticular synthesis ................................................................................................... 15<br />
2.3.3 Way to the modification of MOFs ....................................................................... 16<br />
2.3.4 Application of MOFs ................................................................................................. 23<br />
3 Controlled secondary building unit approach to the formation of the<br />
isostructural Ru II,II and Ru II,III analogs of [M3(BTC)2]n ........................................................... 26<br />
3.1 Preparation and investigation of the Ru II,III -analogs of [M3(BTC)2]n ...................... 28<br />
3.1.1 The family of [M3(BTC)2]n...................................................................................... 28<br />
3.1.2 Background and the state-of-the-art in research on Ru-analogs of<br />
[M3(BTC)2]n.................................................................................................................. 29<br />
3.1.3 [Ru3(BTC)2Yy]n·G g obtained by CSA using [Ru2(OOCR)4X] and<br />
[Ru2(OOCCH3)4]A: synthesis and characterization ..................................... 31<br />
3.1.4 Pre-activation by solvent exchange ................................................................... 37<br />
3.1.5 Study of [Ru3(BTC)2Yy]n·G g after solvent exchange .................................... 38<br />
3.1.6 Summary ....................................................................................................................... 48<br />
3.2 Elaboration of Ru II,II analog of [M3(BTC)2]n........................................................................ 50
II<br />
3.2.1 Synthesis and characterization of SBU-e and Ru-MOF 5.......................... 50<br />
3.2.2 Investigation on the Ru oxidation state and porosity of Ru-MOF 5 .... 53<br />
3.2.3 Conclusions .................................................................................................................. 55<br />
4 Linker-based MOF solid solutions: Defect-Engineered MOFs (DEMOFs) .................... 56<br />
4.1 Introduction .................................................................................................................................... 58<br />
4.1.1 Solid solutions ............................................................................................................ 58<br />
4.1.2 Defects in MOFs and its “engineering”............................................................. 60<br />
4.2 Ruthenium Metal-Organic Frameworks featuring Different Defect Types ......... 65<br />
4.2.1 Synthesis and characterization of the Ru-DEMOF materials ................. 65<br />
4.2.2 Porosity of Ru-DEMOF samples and the confirmation of the DL<br />
incorporation .............................................................................................................. 76<br />
4.2.3 XANES, XPS and UHV-FTIR studies: ruthenium oxidation state<br />
variation as indication of defect type formation ......................................... 79<br />
4.2.4 CO2, CO and H2 sorption properties of Ru-DEMOFs ................................... 91<br />
4.2.5 Catalytic test reactions ......................................................................................... 100<br />
4.2.6 Conclusions ............................................................................................................... 106<br />
4.3 Defects Engineering in [Cu3(BTC)2]n: Effect of the synthetic parameters ......... 108<br />
4.3.1 Preparation and characterization of Cu-DEMOF samples<br />
[Cu3(BTC)2-x(ip)x]n.................................................................................................. 109<br />
4.3.2 Composition and porosity of the prepared Cu-DEMOFs ....................... 116<br />
4.3.3 Oxidation state(s) of metal-sites in prepared Cu-DEMOFs .................. 119<br />
4.3.4 Conclusions ............................................................................................................... 121<br />
5 Simultaneous introduction of various palladium active sites into MOF via onepot<br />
synthesis: Pd@[Cu3-xPdx(BTC)2]n ......................................................................................... 122<br />
5.1 Introduction on the selection of metal type in MOFs ................................................. 123<br />
5.2 Preparation and Structure of the Cu/Pd-BTC_1-3 ....................................................... 126<br />
5.3 Compositional characterization and sorption properties of the prepared<br />
Cu/Pd-BTC_1-3 ........................................................................................................................... 130
III<br />
5.4 Synthesis, compositional characterization and sorption properties of<br />
Cu/Pd-BTC_4 ............................................................................................................................... 136<br />
5.5 Catalytic test reaction .............................................................................................................. 143<br />
5.6 Conclusions ................................................................................................................................... 146<br />
6 Summary and Outlook ...................................................................................................................... 147<br />
7 Experimental Section ........................................................................................................................ 150<br />
7.1 General methods ........................................................................................................................ 150<br />
7.1.1 X-ray Diffraction (XRD) ....................................................................................... 150<br />
7.1.2 FT-IR spectroscopy ................................................................................................ 151<br />
7.1.3 Nuclear Magnetic Resonance (NMR) Spectroscopy ................................ 153<br />
7.1.4 Thermogravimetric analyses (TGA)............................................................... 154<br />
7.1.5 Scanning Electron Microscopy (SEM) and Energy-dispersive X-ray<br />
spectroscopy (EDX)............................................................................................... 154<br />
7.1.6 Transmission electron microscope (TEM) and EDX ............................... 154<br />
7.1.7 Elemental Analysis / Atomic absorption spectroscopic (AAS) .......... 154<br />
7.1.8 Gas Sorption ............................................................................................................. 155<br />
7.1.9 X-ray absorption near edge structure (XANES)........................................ 157<br />
7.1.10 X-ray photoelectron spectroscopy (XPS)..................................................... 158<br />
7.1.11 High Performance Liquid Chromatography (HPLC) ............................... 158<br />
7.1.12 Catalytic studies ...................................................................................................... 159<br />
7.2 Experimental data on chapter 3........................................................................................... 160<br />
7.2.1 Synthesis of the ruthenium precursors ([Ru2(OOCR)4X] and<br />
[Ru2(OOCCH3)4]A).................................................................................................. 160<br />
7.2.2 Synthesis of Ru-MOFs [Ru3(BTC)2Xx]·Gg ...................................................... 168<br />
7.3 Experimental data on chapter 4........................................................................................... 173<br />
7.3.1 Synthesis of Ru-DEMOF samples (1a-1d, 2a-2d, 3a-3d, 4a-4c) .......... 173<br />
7.3.2 Catalytic reactions using Ru-DEMOFs as catalysts .................................. 177<br />
7.3.3 Synthesis of [Cu3(BTC)2]n (Cu-BTC)............................................................... 177
IV<br />
7.3.4 Synthesis of Cu-DEMOF samples (D1-8)...................................................... 178<br />
7.4 Experimental data on chapter 5........................................................................................... 186<br />
7.4.1 Synthesis of [Cu3-XPdx(BTC)2]n ......................................................................... 186<br />
7.4.2 Hydrogenation of PNP to PAP ........................................................................... 190<br />
7.5 Supplementary details in Outlook ...................................................................................... 192<br />
8 Bibliography.......................................................................................................................................... 194<br />
Appendix ........................................................................................................................................................... 205<br />
List of Publications<br />
List of Presentations<br />
Curriculum Vitae
V<br />
Abbreviations<br />
4-btapa<br />
5-Br-ip<br />
5-Br-ipH2<br />
5-NH2-ip<br />
5-NH2-ipH2<br />
5-OH-ip<br />
5-OH-ipH2<br />
AAS<br />
AcO<br />
AcOH<br />
BBR<br />
bdc<br />
BET<br />
bpy<br />
BTC<br />
BTT<br />
CP<br />
CPO<br />
CSA<br />
CUS<br />
DEMOFs<br />
DL<br />
DMF<br />
1,3,5-benzene tricarboxylic acid tris[N-(4-pyridyl)amide]<br />
5-bromoisophthalate<br />
5-bromoisophthalic acid<br />
5-aminoisophthalate<br />
5-aminoisophthalic acid<br />
5-hydroxyisophthalate<br />
5-hydroxyisophthalic acid<br />
atomic absorption spectrascopy<br />
acetate<br />
acetic acid<br />
building block replacement<br />
1,4-benzenddicarboxylate<br />
Brunauer-Emmett-Teller<br />
bipyridine<br />
1,3,5-benzenetricarboxylate<br />
1,3,5-benzenetristetrazolate<br />
coordination polymer<br />
coordination polymer from Oslo<br />
controlled secondary building unit approach<br />
coordinatively-unsaturated metal sites<br />
defect-engineered metal-organic framworks<br />
defect linker<br />
N,N-dimethylformamid
VI<br />
DMSO<br />
dobdc<br />
e.g.<br />
EA<br />
EDX<br />
EtOH<br />
EXAFS<br />
FT-IR<br />
GC<br />
H2ip<br />
H2pydc<br />
H3BTC<br />
HKUST<br />
HML<br />
HPLC<br />
i.e.<br />
IML<br />
ip<br />
IRMOF<br />
IUPAC<br />
MC<br />
mCUS<br />
MeOH<br />
MIL<br />
MOF<br />
dimethyl sulfoxide<br />
2,5-dioxido-1,4-benzenedicarboxylate<br />
exempli gratia (from latin = for example)<br />
elemental analysis<br />
energy-dispersive X-ray spectroscopy<br />
ethanol<br />
extended X-ray absorption fine structure<br />
fourier transformation infrared (spectroscopy)<br />
Gas chromatography<br />
isophthalic acid<br />
pyridine-3,5-dicarboxylic acid<br />
1,3,5-benzenetricarboxylic acid<br />
Hong Kong Unversity of Science & Technology<br />
heterostructural mixed-linker<br />
High performance liquid chromatography<br />
id est (from Latin = it is, namely)<br />
isostructural mixed-linker<br />
isophthalic<br />
isoreticular metal-organic framework<br />
International Union of Pure and Applied Chemistry<br />
mixed-component<br />
modified coordinatively-unsaturated metal sites<br />
methanol<br />
Matériaux de l′Institut Lavoisier<br />
metal-organic framework
VII<br />
MTV<br />
Mw<br />
NMR<br />
NP<br />
PAP<br />
PivO<br />
PivOH<br />
PNP<br />
PSM<br />
PW<br />
PXRD<br />
pydc<br />
pyz<br />
r.t.<br />
redox<br />
rion<br />
SALE<br />
SBET<br />
SBU<br />
SEM<br />
STP<br />
TEM<br />
TGA<br />
THF<br />
TML<br />
multivariate<br />
molecular weight<br />
nuclear magnetic resonance<br />
nano-particle<br />
p-aminophenol<br />
pivalate<br />
pivalic acid<br />
p-nitrophenol<br />
post-synthetic method<br />
paddlewheel<br />
powder X-ray diffraction<br />
pyridine-3,5-dicarboxylate<br />
pyrazine<br />
room temperature<br />
reduction-oxidation<br />
ionic radii<br />
solvent-assisted linker exchange<br />
BET surface area<br />
secondary building unit<br />
scanning electron microscopy<br />
standard temperature and pressure<br />
transmission electron microscopy<br />
thermal gravimetric analysis<br />
tetrahydrofuran<br />
truncated mixed-linker
VIII<br />
TOF<br />
UHV<br />
UiO<br />
UMCM<br />
vs<br />
WCA<br />
XANES<br />
XAS<br />
XPS<br />
ZIF<br />
turnover frequency<br />
ultra high vacuum<br />
Universitetet i Oslo<br />
University of Michigan Crystalline Material<br />
versus<br />
weakly coordinating anion<br />
X-ray absorption near edge structure<br />
X-ray absorption sepctroscopy<br />
X-ray photoelectron spectroscopy<br />
zeolitic imidazolate framework
1 Motivation<br />
Looking through the essential fields in nature and in our daily life, one can find that porous<br />
materials play an important role. For example, porous rocks can store water, petroleum<br />
and natural gas. Activated carbon as a prominent example of porous materials have been<br />
widely used in various applications involving purification of gas, gold and water, as well<br />
as filters in gas masks and respirators, etc. Another famous example is zeolites, which are<br />
broadly used as ion-exchange beds in domestic and commercial water purification and<br />
softening, catalysts in oil tracking, etc.<br />
As zeolite-like architectures, metal-organic frameworks (MOFs) represent a young class<br />
of hybrid inorganic-organic crystalline porous materials, formed from organic linkers and<br />
inorganic build blocks (metal nodes). Ability to tune the inorganic building blocks as well<br />
as the diverse characteristics of the organic moieties featured in MOFs ensures its great<br />
advantage in comparison with the conventional porous materials (e.g. zeolites and<br />
activated carbons), which attracted huge attentions over last decades. Nowadays, MOFs<br />
are also extensively investigated as porous materials promising for gas<br />
storage/separation, sensing, drug delivery and catalysis, etc.<br />
Various synthetic approaches applied to MOFs afford to achieve their rich diversity, high<br />
level of complexity and functionality. For example, reticular synthesis (versatile design of<br />
functionalized organic linkers), design of mixed-component MOFs via post-synthetic<br />
modification (including metal and linker exchange), or mixed-linker/metal copolymerization<br />
has attracted huge attention with this regard. To note, the coordinatively<br />
unsaturated metal sites (CUS) in MOFs play a key role in many applications, especially in<br />
enhanced catalytic activity and effective gas sorption/separation. Hence, increased<br />
complexity by means of mixed-component MOFs can be combined with the generation of<br />
defects around the metal centers, which could lead to more open metal sites, or in the case<br />
of clustering of the point defects, mesoporous MOFs can be obtained. Thus, it comes to the<br />
“so-called” defect-engineering MOFs (DEMOFs). This manner of advanced modification of<br />
MOFs holds enormous potential to optimize the materials properties beyond the
2 Chapter 1<br />
limitations of the (non-doped) parent MOFs. In particular, increased sorption capacity,<br />
selectivity and enhanced catalytic activity could be expected. Up to date, only limited<br />
reports have been dealing with the studies on DEMOFs and their application.<br />
Among the MOFs featuring CUSs and showing good performance on applications, HKUST-<br />
1 ([Cu3(BTC)2]n) is one of the widely and well investigated MOFs. Besides, its mixedvalence<br />
structural analogue [Ru3(BTC)2Yy]n (Y = counter-ions, 0≤y≤1.5) exhibits sufficient<br />
chemical and thermal stability, and can offer rich photo/redox chemistry. Hence, in this<br />
thesis those two kinds of MOFs with the general formula [M3(BTC)2]n have been chosen<br />
as candidates on the study of defect-engineering.<br />
However, before starting with the exploration of such intriguing DEMOFs, the formation<br />
of both “intrinsic” and “intentional” defects in MOFs should be wisely taken into account.<br />
Especially, in the case of [Ru3(BTC)2Yy]n, due to the kinetic reason, its formation should be<br />
carefully monitored. Hence, Chapter 3 in this thesis mainly focus on the parent<br />
[Ru3(BTC)2Yy]n for the study of possible intrinsic defects, optimized exclusion of the guest<br />
molecules and elaboration of mono-valence Ru analog of HKUST-1. Further, intentional<br />
introduction of defects to [Cu3(BTC)2]n and [Ru3(BTC)2Yy]n respectively by linker and/or<br />
metal doping will be worth investigating. Modifications of the metal sites, generation of<br />
(additional) accessible coordination sites as well as the complexity of the developed<br />
DEMOFs will be studied in detail in Chapters 4 and 5. Moreover, the impact of the defects<br />
engineering on gas sorption and catalysis properties of the resulting DEMOFs will be<br />
explored. It is expected that these study show a comprehensive picture on the DEMOF<br />
derivatives of the selected M-BTC structure and give us deep insights on the defectengineering<br />
of other MOFs.
2 General introduction<br />
The aim of this chapter is to give a general introduction on the research progress of metalorganic<br />
frameworks (MOFs) including the origin of MOFs, their chemistry, structural<br />
features, synthetic approaches, modification on the structure as well as their applications.<br />
2.1 Origin of MOFs - Coordination polymers<br />
In 1833, J. J. Berzelius firstly use the term “polymer” to describe any compound that could<br />
be formulated as consisting of multiple units of a basic building block. [1] Later, Werner for<br />
the first time, proposed the correct structure [Co(NH3)6]Cl3 for coordination compounds<br />
containing complex ions in 1893, which developed the groundwork for the study of<br />
coordination polymers (CPs). In 1916, to define dimers and trimers of various cobalt(II)<br />
ammine nitrates, the term “CPs” was firstly employed by Y. Shibata [2] and has been<br />
continuously used in the scientific literature since the 1950's. Moreover, the first review<br />
on CPs was published in 1964. [3] The International Union of Pure and Applied Chemistry<br />
(IUPAC) Red Book of inorganic nomenclature from 2005 gives the following definition of<br />
coordination compounds: “A coordination compound is any compound that contains a<br />
coordination entity. A coordination entity is an ion or neutral molecule that is composed of<br />
a central atom, usually that of a metal, to which is attached a surrounding array of atoms<br />
or groups of atoms, each of which is called a ligand”. [4] Consequently, CPs can be<br />
conceptually considered as coordination compounds with extended arrays structures of<br />
one, two or three dimensions (Figure 2.1). [5] Typically, CP consists of two central<br />
components: metal ions (serving as connectors) and ligands (serving as linkers). Apart<br />
from these two components, blocking ligands, counter-anions, non-bonding guests or<br />
template molecules can be also included (Figure 2.2). The number and orientation of the<br />
binding sites (i.e. coordination numbers and geometries) are the important<br />
characteristics of the connectors and linkers. Their combination in numerous ways via a<br />
self-assembly enables the formation of practically an infinite number of CPs (Figure 2.1).
4 Chapter 2<br />
For the synthesis of CPs, transition metals and lanthanides are often utilized as connectors.<br />
According to the type of the metal and its oxidation state, coordination numbers can vary<br />
from 2 to 7, resulting in a variety of coordination geometries such as linear, T- or Y-<br />
shaped, tetrahedral, square-planar, square-pyramidal, trigonal-bipyramidal, octahedral,<br />
trigonal-prismatic, pentagonal-bipyramidal and the corresponding distorted forms<br />
(Figure 2.2). In addition, metal-complexes might be also used as connectors instead of<br />
(naked) metal-ions. It has an advantage of offering the bond angles control and restricting<br />
the number of coordination sites via “ligand-regulation” of a connector, where chelating<br />
or macrocyclic ligands directly bound to a metal connector block the redundant sites and<br />
the linkers are left free for specific sites. [6]<br />
Figure 2.1. Schematic demonstration of the CP construction via the self-assembly of connector<br />
(metal nodes) and the simplest linker (ligands) in 1-3D.<br />
Figure 2.2. Components of CPs. Inspired by the report from Kitagawa, et al. [7]
Chapter 2 5<br />
On the other hand, linkers provide various connecting sites with tuned binding strength<br />
and directionality. Linkers utilized in the CP construction may be halides (F, Cl, Br and I),<br />
CN - and SCN - ions, [8-9] cyanometallate anions ([M(CN)x] n- ) as well as neutral, anionic and<br />
cationic organic ligands. Among all these ligands, halides as the smallest and simplest one<br />
are broadly employed to form quasi-1D halogen-bridged mixed-valence compounds (MX<br />
chains), which feature extensive physical properties. [10] Furthermore, halides can be well<br />
incorporated along with neutral organic ligands in the coordination frameworks. [11]<br />
Cyanometallate anions could perform various geometries, similar to the metal ions with<br />
coordination number from 2 to 7 mentioned above. With respect to the neutral organic<br />
ligands, pyrazine (pyz) and 4, 4’-bpy (bpy = bipyridine) are the most often used in the<br />
reports. [12] As to the anionic ligands, di-, tri-, tetra- and hexacarboxylate molecules are<br />
typically employed. [13-15] On the contrary, CPs with cationic ligands are not very common<br />
due to their low affinity for cationic metal ions. [16-17]<br />
The bonding interactions between connectors and linkers in the CPs are mainly<br />
coordination bonds. Additional weak interactions such as hydrogen and metal-metal<br />
bonds, π- π and CH- π, electrostatic and van der Waals interactions can also participate to<br />
construct the structure of CPs. Consequently, both robust and flexible networks could be<br />
made. Many CPs studied in the earlier stage (1 st generation) feature open voids, cavities<br />
or channels which are usually occupied by the solvent molecules or counter-anions. Such<br />
guests might be exchanged post-synthetically against other ions or solvents, what is of<br />
highly interest to study (host-guest chemistry, ion-exchange, etc.). [18-19] However,<br />
complete removal of the guests molecules in this type of polymers is accompanied with<br />
an irreversible structure collapse, what considerably restrict their application in the fields<br />
of gas storage and separation as a result of low structural rigidity and absence of<br />
permanent porosity. On the other hand, structural interpenetrations, in which the voids<br />
constructed by one framework are occupied by one or more other independent<br />
frameworks, [20] frequently happens in chemistry of CPs and might facilitate formation of<br />
robust structures. Providing structural rigidity, this way, however, often leads in<br />
considerable reduction of the pore sizes and precludes creation of highly porous<br />
frameworks. Therefore, in spite of the abundant study on this class of CPs (1 st generation)<br />
in the early stage (before 1990s), synthesis of coordination networks exhibiting<br />
permanent porosity was still an open question until the exploration of [Co2(4,4′-<br />
bpy)3(NO3)4]n(H2O)4 in 1997 by S. Kitagawa. [21] This compound featuring channeling
6 Chapter 2<br />
cavities is able to reversibly adsorb CH4, N2, and O2 in the pressure range of 1–36 atm<br />
without deformation of the crystal framework.
Chapter 2 7<br />
2.2 Definition, Chemistry and features of MOFs<br />
2.2.1 Definition and nomenclature of MOFs<br />
The IUPAC group recommends the following definition of MOFs: “A metal–organic<br />
framework, abbreviated to MOF, is a coordination network with organic ligands containing<br />
potential voids.” Moreover, the hierarchical terminology is also recommended, where the<br />
most general term is CP, followed by the coordination networks acting as a subset of CPs<br />
and MOFs, a further subset of coordination networks (Figure 2.3). [5] It is worth<br />
mentioning that other terms like “porous CPs” or “porous coordination network”, which<br />
have basically the same meaning as MOFs, are also present in many scientific publications.<br />
In addition, another term “hybrid inorganic-organic material” was occasionally used for<br />
MOFs, however is not recommended by the IUPAC group due to its imprecise description.<br />
Owing to the cumbersome work, the systematic nomenclature of MOFs has not been given<br />
yet. Nevertheless, assigning to some conceptually important compounds the trivial names<br />
or nicknames in accordance with place of their origin followed by a number, such as<br />
HKUST-1 (Hong Kong University of Science and Technology), MIL-53 (Matériaux de<br />
l′Institut Lavoisier) and UiO-66 (Universitetet i Oslo), is also acceptable.<br />
Figure 2.3. The hierarchical terminology of the CPs, coordination networks and MOFs based on<br />
the recommendations of the IUPAC group.
8 Chapter 2<br />
2.2.2 MOF features<br />
Advantages of MOFs combining the features of CPs and porous solids<br />
MOFs (i.e. porous coordination networks) could be considered like a combination of both<br />
CPs and porous solids. As a subclass of CPs, MOFs feature even more diverse and robust<br />
structures. The construction of MOFs is commonly realized by the connection of “rigid”<br />
secondary building units (SBUs) rather than the simple linking of node and spacer in<br />
coordination networks where usually single atoms are joined by ditopic linkers. On the<br />
other hand, the feature of being microporous compounds, which is very important<br />
motivation to design MOFs, should not be underrated. Classical porous solids including<br />
zeolites, silica, alumina, carbon-based materials, etc. are known in various research fields<br />
of not only chemistry but also physical and material science due to their versatile<br />
application related to separation, storage and heterogeneous catalysis. For example,<br />
zeolites can be effectively utilized as molecular sieves for adsorbent of gases and liquids,<br />
builders for the production of laundry detergents, etc. Moreover, the usage of activated<br />
carbon in air filters and gas masks is seen in our daily life. MOFs as a novel class of porous<br />
solids are expected to behave in a similar manner as other mentioned porous solids. In<br />
fact, they exhibit uniform pores or open channels which might be preserved upon careful<br />
removal of the guest molecules. Compared to the CPs of 1 st generation, this essential<br />
characteristic allows MOFs to hold huge potential for a wide variety of applications such<br />
as gas sorption/separation, [22-23] gas storage [24-26] and catalysis, [27-29] for which previously<br />
only conventional purely inorganic (e.g. zeolites, alumina, silica) or purely organic porous<br />
solids (e.g. activated carbons) were suitable.<br />
Features highlight 1 –Structure diversity and porosity<br />
As mentioned above, MOFs are constructed from metal nodes (also known as inorganic<br />
building blocks or SBUs) and multidentate organic linkers (e.g. carboxylates, [13, 30]<br />
azolates, [31-33] etc.). One of the common clusters, the octahedral Zn4O(CO2)6 cluster(Figure<br />
2.4) composed of four ZnO4 tetrahedra with a common vertex and six carboxylate C atoms<br />
can be as SBUs and further joined together by the benzene links, which leads to a 3D MOF<br />
Zn4O(bdc)3∙(DMF)8(C6H5Cl) (known as MOF-5, bdc = 1,4-benzenddicarboxylate, DMF =<br />
N,N-Dimethylformamid), where the vertices are the octahedral SBUs and the edges are<br />
the benzene struts. [18] The obtained framework exhibit high thermal stability(300 °C) and<br />
porosity (Brunauer-Emmett-Teller (BET) surface area well above 3500 m 2 /g). The same
Chapter 2 9<br />
inorganic SBU can be connected by distinct ditopic linkers to afford various materials with<br />
the same structural topology (so-called IRMOFs) featuring predetermined cavity size and<br />
functions (Figure2.5).[25, 34]<br />
Figure 2.4. Construction of the MOF-5 framework. Top, the Zn 4 O(CO 2 ) 6 cluster. Bottom, one of the<br />
cavities in the MOF-5 framework. Reprinted by permission from Macmillan Publishers Ltd:<br />
Nature, 402, 276-279, copyright 1999. [18]<br />
Consideration on the chemical and geometric attributes of the essential SBUs and linkers can<br />
afford prediction of the framework topology, and subsequently result in the design and targeted<br />
synthesis of a new class of porous materials featuring robust structures and high porosity.<br />
Transition-metal carboxylate clusters may serve as SBUs with different points of extension<br />
varying from 3 to 66. [30] In addition to the typical octahedral zinc acetate cluster (Zn 4 O(CO 2 ) 6 ) as<br />
SBU, one of the other metal cluster commonly employed as a build blocks in the MOF synthesis is<br />
square bimetallic PW (M 2 (CO 2 ) 4 ) (Figure 2.6), in which four carboxylates are connected to two<br />
metal centers. Each metal center is often capped by labile solvent molecules (such as H 2 O). A<br />
typical example composed of such building blocks is the 3D porous framework [Cu 3 (BTC) 2 ] n (also<br />
known as HKUST-1 [35] or MOF-199 [36] ) reported by Chui. et al. in 1999.
10 Chapter 2<br />
Figure 2.5. A series of isoreticular MOFs (IRMOFs). [34] Reprinted from Micropor. Mesopor.<br />
Mater.,73, J. L. C. Rowsell, O. M. Yaghi, Metal–organic frameworks: a new class of porous materials,<br />
3‐14. Copyright 2004, with permission from Elsevier.<br />
Figure 2.6. Square PW cluster (M 2 (CO 2 ) 4 )with two terminal ligand sites (left) and the structure of<br />
HKUST-1.<br />
Features highlight 2-Flexibility
Chapter 2 11<br />
Figure 2.7. a, Three classes of host materials categorized according to attributes of softness,<br />
hardness (rigidity) and regularity. The overlapping zone of the two stages indicates materials<br />
belonging to either of the ends. b, Classification of porous CPs into three categories. Reprinted by<br />
permission from Macmillan Publishers Ltd: Nature Chemistry, 1, 695–704, copyright 2009. [37]<br />
Besides features mentioned above (structural versatility and permanently porosity),<br />
MOFs might also be flexible. Kitagawa et. al classified porous CPs into three generations<br />
(Figure 2.7). [37-38] The 1 st generation, which have been earlier mentioned in this chapter,<br />
represents porous coordination networks, which are comparably labile and collapse upon<br />
removal of the guests from the pores. The 2 nd generation includes robust frameworks<br />
exhibiting permanent porosity (reversible adsorption/desorption of guest molecules)<br />
with complete preservation of the crystalline order. The 3 rd generation, identified as<br />
flexible or dynamic porous frameworks, is able to undergo defined (and reversible) phase<br />
transitions as a respond to such external stimuli as thermal, [39] , guest molecule<br />
adsorption/desorption, [40] mechanical stress, [41] or light. [42] However, such structural<br />
transitions do not lead to breaking of coordination bonds and the internal connectivity of
12 Chapter 2<br />
the material is retained. Materials undergoing such kinds of phase transitions are often<br />
called soft porous crystals. [37] The effect of large framework flexibility induced by specific<br />
host-guest interaction is also known as “breathing”. [43] One of the best-studied flexible<br />
systems is the MIL-53 system ([M(bdc)(OH)]n, M 3+ =Al 3+ , [44] Fe 3+ , [45] Cr 3+ , [46] Ga 3+ , [47]<br />
In 3+ , [48] Sc 3+ , [49] ). These frameworks demonstrate different crystal phases according to the<br />
activation state and the incorporation of guest molecules. Thus, after activation MIL-53<br />
reveals a high-temperature phase with large pores (lp), which can shrinks to a narrowpore<br />
phase (np) upon the adsorption of low amounts of polar molecules (Figure 2.8).<br />
Moreover, a closed-pore phase was observed after activation of MIL-53(Fe) [45] and MIL-<br />
53(Sc). [49] In addition to these famous MILs-53, some M2-PW based pillared-layered MOFs<br />
also exhibit certain degree of flexibility upon guest adsorption. [50-52]<br />
Figure 2.8.The different forms of MIL-53: (a) as synthesized (as); disordered terephthalic acid<br />
molecules lie within the tunnels; (b) high temperature (open), lp; (c) room temperature hydrated<br />
form (hydr.), np. Note the changes in the cell parameters during the thermal treatments<br />
Reproduced from Chem. Soc. Rev., 2008, 37, 191-214 with permission of The Royal Society of<br />
Chemistry. [53]<br />
Features highlight 3-Good thermal stability even good chemical stability<br />
Thermal stability of MOFs ranges from 250 °C to 500 °C. [25, 31, 54-55] . Chemically stable<br />
MOFs, however, are challenging to be made due to their susceptibility to linkdisplacement<br />
reactions under the treatment with solvents over extended periods of time.<br />
Zeolitic imidazolate framework ZIFs, in particular ZIF-8 (Zn(MIm)2, MIm = 2-<br />
methylimidazolate) is one of the prominent examples which reveals exceptional chemical<br />
stability. [31] Remarkably, the structure integrity is retained after immersion ZIF-8 into<br />
boiling methanol, benzene, or water for up to 7 days. Besides, its treatment in
Chapter 2 13<br />
concentrated sodium hydroxide at 100°C for 24 hours does not alter the framework.<br />
Another well-known example exhibiting high chemical stability is MOFs based on the<br />
Zr(IV) cuboctahedral SBUs. In fact, high acid (HCl, pH = 1) and base resistance (NaOH, pH<br />
= 14) of UiO-66 (Zr6O4(OH)4(bdc)6) and its NO2 - and Br - functionalized derivatives was<br />
observed. [54-55] Furthermore, a structure of pyrazolate-bridged MOF (Ni3(BTP)2; BTP3 - =<br />
4,4’,4’’-(benzene-1,3,5-triyl)tris(pyrazol-1-ide)) was fully preserved after treatment in<br />
aqueous solutions within a wide pH value range (from 2 to 14) at 100 °C for 2 weeks. [56]<br />
Thus, such MOFs featuring high chemical stability are promising to afford benefit of<br />
enhancing their performance in carbon dioxide capture from humid flue gas, pave the way<br />
of their applications to water-containing processes, etc.<br />
To summarize, characteristic features of MOFs include (i) well-ordered porous structures<br />
and designable channel surface functionalities, (ii) flexible, dynamic behavior in response<br />
to guest molecules, and (iii) good thermal stability and (in some cases) also chemical<br />
stability. It can be expected that the diverse chemistry of MOFs (i.e. huge variety of<br />
inorganic SBUs and organic linkers bearing distinct functionalities) can result in a wide<br />
range of different framework structures as well as in deliberate tuning of their properties,<br />
which eventually leads to their applications in various fields.
14 Chapter 2<br />
2.3 Synthetic approaches, modification and applications of MOFs<br />
2.3.1 Traditional synthesis approaches<br />
Figure 2.9. Overview of the synthetic methods applied to MOFs. Reprinted with permission from<br />
N. Stock and S. Biswas, Chem. Rev., 2012, 112, 933-969. Copyright (2012) American Chemical<br />
Society. [57]<br />
As has been earlier mentioned, self-assembly of various metal ions and organic linkers<br />
leads to a large variety of networks featuring high porosity. However, it should be noted,<br />
that MOFs formation is also strongly affected by diverse synthetic parameters and<br />
conditions, such as nature of metal-precursors along with structural characteristics of<br />
linkers, concentration and stoichiometry of the employed reagents, usage of modulator,<br />
kind of solvent(s) and pH of the reaction solution), heating source, reaction temperature,<br />
time, pressure, etc. Figure 2.9 summarizes various synthetic approaches reported so far<br />
for MOFs. Conventional methods imply usage of either room or elevated temperatures<br />
and solvothermal/hydrothermal conditions (i.e. closed vessels under autogenous<br />
pressure above the boiling point of the solvent [58] ) (Figure 2.9). In addition to typical<br />
electric heating, other synthetic approaches such as microwave heating, electrochemical,<br />
mechanochemical, ultrasonic methods have been also emerging(Figure 2.9) [57, 59] and<br />
resulted in materials with various particle sizes and properties. High-throughput methods
Chapter 2 15<br />
afford a good way to study synthesis of MOFs in a systematic way and under well-defined<br />
conditions. Scaling-up of the synthesis on industrial-scale has been also achieved for<br />
several MOFs. In particular, BASF produces Cu-BTC (Basolite ® C300), Fe-BTC (Basolite ®<br />
F300), MIL-53 (Basolite ® A100), and ZIF-8 (Basolite ® Z1200), which are commercial<br />
available through Sigma-Aldrich.<br />
2.3.2 Reticular synthesis<br />
Reticular chemistry is a commonly used synthesis approach in the earlier stage for the<br />
versatile design of expansion of MOF structure to generate ultrahigh porosity and large<br />
pore openings. [60] Isoreticular principle allows the vary of size and nature of a structure<br />
while the underlying topology is kept. After the exploration of MOF-5, Yaghi et al. obtained<br />
a series of isoreticular MOFs on the basis of MOF-5 (Figure 2.5). Indeed, one of these<br />
compounds, namely isoreticular MOF–6 (IRMOF-6, Figure 2.5.6), displays rather high<br />
methane storage capacity (155 cm 3 (STP) / cm 3 ] at 298 K and 36 atm.<br />
Figure 2.10. Isoreticular expansion of HKUST-1. From H. Furukawa, K. E. Cordova, M. O’Keeffe<br />
and O. M. Yaghi, Science, 2013, 341. [66] Reprinted with permission from AAAS.
16 Chapter 2<br />
Expansion of this structures (i.e. isoreticular series of HKUST-1) could be obtained via<br />
employing other tritopic linkers of various lengths such as TATB 3- (4,4’,4’’-(s-triazine-<br />
2,4,6-triyl-tribenzoate) [61] and BBC 3- (4,4’,4’’-(benzene-1,3,5-triyl-tris(benzene-4,1-<br />
diyl))tribenzoate), for example (Figure 2.10). [62] In facts, the cell volume of the largest<br />
reported member of this series (MOF-399 ([Cu3(BBC)2]n)) is 17.4 times than that of<br />
HKUST-1. Moreover, the isoreticular construction of MOFs to enlarge the pores is also<br />
implemented through the expansion of the original phenylene unit of MOF-74-M [63] or<br />
CPO-27-M (M2(dobdc), dobdc = 2,5-dioxido-1,4-benzenedicarboxylate; M = Mg, Mn, Fe,<br />
Co, Ni, Zn, etc.). [64-65]<br />
Synthesis of MOFs, especially reticular synthesis, has earlier mainly focused on the<br />
preparation of new frameworks with new topologies and open structures with high<br />
porosity which are aimed for the gas storage capacities such as hydrogen, methane and<br />
carbon dioxide. [25, 60] Nowadays, the applications of MOFs have been more widely<br />
explored, including some fields of physics and biology. Consequently, modification of<br />
MOFs towards targeted applications has been more widely developed as well.<br />
2.3.3 Way to the modification of MOFs<br />
Beyond the traditional synthesis approaches, controlled modifications of MOFs at the<br />
organic linkers and/or at the metal nodes, could be mainly realized in several approaches:<br />
2.3.3.1 Direct decoration on the utilized linkers<br />
Ligands are often decorated with various organic groups to provide guest-accessible<br />
functional sides. [67-69] For example, Kitagawa et al. reported [Cd(4-<br />
btapa)2(NO3)2]n∙6H2O∙2DMF (4-btapa = 1,3,5-benzene tricarboxylic acid tris[N-(4-<br />
pyridyl)amide]) framework with amide-functionalized linker, where the highly ordered<br />
amide groups play an important role in the interaction with the guest molecules. [68]<br />
Moreover, the material shows selective base catalytic activity in the Knoevenagel<br />
condensation reaction. Furthermore, introduction of the thioether side CH3SCH3CH3Schain<br />
to the 2,5-position of 1,4-bdc and its co-assembly with Zn(II) ions lead to porous<br />
cubic network [Zn4O(L)3], whose topology is the same as MOF-5. [69] The obtained material<br />
exhibits a notable sensing response to nitrobenzene in the form of fluorescence<br />
quenching. Besides, it is able to absorb HgCl2 from the ethanol solution at low
Chapter 2 17<br />
concentrations (e.g. 84 mg/L). The pre-functionalization method is, however, somehow<br />
limited because certain kinds of groups favor to coordinate to metal ions, which result<br />
into frameworks with completely blocked organic sides.<br />
2.3.3.2 Introduction of open metal sites<br />
Open metal sites are CUS where an actual coordination number of the metal center is<br />
lower than typically expected for its oxidation state, charge or actual ligand field. Such<br />
CUSs can serve as binding sites for certain guest molecules (hydrogen, methane, etc.) as<br />
well as catalytic active sites for particular reactions under Lewis acidic conditions. The<br />
most common method to obtain CUSs is to activate (i.e. heat under vacuum) MOFs to<br />
remove the metal-bound volatile species (e.g. water, DMF, methanol, etc.). Indeed, this is<br />
often a case for several well-known MOFs such as HKUST-1 ([Cu3(BTC)2]n) and other<br />
members of this family, as well as MOF-74 ([(M2(dobdc)H2O]n) (Figure 2.11). [70-71]<br />
Figure 2.11. Representation of the crystal structure of HKUST-1 as well as the generation of Cu-<br />
CUS at the PW units upon activation. Green, Cu atoms; red, O atoms; gray, C atoms. Hydrogen<br />
atoms are omitted for clarity.<br />
Apart from this conventional method, the unsaturated metal centers can be introduced by<br />
employing similar metal chelating dicarboxylates, [72-74] 2,2’-bipyridine-5,5’-dicarboxylate
18 Chapter 2<br />
(H2BPDC) [75] or other bridging ligands, [76] which are not part of the inorganic building<br />
blocks of a given framework. Moreover, MOFs with open metal sites featuring diverse or<br />
enhance property can be achieved by using other metal ions in place of those metal<br />
precursors used in the known MOFs. By directly employing metal precursors containing<br />
another metal-ions and the same linkers during the synthesis of MOFs, the formation of<br />
the isostructural MOFs is expected. For example, analogs of HKUST-1 with the general<br />
formula [M3(BTC)2]n where M =Zn, [77] Cr, [78] Ni, [79] Fe, [80] Mo, [81] and Ru [82] etc. were<br />
reported by serveal groups after the appearance of [Cu3(BTC)2]n. [35] These analogs of<br />
HKUST-1 behave rather different properties such as in gas sorption/selectivity. [78,<br />
83] Similarly, by varying the metal in the infinite inorganic rod-type SBUs utilized for the<br />
construction of MOF-74,([Zn2(dobdc)]n) [63] a series of isostructural M-MOF-74 with<br />
various divalent metal ions like Mg, Co, Ni, Mn, Cd, Cu and Fe were described. [84-88] Other<br />
families of the homologous structures prepared using the same principle are M-BTT (BTT<br />
= 1,3,5-benzenetristetrazolate, M = Mn, Fe, Co, Cu, Cd), [89-92] for example.<br />
2.3.3.3 Post-synthetic modification and beyond<br />
Post-synthetic method (PSM), where the modification of ligands or metal containing<br />
nodes is implemented after the formation of MOFs (Figure 2.12), offers an effective way<br />
to overcome the potential for functional-group interference during MOF assembly.<br />
Several research groups, in particular the group of Cohen, have investigated the<br />
modification of amino and aldehyde groups in MOFs via the formation of new covalent<br />
bonds (Figure 2.12 top). [93-100] Still, employing PSM, one can face the problem of the pore<br />
volume decrease (caused by the functionalization reaction), which can lead to the<br />
reduction of gas absorption capacity. Therefore, an optimized method called “postsynthetic<br />
deprotection” was developed (Figure 2.12 bottom). [101] In this case, an organic<br />
linker bearing protected or “masked” functional group is incorporated into a MOF under<br />
standard solvothermal conditions, and the protecting group is subsequently removed by<br />
a thermal [102-103] or light [98, 104] induced deprotection reaction to reveal the desired<br />
functionality. One of the earliest example was presented by Kitagawa with the term of<br />
“protection-complexation-deprotection” process. [102] During the protection step,<br />
hydroxyl group of the 2,5-dihydroxyterephthalic acid (H2dhybdc) was protected by acetyl<br />
group via acetylation to form the 2,5-diacetoxyterephthalic acid (H2dacobdc). In the<br />
complexation/deprotection step, a MOF with a layered-pillared structure was obtained by
Chapter 2 19<br />
the rection of H2dacobdc, bipyridine and Zn(II) in DMF, with the simultaneous removal of<br />
the acetoxyl groups completely. This strategy was found to be useful for preventing<br />
interpenetration, introducing functionality, and controlling pore diameter. [105]<br />
Figure 2.12. A general scheme illustrating the concept of post-synthetic modification (PSM) on<br />
organic likers or metal-containing nodes of MOFs. Top, covalent PSM; Middle, dative PSM; Bottom,<br />
PSD. Reprinted with permission from S. M. Cohen, Chem. Rev., 2012, 112, 970-1000. [101] . Copyright<br />
(2012) American Chemical Society.<br />
Moreover, dative PSM (Figure 2.12 middle) involves heterogeneous chemical reactions to<br />
functionalize preassembled MOF structures via modification of metal-containing nodes<br />
(SBUs) [106-107] or organic linkers [108] can be reached via the formation of dative (i.e. metalligand)<br />
bond. [101] One of the first representative studies on dative PSM was reported by<br />
Hupp et al. [106] It was found that axially bound DMF solvent molecules in the PW SBUs<br />
could be fully removed from the Zn(II) PW-derived MOF by heating under vacuum.<br />
Subsequently the desolvated MOF was treated with pyridine derivatives in CH2Cl2, leading<br />
to materials in which the axial sites left vacant on the SBUs can be bound with pyridine<br />
derivatives. Those obtained MOF materials demonstrated dependent H2 uptake on the<br />
pyridine species coordinated to the SBUs, indicating properties could be<br />
modulated/optimized by dative PSM. Férey and co-workers reported amine grafting on
20 Chapter 2<br />
Cr III CUSs of MIL-101, displaying enhanced activities in the Knoevenagel condensation of<br />
benzaldehyde and ethyl cyanoacetate.<br />
Beyond the above mentioned PSM approaches, numerous conceptually different postsynthesis<br />
routes have been emerging. Intriguing building block replacement (BBR), which<br />
involves replacement of key structural components of the MOF, opens up a very broad<br />
strategy for the synthesis of functionalized isostructural MOFs featuring gradient<br />
compositions and chemical properties. Solvent-assisted linker exchange (SALE), [109-113]<br />
which is also termed as “stepwise synthesis”, [114] , “bridging linker replacement”, [114] “postsynthetic<br />
ligand exchange”, [115] isomorphous ligand replacement, [116] , is one of the<br />
important method to achieve this kind of modification on MOFs. Conceptually, by the<br />
reaction of a parent MOF and a solution of a second linker, a daughter MOF retaining the<br />
parent MOF topology can be obtained. Besides, partial substitution of the metal ions in a<br />
given framework with other metal ions of similar size and coordination chemistry could<br />
be accomplished by the so-called “post-synthetic metal ion exchange”, [117] (also known as<br />
“transmetalation”, [118] “metal metathesis” [119] or “metal-ion exchange” [120-121] ). Kahr et al.<br />
obtained a series of mixed-metal material Mg/Ni-MOF-74 with various degrees of Ni 2+<br />
incorporation by the post-treatment of Mg-MOF-74 and Ni 2+ solution with weak acid. [122]<br />
These materials showed increased stability and improved accessible porosity compared<br />
with the parent Mg-MOF-74 and Ni-MOF-74.<br />
2.3.3.4 Mixed-component co-assembly MOFs<br />
In addition of the post-synthetic modification on MOFs, co-assembly mixed-component<br />
(MC) MOFs which is related to the co-crystallizing of linker or metal-nodes mixtures for<br />
the introduction of functionalization should not be overlooked. Several research groups<br />
reported simultaneous utilizing two or more functionalized linkers during synthesis<br />
yielding to the formation of mixed-linker MOFs (MIXMOFs) or multivariate MOFs (MTV-<br />
MOFs). [123-128] In fact, Yaghi et al. revealed that a number of linkers with distinct functional<br />
groups (up to eight) can be incorporated into MOF-5 within one phase (Figure 2.13). [123]<br />
Curiously, the properties of MTV-MOFs are not just simply a linear combination of those<br />
of the pure components. For instance, MTV-MOF-5-EHI, as a member of this series,<br />
demonstrates strikingly better selectivity for CO2/CO in comparison with its best samelink<br />
counterparts. Moreover, partial metal substitution can be achieved by directly<br />
copolymerization via mixed-metal solid solutions, [126, 129-135] where more than one type of
Chapter 2 21<br />
metal-precursors are employed to react with the organic linkers during the synthesis<br />
(Figure 2.14). For instance, partial substitution of Cu 2+ by Ru 3+[134] and Zn 2+[133] in the PWs<br />
of HKUST-1 were obtained by mixing the Cu-salt with the corresponding Ru-salt and Znsalt<br />
directly during the synthesis, respectively. Orcajo et al. prepared Co-doped MOF-5 via<br />
co-assembly of Co(NO3)2·6H2O, Zn(NO3)2·4H2O and H2bdc during the synthesis. This<br />
obtained material exhibited enhanced adsorption capacities for H2, CO2, and CH4 at high<br />
pressure in comparison with Co-free MOF-5.<br />
Figure 2.13. Schematic representation of MTV-MOF-5 structures containing up to eight different<br />
functionalities distributed in one phase. From H. Deng, C. J. Doonan, H. Furukawa, R. B. Ferreira, J.<br />
Towne, C. B. Knobler, B. Wang and O. M. Yaghi, Science, 2010, 327, 846-850. [123] Reprinted with<br />
permission from AAAS.
22 Chapter 2<br />
Figure 2.14. Schematic presentation of the metal-based solid solution approach by mixing two<br />
different metal centers during the synthesis. Inspired by Burrows. [126]<br />
2.3.3.5 Defect-engineered MOFs<br />
On the basis of the concept of mixed-component MOFs, a very new approach to introduce<br />
functionalized MOFs has been reported very recently. [136] This is related to generation of<br />
so-called “defect-engineering MOFs” (DEMOFs), where in most cases the CUSs are<br />
modified or generated through the incorporation of additional “defect” linkers,<br />
modulators or through post-synthetic treatment. [137] The distinction of DEMOFs mainly<br />
related to the degree of deviation of the local structure as well as the long-ranging<br />
ordering of a variable fraction of the linkers and metal nodes in comparison with the<br />
parent MOF. [138-143] However, this kind of deviation barely can be observed from MC-<br />
MOFs. Only intrinsic defect may be present in certain conditions. [144-145] Besides, another<br />
important features of DEMOFs which should not be overlooked is the correlation and<br />
clustering of defect sites. Goodwin et. al used a combination of measurements and<br />
demonstrated the controlled introduction of nanoscale correlated defects within a<br />
hafnium terephthalate MOF UiO-66. [146] In particular, Fischer et al. reported the<br />
incorporation of pyridine-3,5-dicarboxylate (pydc) into the HKUST-1 and its Ru analog<br />
(Ru-MOF). [138-139] Remarkably, doping pydc resulted in the formation of mCUSs in the<br />
obtained Ru-DEMOFs, in which along with the Ru 2+ -/Ru 3+ -species typically found in the<br />
parent Ru-MOF framework, reduced Ru δ+ -species (0 < δ < 2) were generated. Moreover,<br />
such Ru-mCUSs appeared to be responsible for the activity of Ru-DEMOFs in the CO<br />
sorption as well as the catalytic hydrogenation of olefins. [138] Furthermore, doping pydc<br />
or other similar defect linker (DL) such as 5-hydroxyisophthalic acid (5-OH-ip) into<br />
HKUST-1(Cu-MOF), the creation of mesopores in the final Cu-DEMOFs was observed<br />
dependent on the utilized Cu-precursors and the incorporated level of DL. [139] Due to
Chapter 2 23<br />
appealing perspectives of this method on CUSs modification/introduction, this method is<br />
expected to receive much attention in next years. This kind of modification of MOFs are<br />
also involved in this dissertation. Further details will come in Chapter 4 and 5.<br />
2.3.4 Application of MOFs<br />
What have been addressed above show rather a broad picture demonstrating that MOFs<br />
are attractive porous materials with a huge diversity of structures, functionalities, and<br />
facile modification. All these make MOFs very promising for a range of applications<br />
(Figure 2.15), [147] especially in gas storage, selective adsorption and separation.<br />
Hydrogen and methane are good candidates for on-board fuel. A tank loaded with porous<br />
absorbent allows gas to be stored at much lower pressure in comparison with the<br />
identical tank without an adsorbent. Due to the high porosity and well-defined structures,<br />
MOFs has gained significant attention being a new class of adsorbents. A lot of MOFs have<br />
been evaluated for gas storage such as hydrogen and methane, [24, 26] which provides a<br />
safer and more economical gas storage method. For example, MOF-5 has shown a rapid<br />
and fully-reversible H2 storage density (66 g L -1 at 77 K, 100 bar), [148] which is very close<br />
to the value observed for liquid hydrogen (71 g L -1 at 20.4 K, 1 bar). Later, it was found<br />
that most of the MOFs like MOF-5 demonstrate poor performance at 298 K due to rather<br />
weak interactions between H2 and the framework. However, remarkable enhancement of<br />
H2 adsorption enthalpy can be achieved by designing MOFs with CUSs, [65, 70, 89]<br />
catenation/interpenetration [149] or MOFs with heavy transition metals (e.g. Pd) which can<br />
afford spillover effect for hydrogen storage. [150] For instance, respectively designed<br />
Mn3[(Mn4Cl)3(BTT)8]2 bearing CUSs exhibits H2 uptake of 1.49 total wt% and 12.1 g L -1 at<br />
298 K and 90 bar, [89] what is 77% greater than that of compressed H2 under the same<br />
conditions. Furthermore, HKUST-1 and Ni2(dobdc) have also demonstrated high total<br />
volumetric methane uptakes at 35 bar (225 and 235 v/v, respectively). [26] Significantly,<br />
PCN-14 (Cu2(adip) (adip 4- = 5,5’-(9,10-anthracenediyl)di-isophthalate) containing Cu-<br />
CUSs is also one of the best reported so far MOFs for methane storage (230 v/v, 290K, 35<br />
bar). Note, that 35 bar is the maximum pressure achievable by most inexpensive singlestage<br />
compressors, [151] which is also a widely used standard pressure for evaluating<br />
adsorbents for adsorbed natural gas storage. Both rigid and flexible MOFs as well as MOF<br />
membranes can be utilized as adsorbents for selective gas adsorption on the basis of
24 Chapter 2<br />
adsorbate-surface interactions and/or size-exclusion (molecular sieving effect), such as<br />
selective adsorption of N2/O2,CO2/N2, CO2/H2, etc. [23, 152-156] Moreover, separation of<br />
alkane isotherms from natural gas is also able to be achieved by suitable design of<br />
MOFs. [22-23, 157-158]<br />
Figure 2.15. Widespread potential applications of MOFs. Reproduced from S. Chaemchuen, N. A.<br />
Kabir, K. Zhou and F. Verpoort, Chem. Soc. Rev., 2013, 42, 9304-9332, with permission of The Royal<br />
Society of Chemistry. [159]<br />
Another widely investigated direction of MOFs applications is catalysis. Size- and shapeselective<br />
catalytic behavior could be achieved by utilizing MOFs with suitable porosity and<br />
functional groups/sites. [68, 160] For instance, functionalized 3D MOF with amide groups,<br />
[Cd(4-btapa)2(NO3)2]n∙6H2O∙2DMF, demonstrates catalytic selectivity in the Knoevenagel<br />
condensation reaction due to the relationship between the size of the reactants and the<br />
pore window of the host. [68] Significantly, the presence of catalytically active transitionmetal<br />
centers (loaded nano-particles (NPs), grafted metal complex, or active metal sites)<br />
as well as the organic functional sites in MOFs also enable this kind of porous materials to<br />
be catalysts in a variety of reactions. [27-29, 161] It is typical, that CUSs in MOFs serve as<br />
Lewis-acid catalytic sites to speed up the reactions run under Lewis-acid conditions. [161]<br />
For example, both MIL-101([Cr3F(H2O)2O(bdc)3]) and HKUST-1(Cu3(BTC)2)n) featuring<br />
exposed CUSs have been reported as good catalysts for cyanosilylation of aldehydes. [162-<br />
163] Besides, Lin, Kim and Kaskel demonstrated applications of homochiral MOFs in
Chapter 2 25<br />
asymmetric catalysis. [164-166] Very recently, the application of MOFs as biomimetic<br />
catalysts has been reviewed as well. [167-168] Some researchers also exploit the advances of<br />
MOFs as photocatalysis. [169-170] Apart from these two highlighted fields, applications of<br />
MOFs are certainly studied also in magnetism (ferromagnetic, antiferromagnetic,<br />
ferromagnetic, frustration and canting properties), [171-173] proton [174-178] and electrical [179-<br />
181] conductivity, luminescence and sensors chemistry, [182-186] drug storage and<br />
delivery. [187-188] Thus, in the near future breakthroughs with the continual developments<br />
in these and new applications are expected.
3 Controlled secondary building unit approach to the<br />
formation of the isostructural Ru II,II and Ru II,III analogs of<br />
[M3(BTC)2]n<br />
Abstract<br />
Controlled secondary building unit approach (CSA) was employed to derive a series of<br />
ruthenium metal-organic frameworks (MOFs) of the general formula [Ru3(BTC)2Yy]n·G g<br />
(BTC = 1,3,5-benzenetricarboxylate; Y = counter-anion, G = guest molecules, 0 ≤ y ≤ 1.5),
Chapter 3 27<br />
which are structural analogs of [M3(BTC)2]n (M = Cu, Zn, Ni, Cr, Mo). As Ru-precursors for<br />
CSA mixed-valence [Ru2 II,III (OOCR)4X] and [Ru2 II,III (OOCCH3)4]A compounds, with various<br />
nature of the anions X and A (strong coordinating X (like Cl - ) and weakly coordinating A<br />
(like [BF4] - or [BPh4] - )) as well as alkyl groups at the carboxylate ligand R (R = CH3 or<br />
C(CH3)3 ), were employed. Additionally, [Ru2 II,II (OOCR)4] complexes without any counterions<br />
were tested as Ru-source for Ru-MOF preparation. Systematic studies were<br />
conducted and five phase-pure Ru-MOFs were obtained. The set of characterization data<br />
support indicated the analytical compositions and the structural analogy of the prepared<br />
Ru-MOFs with the [M3(BTC)2]n family. The oxidation state of the Ru-sites in the obtained<br />
solids was studied by the X-ray absorption near edge structure (XANES) spectroscopy.<br />
The chosen Ru-precursors, optimized synthetic and activation protocols allowed<br />
improvement of the overall crystallinity, purity (in terms of residual solvent molecules)<br />
and porosity of the Ru-MOF materials.
28 Chapter 3<br />
3.1 Preparation and investigation of the Ru II,III -analogs of [M3(BTC)2]n *<br />
3.1.1 The family of [M3(BTC)2]n<br />
Figure 3.1. 3D crystal structure of [Cu 3 (BTC) 2 ] n (Cu-HKUST-1) viewed along the (100) direction.<br />
Green, red and gray balls stand for Cu, O and C atoms, respectively. Hydrogen atoms are omitted<br />
for clarity.<br />
[Cu3(BTC)2]n (also known as HKUST-1 [35] or MOF-199 [36] , BTC = 1,3,5-<br />
benzenetricarboxylate), first reported by Chui et al. in 1999, represents one of the most<br />
well investigated MOFs synthesized at the early stages of MOF chemistry. The 3D<br />
structure of [Cu3(BTC)2]n, with the space group Fm-3m, features paddlewheel (PW)<br />
dicopper(II) tetracarboxylate building blocks where Cu II -ions adopt pseudo-octahedral<br />
coordination geometry with the axial sites occupied by H2O (Figure 3.1). These<br />
coordinated water molecules H2O can be easily removed by heating the samples under<br />
vacuum (i.e., activation) leading to exposed Cu II -ions, which subsequently could serve as<br />
active Lewis acid sites in catalytic reactions (Figure 3.2). [189-190] Moreover, the interaction<br />
* The main results of this part are covered in the following publication: W. Zhang, O. Kozachuk, R. A. Fischer,<br />
et al. Eur. J. Inorg. Chem. 2015, 3913–3920.
Chapter 3 29<br />
between gas molecules and such coordinatively unsaturated sites (CUS) center often<br />
enhance the general adsorption properties of the MOF materials. [191-192]<br />
Figure 3.2. Modification of the Cu-sites in Cu-HKUST-1 after activation (and i.e., formation of Cu-<br />
CUS) and substrate coordination. Green, red, gray and violet balls represent Cu, O, C atoms and<br />
substrate (either gas or liquid molecules), respectively.<br />
Given the presence of metal CUSs and the permanent porosity, a number of isostructural<br />
[M3(BTC)2]n frameworks with various 3d and 4d metal-ions (M = Mo, [81, 83] Cr, [78, 83] Fe, [80]<br />
Ni, [79, 83] Ru [82, 138] and Zn [77] ) were reported later. Among them, [Cr3(BTC)2]n featuring Cr II<br />
open metal sites exhibited reversible and highly-selective binding of O2. More<br />
interestingly, among this formally homologous series as suggested by the (simplified)<br />
general formula [M3(BTC)2]n, the Fe and Ru analogs (abbreviated hereafter as Fe-MOF and<br />
Ru-MOF) were found to possess mixed-valence M II,III PW units, which might be of great<br />
use due to their potential photo and redox properties. [193] However, Fe-MOF was reported<br />
with no measurable porosity while Ru-MOF presented quite high porosity as well as good<br />
thermal and chemical stability. In fact, as a consequence of the mixed-valence state, the<br />
actual chemical composition and microstructure of these (Fe, Ru)-MOFs turned out to be<br />
more sophisticated. Counter-ions (X) and strongly bound guest molecules (G) seem to be<br />
notoriously present even after activation. The incorporation of these components as a<br />
function of synthetic conditions must be taken into account. Thus, the empirical formula<br />
of these materials should be more precisely written as [M3(BTC)2Yy]n·G g.<br />
3.1.2 Background and the state-of-the-art in research on Ru-analogs of<br />
[M3(BTC)2]n<br />
Looking through all the reports, the parent material [Cu3(BTC)2]n (HKUST-1) can be<br />
obtained through solvothermal, [35] electrochemical [194] , microwave syntheses [195] and<br />
others [196-197] . However, the synthesis of the Ru-analog is far less investigated. [82, 193] The
30 Chapter 3<br />
formula of [Ru3 II,III (BTC)2Cl1.5]n was initially assigned and obtained either from RuCl3 or<br />
[Ru2(OOCCH3)4Cl]n. The powder X-ray diffraction (PXRD) data support an analogous<br />
structure as [Cu3 II,II (BTC)2]n. Element-analytical, magnetic, X-ray photoelectron<br />
spectroscopy (XPS) and probe molecule adsorption combined with IR spectroscopy<br />
pointed to a mixed-valence Ru2 II,III PW units as the framework’s nodes. The Cl - counterions<br />
are most likely strongly coordinated to the Ru-centers to balance the overall charge<br />
of the framework. This material shows both good chemical and thermal stability;<br />
however, the Ru-centers are partly occupied and coordinated Cl cannot be removed by<br />
standard activation protocols. Hence, the number of active sites for catalysis and gas<br />
sorption is obviously reduced. Later, another analog described as [Ru3(BTC)2][BTC]0.5 was<br />
reported by Dincă et al. [83] The authors employed [Ru2(OOCC(CH3)3)4(H2O)Cl] as<br />
ruthenium source. The absence of Cl - in the samples of [Ru3(BTC)2][BTC]0.5 was postulated<br />
based on elemental analysis data only, and extra framework BTC serving as counter-ion<br />
was suggested. This solid showed better Brunauer-Emmett-Teller (BET) surface area<br />
values compared to the [Ru3 II,III (BTC)2Y1.5]n prepared first in our group. However, the<br />
presence of guest molecules such as trimethyl-acetate or acetate (arising from CSA and/or<br />
synthetic conditions) in the structure still could not be unambiguously determined or<br />
ruled out. Thus, modification of the starting Ru-sources used for the synthesis seems to<br />
be interesting for tuning the metal sites (i.e., oxidation state and CUS), composition and<br />
stability of the HKUST-1 analogous Ru-MOFs, which in turn can have a profound impact<br />
on other properties such as porosity and catalysis, for instance.<br />
Previously [Ru3 II,III (BTC)2Y1.5]n has been studied where the mixed-valence Ru II,III state was<br />
characterized in particular by CO and CO2 adsorption monitored by the FT-IR<br />
spectroscopy at low temperature under ultra high vacuum (UHV) conditions. [198] Also, the<br />
co-assembly of BTC with pyridine-3,5-dicarboxylate (pydc) to yield mixed-component<br />
(linker-based) solid solution type samples of the formula [Ru3(BTC)2-x(pydc)xYy]n·G g was<br />
achieved. These so-called “defect engineered” Ru-MOFs showed interesting new<br />
properties (e.g. dissociative chemisorption of CO2). [138] Motivated by these promising<br />
results, it would be of great interest to investigate the synthesis of the parent Ru-MOF in<br />
more systematic fashion, dependence on Ru-precursors featured with diruthenium PW<br />
units (e.g. applying CSA), variation of the reaction conditions, work-up and activation in<br />
order to optimize the sample quality.
Chapter 3 31<br />
In this Chapter CSA is employed to systematically study the factors of synthetic conditions<br />
affecting the overall structure, composition and properties (in particular, thermal<br />
stability, porosity, etc.) of the Ru-based HKUST-1 analogous compounds (Scheme 7.3).<br />
Various Ru precursors, namely [Ru2(OOCR)4X] and [Ru2(OOCCH3)4]A, in which R = CH3 or<br />
C(CH3)3; X = Cl; A = BF4 or BPh4, were adopted as starting materials in order to modify the<br />
properties of the obtained Ru-MOF samples while maintaining the isoreticular<br />
relationship to HKUST-1. Switching from the -CH3 to bulkier R-group (e.g. -C(CH3)3)<br />
should increase the solubility of the polymeric ruthenium precursors, and, subsequently,<br />
would influence the kinetics of the MOF synthesis (better/faster nucleation and growth).<br />
On the other hand, employing weakly coordinating anions (WCA), like [BF4] - or [BPh4] - ,<br />
may allow modulation of the CUS within the Ru-MOF. Utilizing these counter-ions, A<br />
avoids the formation of a polymeric (insoluble) structure of the Ru precursors on one<br />
hand. On the other hand, it is anticipated that A being less prone to be incorporated into<br />
the framework via coordination to the Ru II,III -centers and, thus, may be removed by<br />
washing and activation of the samples. Unless, note, that H2O is always around in the<br />
solvothermal reactions and formation of -OH and its incorporation as component X must<br />
be also considered even in case of using WCA A, such as BF4 or BPh4.<br />
3.1.3 [Ru3(BTC)2Yy]n·G g obtained by CSA using [Ru2(OOCR)4X] and<br />
[Ru2(OOCCH3)4]A: synthesis and characterization<br />
3.1.3.1 CSA-precursors<br />
The Ru-precursors ([Ru2(OOCR)4X] and [Ru2(OOCR)4]A were prepared according to the<br />
literature (Scheme 7.1). [199-202] Characterization of all precursors confirmed the<br />
compositions and structures being expectedly analogous to the reported compounds. All<br />
structures consist of Ru2-clusters coordinated by four carboxylic groups. Thus, this kind<br />
of binuclear units (PWs) are similar to the building units in the [Cu3(BTC)2]n framework,<br />
affording the idea to construct the isostructural [Ru3(BTC)2]n by means of the CSA. The<br />
PXRD patterns of [Ru2(OOCCH3)4Cl] (SBU-a, R = CH3) showed the phase-purity of the<br />
compound (Figure 7.3). [203] Furthermore, following the well documented literature<br />
method, single crystals of [Ru2(OOCC(CH3)3)4(H2O)Cl](CH3OH) (SBU-b, R = C(CH3)3) were<br />
obtained. The cell parameters and other crystal structure data of SBU-b are presented in<br />
Table 7.1 and Figure 7.5. To note, the obtained crystallographic data are of superior
Intensity, a. u.<br />
32 Chapter 3<br />
quality as compared to the literature reference. Complementary characterizations such as<br />
1 H-NMR and PXRD reveal also high purity of SBU-b (Figures 7.6 and 7.7). In addition,<br />
[Ru2(OOCCH3)4(THF)2](BF4) (SBU-c) were obtained as the microcrystalline powder and<br />
was fully characterized (Figure 7.8). The synthesis of [Ru2(OOCCH3)4(H2O)2](BPh4) (SBUd)<br />
reported in the literature lead to the immediate decomposition of the product after<br />
filtration. [204] However, when we employed [Ru2(OOCCH3)4(H2O)2]2(SO4) instead of<br />
[Ru2(OOCCH3)4Cl] [199] as Ru-precursor, our target [Ru2(OOCCH3)4(H2O)2](BPh4) was<br />
successfully obtained (Figure 7.9).<br />
3.1.3.2 Synthesis, activation and thermal properties of Ru-MOF 1-4<br />
4<br />
3<br />
2<br />
1<br />
Cu-BTC_sim<br />
10 20 30 40 50<br />
2, degree<br />
Figure 3.3. PXRD patterns of the as-synthesized samples 1-4 as well as the simulated PXRD<br />
patterns of the reported [Cu 3 (BTC) 2 ](Cu-BTC_sim).
Chapter 3 33<br />
All Ru-MOFs 1-4 of the general formula [Ru3(BTC)2Yy]n·G g (Y = Cl, F, OH…; G = H2O,<br />
CH3COOH, (CH3)3CCOOH, H3BTC,…; 0 ≤ y ≤ 1.5) were obtained employing [Ru2(OOCR)4X]<br />
or [Ru2(OOCCH3)4]A precursors under solvothermal conditions in a similar way as we<br />
reported earlier. [82] The subsequent activation (i.e., removing of the incorporated<br />
solvent/guest molecules) was conducted at 150 °C for 24 h under dynamic vacuum (ca.<br />
10 -3 mbar). As revealed by the PXRD patterns (Figure 3.3), the prepared Ru-MOFs 1-4 are<br />
phase-pure crystalline solids that are isostructural to [Cu3(BTC)2]n. Ru-MOFs 2 and 4<br />
showed better crystallinity compared to the samples 1 and 3. The coordination of the<br />
carboxylic groups of framework BTC in the activated Ru-MOF samples is indicated by the<br />
strong-intensity bands at 1429 cm -1 and 1359 cm -1 in the FT-IR spectra (Figure 3.4).<br />
Notably, the Ru-MOFs obtained from [Ru2(OOCCH3)4]A, in which Y = [BF4] - and [BPh4] - ,<br />
show similar IR spectra with the other two samples. In other words, the incorporation of<br />
[BF4] - counter-ion in the structure of 3 can be ruled out, as no characteristic ν(B-F) band<br />
was observed at 1073 cm -1 . It is not possible to unambiguously determine the presence of<br />
[BPh4] - based only on the IR spectra because of the overlapping vibrations of [BPh4] - and<br />
BTC. Further analytical evidences in this respect will be discussed later.<br />
Figure 3.4. IR spectra of the activated Ru-MOFs 1-4.
34 Chapter 3<br />
After activating the Ru-MOFs, thermal gravimetric analysis (TGA) was performed<br />
demonstrating stability of the samples 1-4 up to 200 °C. Interestingly, Ru-MOF 4 is the<br />
most stable among the samples of discussed series and can be heated up to 250 °C without<br />
decomposition (Figure 3.5). Both as-synthesized and activated phases of the sample 1<br />
showed weight loss around 100 °C, which can be attributed to either a) loss of the residual<br />
coordinated solvent within the framework or b) adsorbed molecules such as water during<br />
transfer of the activated sample from the glovebox to the instrument. Ru-MOF 2 shows a<br />
slow weight decrease at low temperature range (30-150 °C), which is similar to the<br />
sample 1. Noteworthy, no similar observation was found in the curves of 3 and 4, meaning<br />
there are less residual solvent molecules trapped as compared to the other two samples<br />
1 and 2. Thus, it suggests that the pores of the frameworks 3 and 4 are more accessible<br />
and activation (desorption of the guest molecules) is facilitated.<br />
Figure 3.5. TG curves of the activated Ru-MOFs 1-4.
Intensity, a. u.<br />
Chapter 3 35<br />
3.1.3.3 Acid digestion and composition of the obtained Ru-MOFs 1-4<br />
4_ex<br />
4<br />
3_ex<br />
H(BTC)<br />
H(BPh 4<br />
)<br />
H(AcO)<br />
3<br />
2_ex<br />
H(PivO)<br />
2<br />
1_ex<br />
1<br />
10 8 6 4 2 0<br />
, ppm<br />
Figure 3.6. NMR spectra (measured in DCl/DMSO-d 6 ) of the Ru-MOF samples before (1-4) and<br />
after solvent exchange (1-4_ex) . All spectra were normalized by dividing the intensity of H(BTC),<br />
respectively. PivO = pivalate, AcO = acetate. Due to the sensitivity of water peak to the solution<br />
conditions, the proton resonance of H 3 O + varies here in the range of 4-6 ppm, dependent on the<br />
concentration of DCl in the total solution.<br />
To get more insight into the microstructures (i.e. analytical purity) and composition of the<br />
materials 1-4, 1 H-NMR analysis of the acid-digested (in DMSO-d6/DCl mixture) Ru-MOF<br />
samples was performed. Thus, the 1 H-NMR spectra revealed, that besides the signals at δ<br />
= 8.61 ppm attributed to the aromatic protons of BTC, one additional resonance at δ = 1.88<br />
ppm is seen and can be assigned to the protons of the residual acetic acid (AcOH) for all<br />
four Ru-MOFs samples (Figure 3.6). For Ru-MOF 2, the spectrum shows also an additional<br />
signal at δ = 1.05 ppm, which corresponds to the protons of the residual pivalic acid<br />
(PivOH) (Figure 3.7). The spectra suggest that the larger R-group (-C(CH3)3 instead of -<br />
CH3) in the Ru-SBU leads to more impurity in the synthesis of MOFs in addition to the
36 Chapter 3<br />
presence of the residual acetic acid in Ru-MOF 1, 3 and 4. Note, acetic acid has been a<br />
major component of the solvent medium during the synthesis. In the NMR spectrum of the<br />
sample 4 (Figure 7.11), signals assigned to trace amount of [BPh4] - were detected. This<br />
residue can be removed completely after washing and solvent exchange (for further<br />
explanation see the next section). The integrations of these signals for each Ru-MOF are<br />
listed in Table 3.1. In summary, Ru-MOF 3 and 4 contain lower amounts of the residual<br />
acetic acid. This again brings to the conclusion that these two samples are analytically<br />
purer as compared to the 1 and 2. Moreover, samples of 3 and 4 could be more<br />
quantitatively digested by the employed protocol in the same amount of solvent<br />
DCl/DMSO-d6 mixture, providing, therefore, more intense signals in the NMR spectra for<br />
each Ru-MOF sample.<br />
SBU-b<br />
2<br />
H(BTC)<br />
H(AcO) H(PivO)<br />
10 8 6 4 2 0<br />
, ppm<br />
Figure 3.7. Acid-digested (DCl) 1 H-NMR spectra of SBU-b (top) and 2 (bottom) (solvent: DMSOd<br />
6 ). The tiny peaks at around 0.8 and 1.2 ppm are due to H-grease.
Chapter 3 37<br />
Table 3.1. Comparison of the integrals of the 1 H NMR signals in the samples 1-4 (before solvent<br />
exchange) in comparison with 1-4_ex (after solvent exchange) to determine the linker to guest<br />
molecular ratios (BTC = 1, 3, 5-benzentricarboxylate, AcO = acetate, PivO= pivalate).<br />
Ru-MOFs H(BTC) : H(AcO) H(BTC) : H(PivO)<br />
1 1 : 2.4 -----<br />
1_ex 1 : 0.8 -----<br />
2 1 : 1.5 1 : 1.5<br />
2_ex 1 : 1.2 1 : 0.8<br />
3 1 : 1.6 -----<br />
3_ex 1 : 0.9 -----<br />
4 1 : 0.7 -----<br />
4_ex 1 : 0.7 -----<br />
3.1.4 Pre-activation by solvent exchange<br />
The presence of high amounts of acetic acid and pivalic acid arising from both, the Ru<br />
precursor and the reaction solvent mixture (which contains excess of acetic acid)<br />
apparently leads to partly pore-filling with the residual solvent (acid), which<br />
consequently may considerably affect or restrict the Ru-MOF properties. As revealed,<br />
these components cannot be removed completely regardless of the applied activation<br />
procedure (i.e. 150 °C for 24 h under dynamic vacuum (ca. 10 -3 )). Our attempts to slightly<br />
modify the reaction conditions, namely by reducing the quantity of acetic acid and/or<br />
using acetic acid free conditions yielded either amorphous products and/or prevented the<br />
substitution of RCCOOH in Ru-SBUs, affording just non-reacted starting materials (Figure<br />
7.12). Noteworthy, the reactants concentration in synthesis of the Ru-MOF 1 is quite<br />
crucial and attempting to vary the amounts of solvent with the same molar ratio of Ruprecursor<br />
and H3BTC was not so successful to get crystalline materials. Therefore, we<br />
conducted additional experimental studies directed to improve the activation procedure<br />
(i.e., minimize the amount of the strongly retained guest molecules) and, thus, improve<br />
the sample quality and access to the pores and open metal sites. For this reason we<br />
introduced an additional step to the activation procedure earlier mentioned. [138] Namely,
Intensity, a. u.<br />
38 Chapter 3<br />
the as-synthesized Ru-MOF samples were soaked in a large amount of (coordinatively)<br />
more inert solvent (water or ethanol, 80-100 ml) and stirred (for an average of 4 h) in<br />
order to wash out or replace strongly coordinated/adsorbed acetic or pivalic acid.<br />
Subsequently, the solvent was replaced by fresh portion and the samples were left<br />
standing overnight. This “solvent exchange” was repeated for each sample three times.<br />
Afterwards the samples were collected and dried under ambient conditions. The washed<br />
and dried samples (1-4_ex) were then “typically” treated again according to the<br />
established activation procedure for Ru-MOF: heating at 150 °C for 24 h under dynamic<br />
vacuum (ca. 10 -3 bar) in order to finally remove all adsorbed solvent and residual guests.<br />
3.1.5 Study of [Ru3(BTC)2Yy]n·G g after solvent exchange<br />
3.1.5.1 Phase purity and stability<br />
4-ex<br />
3-ex<br />
2-ex<br />
1-ex<br />
Cu-BTC_sim<br />
10 20 30 40 50<br />
2, degree<br />
Figure 3.8. PXRD patterns of the Ru-MOF samples after solvent exchange (1-4_ex) in comparison<br />
with the simulated patterns of Cu-HKUST-1 (Cu-BTC_sim).
Chapter 3 39<br />
Figure 3.9. IR spectra of the activated Ru-MOFs before (1-4) and after “solvent exchange” (1-<br />
4_ex).<br />
The PXRD patterns of the samples 1-4_ex match well with those of the [Cu3(BTC)2]n,<br />
suggesting fully preserved structural integrity of the Ru-frameworks after employed<br />
solvent exchange procedure (Figure 3.8). The IR spectra of the 1-4_ex further substantiate<br />
that the structure of the Ru-MOFs is retained (Figure 3.9). Both reveal the chemical<br />
stability of the 1-4 after solvent exchange. As expected, the amount of residual guest<br />
molecules (in this case, acetic acid, etc.) hosted by the frameworks of 1, 2 and 3 decreases<br />
considerably after applying an additional “solvent exchange”, which is clearly indicated<br />
by the comparison of the 1 H-NMR data of the digested and activated Ru-MOFs samples<br />
before (1-3) and after solvent exchange (1-3_ex) (Table 3.1 and Figure 3.6). In fact, the<br />
integration of the signals attributed to AcOH (δ = 1.88-1.93 ppm) in 1_ex and 1<br />
corresponds to 0.8:1 vs. 2.4:1. Notably, pivalic acid in 2 was removed even to a greater
40 Chapter 3<br />
extent than acetic acid (Table 3.1). At the same time, application of solvent exchange to<br />
Ru-MOF 4, containing the lowest amount of the guest molecules, does not have significant<br />
effect. The integration of the signals due to acetate protons reveals the same values,<br />
suggesting the amount of the acetate before and after exchanging is constant. Comparing<br />
all 1-4_ex samples, Ru-MOF 4 is the most promising one, with the lowest amount of guest<br />
molecules G. In addition, the tiny amount of residual [BPh4] - in 4 was removed after<br />
solvent exchange (Figure 3.6), as confirmed by the absence of the corresponding proton<br />
signals at 7.3 ppm.<br />
Figure 3.10. TG curves of the Ru-MOFs obtained from various Ru-SBUs before (1-4) and after (1-<br />
4_ex) solvent exchange procedure.<br />
From the TGA 1-4_ex samples (Figure 3.10) it is evident that these materials still possess<br />
good thermal stability after utilized solvent exchange and do not decompose until 200 °C.<br />
The shape of the TG curves of the 1_ex and 3_ex does not change after solvent exchange<br />
and suggest a decomposition temperature of 200 °C and 250 °C, respectively (Figure 3.10).<br />
In contrast, of the thermal stability of Ru-MOF 2 substantially decreases after solvent
Chapter 3 41<br />
exchange. This might stem from the presence of at least two different guest molecules<br />
(acetic acid and pivalic acid), meaning there are more molecules which sustain the whole<br />
framework in some extent through (weak) coordination compared to 1 and 3. Hence, the<br />
stability considerably decreases after solvent exchange while maintaining the structure<br />
(Figure 3.10). The same behavior is observed for Ru-MOF sample 4, most likely due to the<br />
removal of [BPh4] - counter-ions, which previously stabilized the framework (Figure 3.10).<br />
3.1.5.2 Composition determination<br />
To quantitatively determine the composition of Ru-MOFs 1-4_ex elemental analysis (EA)<br />
and Energy-dispersive X-ray spectroscopy (EDX) were subsequently performed. From<br />
our earlier reports, [82, 138] EA results indicated the molar ratio of Ru : Cl being 3 : 1.5. The<br />
XPS studies showed two different Ru-species (Ru III and Ru II ) as well as the presence of<br />
chlorine, suggesting Cl - being the major couter-ion to balance the charge of the<br />
framework. [82] As revealed in the present studies, the molar ratio of Ru : Cl in 1_ex slightly<br />
differs from the sample before solvent exchange (Ru : Cl = 3 : 1.5) [138] and equals to ~ 3 :<br />
1 (Table 3.2). The presence of chlorine was additionally confirmed by the EDX elemental<br />
mapping of Ru and Cl (Figure 3.11). It should be noted, that the analytically determined<br />
Ru-content (weight percentage by AAS) in the exchanged materials (1_ex) decreased from<br />
36.29 % to 30.45 %. [82, 138] Nevertheless, all characterizations proved preservation of<br />
crystallinity, porosity as well as thermal stability (by TGA). Based on these observations,<br />
together with the preserved BET surface area (SBET) observed after solvent exchange (see<br />
the details for next section on porosity), creation of the internal “structural defects” (i.e.<br />
missing of Ru-nodes) in the solvent exchanged sample 1_ex could be expected. As<br />
mentioned earlier, acetic acid is present in the discussed Ru-MOFs. The residual acetic<br />
acid (or acetate) could be included into frameworks mainly in three ways: i) it can be<br />
deprotonated and act as the counter-ion (coordinated to the Ru-center or sitting around<br />
the PW units) to compensate the charge of the [Ru2] 5+ units (Figure 3.12a); ii) inherent<br />
structural defects due to the incomplete substitution by the BTC within used Ru-SBUs<br />
(Figure 3.12b and c); iii) the acetic acid molecules (without deprotonation) might be<br />
accommodated within the pores of the frameworks. Activation procedure of the assynthesized<br />
samples could hardly direct remove the residue of the acetic acid in the<br />
framework. Nonetheless, application of additional solvent exchange method results in<br />
partly elimination of the residual acetic acid, and might consequently create the missing
42 Chapter 3<br />
Ru-nodes. Therefore, relatively reduced Ru-content is observed in the sample 1_ex. This<br />
kind of observation is mostly likely related to two possibilities: i) the strong stirring<br />
during the washing procedure; ii) slower substitution kinetics on the acetate coordinated<br />
Ru2 II,III -PW centers in comparison with Cu2-PW centers (rapid substitution kineties).<br />
Table 3.2. The obtained elemental analysis data and the calculated formula of 1-4_ex after solvent<br />
exchange. BTC = 1,3,5-benzenetricarboxylate, H 3 BTC = 1,3,5-benzenetricarboxylic acid, AcO =<br />
acetate, AcOH = acetic acid, PivOH =pivalic acid.<br />
Samples and Formula wt% C wt% H wt% Cl wt% F wt% Ru<br />
1_ex<br />
[Ru 3 (BTC) 2 Cl(AcO) 0.5 ] n·(AcOH) 1.5 (<br />
H 3 BTC) 0.1 (H 2 O) 4<br />
2-ex<br />
[Ru 3 (BTC) 2 Cl 1.2 (OH) 0.3 ] n·(H 3 BTC)<br />
0.15(AcOH) 2.4 (PivOH) 0.45<br />
3_ex<br />
[Ru 3 (BTC) 2 F 0.7 (OH) 0.8 ] n·(AcOH) 2.4<br />
(H 3 BTC) 0.5 (H 2 O) 3<br />
4_ex<br />
[Ru 3 (BTC) 2 (OH) 1.5 ] n·(H 3 BTC) 0.8 (A<br />
cOH) 1.4 (H 2 O) 3<br />
Found 27.26 1.65 3.41 - 30.45<br />
Cal. 28.5 2.31 3.67 - 31.40<br />
Found 31.57 2.11 4.16 - 29.27<br />
Cal. 32.14 2.18 4.31 - 30.73<br />
Found 29.28 1.28 - 1.09 24.18<br />
Cal. 31.30 2.44 - 1.27 29.90<br />
Found 32.15 1.60 - - 26.64<br />
Cal. 32.05 2.30 - - 28.90<br />
Figure 3.11. SEM image and the EDX elemental Ru- and Cl-map of the 1_ex sample.
Chapter 3 43<br />
Figure 3.12. Possible coordination of the acetic acid in the obtained Ru-BTC structures.<br />
In case of Ru-MOF 2, EDX elemental mapping images (Figure 3.13) also indicate the<br />
presence of chlorine. Besides, EA results indicated the Ru : Cl molar ratio to be ~ 3 : 1.2,<br />
suggesting Cl - serving here also as a major counter-ion to balance the charge of the [Ru2] 5+<br />
PW units, in analogy to 1. The EDX, EA results combined with the 1 H-NMR data of 2_ex<br />
match well with a formula [Ru3(BTC)2Cl1.2(OH)0.3]n·(H3BTC)0.15(AcOH)2.4·(PivOH)0.45,<br />
which includes a small amount of unreacted H3BTC, possibly residing in the pores rather<br />
than being deprotonated (as counter-ions). Although Ru-MOF 2_ex features higher<br />
crystallinity than other Ru-MOFs obtained from various Ru-SBUs, changing the R groups<br />
to -C(CH3)3 in the starting ruthenium precursor makes the whole system more<br />
complicated by introducing a new kind of impurity (pivalic acid) with respect to the<br />
analytical purity.<br />
Figure 3.13. SEM image and the EDX elemental maps for Ru and Cl of the 2_ex sample.<br />
In case of sample 3, the Ru : F molar ratio calculated from the EA data of the 3_ex is ~3 :<br />
0.7, suggesting the presence of strongly coordinated F - counter-ions. However, as the F-<br />
amount is rather low, the distribution of F could not be mapped via EDX (Figure 3.14).<br />
Still, this agrees with the absence of BF4 (monitored by IR) and can be explained by in situ
44 Chapter 3<br />
decomposition of [BF4] - into F - and BF3 during the MOF synthesis. As expected, lower<br />
amounts of counter-ions were observed compared to 1 and 2, when adopting WCAs as<br />
counter-ions in the starting Ru-SBU. Although, there are guest molecules in the material,<br />
the characterization of the Ru-solids after applied solvent exchange procedure indicates<br />
a better purity control (i.e. decrease of the types and amounts of guest molecules) than in<br />
case of 2.<br />
Figure 3.14. SEM image and the EDX elemental maps for Ru and F of the 3_ex sample.<br />
Based on the EA and NMR analyses as well as the assumption of the presence of [OH] - to<br />
help the charge balance, the empirical formula of Ru-MOF 4_ex matches well with<br />
[Ru3(BTC)2(OH)1.5]n·(H3BTC)0.8(AcOH)1.4(H2O)3. In this case our data support the<br />
conclusion that the strongly coordinating counter-ion Y of the final mixed-valence Ru-<br />
MOF may not stem from the employed Ru-SBU.<br />
3.1.5.3 Porosity comparison<br />
In order to compare the porosity of HKUST-1 and its Ru-analogs more reasonably due to<br />
the difference on the metal centers, SBET were calculated in the unit of m 2 /mmol according<br />
to the values in m 2 /g unit and the corresponding molecular weight(Mw) of the samples. In<br />
comparison with the experimental SBET value of HKUST-1 (1049 m 2 /mmol), the overall<br />
SBET of the activated Ru-MOF solids, especially, sample 1_ex and 4_ex is measured as 964<br />
and 941 m 2 /mmol, respectively, which suggest the good porosity of these two Ru-MOFs<br />
(Table 3.3 and Figure 3.15). In other words, the porosity of the Ru-MOFs is not affected<br />
after “solvent exchange”. As was indicated by the NMR studies mentioned earlier,<br />
adopting SBU-b as the Ru-precursor revealed a decreased amount of residual AcOH in the<br />
final framework. However, at the same time another kind of residue was introduced and<br />
the total amount of guest molecules do not decrease much after applying the solvent<br />
exchange procedure. Consequently, the BET surface area of the 2_ex amounts 718
Chapter 3 45<br />
m 2 /mmol (based on the N2 isotherm) and does not differ much in contrast to the sample<br />
before “solvent exchange” (i.e. sample 2). Notably, the thermal stability of 2_ex also<br />
slightly decreased after solvent exchange like SBET. Hence, the overall quality of this Ru-<br />
MOF analog is less convincing under the circumstances of this study. Interestingly, in case<br />
of 3_ex, however, an increase of the SBET has been observed from the N2 sorption<br />
isotherms (850 vs. 683 m 2 /mmol) (Table 3.3). The same increase of SBET has also been<br />
observed for the sample 4_ex (941 m 2 /mmol) in comparison with the value before (916<br />
m 2 /mmol), where the residual [BPh4] - has been removed via solvent exchange procedure<br />
although the amount of acetic acid does not differ. Thus, in particular for Ru-MOFs 1 and<br />
3, solvent exchange procedure proved to be a good method to reduce the amount of<br />
residual acid molecules. In both cases the thermal stability, crystallinity and porosity were<br />
preserved. For the material 4, solvent exchange is helpful to wash out the residual [BPh4] -<br />
counter anions to give access to the metal-sites, while keeping the thermal stability and<br />
porosity.<br />
Table 3.3. Comparison of the BET surface area (S BET ) of the Ru-MOFs before (1-4) and after<br />
solvent exchange (1-4_ex) in the unit of m 2 /g and m 2 /mmol. S BET in the unit of m 2 /mmol is<br />
calculated by S BET (m 2 /g) and the corresponding molecular weight (M w ) determined from both EA<br />
and 1 H NMR results. M w of 1-4_ex is obtained from the formula given in Table 3.2. The M w of<br />
sample 1-4 is derived from the difference of the guest molecules between the samples before and<br />
after solvent exchange, namely: M w (1) = M w (1_ex + 3.2 AcOH); M w (2) = M w (2_ex + 0.6 AcOH +<br />
0.2 PivOH); M w (3) = M w (3_ex + 1.4 AcOH); M w (4) = M w (4_ex + 0.13 BPh 4 ).<br />
samples S BET (m 2 /g) S BET (m 2 /mmol)<br />
1 958 1108<br />
1_ex 998 964<br />
2 851 888<br />
2_ex 728 718<br />
3 604 683<br />
3_ex 812 850<br />
4 840 916<br />
4_ex 897 941<br />
[Cu 3 (BTC) 2 ] n<br />
* theoretical accessible surface area.<br />
1734 [83]<br />
2153* [205]<br />
1049<br />
1301
deriv. normalized E)<br />
46 Chapter 3<br />
Figure 3.15. N 2 adsorption (solid symbols) and desorption (open symbols) isotherms (recorded<br />
at 77 K) of the Ru-MOFs obtained from different SBUs. 1-4: before solvent exchange; 1-4_ex: after<br />
solvent exchange. Squares: 1 and 1_ex; triangles: 2 and 2_ex; diamonds: 3 and 3_ex; circles: 4 and<br />
4_ex.<br />
3.1.5.4 Oxidation state study<br />
SBU-a<br />
RuCl 3<br />
SBU-b<br />
SBU-c<br />
Ru<br />
SBU-d<br />
RuO 2<br />
22100 22120 22140 22160<br />
energy, eV<br />
Figure 3.16. XANES spectra (derivative normalized absorption vs. energy) of the Ru-SBUs in<br />
comparison with Ru-standard samples (Ru, RuCl 3 and RuO 2 ).
deriv. normalized E)<br />
Chapter 3 47<br />
In order to gather information on the valence of the Ru-sites in the Ru-MOFs, comparative<br />
X-ray absorption spectroscopy (XAS) measurements were subsequently carried out. The<br />
derivative of the edge-jump energy positions of Ru (22117 eV) and RuO2 (22131 eV) can<br />
be used as standards, representing the oxidation states +0 and +4, respectively. On the<br />
other hand, according to the literature, the oxidation state of Ru-center in SBU-a reveals<br />
+2.5. [203] Hence, the same position of derived edge-jump energy (ca. 22124 eV) for SBU-a<br />
- -d clearly indicates the oxidation state of Ru-centre to be +2.5 (Figure 3.16). To note, Ru-<br />
MOF sample 1_ex with the edge jump position at 22126 eV matches well with its mixed<br />
oxidation state documented in the literature by UHV-IR technique with CO probe. [82] All<br />
the other Ru-MOFs samples (2-4_ex) exhibit their edge-jump at the range of 22123-22128<br />
eV, suggesting the mixed oxidation state of the Ru-centers in their structure as well<br />
(Figure 3.17). The study on deviation of local coordination environments within these Ru-<br />
MOFs due to the change of the counter-ions (in particular by Extended X-Ray Absorption<br />
Fine Structure (EXAFS)) is one of our further direction.<br />
Ru<br />
Ru NP<br />
3_ex<br />
4_ex<br />
RuO 2<br />
2_ex<br />
1_ex<br />
22100 22120 22140 22160<br />
energy, eV<br />
Figure 3.17. XANES spectra (derivative normalized absorption vs. energy) of Ru-MOFs obtained<br />
from various Ru-SBUs (1-4_ex) in comparison with Ru-standard samples (Ru, Ru NP and RuO 2 ).
48 Chapter 3<br />
3.1.6 Summary<br />
Applying CSA, a series of Ru-MOFs [Ru3(BTC)2Yy]n·G g were synthesized under<br />
solvothermal conditions and fully characterized(Table 3.4). Varying the R-group and<br />
nature of the counter-ion in the Ru-SBU ([Ru2(OOCR)4X] and [Ru2(OOCCH3)4]A), tuning<br />
(up to a certain extent) the local environment of the metal sites while retaining the same<br />
structure were achieved. Changing the R-group at the carboxylate in the Ru-SBU from -<br />
CH3 to bulkier –Rs, for example -C(CH3)3, leads to a striking improvement of the<br />
crystallinity of the final MOFs. However, considering the MOF compositions, the whole<br />
picture gets complicated, as residual guest molecules/species G could stem from both<br />
different R-groups in the Ru-SBU ([Ru2(OOCR)4X]) and solvents (including used<br />
carboxylic acids).<br />
Table 3.4. Summary of the preparation, composition and S BET in [Ru 3 (BTC) 2 Y y ] n·G g (1-4_ex). BTC<br />
= 1,3,5-benzenetricarboxylate, H 3 BTC = 1,3,5-benzenetricarboxylic acid, AcO = acetate, AcOH =<br />
acetic acid, PivOH =pivalic acid.<br />
sample<br />
employed SBUs for synthesis<br />
Counter-ions<br />
Y<br />
guest<br />
molecule G<br />
S BET<br />
(m 2 /mmol)<br />
1_ex<br />
SBU-a<br />
[Ru 2 (OOCCH 3 ) 4 Cl] n<br />
Cl, AcO<br />
1.5AcOH,<br />
0.1H 3 BTC,<br />
4H 2 O<br />
963<br />
2_ex<br />
SBU-b<br />
[Ru 2 (OOCC(CH 3 ) 3 ) 4 (H 2 O)Cl](CH 3 OH)<br />
Cl, OH<br />
2.4AcOH,<br />
0.15H 3 BTC,<br />
0.45PivOH<br />
718<br />
3_ex<br />
SBU-c<br />
[Ru 2 (OOCCH 3 ) 4 (THF) 2 ](BF 4 )<br />
F, OH<br />
2.4AcOH,<br />
0.5H 3 BTC,<br />
3H 2 O<br />
850<br />
4_ex<br />
SBU-d<br />
[Ru 2 (OOCCH 3 ) 4 (H 2 O) 2 ](BPh 4 )<br />
OH<br />
1.4AcOH,<br />
0.8H 3 BTC,<br />
3H 2 O<br />
941<br />
Besides this, the counter-ion Cl - is still present to compensate the charge of the [Ru2] 5+ PW<br />
units. Therefore, keeping the same R-group (-CH3) in the Ru-SBU, the Cl - counter-ions<br />
were replaced by WCAs. As expected, the ruthenium centers were modified through<br />
introducing more weakly coordinating anions. The more coordinatively active the<br />
counter-ions in the Ru-SBU are, the easier they coordinate to the metal centers in the final<br />
MOF structure. In spite of the fact, that BF4 was absent in the structure of 3_ex, F - was<br />
found in the material by EDX and EA. Therefore, Ru-SBUs with more stable WCA, like BPh4,
Chapter 3 49<br />
were investigated as well. Remarkably, by introducing [BPh4] - to the Ru-SBUs, MOF<br />
materials that do not include BPh4 were successfully obtained. Interestingly, the amount<br />
of residual included guest molecules G in the modified MOFs (3_ex and 4_ex) decreases<br />
compared to respective Ru-MOFs obtained starting from [Ru2(OOCR)4Cl]. In particular,<br />
sample 4_ex which contains the lowest amount of the guest molecules (acetic acid), is the<br />
first material obtained in the series of Ru-analogs of [Cu3(BTC)2]n that includes no strongly<br />
coordinating counter-ions X originating from the used Ru-SBUs.<br />
Solvent exchange procedure was introduced to achieve better removal of the guest<br />
molecules without damaging the framework integrity after activation. As expected, after<br />
applying such improved activation procedure, the counter-ions [BPh4] - and most of the<br />
guest and solvent molecules (like acetic acid) were washed out of the material while the<br />
crystallinity and thermal stability are retained. These studies are particularly crucial for<br />
the future investigation and elaboration of these materials for targeted applications, such<br />
as in selective sorption and catalysis. In summary, the synthesis of the Ru-MOF is still<br />
difficult to optimize further. Nevertheless, the investigations herein afford better<br />
understanding and directions towards not only HKUST-1 analogs but also other MOFs<br />
with PW SBU.
50 Chapter 3<br />
3.2 Elaboration of Ru II,II analog of [M3(BTC)2]n<br />
The results summarized in this Chapter 3.2 are initial studies directed to solve the<br />
remaining issues mentioned in Chapter 3.1 and to target Ru II, II analog of [M3(BTC)2]n.<br />
The study mentioned earlier (in Chapter 3.1) involving the investigation of Ru II,III analogs<br />
of HKUST-1 shows rather a complicated picture. As described, the residual acids and the<br />
inevitable counter-ions in the frameworks, to some extent, obstruct the porosity of the<br />
Ru-MOFs. One can imagine that the catalytic activity and the sorption properties of these<br />
materials can be definitely enhanced if the CUSs could be fully available without the<br />
additional coordination (“blocking”) by the counter-ions Y (Cl - , F - , OH - or AcO - , etc.). The<br />
pre-activation procedure (i.e. solvent exchange) helps largely to decrease the<br />
concentration of the incorporated guest molecules such as acetic acid. Getting rid of the<br />
acetic acid as well as the counter-ions are indeed of great importance to elaborate Ru II,II<br />
analog of [M3(BTC)2]n in which the Ru-centers would be the same (in terms of oxidation<br />
state and coordination geometry) as Cu sites in Cu-HKUST-1. One approach to improve<br />
the situation could be the strict exclusion of any additional carboxylic acid as component<br />
of the solvothermal reaction medium. Acid catalysis seems to be needed to facilitate the<br />
coordination equilibria and kinetics of the substitution chemistry at the Ru-centres.<br />
However, every attempt in this direction has not been successful so far (Figure 7.12). On<br />
the other hand, the requirement of avoiding the substitution inert mixed valence Ru II,III -<br />
SBUs for CSA and moving to the Ru II,II -SBUs as well as the strict exclusion of redoxchemistry<br />
(inert conditions) together with any source of coordinating counter-ions Y is<br />
another way to sort out the complexity of the coordination environment (i.e. mixed<br />
valences of Ru centers, residual acids from the starting reactant-solvent and/or the<br />
starting precursors) of the Ru-analogs of HKUST-1.<br />
3.2.1 Synthesis and characterization of SBU-e and Ru-MOF 5<br />
Ru II,II -SBU ([Ru2(OOCCH3)4],SBU-e) was obtained from a blue solution of ruthenium(III)<br />
chloride according to the reported method. [206] The cell parameters obtained from the<br />
single crystal XRD measurements of [Ru2(OOCCH3)4](THF)2 (crystallized from the hot<br />
THF solution) are in a good agreement with the corresponding values communicated in<br />
the literature (Table 7.2). [207] As appeared, prepared complex is air sensitive and loses its<br />
crystallinity after solvent de-coordination. Nonetheless, the FT-IR bands of the symmetric
Intensity, a. u.<br />
Chapter 3 51<br />
and asymmetric COO - vibrations at 1425 and 1541 cm -1 , respectively, match well with the<br />
reported values (Figure 7.10). [82, 208]<br />
Cu-BTC_sim<br />
Cu-BTC_ht<br />
5<br />
Ru II, III -BTC<br />
8 12 16 20 24 28<br />
2, degree<br />
Figure 3.18. PXRD patterns of the activated Ru II,III -BTC 1 and sample 5 in comparison with<br />
simulated patterns of the as-synthesized (Cu-BTC_sim) and activated Cu-BTC (Cu-BTC_ht).<br />
Consequently, degassed solvents (H2O and acetic acid) and inert conditions (Ar<br />
atmosphere) were utilized to synthesize Ru-MOF 5. The PXRD patterns of the activated<br />
mixed-valence Ru II,III -BTC sample obtained in our earlier reports [82, 208] exhibit a little shift<br />
of the peaks in comparison with the simulated PXRD patterns of the Cu-BTC_sim, although<br />
the overall structural integrity is fully preserved. This slight shift stem mainly from the<br />
substitution of the copper-ions by ruthenium-ions (which are of different radii) at the PW<br />
SBUs of the MOF. The PXRD patterns of the prepared here activated sample 5 are in a good<br />
accordance with respective PXRD data of both reported earlier Ru II,III -BTC (Ru-MOF 1)<br />
and Cu-BTC_sim(Figure 3.18), providing a good indication for the phase-purity of the<br />
prepared solid. Furthermore, the IR spectra of the synthesized sample 5 matches well
52 Chapter 3<br />
with that of the Ru II,III -BTC (Figure 3.19). The bands corresponding to the νs(COO) and<br />
νas(COO) vibrations appear at 1359 cm -1 and 1429cm -1 , respectively, suggesting the<br />
coordination of the carboxylate groups of framework BTC. However, presence of<br />
unreacted acetic acid and H3BTC cannot be strictly excluded from IR, as the bands<br />
stemming from C=O stretching in Ru-MOF samples is too small to be distinguished. The<br />
1 H-NMR spectrum of acid-digest sample 5 displays peaks at 8.60 and 1.86 ppm (Figure<br />
7.13). The former resonance is originated from the aromatic protons of BTC. However, the<br />
latter one can be attributed to the protons of acetate, suggesting the presence of AcO(H)<br />
in the obtained sample.<br />
H 3<br />
BTC<br />
(C=O)<br />
Ru II,II<br />
2 (OOCCH 3 ) 4<br />
5<br />
Ru II, III -BTC<br />
4000 3500 3000 2500 2000 1500 1000 500<br />
wavenumber, cm -1<br />
Figure 3.19. IR spectra of the Ru-BTC 5 in comparison with Ru II,III -BTC 1, [Ru 2 (OOCCH 3 ) 4 ] and<br />
H 3 BTC. The vertical dash line corresponds to the position of ν(C=O) bands.
Chapter 3 53<br />
3.2.2 Investigation on the Ru oxidation state and porosity of Ru-MOF 5<br />
To get more information on the oxidation state of Ru-centers in the obtained sample 5,<br />
XANES spectra on sample 5, Ru II,III -BTC 1, used Ru-precursors (SBU-a and -e) and RuCl3<br />
were subsequently recorded. Due to the differences in position of edge jump different<br />
valences of Ru, the oxidation state of Ru-centers in the MOF structure can be concluded<br />
from the position of the highest peak in the plot of derivative normalized absorption vs.<br />
energy. As illustrated by the Figure 3.20, Ru II,III -BTC 1 shows an edge jump position<br />
between RuCl3 and its starting precursor SBU-a, indicating its mixed valence state, as<br />
documented earlier. [82] To remark, only Ru II was found in the SBU-e. [207] Thus, the same<br />
edge jump position observed in the XANES spectra of the sample 5 suggests the presence<br />
of Ru II -center in the framework structure (Figure 3.20). Consequently, the obtained solid<br />
5 should feature the exact Ru2-PWs as that in HKUST-1 without any counter-ions around.<br />
In the fact, EA results do not reveal the presence of any Cl in the sample Ru-MOF 5, ruling<br />
out the existence of Cl - and RuCl3 in both SBU-e employed during the synthesis and the<br />
obtained solid Ru-MOF 5. A formula of [Ru3(BTC)2]n∙(AcOH)2.3 match well with the<br />
obtained EA results, which could be another sign of the absence of counter-ions. In<br />
comparison with Ru II,III -BTC (1-4) described in Chapter 3.1, the obtained framework turns<br />
to be simpler in the absence any counter-ions, although the presence of acetic acid cannot<br />
be avoided. Furthermore, N2 sorption isotherms collected at 77 K for Ru-MOF 5<br />
demonstrate type I isotherm (Figure 3.21), indicating the microporosity of this material.<br />
Given the greater bulk density of Ru-BTC than Cu-BTC and in order to have a better<br />
comparison with HKUST-1, SBET is calculated in the unit of m 2 /mmol. Thus, SBET of Ru-MOF<br />
5 amounts to 1173 m 2 /mmol, which is quite comparable with the reported value of Cu-<br />
BTC (1049 m 2 /mmol), [83] indicating the same accessibility of Ru-centers as Cu-sites.<br />
Moreover, the axial positions of the diruthemium PW units in the synthesized Ru II,II -BTC<br />
(5) are expected to be open compared to the Ru II,III -BTC, where the presence of counterions<br />
(Cl - , OH - , AcO - ) is needed to balance the charge of [Ru2] 5+ units. The considerably<br />
higher BET surface area (SBET) of Ru II,II -BTC 5 (1371 m 2 /g) than that respective values<br />
reported for Ru II,III -BTC (704-1180 m 2 /g) [82-83, 138, 208] further supports an assumption on<br />
availability of Ru-CUSs in Ru II,II -BTC 5.
54 Chapter 3<br />
Figure 3.20. (a) XANES spectra of the Ru II,III -BTC 1 and Ru II,II -BTC (5) in comparison with<br />
correspondingly employed Ru-precursors (SBU-a and –e) and the commonly used reference<br />
(RuCl 3 ); (b) XANES spectra of Ru II,II -BTC (5) and the employed precursor Ru II,II -SBU<br />
([Ru 2 (OOCCH 3 ) 4 ],SBU-e). The vertical line stands for the same position of edge jump.
V, cm 3 /g<br />
Chapter 3 55<br />
400<br />
350<br />
300<br />
250<br />
200<br />
150<br />
100<br />
/ Ru II, II -BTC<br />
/ Ru II, III -BTC<br />
50<br />
0<br />
0.0 0.2 0.4 0.6 0.8 1.0<br />
relative pressure, p/p 0<br />
Figure 3.21. N 2 adsorption (solid symbols) and desorption (open symbols) isotherms recorded at<br />
77K for the activated Ru II,III -BTC 1 and Ru II,II -BTC (5). Violet circle- Ru II,II -BTC; orange triangle-<br />
Ru II,III -BTC.<br />
3.2.3 Conclusions<br />
Moving from the usage of the mixed-valence Ru II,III -SBUs to the mono-valence Ru II,II -SBU<br />
in CSA, a Ru-analog ([Ru3(BTC)2]n∙(AcOH)2.3) of [Cu3(BTC)2]n has been obtained and<br />
characterized. Interestingly, XANES spectra suggest Ru II,II sites being present in the<br />
structure of the obtained sample 5. Moreover, the BET surface area of this material is the<br />
highest (1173 m 2 /mmol) among of all reported so far Ru-BTC MOFs and quite comparable<br />
with that of HKUST-1 (1049 m 2 /mmol). Thus, Ru II,II -BTC hold a huge perspectives for<br />
various applications in sorption and catalysis. Even more, obtained results are important<br />
for the following studies on related but more complex defect-engineered Ru-MOFs (see<br />
Chapter 4), and elaborated here Ru II,II -SBU is a good candidate for the synthesis of Rubased<br />
MOFs.
4 Linker-based MOF solid solutions: Defect-Engineered MOFs<br />
(DEMOFs) †<br />
Abstract: Employing the mixed-linker solid solution approach, various functionalized ditopic<br />
isophthalate (ip) defect generating linkers denoted as 5-X-ipH2, with X = OH (1), H<br />
(2), NH2 (3), Br (4) have been introduced into [Cu3(BTC)2] (HKUST-1) as well as its mixedvalence<br />
ruthenium-analogue to yield DEMOFs (DE = “defect-engineered”) of the general<br />
empirical formula [M3(BTC)2-x(5-X-ip)xYy]n (M = Ru or Cu, Y = counter-ions, 0 ≤ y ≤ 1.5).<br />
The framework incorporation of 5-X-ip into DEMOFs has been confirmed by a number of<br />
† Most work of this chapter has been covered in the accepted manuscript: W. Zhang, M. Kauer, et al. R. A.<br />
Fischer, Chem. Eur. J. 2016.
Chapter 4 57<br />
techniques. Interestingly, Ru-DEMOF (1c) with 32% framework incorporated 5-OH-ip<br />
reveals the highest BET surface area (1300 m 2 /g, N2 adsorption, 77 K) among all related<br />
samples (including the parent framework [Ru3(BTC)2Yy]n). The characterization data are<br />
consistent with two kinds of structural defects induced by 5-X-ip framework<br />
incorporation: type A, modified paddlewheel nodes featuring reduced metal sites and<br />
type B, missing nodes leading to enhanced porosity. Their relative abundances depend on<br />
the choice of the functional group X in the DLs and its doping level. The defects A and B in<br />
Ru-DEMOFs appear also to play a key role in sorption of small molecules (i.e., CO2, CO, H2)<br />
as well as for the catalytic properties of the samples (i.e., ethylene dimerization and Paal-<br />
Knorr reaction). In addition, synthetic parameters such as anions from the metal salts and<br />
the solvent can also influence the formation of Cu-DEMOFs as well as the generation of<br />
defects.
58 Chapter 4<br />
4.1 Introduction<br />
4.1.1 Solid solutions<br />
Among the well-known mixed-component MOFs, the class of MOF solid solutions (also<br />
known as molecular substitutional alloys) attract huge attention. It implies MOFs where to<br />
two or more types of the related components (either linkers, metals, or both) are<br />
randomly mixed within single-phased framework. Remarkably, this often allows the fine<br />
modulation of the MOF’s functionalities and properties. Considering the nature of the<br />
mixed components, MOF solid solutions could be sub-divided mainly into two groups:<br />
linker-based and metal-based MOF solid solutions. The first group covers MOF solids<br />
where two or more homologous linkers (usually of similar size and functionality) are<br />
integrated in various proportions while the structural integrity of MOF is preserved. The<br />
metal-based MOF solid solutions will be discussed in details in Chapter 5 and involve<br />
mixed-metal frameworks where ions of one metal type is partly isomorphous substituted<br />
by the other metal ions.<br />
Figure 4.1. Mixed-linker approaches to the formation of MOF solid solutions. Magenta balls, metal<br />
nodes; cyan sticks, parent linker; green sticks, isostructural mixed-linker; wine short sticks,<br />
truncated mixed-linker; violet sticks, heterostructural mixed-linker. Inspired by the reports of<br />
Bunck [127] and Fang et al. [137]<br />
Approaches for the synthesis of linker-based MOF solid solutions go basically into three<br />
directions depending on the utilized linker mixtures (Figure 4.1): [127]<br />
i) isostructural mixed-linker (IML) approach where mixed linkers feature identical linking<br />
geometry. [123-124, 209-212]
Chapter 4 59<br />
This is the most straightforward way and commonly used to incorporate some specific<br />
functionality, decorate the walls of a framework with particular (active) organic groups .<br />
Thus, Yaghi’s multivariate MOFs (MTV-MOF-5) are typical representatives of such solid<br />
solutions. [123] In fact, by mixing the terephthalic acid and its derivatives in various<br />
combinations, eighteen single phased MTV-MOFs-5 were prepared and, remarkably,<br />
demonstrated the enhancement of H2 storage capacity as well as adsorption selectivity for<br />
CO2 over CO. Furthermore, Baiker et al. reported mixed-linker amine-functionalized MOFs<br />
(MIXMOFs) with the general formula Zn4O(bdc)x(abdc)3–x (bdc = benzene-1,4-<br />
dicarboxylate; abdc = 2-aminobenzene-1,4-dicarboxylate). Notably, obtained solid<br />
solution materials could be used as both nucleophilic catalysts [124] and support to<br />
immobilize Pd-species for Pd-catalyzed cross-coupling reactions. [212]<br />
ii) truncated mixed-linker (TML) approach, in which one linker is truncated in comparison<br />
with the other.<br />
Figure 4.2. Schematic illustration of the formation of the MOF-5 analogs: spng-MOF-5 and pmg-<br />
MOF-5. Reprinted with permission from K. M. Choi, H. J. Jeon, J. K. Kang and O. M. Yaghi, J. Am.<br />
Chem. Soc., 2011, 133, 11920-11923. Copyright (2011) American Chemical Society. [215]<br />
This strategy is strongly related to the modulation approach, whereby a monocarboxylic<br />
acid is commonly added during the MOF synthesis to influence crystal growth and<br />
morphology. For instance, Kitagawa et al. used acetic acid as a modulator to directly affect<br />
the coordination equilibrium, which in turn controls the crystal growth of nanosized
60 Chapter 4<br />
framework [Cu2(ndc)2(dabco)]n (ndc=1,4-naphthalene dicarboxylate; dabco=1,4-<br />
diazabicyclo[2.2.2]octane). [213] Subsequently, similar morphological control of<br />
[Cu3(BTC)2]n (BTC = 1,3,5-benzenetricarboxylate) from octahedral to cuboctahedral to<br />
cubic by addition of lauric acid has been achieved. [214] Moreover, by utilizing various<br />
amounts of dodecyloxybenzoic acid, Yaghi and co-workers have modified the crystals of<br />
MOF-5 to develop isostructural sponge-/pomegranate- like crystal analogs featuring<br />
meso- and macropores, respectively(Figure 4.2). [215]<br />
iii) heterostructural mixed-linker (HML) strategy, where the employed mixed linkers bear<br />
different linkage geometries. [142, 216-219]<br />
UMCM-1 (University of Michigan Crystalline Material-1) reported by Matzger et al. is a<br />
first rigorous example derived following this approach by the usage of dicarboxylate and<br />
tricarboxylate linkers. This MOF contains 3.1 nm mesoporous hexagonal channels<br />
surrounded by 1.4 nm microporous cages and exhibits exceptionally high surface area. [217]<br />
Thus, variation of the relative lengths of the linkers mixed (di- and trifunctional linkers)<br />
may result frameworks of different topologies. [218] In this manner, HML strategy has<br />
paved up a way to unavailable topologies and larger pore sizes which are not easily<br />
achieved in single-component frameworks. However, careful control over MOF synthesis<br />
to avoid the formation of physical mixtures of different phases needs to be considered.<br />
The latter two synthetic strategies, especially TML approach, can be successfully<br />
employed to prepare defect-engineered MOFs (DEMOFs), which will be described in this<br />
Chapter below.<br />
4.1.2 Defects in MOFs and its “engineering”<br />
It has been recognized that MOFs, similar to other (crystalline) solid-state materials, are<br />
typically not perfect crystals with infinite periodic repetition or ordering of the identical<br />
groups of atoms in space. In fact, defects of various types and length scales (even more<br />
generally: structural heterogeneity) cannot be rigorously avoided during synthesis and<br />
crystal growth and often play an important role for the material properties. [220-222] The<br />
diversity of MOF structures connected with the issues of intrinsic and intentional<br />
structural defects, non-stoichiometry and heterogeneity suggests a much broader<br />
approach for understanding and tailoring their chemical and physical properties. [137] In<br />
fact, Ravon and co-workers has reported MOFs featuring structural defects in which acidic
Chapter 4 61<br />
active catalytic centers were generated through fast precipitation and partial substitution<br />
of dicarboxylic by mono-carboxylic acid linkers. Interestingly, the obtained in this manner<br />
defect-engineered Zn-MOFs show shape selectivity in catalyzing alkylation of large<br />
aromatics molecules. [144] Furthermore, by using CF3COOH and HCl during the synthesis,<br />
Vermoortele et al. demonstrated that UiO-66(Zr) can be modified via partial substitution<br />
of terephthalates by trifluoroacetate. Interestingly, subsequent thermal activation lead to<br />
post-synthetic removal of the trifluoroacetate groups in addition to the dehydroxylation<br />
of the hexanuclear Zr-clusters. All together, this yielded more open defect framework with<br />
a large number of open sites. Remarkably, produced defects at metal sites enhanced UiO-<br />
66(Zr) activity in several Lewis acid catalyzed reactions(Figure 4.3). [141] As a result, better<br />
catalytic performance in several Lewis-acid catalyzed reactions was observed for the<br />
DEMOFs. Controlled introduction and characterization of specific defects into MOFs is<br />
quite a challenge including the comparison with the parent (more or less) “defect-free”<br />
reference samples.<br />
Figure 4.3. The generation of defects in UiO-66(Zr). Reprinted with permission from F.<br />
Vermoortele, B. Bueken, G. Le Bars, B. Van de Voorde, M. Vandichel, K. Houthoofd, A. Vimont, M.<br />
Daturi, M. Waroquier, V. Van Speybroeck, C. Kirschhock and D. E. De Vos, J. Am. Chem. Soc., 2013,<br />
135, 11465-11468. Copyright (2013) American Chemical Society. [141]<br />
[Cu3(BTC)2]n (also known as HKUST-1) [35] as well as the isostructural family [M3(BTC)2]n<br />
(M = Mo, [81, 83] Cr, [78, 83] Ni, [79, 83] Ru, [82-83, 198] Zn, [77, 83] , BTC = benzene-1,3,5-tricarboxylate)<br />
attracted considerable attention over last years, mainly due to presence of coordinatively<br />
unsaturated metal-sites (M-CUS), as has been already introduced in Chapter 3. Intentional<br />
defect generation in [Cu3(BTC)2]n was initially reported by Baiker et al. who studied
62 Chapter 4<br />
partial replacing of BTC by the homologous pyridine-3,5-dicarboxylate (pydc) linker and<br />
revealed enhanced catalytic activity of the modified MOF in the oxidation of benzene<br />
derivatives related to modified M-CUS at the nodes. [136] Subsequently, studies conducted<br />
at our group demonstrated that not only pydc, but also a series of other defect generating<br />
linkers can be framework incorporated in case of [Cu3(BTC)2]n. [139] Interestingly,<br />
functionalized mesopores along with the M-CUS appeared to be generated in such defectengineered<br />
MOFs (DEMOFs) (Figure 4.4).<br />
Figure 4.4. The modulation of the defect structure on the micro- and mesoscales by doping of the<br />
framework with DL. The blue and short red sticks represent perfect and defective linkers. The<br />
yellow and black balls represent perfect and defective metal sites, respectively. The green<br />
highlighted unit indicates parent micropores. Reprinted with permission from Z. Fang, J. P.<br />
Dürholt, M. Kauer, W. Zhang, C. Lochenie, B. Jee, B. Albada, N. Metzler-Nolte, A. Pöppl, B. Weber, M.<br />
Muhler, Y. Wang, R. Schmid and R. A. Fischer, J. Am. Chem. Soc., 2014, 136, 9627-9636. Copyright<br />
(2014) American Chemical Society. [139]<br />
In parallel, Hupp et al. gave an account of the enhanced porosity by introducing<br />
isophthalate (ip) into [Cu3(BTC)2]n. [140] The concept of defect engineering by a mixed<br />
component approach using fragmented linkers together with the parent one was also<br />
expanded to the isostructural Ru-analogue. [138] Ru-DEMOFs [Ru3(BTC)2-x(pydc)xYy]n (Y =<br />
counter-ion, Cl - , OH - , OAc, etc.; 0 < y≤ 1.5) were obtained through direct mixing of H2pydc<br />
and H3BTC in one-step solvothermal synthesis. The generation of reduced Ru δ + (0
Chapter 4 63<br />
compared with the parent material, the actual compositions of these Ru-DEMOFs are very<br />
difficult to establish and are not entirely clear. This stems from the structural complexity<br />
of such multi‐component solid solution MOFs and a range of possible compositional<br />
variations, which are not mutually exclusive (counter-ions, residual synthesis<br />
components such as linkers, coordination modulators etc.).<br />
Figure 4.5 Design concept of the DEMOFs applying the mixed component/fragmented linker solid<br />
solution approach and sketch of the two possible, most important paddlewheel-node related<br />
defects.<br />
Figure 4.5 summarizes the concept of defects introduction into mixed-valence<br />
[M3(BTC)2Yy]n by using divalent isophthalate linkers as fragmented variants of trivalent<br />
BTC. Mainly, two types of defects need to be distinguished: Type A refers to structurally<br />
and electronically modified paddlewheel units (missing one carboxylate ligator function),<br />
in which (at least) one out of the four bridging carboxyl groups from the parent BTC linker<br />
in the regular paddlewheels has been partly substituted by the (neutral) functional group<br />
of the DL. Consequently, for charge compensation, the metal sites could be either partly<br />
reduced (mixed-valence state) or may carry additional anionic (mono-valent) ligands<br />
(Y) [137-138] However, apart from such type A, defects of type B could be formed, where<br />
whole paddlewheel nodes are eliminated from the structure, as it has been demonstrated
64 Chapter 4<br />
in the case of ip introduction into [Cu3(BTC)2]n. [140] It is conceivable, that such missing<br />
node defects could be formed in a correlated fashion during the MOF crystal growth<br />
process and in such a case larger areas of missing nodes may be generated to yield<br />
mesopores.
Chapter 4 65<br />
4.2 Ruthenium Metal-Organic Frameworks featuring Different Defect Types<br />
Being mainly studied in Cu-HKUST-1, a comprehensive understanding of the nature and<br />
formation of different types of isolated local and larger scale correlated defect sites in<br />
DEMOFs of the [M3(BTC)2]n family and MOFs in general is very limited and this research<br />
is still at its infancy. [137] The work in this chapter is a follow-up of the previous<br />
investigations on defect engineering in [Ru3(BTC)2Yy]n using H2pydc as (single) defect<br />
generating linker. [138] Similar to the previous more elaborate study on defect-engineered<br />
Cu-HKUST-1 [139] , a series of 5-X-isophthalic acids (5-X-ipH2, X = OH, H, NH2, Br) are<br />
selected and mixed them with H3BTC to yield the Ru-DEMOFs of the general formula<br />
[Ru3(BTC)2-x(5-X-ip)xYy]n (Figure 4.5). The choice of the functional group X in DL is on the<br />
basis of two aspects: i) modulating the coordination binding strength between linkers and<br />
Ru-nodes, namely, changing one of the carboxylate group in parent H3BTC linker to<br />
weaker binding groups (OH, NH2) or even inert coordination groups (H, Br); ii) labeling<br />
DL with easily tracked elements such as Br, NH2, etc. for analytical purpose. Thus, a<br />
number of complementary characterization methods are applied to obtain compositional<br />
and microstructure data of the materials. The aim is to at least qualitatively assess the<br />
tendency of type A and type B defect formation as a function of synthetic conditions and<br />
the chosen 5-X-ip linker. Several catalytic reactions, such as ethylene dimerization and<br />
Paal-Knorr reaction (usually running under Lewis acidic conditions) as well as low<br />
temperature CO2→CO dissociative chemisorption in the dark under UHV conditions, have<br />
been chosen as test reactions to monitor the influence of defects on the performance of<br />
the Ru-DEMOFs.<br />
4.2.1 Synthesis and characterization of the Ru-DEMOF materials<br />
In the following, a comprehensive account on the conducted experiments, obtained<br />
analytical and characterization data is provided for elucidation of the defect structure of<br />
Ru-DEMOFs of the general formula [Ru3(BTC)2-x(5-X-ip)xYy]n. The main goal of the<br />
presented study is to substantiate the hypothesis of type A and type B defect formation in<br />
these systems as introduced above (Figure 4.5).
66 Chapter 4<br />
4.2.1.1 Crystallinity and stability of the obtained samples<br />
Figure 4.6. PXRD patterns of the solvated Ru-DEMOF materials 1a-1d, 2a-2d, 3a-3d, 4a-4c<br />
compared with the solvated parent Ru-MOF, respectively. 1a-1d: DL is 5-OH-ip; from 1a to 1d,<br />
feeding level is increasing: 10%, 20%, 30%, 50%, respectively. 2a-2d: DL is ip; from 2a-2d,<br />
feeding level is increasing: 10%, 20%, 30%, 50%, respectively. 3a-3d: DL is 5-NH 2 -ip, from 3a to<br />
3d, feeding level is increasing: 10%, 20%, 30%, 50%, respectively. 4a-4c: DL is 5-Br-ip, from 4a<br />
to 4c, the feeding level is increasing: 10%, 20%, 30%, respectively. Vertical lines at 42.1°and 44°<br />
stand for the respective reflections of (001) and (101) faces of hexagonal close‐packed metallic<br />
Ru-particles or Ru-NPs.<br />
Parent Ru-MOF in this chapter for comparison was prepared according to the synthetic<br />
method for Ru-MOF 1_ex in Chapter 3. All Ru-DEMOF samples were obtained according<br />
to the previously published procedure, [138] using [Ru2(OOCCH3)4Cl]n, H3BTC and defect<br />
generating 5-X-ipH2 as starting materials in the acetic acid/water solution under<br />
solvothermal conditions. The sample-numbering scheme is based on the framework
Chapter 4 67<br />
incorporated 5-X-ip linker: X= OH (1), H (2), NH2 (3) or Br (4). Further labeling (a, b, c<br />
etc.) refers to various levels (molar%) of DL incorporation. The PXRD patterns of the assynthesized<br />
and activated samples indicate that all materials (except 2d) are crystalline<br />
and isostructural with the parent Ru-MOF that is obtained employing the same method<br />
with H3BTC, only (Figures 4.6 and 4.7). It should be noted that Ru 2+/3+ ions can be possibly<br />
reduced to eventually yield metallic ruthenium. Therefore, the solvothermal synthesis<br />
Figure 4.7. PXRD patterns of the activated Ru-DEMOF materials 1a-1d, 2a-2d, 3a-3d, 4a-4c<br />
compared with the solvated parent Ru-MOF, respectively. 1a-1d: DL is 5-OH-ip; from 1a to 1d,<br />
feeding level is increasing: 10%, 20%, 30%, 50%, respectively. 2a-2d: DL is ip; from 2a-2d,<br />
feeding level is increasing: 10%, 20%, 30%, 50%, respectively. 3a-3d: DL is 5-NH 2 -ip, from 3a to<br />
3d, feeding level is increasing: 10%, 20%, 30%, 50%, respectively. 4a-4c: DL is 5-Br-ip, from 4a<br />
to 4c, the feeding level is increasing: 10%, 20%, 30%, respectively. Vertical lines at 42.1°and 44°<br />
stand for the respective reflections of (001) and (101) faces of hexagonal close‐packed metallic<br />
Ru-particles or Ru-NPs.<br />
conditions have to be carefully monitored. However, no PXRD-peaks in the 2θ range of 40-<br />
45° were found, neither for the as-synthesized nor for the activated samples, thus
68 Chapter 4<br />
suggesting the absence of a substantial amount of Ru 0 nano-particles (Ru-NPs).<br />
Reflections at 42.1°and 44°are usually assigned to (001) and (101) faces of hexagonal<br />
close‐packed metallic Ru-particles or Ru-NPs. [223] Further data to rule out Ru 0 , XANES in<br />
particular, will be described below. The corresponding results provide additional<br />
evidence for the absence of Ru/RuOx‐NPs in the obtained Ru-DEMOFs. With the exception<br />
of 2d, thermal gravimetric analysis (TGA) shows no decomposition of the prepared<br />
materials for temperatures below 250 °C, suggesting that thermal stability of Ru-DEMOFs<br />
is preserved as compared to the parent MOF (Figure 4.8).<br />
Figure 4.8. TG curves of the prepared Ru-DEMOFs 1a-1d (with 5-OH-ip DL), 2a-2c (with ip DL),<br />
3a-3d (with 5-NH 2 -ip DL), 4a-4c (with 5-Br-ip DL) in comparison with the parent Ru-MOF,<br />
respectively.
Chapter 4 69<br />
4.2.1.2 The incorporation amount of DLs as well as the composition of the<br />
materials<br />
The incorporation and quantification of DLs have been initially testified by NMR<br />
spectroscopy of the digested samples after activation and the assessment of porosity<br />
(Table 4.1). Thus, in the 1 H-NMR spectra of the samples 1a-d, appearance of two<br />
additional peaks (compared with the parent Ru-MOF) at 7.51 ppm and 7.89 ppm is clearly<br />
seen (Figure 4.9). These two resonances can be assigned to the aromatic protons of 5-OHip<br />
linkers. Expectedly, upon increasing the feeding amount of the DL (5-OH-ipH2), the<br />
intensities of its characteristic resonances also increases in the digested sample solution.<br />
Figure 4.9. 1 H-NMR spectra of the Ru-DEMOFs (1a-1d) digested in DCl/DMSO-d 6 mixture. DL is<br />
5-OH-ip. H 3 O + comes from H 2 O and HCl contained in DCl. Due to the sensitivity of H 2 O peak to the<br />
solution conditions, the proton resonance of H 3 O + varies here in the range of 4-6 ppm, dependent<br />
on pH value of the total solution.
70 Chapter 4<br />
Table 4.1. The molar fractions (%) of the DLs used for the synthesis and observed in the final Ru-<br />
DEMOFs in respect to the total amount of linkers (H 3 BTC + 5-X-ipH 2 = 100%). The values were<br />
obtained from the integrals of proton peaks in 1 H-NMR spectra of the acid-digest sample. For the<br />
samples 1a-1d DL is 5-OH-ip; for 2a-2c – ip; for 4a-4c – 5-Br-ip, respectively.<br />
Sample<br />
Feeding<br />
(used for synthesis)<br />
Obtained<br />
1a 10% 8%<br />
1b 20% 20%<br />
1c 30% 32%<br />
1d 50% 37%<br />
2a 10% 15%<br />
2b 20% 28%<br />
2c 30% 47%<br />
4a 10% 17%<br />
4b 20% 25%<br />
4c 30% 42%<br />
A similar scenario was observed also for the samples with ip DL (series 2a-c). Resonances<br />
corresponding to the protons of ip are seen at 8.4 ppm, 8.1 ppm and 7.6 ppm (Figure 4.10).<br />
The framework incorporation amount of ip in 2a-c increases upon increasing the<br />
concentration of the DL in the reactant solutions. However, the incorporated amount of ip<br />
was found to be higher than expected from the H3BTC:H2ip feeding ratio, which is in<br />
contrast with that in the case of Ru-DEMOF series 1 where the incorporation of 5-OH-ip<br />
stay the same (or a little less) than the feeding concentration in the starting reactants. This<br />
result might be attributed to the slightly different coordination equilibria that correlate<br />
with the Brønsted acid dissociation constants of the used linkers: pKa (H3BTC) = 3.12,<br />
3.89, 4.70 and pKa (H2ip) = 3.46, 4.46. [224] However, the pKa differences are small and a<br />
conclusive explanation based on pKa is not straightforward. Dincă et al. argued that<br />
deprotonated BTC could serve as a counter-ion to provide the charge balance of [Ru2] 5+<br />
units in Ru-analogue of Cu-HKUST-1. [83] From our earlier investigation we concluded that<br />
H3BTC is present in the pores of [Ru3(BTC)2Yy]n in the form of fully protonated species,<br />
rather than as deprotonated counter-ions. [208] Both studies indicate that the linker used<br />
for the synthesis could still be present in the obtained materials. Hence, it is conceivable<br />
that the defect generating H2ip linker can also reside either as a counter-ion or as a guest
Chapter 4 71<br />
molecule in the pores of the Ru-DEMOFs (2a and 2b). On the basis of these arguments it<br />
can be understood why the amount of incorporated ip can be higher than expected from<br />
the H2ip:H3BTC feeding ratio. Indeed, very weak IR-bands in the range of ν(C=O), ν(C=C)<br />
or νas(COO) vibrations (1736-1521 cm -1 ) have been observed in case of samples 2a-2d.<br />
However, the small separation of the ν(C=O) bands of non-coordinated acetic acid (1715-<br />
1640 cm -1 ), [225] protonated/non-coordinated H2ip (1670 cm -1 ) and H3BTC (1680 cm -1 )<br />
(see Figure 4.11.2) makes it hard to unambiguously determine the exact origin of these<br />
weak vibrations.<br />
Figure 4.10. 1 H-NMR spectra of the Ru-DEMOFs (2a-2c) digested in DCl/DMSO-d 6 mixture. DL is<br />
ip. H 3 O + comes from H 2 O and HCl contained in DCl. Due to the sensitivity of H 2 O peak to the<br />
solution conditions, the proton resonance of H 3 O + varies here along with the variation of pH value<br />
of the total solution.
72 Chapter 4<br />
Figure 4.11. IR spectra of the prepared Ru-DEMOFs 1a-1d (with 5-OH-ip DL), 2a-2d (with ip DL),<br />
3a-3d (with 5-NH 2 -ip DL), 4a-4c (with 5-Br-ip DL) in comparison with the parent Ru-MOF and<br />
the corresponding DL used in the synthesis, respectively. The vertical dash lines in Figure 4.11.3<br />
indicate position of the vibrations of N-H and C-N bonds.<br />
Here it should be pointed out that in all 1 H-NMR spectra of the digested Ru-DEMOF<br />
samples the resonance at ca. 1.91 ppm, originated from the –CH3 groups of acetate, has<br />
been detected. This is in line with our previous investigations on the parent single-linker<br />
Ru-MOFs obtained from various Ru-precursors and the Ru-DEMOFs with pydc DL, where<br />
the same resonance due to acetate in the digested samples with the molar ratio of<br />
n(AcO):n(BTC) in the range from 0.7 to1.8 was always observed as well. [138, 208] . We<br />
anticipate three main origins of the presence of acetate in the discussed Ru-MOFs:<br />
i) it may act as a counter-ion to compensate the overall charge of the framework (Figure<br />
4.12a);
Chapter 4 73<br />
ii) owing to the competition with BTC and 5-X-ip, it could be residual/non-substituted and<br />
paddle wheel coordinated acetate-groups of the used Ru-precursor ([Ru2(OOCCH3)2Cl]n)<br />
(Figure 4.12b);<br />
Figure 4.12. Schematic representation for the two possible origins of acetate in the Ru-DEMOFs.<br />
iii) finally, it might reside as AcOH in the pores of the framework through weak<br />
interactions and, therefore, cannot be easily removed by washing and subsequent thermal<br />
activation (i.e., heating at 150 °C under dynamic vacuum).<br />
To recall, the glacial acetic acid/water mixture (AcOH:H2O = 0.05:1) was found to be<br />
essential for a successful synthesis and was always used for all reported Ru-(DE)MOFs<br />
(see Experimental Section). Besides, employed linkers may also serve as guest molecules<br />
as has been mentioned above. Attempts to evaluate the presence of acetic acid and linkers<br />
from the IR spectra is not quite feasible due to the overlapping of the bands of νas(COO)<br />
and νs(COO) (coordinated in a bidentate-bridging mode and free-coordinated carboxylate<br />
group) [226] as well as low intensity of the respective bands. Although one can monitor<br />
acetate groups in IR-spectroscopy by employing F-labled acetate (eg. perfluoro-acetate<br />
instead of acetate) for synthesis, [227] the crucial synthesis parameters of Ru-MOFs make<br />
this attempt impossible. Earlier effort of using various acids as the reaction solvent failed<br />
to form crystalline parent Ru-MOF. [208] Consequently, the presence of acetate (mainly)<br />
and non-reacted free linkers used in Ru-DEMOFs raises questions about the actual sample<br />
compositions and local structures and, thus, causes more complications with ambiguous<br />
interpretation of the analytical data than in case of the homologous Cu-DEMOFs. [139] The<br />
compositions of the Ru-DEMOFs samples discussed in this work have been derived by
74 Chapter 4<br />
taking into account the complete set of experimental results and a full account is given in<br />
Tables 4.2 and 4.3).<br />
Table 4.2. Elemental analysis results (calculated and found) of the activated Ru-DEMOFs (1a, 1c<br />
and 1d) in comparison with the parent Ru-MOF. Molar ratio of Ru : Cl calculated based on the<br />
found mass percentages are also given below.<br />
Sample<br />
C, wt % H, wt % Ru, wt % Cl, wt %<br />
cal. found cal. found cal. found cal. found<br />
Ru : Cl<br />
parent 28.5 27.26 2.31 1.65 31.40 30.45 3.67 3.41 3: 1<br />
1a 29.3 28.4 2.28 1.49 31.55 30.08 3.69 3.47 3: 1<br />
1c 31.67 31.26 1.89 1.37 32.03 31.08 3.37 3.27 3: 0.9<br />
1d 30.26 29.43 2.06 1.59 31.36 30.41 3.30 3.35 3: 0.9<br />
Table 4.3. Proposed formula* and the molecule weight of the activated Ru-DEMOFs (1a, 1c and<br />
1d) as well as the parent Ru-MOF.<br />
Sample<br />
Parent Ru-<br />
MOF 1_ex<br />
1a<br />
1c<br />
1d<br />
Formula<br />
[Ru 3 (C 9 H 3 O 6 ) 2 Cl(CH 3 COO) 0.5 ]·(CH 3 COOH) 1.5 (C 9 H 6 O 6 ) 0.1 (H 2 O) 4<br />
([Ru 3 (BTC) 2 Cl(AcO) 0.5 ]·(AcOH) 1.5 (H 3 BTC) 0.1 (H 2 O) 4 )<br />
[Ru 3 (C 9 H 3 O 6 ) 1.84 (C 8 H 3 O 5 ) 0.16 Cl(OH) 0.5 ]·(CH 3 COOH) 2.8 (H 2 O) 2<br />
([Ru 3 (BTC) 1.84 (5-OH-ip) 0.16 Cl(OH) 0.5 ]·(AcOH) 2.8 (H 2 O) 2 )<br />
[Ru 3 (C 9 H 3 O 6 ) 1.36 (C 8 H 3 O 5 ) 0.64 Cl 0.9 (OH) 0.6 ]·(CH 3 COOH) 2.2 (C 8 H 6 O 5 ) 0.4<br />
([Ru 3 (BTC) 1.36 (5-OH-ip) 0.64 Cl 0.9 (OH) 0.6 ]·(AcOH) 2.2 (5-OH-ipH 2 ) 0.4 )<br />
[Ru 3 (C 9 H 3 O 6 ) 1.26 (C 8 H 3 O 5 ) 0.74 Cl 0.9 (OH) 0.6 ]·(CH 3 COOH) 1.3 (C 9 H 6 O 6 ) 0.5 (H 2 O) 2.5<br />
([Ru 3 (BTC) 1.26 (5-OH-ip) 0.74 Cl 0.9 (OH) 0.6 ]·(AcOH) 1.3 (H 3 BTC) 0.5 (H 2 O) 2.5 )<br />
Molecular<br />
weight<br />
965.6<br />
961.1<br />
946.6<br />
982.6<br />
* The proposed formula of all the samples above have been calculated according to the facts and<br />
considerations listed below:<br />
<br />
<br />
Parent (BTC) to DL (5-OH-ip) ratios have been calculated based on the 1 H-NMR spectra (i.e.,<br />
integration of the linker-related signals) of the respective acid-digested samples.<br />
The parent Ru-MOF and reported Ru-DEMOFs are isostructural. At this point it is hard to<br />
quantitatively estimate contribution from the defects B (missing metal-nodes), therefore, for initial<br />
evaluations assumption that the general composition of the prepared solids is [Ru3(L)2Yy]n (L = total<br />
linker amount) was employed. Thus, the Ru : L molar ratio can be taken as a fixed value – 3 : 2.<br />
Further, having in mind there is generally 3 molar equivalents of Ru per 1 molecular unit of MOF,
Chapter 4 75<br />
the Cl-amount was subsequently calculated based on the measured EA values and respective Ru :<br />
Cl ratios.<br />
<br />
<br />
As observed by the 1 H-NMR, TG and IR analyses, the contribution of the counter-ions and guest<br />
molecules are mainly from Cl, OH, acetate, H2O and used linkers. In analogy to the previously<br />
reported parent Ru-MOF [208] and the Ru-DEMOF with pydc DL, [138] in the currently discussed Ru-<br />
DEMOFs acetic acid is also present, which is clearly evidenced by the 1 H-NMR spectra of the<br />
digested samples. To note, the amount of the acetic acid can be considerably reduced by additional<br />
solvent exchange procedure, namely, soaking of the activated samples in a large amount of water<br />
while intense stirring to exchange the residue acetic acid. However, the risk of leaching out of Ru<br />
needs also to be taken into account here. [208] Hence, our current studies dealt with the obtained<br />
powders applying gently water soak as solvent exchange procedure to decrease the residue of the<br />
acetic acid. And the overall concentration of the acetic acid decreased in comparison with our<br />
previously report on the Ru-DEMOF with pydc DL in spite of the slightly decrease of Ru content.<br />
In addition of the multiple possible status of acetic acid, starting reactant (i.e. linkers) can be also<br />
accommodated into the framework as guest molecules or served as counter-ions, since based on<br />
the NMR data the amount of the DL in some cases appeared to be higher than its respective feeding<br />
amount. Besides, minor quantities of the coordinated H2O might be occluded / resided in the pores<br />
as well, as the TG curves of the activated samples show the slight decrease in the range of 100-250<br />
°C.<br />
Figure 4.13. EDX spectra of the Ru-DEMOFs 4a-4c (with 5-Br-ip DL). The detection of Br<br />
clearly indicates the presence of the employed DL.
76 Chapter 4<br />
As quantitative digest of the samples 3a-d is not sufficient, detection and determination<br />
of the DL contents (5-NH2-ip) from 1 H-NMR measurements was not possible.<br />
Nevertheless, the IR spectra of these samples provide a qualitative evidence for the 5-NH2-<br />
ip incorporation. Indeed, the observed bands at 1651 cm -1 and 1264 cm -1 stem from δ(N-<br />
H) and ν(C-N) vibrations of the 5-NH2-ip (Figure 4.11). In case of the 5-Br-ip (samples 4ac),<br />
the gradual increase of intensities of the respective signals in both 1 H-NMR and TEM-<br />
EDX spectra suggests the presence of DL in these Ru-DEMOFs (see Figures 4.13 and 4.14).<br />
Figure 4.14. 1 H-NMR spectra of the Ru-DEMOFs (4a-4c) digested in DCl/DMSO-d 6 mixture.<br />
DL is 5-Br-ip. H 3 O + comes from H 2 O and HCl contained in DCl. Due to the sensitivity of H 2 O<br />
peak to the solution conditions, the proton resonance of H 3 O + varies here, dependent on pH<br />
value of the total solution.<br />
4.2.2 Porosity of Ru-DEMOF samples and the confirmation of the DL incorporation<br />
To support further the framework incorporation of the DL and rule out its extra<br />
framework inclusion within the pores in a high quantity, we have carried out N2 sorption<br />
measurements for the activated samples. The N2 sorption isotherms at 77 K for all samples
Chapter 4 77<br />
Figure 4.15. N 2 sorption isotherms collected at 77 K for Ru-DEMOF samples 1a-1d, 2a-2c, 3a-3d,<br />
4a-4c. 1a-1d: DL is 5-OH-ip, incorporation amount is 8%, 20%, 32% and 37%, respectively; 2a-<br />
2c: DL is ip, incorporation amount is 15%,28% and 47%, respectively; 3a-3d: DL is 5-NH 2 -ip; 4a-<br />
4c: DL is 5-Br-ip, incorporation amount is 17%, 25% and 42%, respectively. Closed and open<br />
symbols represent the adsorption and desorption isotherms, respectively. Black circles – parent<br />
Ru-MOF; blue triangles – a samples of the respective series 1-4; dark cyan diamonds – b samples<br />
of the respective series 1-4; magenta squares – c samples of the respective series 1-4; dark yellow<br />
stars – d samples of the respective series 1-4.<br />
(1a-d, 2a-d, 3a-d and 4a-c) reveal type I isotherm without any hysteresis loop (Figure<br />
4.15), indicating that all Ru-DEMOFs are microporous materials. [228] In general, while<br />
comparing with the Brunauer-Emmett-Teller (BET) surface area (SBET) of the parent Ru-<br />
MOF (998 m 2 /g), one can consider Ru-DEMOFs being analogous when the value (SBET) is<br />
in/above the range of the parent one. In other words, the considerably high SBET of the<br />
discussed Ru-DEMOFs rules out substantial guests occlusion and pore blocking such as by<br />
non-reacted DLs, acetate or Ru/RuOx‐NPs. Interestingly, when 5-OH-ipH2 is used as DL,<br />
SBET of the Ru-DEMOFs gradually increases until 5-OH-ip is incorporated up to 32% (1c)
78 Chapter 4<br />
(Figure 4.16). Notably, the SBET of this sample 1c is the highest among all [Ru3(L)2Yy]n (L =<br />
linker) isostructural MOFs (including the single-linker and other mixed-linker Ru-<br />
DEMOFs reported so far). [82, 138] This indicates that the 5-OH-ip is a good candidate for<br />
defects engineering in Ru-MOFs.<br />
Figure 4.16. The variation of the BET surface area (S BET ) derived based on measured N 2 sorption<br />
isotherms (77 K) upon increase of the DL doping. 'Parent' stands here for parent single-linker Ru-<br />
MOF (with only BTC). In the samples 1a-1d, 5-OH-ip serves as a DL; 2a-2c – ip; 3a-3d – 5-NH 2 -<br />
ip; 4a-4c – 5-Br-ip, respectively. The values of S BET have been summarized in Table 7.4 in Chapter<br />
7.<br />
In contrast with the Ru-DEMOFs series 1 with 5-OH-ip DL, the integration of the ip DL<br />
generally results in lower porosities, as demonstrated by the results for samples 2a-d.<br />
However, the SBET of samples 2a and 2b are still higher than the SBET of the parent Ru-MOF.<br />
Nonetheless, upon increasing the ip content, the surface area decreases. Thus, considering<br />
porosity characteristics, the optimum incorporation extent of DL in these series stays at<br />
28% (sample 2b). In case of 5-NH2-ip DL, the porosity of the Ru-DEMOFs (3a-c) is fully<br />
maintained, while increasing of the feeding level to 50% leads to porosity decrease<br />
instead (sample 3d, SBET = 781 m 2 /g). These observations in 2a-d and 3a-d series are<br />
probably due to the accommodation of unreacted 5-X-ipH2 in the pores. Along with the
Chapter 4 79<br />
increasing feeding of 5-X-ipH2 the competition between BTC and 5-X-ip increases.<br />
Subsequently, it is more difficult to rule out the presence of unreacted 5-X-ipH2 as the<br />
reason of the decreasing SBET. In the same line of reasoning, the SBET of the samples 4a-c<br />
dramatically decreased from 996 to 693 m 2 /g. Hence, the optimized incorporation of 5-<br />
Br-ip can only reach up to 17% (4a). Notably, in our previous studies on the defectengineered<br />
Cu-HKUST-1, the generation of mesopores was observed. [139] Curiously, in the<br />
present case of the homologous Ru-DEMOFs, an opposite trend was observed, which<br />
might be attributed to the preference of isolated defects rather than to the correlated<br />
defects in the framework (Figure 4.17). During the formation of Ru-DEMOFs, the<br />
substitution of [Ru]-L + DL ⇌ [Ru]-DL +L (L = AcO/BTC, DL = 5-X-ip) is kinetically<br />
hindered by higher activation energy in comparison to that in the case of Cu-DEMOFs.<br />
Consequently, the substitution is possibly much slower and lead to only isolated defects.<br />
Figure 4.17. Schematic representation of point defects and correlated defects in DEMOFs. Figure<br />
is provided by Dr. O. Halbherr.<br />
4.2.3 XANES, XPS and UHV-FTIR studies: ruthenium oxidation state variation as<br />
indication of defect type formation<br />
As earlier mentioned, in our previous studies on doping of the Ru-MOF with defect pydc<br />
linker, we have assigned the introduced local defects, according to Baiker et al., [136] as<br />
modified Ru-paddlewheels with three coordinating BTC and one pydc linker, in which the<br />
pyridyl-N site acts as a weakly binding ligator-site over the Ru-dimer. Such structural<br />
irregularities are associated with (partially) missing linker function (i.e., carboxylate) and<br />
consequently steric and electronic modification of the Ru-SBUs (see Figure 4.5).<br />
Additionally, partial ruthenium reduction has been observed. Namely, apart from the<br />
expected Ru 2+ and Ru 3+ (as in the parent Ru-MOF), we revealed also distinctly reduced
80 Chapter 4<br />
framework Ru-species (Ru δ+ , 0
Chapter 4 81<br />
XANES spectra (Figure 4.18) show deviation of the edge jump derivative for the samples<br />
1a-d from that one of the parent Ru-MOF. For 1a-c, the position of edge jump gradually<br />
shifts to the lower energies, suggesting reduced Ru-sites with oxidation states lower than<br />
2+ or 3+. We relate this observation to the generation of defects A in the samples 1a-c.<br />
However, the position of the edge jump in case of the sample 1d moved again to higher<br />
energies, illustrating that the amount of reduced Ru-species is now decreased with<br />
respect to samples 1a-c. The different tendency suggests that defects B may also be<br />
created when 5-OH-ip linker was incorporated into the framework at ratios higher than<br />
32%. The same trend has been observed for the 5-NH2-ip linker (samples 3a-c). Indeed,<br />
the XANES spectra of the samples 3a-b suggest again the presence of reduced Ru δ+<br />
(0
82 Chapter 4<br />
Figure 4.20. XANES spectra of the parent Ru-MOF and Ru-DEMOF sample 4a (with 17% 5-Br-ip<br />
DL, derivative of the normalized intensity vs. Energy). Black: parent Ru-MOF; blue: 4a.<br />
Figure 4.21. XANES spectra (derivative of the normalized intensity vs. Energy) of the Ru-DEMOF<br />
materials 2a and 2b compared with the parent Ru-MOF. Black: parent Ru-MOF; blue: 2a (15% ip);<br />
dark cyan: 2b (28% ip)..
Chapter 4 83<br />
Interestingly, the position of the edge jump in case of the ip-doped samples 2a-b does not<br />
change compared with that in the parent Ru-MOF (Figure 4.21). The Ru oxidation state is<br />
not affected by the incorporation of ip, which could be taken as indication of a<br />
predominance of defects B for samples 2a-b. When the functional group of the DLs<br />
changes from small, coordinative inert H to the somewhat larger and coordinative more<br />
suitable ligator-sites like -OH, -NH2 or -Br, the defects A are favored in case of relatively<br />
low doping level. However, upon rising the doping level, defects B are increasingly created<br />
along with some remaining defects A, resulting in less pronounced variation of the<br />
oxidation state of Ru in the defect-engineered samples compared with the parent material.<br />
Figure 4.22. XANES spectra (normalized absorption vs. Energy) of the Ru-DEMOF materials (1a-<br />
1d, 2a, 2b, 3a-3c and 4a) compared with the parent Ru-MOF as well as some Ru references. Solid<br />
Black: parent Ru-MOF; solid blue: a samples of the respective series 1-4; solid dark cyan: b<br />
samples of the respective series 1-4; soid magenta: c samples of the respective series 1-4; solid<br />
dark yellow: d samples of the respective series 1-4; dash dot violet: Ru; solid orange: RuO 2 ; short<br />
dash wine: Ru nano-particles(NPs).
84 Chapter 4<br />
It is important to note that the white line in the XANES spectra (normalized absorption vs.<br />
energy, Figure 4.22) of all the Ru-DEMOFs samples as well as the parent Ru-MOF are<br />
strikingly different from those measured for the Ru-NPs, metallic Ru and RuO2. These<br />
observations support PXRD results (see above and Figures 4.6 and 4.7) and allow also to<br />
rule out the presence of other Ru-phases as significant impurities in the Ru-DEMOFs<br />
including parent Ru-MOF. [223] Thus, we assume that it is valid to assign all Ru-species to<br />
the metal-nodes of the frameworks. Further information on the local environment of Ru<br />
can be obtained also from EXAFS. The analysis of the experimental data is, however, a<br />
formidable effort, since many different models for Ru-DEMOFs have to be considered and<br />
a variety of local structures may be present in parallel in the samples as discussed before.<br />
Therefore, a thorough analysis of the EXAFS-data is outside the scope of this dissertation<br />
project.<br />
The different samples fabricated in this study have also been characterized using Highresolution<br />
X-ray photoelectron spectroscopic (XPS) in order to confirm the assignments<br />
based on XANES and for a more quantitative estimation of the relative abundance of the<br />
different Ru-species (Ru 3+ , Ru 2+ and Ru δ+ ) in the Ru-DEMOFs. The samples 1a, 1c, 1d, 2a<br />
and 2b with 5-OH-ip and ip DLs, respectively, have been selected. Remarkably, similar to<br />
the related pydc-doped Ru-DEMOFs we elaborated earlier, [138] reduced Ru δ+ -species have<br />
been found in the Ru-DEMOFs (samples 1a, 1c and 1d) in addition to the Ru 2+ - and Ru 3+ -<br />
species. Two Ru 3d doublets (3d5/2 and 3d3/2) at ca. 281.6 and 285.8 eV as well as at 282.6<br />
and 286.8 eV, attributed to the Ru 2+ - and Ru 3+ -species, respectively, are seen in the<br />
deconvoluted XP spectra of all measured samples (Figure 4.23). In addition, another Ru<br />
3d doublet appears at ca. 280.5 and 284.7 eV in the Ru-DEMOFs samples 1a, 1c and 1d.<br />
On the basis of quantitative estimations of the XP spectra, some variation of the Ru 3+ /Ru 2+<br />
ratio and, in particular, reduction to Ru δ+ in 1a, 1c and 1d can be clearly seen (Table 4.4).<br />
From the parent Ru-MOF to the Ru-DEMOF sample 1a, the ratio of Ru 3+ / Ru 2+ / Ru δ+ varies<br />
from 1 / 1.24 / 0 to 1 / 1.75 / 0.08, indicating that the incorporation of DL induces partial<br />
ruthenium reduction (i.e., relative concentrations of the Ru 2+ and Ru δ+ increase).<br />
Moreover, upon increasing the incorporation level of 5-OH-ip to 32% for 1c (feeding level<br />
30%), the amount of the reduced Ru δ+ -species considerably increases to the highest value<br />
(Ru 3+ / Ru 2+ / Ru δ+ = 1 / 1.69 / 0.59) among all studied samples. Importantly, the Ru δ+ -<br />
related doublet decreases significantly in intensity with further increase of the<br />
incorporation to 37% for 1d (feeding level 50%). This is in contrast to the observation for
Chapter 4 85<br />
Figure 4.23. Deconvoluted XP spectra of the Ru-DEMOFs samples (A)1a (8% of 5-OH-ip), 1c (32%<br />
of 5-OH-ip) and 1d (37% of 5-OH-ip), (B) 2a (15% of ip) and 2b (28% of ip) in Ru 3d and C 1s<br />
regions in comparison with parent Ru-MOF. Original figures are provided by P. Guo.<br />
pydc-doped Ru-DEMOFs, where a continuous rise of the Ru δ+ signals was detected along<br />
with increasing degree of pydc incorporation. [138] The relatively lower concentration of<br />
Ru 2+ and Ru δ+ in 1d (Ru 3+ / Ru 2+ / Ru δ+ = 1 / 1.23 / 0.09), as compared to the respective<br />
ratios estimated for 1c, can be explained by our assumption of simultaneous generation<br />
of both defects A and B with distinct preference of B over A at higher feeding<br />
concentrations of 5-OH-ip. Interestingly, for the ip-doped samples 2a-b no highly reduced
86 Chapter 4<br />
Ru δ+ have been observed in the XP spectra (no Ru3d doublets at ca. 280.5 and 284.7 eV;<br />
Figure 4.23). These data confirm the assignment deduced from XANES data, suggesting<br />
that application of DL with the coordinatively inactive functional group H (2a-b) is likely<br />
to more selectively induce missing node defects B in the Ru-DEMOFs without Ru<br />
reduction (as this is indicative for a type A defect). According to the results of XANES and<br />
XPS, we thus conclude that the Ru-DEMOFs materials with 5-X-ip (X= OH, NH2 and Br)<br />
contain predominantly defects A, especially at moderate incorporation levels. However,<br />
the simultaneous generation of defects B in these samples is also likely as indirectly<br />
deduced from the non-linear dependence of the XANES and XPS data on the doping level.<br />
Table 4.4. The assignments of binding energies as well as the ratio of Ru 3+ / Ru 2+ / Ru δ+ (calculated<br />
from the deconvoluted spectra) in the parent Ru-MOF sample and Ru-DEMOFs (1a, 1c 1d, 2a and<br />
2b). 1a, 1c and 1d - 8%, 32% and 37% of 5-OH-ip, respectively; 2a and 2b - 15% and 28% of ip,<br />
respectively. Data provided by P. Guo.<br />
Sample Binding energy, eV Assignment Ru 3+ / Ru 2+ / Ru δ+ ratio<br />
Parent Ru-MOF<br />
1a<br />
1c<br />
1d<br />
2a<br />
285.86 / 281.66 Ru 2+<br />
286.86 / 282.66 Ru 3+<br />
285.86 / 281.66 Ru 2+<br />
286.86 / 282.66 Ru 3+<br />
284.65 / 280.45 Ru δ+<br />
285.71 /281.51 Ru 2+<br />
286.71 / 282.60 Ru 3+<br />
284.60 / 280.40 Ru δ+<br />
285.72 / 281.52 Ru 2+<br />
286.72 / 282.52 Ru 3+<br />
284.65 / 280.45 Ru δ+<br />
285.86 /281.66 Ru 2+<br />
286.86 / 282.66 Ru 3+<br />
1 / 1.24 / -*<br />
1 / 1.75 / 0.08<br />
1 / 1.69 / 0.59<br />
1 / 1.23 / 0.09<br />
1 / 1.73/ -*<br />
285.88 / 281.68 Ru 2+<br />
2b<br />
286.88 / 282.76 Ru 3+<br />
* no species have been determined.<br />
1 / 1.42 / -*<br />
Consequently, UHV-IR spectroscopic investigations employing CO as a probe molecule<br />
have been carried out on two representative samples 1c and 1d to gain complementary
Chapter 4 87<br />
evidence on the valence states of framework Ru sites and the associated defect types.<br />
Parent Ru-MOF was reported to reveal bands at 2172 and 2127 cm -1 , arising from CO<br />
interactions with Ru 3+ and Ru 2+ , respectively (Figure 4.24). [138] Apart from these two<br />
bands, the spectra of the samples 1c and 1d show additional bands at 2041 and 1998 cm -<br />
1 , which can be attributed to CO bound to reduced Ru δ+ (0
88 Chapter 4<br />
Figure 4.25. UHV-IR spectra of Ru-DEMOF 1c and 1d compared with parent Ru-MOF and Ru-<br />
DEMOF with 30% pydc incorporation upon CO 2 dosing at 90-95 K after annealing the sample at<br />
475-500 K. The bands at 2041 cm -1 and 1993 cm -1 are assigned to vibrations of CO bound to<br />
reduced Ru δ+ -sites and indicate dissociative chemisorption of CO 2 . Original figures are provided<br />
by M. Kauer.<br />
ration (1d). The formation of defect B, namely missing Ru-paddlewheels, is accompanied<br />
by lowering the abundance of Ru 2+ and Ru δ+ metal centers in the framework, which
Chapter 4 89<br />
explains the observed changes of the decreased intensity of Ru 2+ and Ru δ+ in the sample<br />
1d.<br />
In our earlier report on pydc-doped Ru-DEMOFs, we communicated on the low<br />
temperature CO2→CO dissociative chemisorption under UHV conditions in a dark<br />
environment, a feature which is not inherent for the parent Ru-MOF. [138] We concluded<br />
that the CO2→CO reduction might be triggered by the reduced Ru δ+ -sites and the pyridyl<br />
N-sites in the proximity of the modified Ru-centers at the nodes. In order to confirm these<br />
assumptions further, we have studied the same reaction at Ru-DEMOFs that feature<br />
reduced Ru δ+ -sites. As these sites have been created by the incorporation of the 5-OH-ip<br />
linker in 1a-d, we have selected two representative samples, 1c and 1d, both exhibiting<br />
high 5-OH-ip incorporation but quite different levels of Ru 2+ and Ru δ+ . As shown in Figure<br />
4.25, upon CO2 dosing for both the parent Ru-MOF and Ru-DEMOFs 1c, an intense and<br />
broad IR band appears at 2336 cm -1 that is assigned to the asymmetric stretching mode<br />
νas(CO2) of physisorbed CO2 binding linearly at various Ru-sites. [198] The weak band at<br />
2273 cm -1 indicates the presence of a minority CO2 species originating probably from the<br />
adsorption of a small amount of 13 CO2 with an expected isotopic shift of 1.03. Apart from<br />
the CO2-related bands, two other bands at 2041 cm -1 and 1993 cm -1 have been observed<br />
in 1c, that are assigned to vibrations of CO bound to the reduced Ru δ+ -sites, matching our<br />
previous data on pydc-doped Ru-DEMOF. [138] This result indicates dissociative<br />
chemisorption of CO2 to CO (reduction) in Ru-DEMOF with 5-OH-ip DL (1c), whereas the<br />
parent Ru-MOF is essentially inactive. However, in comparison to the extremely high<br />
reactivity of pydc-doped Ru-DEMOFs, in which CO2 is nearly totally converted to CO at<br />
higher concentrations of pydc defective linker (e.g. 30%), [138] the production of CO is<br />
rather limited for 5-OH-ip doped Ru-DEMOFs (Figure 4.25). Interestingly, Ru-DEMOF 1d,<br />
is almost inactive for CO2 dissociation. We correlate this observation to the much less Ru δ+<br />
and in turn to the more significant formation of missing node defects (type B) for 1d as<br />
compared to 1c. Overall, the presented IR data demonstrate that the 5-OH-ip doped Ru-<br />
DEMOF samples show much less reactivity for CO2 activation as compared to pydc doped<br />
samples. This cannot be attributed only to the relatively low concentration of reduced<br />
Ru δ+ . In previous study it was suggested that the CO2 activation being promoted by pydc<br />
linker due to the presence of basic pyridyl N sites in proximity to the reactive Ru δ+ . [138]<br />
This hypothesis is indirectly supported by the properties of samples 1c and 1d.
90 Chapter 4<br />
Table 4.5. Possible defect combinations in the prepared Ru-DEMOFs according to the conducted<br />
XANES, UHV-IR and XPS studies.<br />
DL Sample Assumption I Assumption II<br />
1a defectsA* + B defects A*<br />
5-OH-ip<br />
1c defects A*** + B defects A***<br />
1d defects A* + B defects A* + B<br />
ip<br />
2a<br />
2b<br />
defects B<br />
defects B<br />
3a defects A** + B defects A**<br />
5-NH 2 -ip<br />
3b defects A*** + B defects A***<br />
3c defects A* + B defects A* + B<br />
5-Br-ip 4a defects A + B defects A<br />
* expresses relative defects concentration.<br />
Figure 4.26. Other possible defect fragments in the structure of Ru-DEMOFs. a). Two DLs and two<br />
BTC in a fragment of modified paddlewheel b). Two DLs and two HBTC in a fragment of missing<br />
node. Free carboxylates of HBTC were bound with each other via hydrogen bounds. c). Correlated<br />
modified paddlewheel and missing paddlewheel.<br />
The combined spectroscopic characterization data (XANES, XPS, UHV-FTIR with CO and<br />
CO2 as probes) presented above suggest more or less consistent, but complicated picture<br />
on the abundance of the two kinds of defects. Overall, we assume both types A and B being<br />
simultaneously generated in the Ru-DEMOFs in the case of coordinative weakly binding<br />
ligator-sites at the fragmented linkers. Type A appears to be favored at low incorporation<br />
levels, e.g. 1a (8%) and becomes more abundant up to a certain threshold, e.g. 1c (32%).<br />
Along with a further increase of incorporation level, e.g. 1d (37%), defects of type B
Chapter 4 91<br />
appear to dominate over type A. One should be aware that the possibility of formation and<br />
distribution of various defect types is rather diverse and may not be restrict to those<br />
mentioned here. The arrangement of the two defect types in Ru-DEMOFs (1a, 1c and 1d)<br />
is rather diverse. Still, based on the information on XANES and UHV-IR with CO probing,<br />
we can assume two possibilities:<br />
i) both defects of type A and B might be generated in the Ru-DEMOFs (1a-1d) with the<br />
incorporation of 5-OH-ip. The defects of type A are much more competitive and became<br />
gradually dominant in case of the lower doping (samples 1a (8%) and 1c (32%)). Along<br />
with increase of doping level (1d, 37%) of 5-OH-ip, the dominant effect of defects A is<br />
substituted slowly by the defects B;<br />
ii) the defects of type A are generated and becomes gradually dominant in case of<br />
relatively low doping (samples 1a and 1c). Afterwards, defects B are created<br />
simultaneously when the doping level reaches 37% in case of 1d. Therefore, the influence<br />
caused by the defects A could be partly eliminated. Nevertheless, both assumptions<br />
indicate that the defects A play a major role in Ru-DEMOFs 1c (32% of 5-OH-ip). A<br />
comprehensive table summarizing possible defect combinations in the particular Ru-<br />
DEMOFs (based on the performed analyses) is given in Table 4.5 and Figure 4.26.<br />
Additional characterization and quantitative determination of the defect types requires<br />
additional work and support by theoretical modeling.<br />
4.2.4 CO2, CO and H2 sorption properties of Ru-DEMOFs<br />
The previous characterizations suggest the existence of two types of defects (A and B)<br />
being present in the samples in different absolute and relative amounts as a consequence<br />
of the 5-X-ip framework incorporation. Both are likely to influence the gas sorption<br />
properties of the Ru-DEMOFs. Hence, we studied the adsorption of CO2, CO and H2 at range<br />
of samples. In general, the results obtained and discussed in the following are not very<br />
conclusive as the observed changes in gas uptake as a function of DL incorporation are<br />
small or even close to the error of the measurements. Nevertheless, we present the data<br />
and provide a tentative discussion with respect to the possible counter acting effects of<br />
the two types of defects in the samples.
CO 2<br />
adsorbed, mmol/g<br />
92 Chapter 4<br />
3<br />
parent Ru-MOF<br />
1a<br />
1c<br />
1d<br />
2<br />
1<br />
0<br />
0 200 400 600 800 1000<br />
P, mbar<br />
Figure 4.27. CO 2 isotherms collected at 298 K for the parent Ru-MOF and DEMOF derivatives 1a<br />
(8%), 1c (32%) and 1d (37%) with 5-OH-ip DL. Black circles – parent Ru-MOF; blue triangles –<br />
1a; magenta squares – 1c; dark yellow stars – 1d.<br />
CO2 adsorption isotherms (298 K) of the parent reference Ru-MOF sample and 1a and 1c<br />
display a gradual enhancement of the adsorption capacity in the order Ru-MOF < 1a < 1c<br />
along with rising incorporation degree of DL (Figure 4.27). However, the CO2 uptake of<br />
the sample 1d revealed to be 2.9 mmol/g at 1 bar, and lies within the order Ru-MOF < 1d<br />
< 1c (Table 4.6). According to our studies on different defects in the series 1a-1d, these<br />
results are not unexpected. The increase of the CO2 uptake is attributed to the reduced Rusites<br />
at the type A defects and somewhat lowered uptake of 1d is attributed to less<br />
abundant Ru-sites as a consequence of missing metal-nodes (i.e., type B defects). Hence,<br />
higher incorporation level of DL in the sample 1d does not promote the increase of the<br />
CO2 uptake.
CO uptake, mmol/g<br />
Chapter 4 93<br />
Table 4.6. H 2 (77 K) and CO 2 (298 K) uptakes for the parent Ru-MOF and its defect-engineered<br />
variants 1a, 1c, 1d, 2a, 2b, 3a-3c and 4a at 1000 mbar. 1: DL is 5-OH-ip; 2: DL is ip; 3: DL is 5-<br />
NH 2 -ip; 4: DL is 5-Br-ip.<br />
Sample name CO 2 uptake (mmol/g) H 2 uptake (mmol/g)<br />
Parent Ru-MOF 2.7 6.8<br />
1a 3.2 9.6<br />
1c 3.4 8.9<br />
1d 2.9 7.6<br />
2a 3.0 7.4<br />
2b 2.8 6.7<br />
3a 3.4 8.3<br />
3b 3.2 7.8<br />
3c 2.9 7.4<br />
4a 2.6 7.1<br />
2.5<br />
2.0<br />
parent Ru-MOF<br />
1a<br />
1c<br />
1.5<br />
1.0<br />
0.5<br />
0.0<br />
0 200 400 600 800 1000<br />
P, mbar<br />
Figure 4.28. CO isotherms measured at 298 K for the parent Ru-MOF and Ru-DEMOF samples 1a<br />
(8%) and 1c (32%) with 5-OH-ip DL. Black circle – parent Ru-MOF; blue triangles – 1a; magenta<br />
squares – 1c.
H 2<br />
adsorbed, mmol/g<br />
94 Chapter 4<br />
Furthermore, CO adsorption of the parent Ru-MOF, 1a and 1c at 298 K also illustrates the<br />
tendency of enhanced uptake in case of the Ru-DEMOF samples (Figure 4.28). The small<br />
difference between the sample 1a and the parent Ru-MOF on CO adsorption is attributed<br />
to the low incorporation degree of the 5-OH-ip DL (8%). Along with the increase of the DL<br />
incorporation (such as in 1c), the CO uptake rises even at very low pressure (ca. 4 mbar).<br />
This increase of the CO capacity of the Ru-DEMOF is probably due to the generation of the<br />
modified paddlewheels of type A, which expose more open sites as one carboxylate<br />
ligator-site of BTC is substituted by the hydroxyl-group of 5-OH-ip. Besides, the average<br />
electronic density is varied as the oxidation state of ruthenium at the CUS is changed. Both<br />
could contribute to the enhancement of the adsorption properties.<br />
10<br />
8<br />
6<br />
4<br />
2<br />
parent Ru-MOF<br />
1a<br />
1c<br />
0<br />
200 400 600 800 1000<br />
P, mbar<br />
Figure 4.29. H 2 isotherms measured at 77 K for the parent Ru-MOF and DEMOFs 1a (8%) and 1c<br />
(32%) with 5-OH-ip DL. Black circles – parent Ru-MOF; blue triangles – 1a; magenta squares – 1c.<br />
The H2 adsorption isotherms (at 77 K) of the parent Ru-MOF and the Ru-DEMOFs 1a and<br />
1c follow nearly the same trend as in case of CO2 and CO adsorption (Figure 4.29). Both<br />
defect-engineered materials 1a and 1c exhibit higher H2 uptake at 1 bar than the parent<br />
intact framework. In fact, there should be two main kinds of adsorption sites in the Ru-
-Q st<br />
, kJ/mol<br />
Chapter 4 95<br />
DEMOFs (1a and 1c): 1) strong binding affinity between Ru-CUSs and hydrogen, namely<br />
Ru 2+/3+ -sites in the regular paddlewheel units and the Ru δ+ -sites in the modified<br />
paddlewheels (in defects A); 2) the relatively weaker interactions (ie. physisorption and<br />
van der Waals induced interactions) between the hydrogen and ligands/pores walls in the<br />
framework. Obviously, due to the lack of Ru δ+ -sites in the parent Ru-MOF, the Ru-DEMOFs<br />
exhibit higher H2 uptake than the parent Ru-MOF. To quantitatively understand the H2<br />
binding affinity of these samples, the isosteric heats of H2 adsorption (–Qst) was calculated<br />
and reveal an order with 1c > 1a > parent Ru-MOF when comparing the respective values<br />
at 1 mmol (H2) / Ru2-paddlewheel (what might be considered as the saturation<br />
adsorption of H2 at the regular paddlewheel) (Figure 4.30). This suggests stronger binding<br />
affinity of H2 for Ru-DEMOF with 32% of incorporated 5-OH-ip (sample 1c), which again<br />
is attributed to the relative higher amount of Ru δ+ -sites in 1c.<br />
8 parent Ru-MOF<br />
1a<br />
1c<br />
7<br />
6<br />
5<br />
0.0<br />
0.0 0.5 1.0 1.5 2.0 2.5 3.0<br />
H 2<br />
adsorbed, mmol/Ru 2<br />
pw<br />
Figure 4.30. Isosteric heats of adsorption of 1a and 1c calculated from the H 2 adsorption<br />
isotherms at 77K and 87K. The vertical line stands for the position where one H 2 molecule is<br />
absorbed per Ru 2 -paddlewheel.
CO 2<br />
adsorbed, mmol/g<br />
96 Chapter 4<br />
Moving further to the 5-NH2-ip DL, respective Ru-DEMOFs (3a-3c) display the same<br />
tendencies in their absorption behavior of CO2 and H2 as in their SBET (N2). From the results<br />
of the XANES studies, we have already revealed that defects B are likely to be generated<br />
at lower doping levels 3a-c (5-NH2-ip) as compared to the samples 1a-d (5-OH-ip). This<br />
difference in defect A/B abundance leads to variation of the CO2 and H2 adsorption in case<br />
of the 3a-c series. Even though 3a-c display higher uptake of CO2 and H2 than the parent<br />
Ru-MOF, the uptake of CO2 and H2 does not further increase after the feeding level of 5-<br />
NH2-ip is raised above 10% (3a) (Figures 4.31 and 4.32). Similar to 1d, we assign the<br />
decrease of the uptake of CO2 and H2 at 1 bar observed for 3c as compared with 3a-b to<br />
more abundant type B defects.<br />
3<br />
parent Ru-MOF<br />
3a<br />
3b<br />
3c<br />
2<br />
1<br />
0<br />
0 200 400 600 800 1000<br />
P, mbar<br />
Figure 4.31. CO 2 isotherms collected at 298 K for the parent Ru-MOF and its derivatives 3a, 3b<br />
and 3c with 5-NH 2 -ip DL. Black circles – parent Ru-MOF; blue triangles – 3a; dark cyan diamonds<br />
– 3b; magenta squares – 3c.
CO 2<br />
adsorbed, mmol/g<br />
H 2<br />
adsorbed, mmol/g<br />
Chapter 4 97<br />
8<br />
6<br />
4<br />
2<br />
parent Ru-MOF<br />
3a<br />
3b<br />
3c<br />
0<br />
0 200 400 600 800 1000<br />
P, mbar<br />
Figure 4.32. H 2 isotherms collected at 77 K for the parent Ru-MOF and its derivatives 3a, 3b and<br />
3c with 5-NH 2 -ip DL. Black circles – parent Ru-MOF; blue triangles – 3a; dark cyan diamonds – 3b;<br />
magenta squares – 3c.<br />
3.0<br />
2.5<br />
2.0<br />
parent Ru-MOF<br />
4a<br />
1.5<br />
1.0<br />
0.5<br />
0.0<br />
0 200 400 600 800 1000<br />
P, mbar<br />
Figure 4.33. CO 2 isotherms measured at 298 K for the parent Ru-MOF and Ru-DEMOF 4a (17%)<br />
with 5-Br-ip DL. Black circles – parent Ru-MOF; blue triangles – 4a.
H 2<br />
adsorbed, mmol/g<br />
98 Chapter 4<br />
8<br />
6<br />
4<br />
2<br />
parent Ru-MOF<br />
4a<br />
0<br />
0 200 400 600 800 1000<br />
P, mbar<br />
Figure 4.34. H 2 isotherms measured at 77 K for the parent Ru-MOF and Ru-DEMOF 4a (17%) with<br />
5-Br-ip DL. Black circles – parent Ru-MOF; blue triangles – 4a.<br />
Another indication of the suggested counter acting effects of the defect sites is the<br />
comparison of the CO2 and H2 uptakes at 2a, 2b and 4a with the parent Ru-MOF (Figures<br />
4.33, 4.34, 4.35 and 4.36). However, the variations are too small to be regarded as<br />
significant. Still, some assumptions can be concluded, which afford us some ideas on the<br />
future design of DEMOFs towards considerable optimization of sorption properties. In<br />
spite of the creation of defects A with Ru δ+ -sites, the rather small change of the H2 and CO2<br />
uptake in the sample of 4a (17% 5-Br-ip) might be contributed to the functional –Brgroups<br />
from the 5-Br-ip linker at the defect-sites. One the one hand, they may create larger<br />
steric hindrances (compared to the other DLs used) blocking, thus, the access for the gas<br />
molecules in spite of the modified paddlewheels with more rooms around Ru-sites. On the<br />
other hand, weaker H2 binding affinity has been found in MOFs composed of ligands with<br />
electron-withdrawing groups. [229-230] Although this influence caused from the interaction<br />
between H2 and ligands is smaller in comparison with the strong one of H2-M sites, it can<br />
be one reason of the observation study in the sample 4a.
CO 2<br />
adsorbed, mmol/g<br />
Chapter 4 99<br />
3.5<br />
3.0<br />
2.5<br />
parent Ru-MOF<br />
2a<br />
2b<br />
2.0<br />
1.5<br />
1.0<br />
0.5<br />
0.0<br />
0 200 400 600 800 1000<br />
P, mbar<br />
Figure 4.35. CO 2 isotherms collected at 298 K for the parent Ru-MOF and DEMOF derivatives 2a<br />
(15%) and 2b (28%) with ip DL. Black circles – parent Ru-MOF; blue triangles – 2a; dark cyan<br />
diamonds – 2b.<br />
The CO2 and H2 adsorption isotherms of 2a and 2b show that 2a exhibits higher uptake.<br />
The adsorption capacity of the sample 2b revealed to be a little lower compared to 2a<br />
while it is still the same as with the parent Ru-MOF (Figures 4.35 and 4.36). Although the<br />
defects B in the Ru-DEMOFs 2a and 2b do not induce ruthenium reduction, vacant-sites<br />
caused from the creation of defects B (missing of Ru-paddlewheels) could still<br />
accommodate gas molecules. In addition, the vacant-sites in the defects B make the gas<br />
molecules access to the surrounding CUS easier. This could be the positive effect of the<br />
defects B in the Ru-DEMOFs with ip DL. On the other hand, the generation of defects B<br />
leads to the partial missing of the di-ruthenium PW units and, hence, the overall CUSs in<br />
Ru-DEMOFs decrease. In the case of Ru-DEMOF 2a, the positive effect of the defects B is<br />
rather dominant and results in the higher H2 and CO2 capacity. But when it comes to 2b,<br />
the negative effect of the defects B eliminates the positive influence on the gas uptake,<br />
which leads to the observation we see in Figures 4.35 and 4.36. The Ru-DEMOFs 1a and<br />
1c featuring higher gas (H2 and CO2) uptake in comparison with 2a (Table 4.6), implying
H 2<br />
adsorbed, mmol/g<br />
100 Chapter 4<br />
that the enhancement of sorption of small molecules (CO2 and H2) attributed to defects A<br />
is stronger than the influence caused from defects B.<br />
8<br />
6<br />
4<br />
2<br />
parent Ru-MOF<br />
2a<br />
2b<br />
0<br />
0 200 400 600 800 1000<br />
P, mbar<br />
Figure 4.36. H 2 isotherms measured at 77 K for the parent Ru-MOF and its derivatives 2a (15%)<br />
and 2b (28%) with ip DL. Black circles – parent Ru-MOF; blue triangles – 2a; dark cyan diamonds<br />
– 2b.<br />
4.2.5 Catalytic test reactions<br />
Ethylene dimerization utilizing MOF supported catalysts has recently attracted a lot of<br />
attention due to its modifiable characteristic under molecular level. [231-234] Most of the<br />
reported MOF catalysts bear isolated single-metal (e.g., Ni, Ir) active-sites. Ru-MOF<br />
materials as heterogeneous catalysts for the ethylene dimerization have not been studied<br />
yet, although chemisorbed Ru-complex on de-aluminated zeolite Y and Ru-complex itself<br />
catalyzing ethylene to butene have been already reported. [235-237] It is known that the<br />
redox activity of Rh in RhCa-X Zeolite plays an important role on catalyzing ethylene<br />
dimerization. [238] Having distinct Ru-CUS available in the Ru-DEMOFs (i.e., different Ru n+ -<br />
species being potentially involved into the redox-process(es) of the reaction flow),
Chapter 4 101<br />
samples 1a (8% of 5-OH-ip) and 1c (32% of 5-OH-ip) have been selected for testing them<br />
as catalysts for ethylene dimerization. In addition, parent Ru-MOF has been used as a<br />
reference. Thus, activated Ru-DEMOFs were loaded into a reactor to catalyze ethylene<br />
Table 4.7. The conversion of ethylene to butene in toluene under different conditions.<br />
Entry Catalyst (mg) Temperature ( °C) Time (h) Additive TOF (h -1 )<br />
1 1c (2.5) 80 24 ---- 0.92<br />
2 1c (2) 80 1 Et 2 AlCl 4.38<br />
3 1c (2) 80 1 ---- 0.88<br />
4 1c (2.4) 26 2 Et 2 AlCl 2.15<br />
5 1c (2.1) 80 2 Et 2 AlCl 4.36<br />
6 1a (2) 80 2 Et 2 AlCl 2.3<br />
7 Parent Ru-MOF (1.8) 80 2 Et 2 AlCl 2.05<br />
dimerization in toluene at different temperatures under the pressure of 800 psi (≈ 55 bar).<br />
In general, all reactions led to the formation of butene without producing any other α-<br />
olefins (Tables 4.7). Addition of Et2AlCl as co-catalyst accelerates the conversion (Table<br />
4.7, entry 2 vs. entry 3). When the reaction has been conducted at 26 °C, lower yield has<br />
been obtained compared to those at 80 °C (Table 4.7, entry 4 vs. entry 5). However,<br />
reactions conducted for 1 h and 24 h give almost the same TOF (0.88 vs. 0.92 h -1 ),<br />
suggesting that the Ru-DEMOF 1c does not suffer the deactivation as a function of onstream<br />
time. Therefore, parent Ru-MOF and Ru-DEMOFs 1a and 1c have been employed<br />
to study the dimerization of ethylene in toluene under optimized condition (800 psi, 80<br />
°C, 2 h) in the presence of Et2AlCl. The obtained product was analyzed by gas<br />
chromatography. As it can be seen from entry 5-7 in Table 4.7 and Figure 4.37, the TOF<br />
value of 1a and 1c increase along with increase of the incorporation level of DL in<br />
comparison with the parent Ru-MOF. Since the contents of the reduced Ru δ+ -sites in 1c is<br />
the highest among the 1a-d series (according to our study above), there should be more<br />
M-CUSs in 1c and therefore it affords the chance to enhance the catalytic activity in the<br />
reaction. Indeed, the transformation of ethylene to butene is the highest (TOF = 4.36 h -1 )<br />
when employing 1c as a catalyst. This value is still much lower than that using zeolite<br />
supported Ru-complex catalysts in the presence of H2 (4.36 vs. 216 h -1 ). However, it is<br />
higher than the TOF value (1 × 10-4 s -1 = 0.36 h -1 ) in the reported reaction without the
102 Chapter 4<br />
presence of H2. [236] Distinction between butene isomers, optimization of the reaction<br />
conditions using Ru-DEMOF materials (such as usage of H2) as well as clarifying the<br />
mechanism of this reaction are outside the scope of this thesis. Nevertheless, the<br />
preliminary results give a rather clear hint that obtained Ru-materials could be utilized as<br />
catalyst for the dimerization of ethylene. Due to the diverse modification of MOF materials<br />
themselves, our current investigations on the ethylene dimerization using Ru-DEMOFs<br />
can afford a platform for further studies on MOFs as catalysts in this field.<br />
Figure 4.37. The tendency of TOF value for parent Ru-MOF and Ru-DEMOF samples 1a and 1c<br />
utilized as catalysts for transformation of ethylene into toluene (800 psi, 80 °C, 2h) in the presence<br />
of Et 2 AlCl (0.81 ml, 1M in heptane). TOF (turnover frequency) = mol product / (mol Metal<br />
(catalyst)*h).<br />
Paal-Knorr pyrrole synthesis has attracted great attention due to the huge synthetic<br />
variety of pyrroles and their derivatives, which are key intermediates for various<br />
pharmaceutical drugs. [239-240] The reaction is typically performed under protic or Lewis<br />
acidic conditions, [241-243] using primary amines and diketones. Ruthenium complex as<br />
catalysts for pyrrole synthesis was rather rare, [244] where the usage of formate salts such<br />
as sodium formate as activators is required. Due to the ability of MOFs on tuning the pore<br />
size and modifying the diverse structure, MOFs have explored to be as catalysts on various<br />
reaction. [29] Phan et al. reported IRMOF-3 as heterogeneous catalyst for the Paal–Knorr
Chapter 4 103<br />
reaction of benzyl amine with 2,5-hexanedione, where it was mentioned that the catalytic<br />
sites might be related to the structure defects. As we know from earlier reports, parent<br />
Ru-MOF ([Ru3(BTC)2Y1.5]n) is constructed from Ru2-paddlewheels, in which the axial Rupositions<br />
are partly occupied by strongly binding Y or by other weakly guest molecules.<br />
After thermal treatment, a fraction of the axial positions can be exposed as open Lewis<br />
acidic sites (useful as catalytic site, for instance). With regard to the structure of the Ru-<br />
DEMOFs discussed in this contribution, two kinds of defects are present. The modified<br />
paddlewheel units (defects A) could provide the materials with additional sites around<br />
the partly reduced Ru-centers. On the other hand, the eliminated entire Ru-paddlewheel<br />
clusters (defects B) can form vacant-sites to play a role on affecting the adsorption<br />
properties, especially when the functional X-group at the defect generating linker is as<br />
small as H. Hence, Ru-DEMOFs 1a-1c, 2a and 2b have been utilized for catalyzing the<br />
reaction of 2,5-hexadione and aniline in toluene at 90 °C to form dimethyl-phenyl-1Hpyrrole<br />
(Scheme 4.1).<br />
Scheme 4.1. Scheme of the Paal-Knorr reaction.<br />
It is interesting to note that all of the selected Ru-DEMOFs show apparently enhanced<br />
conversion of aniline to the pyrrole within the initial 4 hours in comparison with the<br />
parent Ru-MOF (Figure 4.38). Among the used materials, Ru-DEMOFs 1a and 2a exhibit<br />
the highest catalytic activity, although the other Ru-DEMOFs (1b, 1c, 1d and 2b)<br />
incorporate more DL (Table 4.8). The steric hindrances and distinct defect types (A vs. B)<br />
could be the main reason of this phenomenon. When Ru-DEMOF samples with 5-OH-ip DL<br />
(1a-d) were employed as catalysts, the yield of pyrrole has been increased from 48%<br />
(using parent Ru-MOF as the catalyst) to 58% (1d), 65% (1c), 73% (1b) and 77% (1a),<br />
respectively. This is assigned to the presence of the reduced Ru-centers (defects A) in<br />
these materials. Reduced, softer binding Ru δ+ -sites can be more easily coordinated to the<br />
O atom of the carbonyl group, which favors the nucleophilic attack from the lone-pair of<br />
the amino group of aniline. However, when the incorporation of 5-OH-ip increases, the<br />
gradual dominance of the defects B in these materials probably eliminates part of the
104 Chapter 4<br />
reactive metal centers, thus, affecting the catalytic activity of the 1b-d samples. On the<br />
other hand, Ru-DEMOF 2a displays higher yield of pyrrole compared to the parent Ru-<br />
MOF (82% vs. 48%), regardless of the partial absence of the metal centers (defects B)<br />
(Figure 4.39). This could be a result of the smaller steric hindrance surrounding the Ru-<br />
CUSs while employing the H2ip DL. When the contents of the incorporated DLs are rather<br />
small (i.e., as in 2a), the negative influence caused by missing metal centers is relatively<br />
insignificant compared with the positive effect of the smaller steric hindrance. Therefore,<br />
2a Ru-MOF material shows as high catalytic activity in present reaction as 1a. Similar<br />
observations have been found for the samples 1b-c because of the somewhat larger steric<br />
hindrance of OH-groups in spite of the type A defect in these materials. To note, using<br />
IRMOF-3 as catalysts in the same reaction, 96% conversion after 60 min was achieved.<br />
However, this could be attributed to the higher regent ratio (aniline: 2,5-hexanedione =<br />
1:1.7). [245] Nevertheless, the current study using Ru-DEMOFs as catalysts give us insight<br />
into the influence of catalytic activity caused by different defect types. For further<br />
investigation, it would also be interesting to optimize the catalytic activity by improving<br />
the regent ratio.<br />
Figure 4.38. Time-yield plot of Paal-Knorr synthesis of aniline reacting with 2,5-hexadione, giving<br />
the pyrrole employing Ru-DEMOFs 1a-1d (with 8%, 20%, 32% and 37% 5-OH-ip incorporation,<br />
respectively) as catalysts in comparison with the parent Ru-MOF(parent). Blank stands for the<br />
experiment where no catalyst was added into the reaction mixture.
Yield, %<br />
Chapter 4 105<br />
Table 4.8. Comparison of the yields of pyrrole and TOF values after 4 h in the Paal-Knorr reaction<br />
for different Ru-DEMOF samples as well as the parent Ru-MOF (used as a reference).<br />
Sample Ru content (mol %) yield at 4h, % TOF(h -1 )*<br />
Parent Ru-MOF 2 48 6.17<br />
1a 2 77 9.83<br />
1b 2 73 9.25<br />
1c 2 65 8.17<br />
1d 2 58 7.25<br />
2a 2 82 10.36<br />
2b 2 57 7.09<br />
blank - 28 -<br />
* TOF value was calculated by mol of product (mol of Ru) -1 h -1 .<br />
100<br />
80<br />
60<br />
40<br />
20<br />
2a<br />
2b<br />
parent Ru-MOF<br />
blank<br />
0<br />
0 4 8 12 16 20 24<br />
Time, h<br />
Figure 4.39. Time-yield plot of Paal-Knorr synthesis of aniline reacting with 2,5-hexadione, giving<br />
the pyrrol using Ru-DEMOFs 2a (15% ip incorporation) and 2b (28% ip incorporation) as<br />
catalysts in comparison with the parent Ru-MOF. Blank stands for the experiment where on<br />
catalyst was added into the reaction mixture.
106 Chapter 4<br />
4.2.6 Conclusions<br />
Applying the solid solution approach, a range of Ru-DEMOFs ([Ru3(BTC)2-x(5-X-ip)xYy]n)<br />
isostructural to HKUST-1 were obtained with the framework incorporated DLs 5-OH-ip<br />
(1a-d), ip (2a and 2b), 5-NH2-ip (3a-c) and 5-Br-ip (4a)). Comparably high SBET have been<br />
measured for Ru-DEMOF samples (947-1302 m 2 /g) when considering the parent Ru-MOF<br />
material [Ru3(BTC)2Y1.5]n (704-998 m 2 /g). [82, 208] The highest level of DL incorporation<br />
appeared to be 37% (1d, 5-OH-ip). The data are consistent with two kinds of defects (A<br />
and B) being introduced to the Ru-DEMOFs depending on the nature of the functional<br />
groups (X) of the DLs 5-X-ip (see Figure 4.5). DLs with steric less demanding X-groups of<br />
probably still existing, but weaker coordinative binding properties as a carboxylate ligator<br />
are likely to favor type A defects, defined as modified paddlewheel nodes exhibiting<br />
reduced Ru δ+ -sites. Along with the increasing of the DL contents, defects of type B, i.e.<br />
missing node defects, can be created simultaneously in the DEMOFs. When the functional<br />
groups in the DL 5-X-ip are much smaller than carboxylate and non-coordinating X (such<br />
as H), the defects of type B, defined as missing node defects, apparently become more<br />
dominant even in case of low doping level (case of 2a and 2b). The more or less<br />
simultaneous presence of two kinds of defects leads to the synergetic and as well<br />
counteracting effects on the porosity, sorption and catalytic properties. In fact, Ru-DEMOF<br />
1c (32% 5-OH-ip incorporation), in which defects of type A are more dominant, reveals<br />
the highest BET surface area (1302 m 2 /g) among the all samples, including parent Ru-<br />
MOF and its DEMOF derivatives reported so far. [138] Concerning the enhanced gas sorption<br />
properties, type A defects are more important than those effects related to the defects of<br />
type B, as reduced and more accessible Ru δ+ -sites have been produced in defect type A.<br />
When it comes to the catalytic activity, Ru δ+ -sites in Ru-DEMOF 1c are suggested to be<br />
responsible for the significant increase of TOF value of ethylene dimerization, as clearly<br />
seen while comparing with the parent Ru-MOF and 1a, in which no or less Ru δ+ -sites are<br />
present. However, in case of Paal-Knorr pyrrole reaction, the possible steric hindrance<br />
between the functional groups (OH) at the DL and 2,5-hexadione substrate is suggested<br />
to be responsible for the reduced activity of the Ru-DEMOFs 1a-d, although they all<br />
feature enhanced conversion compared with the parent Ru-MOF. All in all, the described<br />
Ru-DEMOFs obtained via solid solution approach employing various DLs turned out to be<br />
rather complex materials to be studied and characterized. Nevertheless, the observed<br />
spectroscopic evidences as well as effects on sorption properties and catalytic
Chapter 4 107<br />
performance reasonably fit into a model of the two types of defects, modified and missing<br />
nodes (see Figure 4.5), respectively.
108 Chapter 4<br />
4.3 Defects Engineering in [Cu3(BTC)2]n: Effect of the synthetic parameters<br />
To date, the introduction of defects into the [M3(BTC)2]n structure has been achieved via<br />
mixed-linker solid solutions approach for frameworks where M = Cu or Ru. [136, 138-140] By<br />
varying the DLs, simultaneously mixed with H3BTC during the synthesis, DEMOFs with a<br />
general formula [M3(BTC)2-x(DL)x]n could be obtained. Interestingly, in spite of the very<br />
similar structural long range order of the DEMOFs, local point defects can influence the<br />
metal environment at the PW and also enhance structural properties such as porosity.<br />
Different types of defect A and B in Ru-DEMOFs as well as their influence on the sorption<br />
and catalytic properties have already been described in Chapter 4.2. More interestingly,<br />
incorporation of pydc into [M3(BTC)2]n, the generation of reduced metal sites was found<br />
in both the formed Ru-DEMOFs ([Ru3(BTC)2-x(pydc)xYy]n) [138] and Cu-DEMOFs<br />
([Cu3(BTC)2-x(pydc)x]n) [139] However, only in the former case, CO2 → CO dissociative<br />
chemisorption (“reduction”) at low temperature (90 K) under UHV conditions was<br />
achieved. Utilizing 5-OH-ip as DL during the MOF synthesis, the mesopores prefer to be<br />
generated in Cu-DEMOFs rather than in Ru-DEMOFs. Moreover, even the modification of<br />
the doping level of the same DL in Cu-DEMOF can control the formation of the framework<br />
with micropores or mesopores. [139] Recently, Hupp et al. reported the formation of<br />
missing Cu 2+ node defects in the obtained Cu-DEMOF with ip incorporation, [140] while<br />
defect type A (modified PW units) related Cu + formation was observed in the Cu-DEMOF<br />
with pydc or other 5-X-ip(X = OH, CN, NO2) incorporation. [139] With regard to these<br />
accounts, it is essential to understand the structural complexity of DEMOFs, which will be<br />
beneficial to tailor their advanced properties. Therefore, in comparison with rather<br />
complicated Ru-(DE)MOFs system and following the description of Cu-DEMOFs reported<br />
by Hupp et al. and Fang et al., the relative simple [Cu3(BTC)2]n has been chosen as a<br />
candidate here to be incorporated by ip DL under different synthetic conditions (e.g.<br />
solvent, nature of the metal salts). Systematically study on the formation of M-DEMOFs<br />
variants of [M3(BTC)2]n structure, namely, types of local defects (i.e. the generation of<br />
reduced metal-sites or not), their origin as well as the dependence on variation of the<br />
synthetic conditions will be investigated.
Intensity, a. u.<br />
Chapter 4 109<br />
4.3.1 Preparation and characterization of Cu-DEMOF samples [Cu3(BTC)2-x(ip)x]n<br />
All samples D1-8 have been prepared via mixed-linker soild solution approach with<br />
distinct relative H3BTC : H2ip molar ratios under solvothermal conditions (80 °C, 20 h).<br />
For each sample, various Cu-salts and solvents (DMF or EtOH) have been employed.<br />
Samples D5 and D6 are prepared following reported method. [140]<br />
4.3.1.1 Solids obtained using Cu(BF4)2∙6H2O as metal precursor<br />
D4<br />
D3<br />
D2<br />
D1<br />
Cu-BTC_sim.<br />
5 10 15 20 25 30<br />
2, degree<br />
Figure 4.40. PXRD patterns of the activated Cu-DEMOF samples D1-4 in comparison with the<br />
patterns simulated from the single-crystal XRD data of the reported [Cu 3 (BTC) 2 ] n (Cu-BTC_sim).<br />
Metal source: Cu(BF 4 ) 2 6H 2 O. Solvent used for synthesis of D1 and D2 (blue patterns): DMF; for<br />
D3 and D4 (red patterns): EtOH.<br />
PXRD patterns of all activated samples D1-4 (Figure 4.40) match well with the simulated<br />
patterns of [Cu3(BTC)2]n (Cu-BTC_sim), suggesting that they all are all phase-pure,<br />
crystalline and isostructural with the non-doped parent Cu-BTC. To note, the small double<br />
reflection of the as-synthesized sample D4_as at around 9.4°and reflections at 5.7°for the
Intensity, a. u.<br />
110 Chapter 4<br />
as-synthesized samples D2-D4_as (Figure 4.41) disappear after samples activation (i.e.<br />
heating under vacuum). Thus, the origin of these reflections might come from coordinated<br />
solvent molecules, which under employed activation conditions are subsequently<br />
removed. FT-IR spectra of all activated Cu-DEMOFs samples do not vary from the FT-IR<br />
spectrum of the parent Cu-BTC, displaying also overlapping of the characteristic bands of<br />
ip and BTC (Figure 4.42). However, the typical νs(COO) and νas(COO) bands of<br />
carboxylates are observed at around 1442 cm -1 and 1366 cm -1 , respectively. Moreover, the<br />
absence of [BF4] - (from the used Cu-salts) is confirmed, as no ν(B–F) band was found at<br />
1073 cm –1 . [208]<br />
D4_as<br />
D3_as<br />
D2_as<br />
D1_as<br />
Cu-BTC_sim.<br />
5 10 15 20 25 30<br />
2, degree<br />
Figure 4.41. PXRD patterns of the as-synthesized Cu-DEMOF samples D1-4_as in comparison<br />
with the patterns simulated from the single-crystal XRD data of the reported [Cu 3 (BTC) 2 ] n (Cu-<br />
BTC_sim). Metal source: Cu(BF 4 ) 2 6H 2 O. Solvent used for synthesis of D1 and D2 (blue patterns):<br />
DMF; for D3 and D4 (red patterns): EtOH.
Chapter 4 111<br />
H 3<br />
BTC<br />
H 2<br />
ip<br />
D4<br />
D3<br />
D2<br />
D1<br />
Cu-BTC<br />
4000 3500 3000 2500 2000 1500 1000 500<br />
wavenumber, cm -1<br />
H 3<br />
BTC<br />
H 2<br />
ip<br />
D4<br />
D3<br />
D2<br />
D1<br />
Cu-BTC<br />
2000 1500 1000 500<br />
wavenumber, cm -1<br />
Figure 4.42. IR spectra of the activated samples D1-D4 in comparison with the spectra of the<br />
parent Cu-BTC, H 3 BTC and H 2 ip. Bottom figure represents selected region from 2000 cm -1 to 350<br />
cm -1 . Metal source: Cu(BF 4 ) 2 6H 2 O. Solvent used for synthesis of the D1 and D2 (blue): DMF; for<br />
the D3 and D4 (red): EtOH.
weight loss, %<br />
112 Chapter 4<br />
100<br />
Cu-BTC<br />
80<br />
60<br />
D3<br />
40<br />
D1<br />
D2<br />
D4<br />
20<br />
100 200 300 400 500 600<br />
T, C<br />
Figure 4.43. TG curves of the prepared Cu-DEMOFs D1-4 in comparison with the parent Cu-BTC.<br />
Metal source: Cu(BF 4 ) 2 6H 2 O. Solvent used for synthesis of the D1 and D2 (blue): DMF; for the D3<br />
and D4 (red): EtOH.<br />
The thermal stability of the all obtained Cu-DEMOF samples D1-4 (Figure 4.43) is<br />
considerable preserved (decomposition temperature equals ca. 300 °C). A little decrease<br />
of thermal stability in comparison with the parent Cu-BTC (decomposition temperature<br />
is ca. 330 °C) might be attributed to the incorporation of ip DL into the MOF structures,<br />
where formation of the defects at Cu2-PW is expected (Figure 4.5). For example, Cu-COO<br />
bonds can be partially substituted by the weak interactions between benzene ring of ip<br />
and Cu-centers in case of defects of type A (modified paddlewheel). In other case (defects<br />
of type B), missing of complete nodes of the Cu2-PWs is probably to happen as well.<br />
Consequently, presence of such defects (either A, B, or both of them) may cause the slight<br />
decrease of the thermal stability of the final DEMOFs.<br />
4.3.1.2 Cu-DEMOFs obtained using Cu(NO3)2·3H2O as metal precursor<br />
The phase purity and crystallinity of all samples D5-8 have been confirmed by the PXRD<br />
analysis of both as-synthesized and activated solids (Figures 4.44 and 4.45). Besides,
Intensity, a. u.<br />
Intensity, a.u.<br />
Chapter 4 113<br />
D8_as<br />
D7_as<br />
D6_as<br />
D5_as<br />
Cu-BTC_sim.<br />
5 10 15 20 25 30<br />
2, degree<br />
Figure 4.44. PXRD patterns of the as-synthesized Cu-DEMOF samples D5-8_as in comparison<br />
with the patterns simulated from the single-crystal XRD data of the reported [Cu 3 (BTC) 2 ] n (Cu-<br />
BTC_sim). Metal source: Cu(NO 3 ) 2·3H 2 O. Solvent employed for the synthesis of the D5 and D6<br />
(olive patterns): DMF plus HBF 4 ; for D7 and D8 (magenta patterns): only DMF.<br />
D8<br />
D7<br />
D6<br />
D5<br />
Cu-BTC_sim.<br />
5 10 15 20 25<br />
2, degree<br />
Figure 4.45. PXRD patterns of the activated Cu-DEMOF samples D5-8 in comparison with the<br />
patterns simulated from the single-crystal XRD data of the reported [Cu 3 (BTC) 2 ] n (Cu-BTC_sim).<br />
Metal source: Cu(NO 3 ) 2·3H 2 O.
weight loss, %<br />
114 Chapter 4<br />
recorded PXRD patterns are in a good agreement with the patterns simulated from the singlecrystal<br />
XRD data of the reported [Cu 3 (BTC) 2 ] n , suggesting all prepared Cu-MOFs being<br />
isostructural analogs of the parent Cu-BTC. These observations indicate that Cu-DEMOFs with ip<br />
DL incorporation can be prepared employing various Cu-precursors. However, only in the case of<br />
using DMF as a reaction medium, phase-pure solids have been obtained. Similarly, synthesis of the<br />
D7 and D8 in EtOH instead of DMF yielded precipitates with additional unknown phases (Figure<br />
7.23).<br />
Like in the case of Cu-DEMOFs D1-4, IR spectra of the samples (D5-8) obtained from the<br />
reaction of Cu(NO3)2·3H2O and mixed linkers do not differ from the parent Cu-BTC (Figure<br />
4.46). The presence of the residues from the starting metal precursors can be ruled out,<br />
as no bands of [NO3] - (845-815 cm -1 ) is observed in the spectra of the prepared DEMOF<br />
solids, which supports the conclusions made above on their phase purity. TGA curves of<br />
all samples D5-8 show a slight decrease of thermal stability (Figure 4.47), in analogy to<br />
the other four Cu-DEMOFs D1-4 obtained using Cu(BF4)2 6H2O as metal precursor,<br />
suggesting no significant influence of the metal source on the thermal stability of the<br />
resulting DEMOFs.<br />
100<br />
80<br />
D8<br />
Cu-BTC<br />
60<br />
D6<br />
40<br />
D5<br />
D7<br />
20<br />
100 200 300 400 500 600<br />
T, C<br />
Figure 4.46. TG curves of the Cu-DEMOFs D5-8 in comparison with the parent Cu-BTC. Metal<br />
source: Cu(NO 3 ) 2·3H 2 O. Solvent used for preparation of the D5 and D6 (olive): DMF plus HBF 4 ; for<br />
D7 and D8 (magenta): only DMF.
Chapter 4 115<br />
H 3<br />
BTC<br />
H 2<br />
ip<br />
D8<br />
D7<br />
D6<br />
D5<br />
Cu-BTC<br />
4000 3500 3000 2500 2000 1500 1000 500<br />
wavenumber, cm -1<br />
H 3<br />
BTC<br />
H 2<br />
ip<br />
D8<br />
D7<br />
D6<br />
D5<br />
Cu-BTC<br />
2000 1750 1500 1250 1000 750 500<br />
wavenumber, cm -1<br />
Figure 4.47. IR spectra of the activated samples D5-D8 in comparison with the parent Cu-BTC as<br />
well as used linkers H 3 BTC and H 2 ip. Right figure represents selected region from 2000 cm -1 to<br />
350 cm -1 . Metal source: Cu(NO 3 ) 2·3H 2 O. Solvent used for preparation of the D5 and D6 (olive):<br />
DMF plus HBF 4 ; for D7 and D8 (magenta): only DMF.
116 Chapter 4<br />
4.3.2 Composition and porosity of the prepared Cu-DEMOFs<br />
In order to determine the presence and amount of the framework incorporated DL ip in<br />
the Cu-DEMOF solids, 1 H-NMR spectroscopic measurements have been performed on all<br />
activated samples (which were previously acid-digested). Apart from the resonance at ca.<br />
8.6 ppm, which originates from the aromatic protons of BTC, three additional peaks<br />
appear at ca. 7.6, 8.1 and 8.4 ppm in all Cu-DEMOF samples D1-8 (Figures 7.15-7.22),<br />
which could be attributed to the aromatic protons of ip DL. The ratio of incorporated ip to<br />
the total linkers-amount (BTC+ ip) in the obtained solids have been estimated from the<br />
integrals of the proton resonances in 1 H-NMR spectra and are listed in Table 4.9.<br />
Table 4.9. The incorporation of ip (calculated from the integration of proton-signals in 1 H-NMR<br />
spectra) and BET surface area (estimated from the N 2 sorption experiments (at 77 K)) of the<br />
obtained Cu-DEMOFs.<br />
Samples<br />
Metal source<br />
Synthesis<br />
solvent<br />
Molar ratio of ip : (BTC + ip)<br />
feeding<br />
incorporation<br />
(obtained)<br />
S BET (m 2 /g)<br />
D1 Cu(BF 4 ) 2·6H 2 O DMF 1/2 20% 1833<br />
D2 Cu(BF 4 ) 2·6H 2 O DMF 2/3 25% 2030<br />
D3 Cu(BF 4 ) 2·6H 2 O EtOH 1/2 12% 1931<br />
D4 Cu(BF 4 ) 2·6H 2 O EtOH 2/3 17% 1973<br />
D5 Cu(NO 3 ) 2·3H 2 O DMF+HBF 4 1/2 23%, 28%* 1841, -*<br />
D6 Cu(NO 3 ) 2·3H 2 O DMF+HBF 4 2/3 33%, 33%* 1305, 2030*<br />
D7 Cu(NO 3 ) 2·3H 2 O DMF 1/2 21% 1818<br />
D8 Cu(NO 3 ) 2·3H 2 O DMF 2/3 30% 1673<br />
* reported values in the literature. [140]<br />
On the whole, it might be concluded, that both metal salts that have been tested in present<br />
studies could be successfully utilized to introduce ip DL into Cu-BTC. Curiously, addition<br />
of HBF4 increases the amount of the incorporated ip (in about 2-3%) when Cu(NO3)2·3H2O<br />
is utilized. However, on the basis of the performed quantitative calculations and taking<br />
into account an error of integrals of the 1 H-NMR signals, this difference might be ignored.<br />
Hence, the incorporation amount of ip in the reproduced sample D5 can be also<br />
considered to be same as the reported values (Table 4.9). [140] In the case of usage<br />
Cu(BF4)2·6H2O, the reaction in DMF yields to higher extent of ip incorporation (about 8%
V, cm 3 /g<br />
Chapter 4 117<br />
more) in comparison with syntheses performed in EtOH. Thus, the protic EtOH solvent<br />
probably slows down to a certain degree the BTC↔ip substitution rate. Therefore, it is<br />
not surprising that the above-mentioned samples prepared from Cu(NO3)2·3H2O using<br />
EtOH instead of DMF are not phase-pure solids (Figure 7.23).<br />
600<br />
500<br />
400<br />
300<br />
200<br />
100<br />
/ Cu-BTC<br />
/ D1<br />
/ D2<br />
/ D3<br />
/ D4<br />
0<br />
0.0 0.2 0.4 0.6 0.8 1.0<br />
relative pressure, p/p 0<br />
Figure 4.48. N 2 sorption isotherms collected at 77 K for the Cu-DEMOF samples D1-4 in<br />
comparison with the parent Cu-BTC. Closed and opened symbols represent the adsorption and<br />
desorption isotherms, respectively. Black circles - Cu-BTC; blue triangles - D1; blue stars - D2; red<br />
diamonds - D3; red squares - D4. Metal source: Cu(BF 4 ) 2 ·6H 2 O. Solvent employed for the synthesis<br />
of the D1 and D2 (blue): DMF; for D3 and D4 (red): EtOH.<br />
All N2 sorption isotherms recorded at 77 K for Cu-DEMOFs D1-8 as well as the parent Cu-<br />
BTC show type I isotherms without any hysteresis loop (Figures 4.48, 4.49), suggesting<br />
their microporosity. To recall and opposed to these observations, in the Cu-DEMOFs with<br />
pydc or 5-X-ip DLs (X = NO2, CN, or OH), the generation of mesopores were reported. [139]<br />
This different behavior indicates, that the defects in Cu-DEMOFs prepared in current work<br />
tend to be isolated rather than correlated as in earlier reported homologous frameworks<br />
(Figure 4.17). Interestingly, all Cu-DEMOFs synthesized from Cu(BF4)2·6H2O (D1-4) show
V, cm 3 /g<br />
118 Chapter 4<br />
500<br />
400<br />
300<br />
200<br />
100<br />
/ Cu-BTC<br />
/ D5<br />
/ D6<br />
/ D7<br />
/ D8<br />
0<br />
0.0 0.2 0.4 0.6 0.8 1.0<br />
relative pressure, p/p 0<br />
Figure 4.49. N 2 sorption isotherms collected at 77 K for the Cu-DEMOF samples D5-8 in<br />
comparison with the parent Cu-BTC. Closed and opened symbols represent the adsorption and<br />
desorption isotherms, respectively. Black circles - Cu-BTC; olive triangles - D5; olive stars - D6;<br />
magenta diamonds - D7; magenta squares - D8. Metal source: Cu(NO 3 ) 2 3H 2 O. Solvent utilized for<br />
the synthesis of the D5 and D6 (olive): DMF +HBF 4 ; for D7 and D8 (magenta): DMF.<br />
increased SBET in comparison with the parent Cu-BTC (1561 m 2 /g) (Table 4.9). In fact, the<br />
porosity of these samples rises along with the increase of incorporated amount of ip, no<br />
matter whether DMF or EtOH has been used. Thus, enhanced porosity provides indirect<br />
indications on absence of unreacted H2ip and proves the in-framework incorporation of<br />
ip in these solids. Remarkably, Cu-DEMOF sample D2 (25% of ip incorporation) reveals<br />
the highest SBET (2030 m 2 /g) among all the samples. Furthermore, solids D6, repeated<br />
following communicated earlier method, show a little lower SBET than the reported values<br />
(2030 m 2 /g). [140] Unfortunately, there is no exact reported SBET value for D5. Only a<br />
general increase trend of SBET value along with the incorporation amount of ip was given<br />
in the earlier report. However, in current study, incorporation of higher quantity of ip, as<br />
in the case of sample D6, leads to the decreased porosity instead in comparison with D5.<br />
Similar trend has been traced for the solids D7 and D8, where the latter sample reveals a<br />
little lower SBET value than the former. Consequently, it might be possible that some guest
Chapter 4 119<br />
(e.g. H2ip, H3BTC, etc.) inclusion happens in the case of D6 and D8. Thus, the highest<br />
incorporation degree of ip in Cu-BTC should be around 25% (D2 or D5). Although utilizing<br />
Cu(NO3)2·3H2O as metal-precursor, the samples with the same incorporation level of ip<br />
could be obtained (D5, 23% ip), the usage of nitrate salt results solids with lower porosity.<br />
Attempts to incorporate even more ip most probably would lead to the guest inclusion in<br />
the pores of DEMOFs. Due to less nucleophilic and basic character of “inert” [BF4] - anion<br />
in comparison with [NO3] - , employing Cu(BF4)2·6H2O probably facilitates the selfassembly<br />
between the metal clusters and the linkers during synthesis and could avoid the<br />
guest inclusion<br />
4.3.3 Oxidation state(s) of metal-sites in prepared Cu-DEMOFs<br />
In the earlier report from Hupp and co-workers, the generation of missing Cu 2+ -nodes was<br />
proposed. [140] In order to gain a deeper understanding of the defects generated in Cu-<br />
DEMOFs under different synthetic conditions, D1 and D2 samples, which are synthesized<br />
from different Cu-salts (Cu(BF4)2·6H2O) and feature high porosity as well as distinct<br />
incorporation level of ip, have been chosen as candidates for CO probing monitored by<br />
UHV-IR spectroscopy. It is interesting to investigate if there is any presence of Cu + in the<br />
obtained solids. Thus, the bands observed at 2178 cm -1 for D1 and D2 appear at the same<br />
position as in the spectra of the parent Cu-BTC and correspond to CO bound to Cu 2+ -sites<br />
in the PW through electrostatic and σ-donation interactions (Figure 4.50). [246] Besides,<br />
additional intense bands at 2120 cm -1 due to C-O stretching vibrations that are associated<br />
with Cu + - species are seen in spectra of both D1 and D2. The appearance of Cu + - species<br />
in sample D1 and D2 can origin from several possibilities:<br />
i) “intrinsic” defects in the framework of Cu-BTC and its analogs. It is known that intrinsic<br />
defects can be present to some extent in the MOF solids. [137, 247-249] Especially, intrinsic<br />
defects in HKUST-1 has been described. [249-250] . The activation procedure (i.e. thermal<br />
treatment under vacuum) lead to some decarboxylation and “missing” COO-sites, [249]<br />
therefore, the generation of Cu + was observed. It is possible that during the thermal<br />
treatment of D1 and D2, such intrinsic defects are formed as well.<br />
ii) “intentional” defects
120 Chapter 4<br />
Figure 4.50. From left to right: UHV-IR spectra of the parent Cu-BTC and Cu-DEMOFs D1 (20% of<br />
ip) and D2 (25% of ip) upon CO dosing (p(CO): 1×10 -6 - 3×10 -4 mbar) collected at 92-98 K after<br />
annealing at 480 K. The low intensity absorption bands at 2127 cm -1 in the parent Cu-BTC indicate<br />
some inherent defects that cannot be avoided during the crystal formation. Figure has been<br />
provided by M. Kauer.<br />
As illustrated in Figure 4.5, two representative types of defects are expected in the<br />
formation of DEMOFs. The generation of defect type A (i.e. modified PWs with the creation<br />
of the reduced Cu-sites) can be also expected in the solids D1 and D2 due to the utilization<br />
of reducing agents (DMF). Although Cu + related CO bands (2127 cm -1 ) appear in parent<br />
HKUST-1, the relative intensity to Cu 2+ related CO bands (2178 cm -1 ) is lower. However,<br />
in both D1 and D2 the CO bands at 2120 cm -1 attributed to Cu + -CO interaction turn to be<br />
dominant in comparison with the bands at 2178 cm -1 . Thus it gives us a hint that presence<br />
of defect type A can be one of the possibilities. Notably, intensity of both Cu 2+ - (2178 cm -<br />
1 ) and Cu + -related bands (2120cm -1 ) decreases from D1 (20% ip) to D2 (25%). The<br />
similar scenario has been also found for the 5-OH-ip incorporated Ru-DEMOF samples<br />
described in Chapter 4.2, suggesting thus simultaneous formation of defects B upon higher<br />
doping of DL, namely missing Cu-PWs. Consequently, lower abundance of Cu 2+ and Cu +<br />
metal centers in the D2 frameworks expected, explaining observed changes of the<br />
decreased intensity of the bands related to Cu 2+ and Cu + . Cu-DEMOFs with ip (obtained<br />
also from Cu(NO3)2·3H2O) reported earlier by Hupp et al. suggest generation of only<br />
defects type B by simulation of defects. Thus, it might be possible that anions of the<br />
utilized metal precursors play an important role on intentional defects formation in Cu-
Chapter 4 121<br />
DEMOFs. Moreover, as the generation of only defect type B was observed in Ru-DEMOF<br />
analogs of HKUST-1 with ip DL, the effect from different metal ions (Cu, Ru) on the<br />
formation of intentional defects in M-DEMOFs should also be taken into account.<br />
4.3.4 Conclusions<br />
Adopting Cu(NO3)2∙3H2O and Cu(BF4)2∙6H2O as metal sources and different feeding of<br />
H2ip DL results in crystalline Cu-DEMOFs, which are isostructural analogs of Cu-BTC. All<br />
obtained Cu-DEMOF solids show good thermal stability, which appeared to be not affected<br />
by the employed reactants (i.e. metal salts and solvents). Based on the composition and<br />
porosity, DMF found to be a better reaction solvent than EtOH leading to higher<br />
incorporation degree of ip and higher porosity of the resulting DEMOFs (for the given<br />
feeding). However, when the feeding of ip is increased, the usage of Cu(NO3)2∙3H2O as<br />
precursor should be carefully monitored owing to accompanied effects of guest(s)<br />
inclusion. Nevertheless, current studies demonstrate the highest ip framework<br />
incorporation into Cu-BTC could reach up to 25%.<br />
More importantly, UHV-IR spectra recorded upon CO dosing suggest generation of Cu + in<br />
the prepared Cu-DEMOF samples D1 and D2. Two important caused factors are<br />
concluded: one is related with the intrinsic defects induced by thermal activation and the<br />
other is intentional defects (i.e. modified PWs). In the case of intentional defects, usage of<br />
reducing agents, modifying the metal precursors including the cations and anions could<br />
be the driven force to generate reduced metal-sites. In one word, even in the “simple<br />
looking” HKUST-1 (in comparison with its Ru analogs), the defect-engineering is<br />
complicated and carefully consideration is required for the elaboration.
5 Simultaneous introduction of various palladium active sites<br />
into MOF via one-pot synthesis: Pd@[Cu3-xPdx(BTC)2]n ‡<br />
Abstract<br />
Simultaneous structural incorporation of palladium within Pd-Pd and/or Pd-Cu<br />
paddlewheels as framework-nodes and Pd nanoparticles (NPs) dispersion into MOF have<br />
been achieved for the first time via one-pot synthesis. The substitution of Cu 2+ by Pd 2+<br />
within polymer carcass as well as the loading of Pd NPs have been confirmed in particular<br />
by XPS. Solids featuring such both Pd-sites show enhanced activity (compared to the<br />
parent “Pd-free” Cu-BTC) in the hydrogenation of p-nitrophenol (PNP) to p-aminophenol<br />
(PAP) using NaBH4 as a reducing agent.<br />
‡ Work in this chapter is covered in the manuscript submitted to Dalton Trans.
Chapter 5 123<br />
5.1 Introduction on the selection of metal type in MOFs<br />
High structural and compositional design ability of metal-organic frameworks (MOFs)<br />
and, hence, the ability of tailoring their properties made MOFs to be among the most<br />
topical materials over last decades. Along with linker(s) modification [64, 123, 251] and<br />
guest(s) inclusion, [252-253] variation of the metal center(s) is also a powerful tool to fine<br />
tune MOFs functionalities. In fact, both control over coordinatively unsaturated metal<br />
sites (CUS) (e.g., via “defects-engineering”) [137] and partial metal substitution (e.g., via<br />
mixed-metal “solid solution” approach) could considerably enhance MOFs activity,<br />
especially in catalysis [138, 141, 254] and selective gas sorption/separation. [255-256]<br />
Figure 5.1. Partial metal (Cu vs Mn, Zn, Co) substitution in Cu-BTC. Reprinted with permission<br />
from D. F. Sava Gallis, M. V. Parkes, J. A. Greathouse, X. Zhang and T. M. Nenoff, Chem. Mater., 2015,<br />
27, 2018-2025. Copyright (2015) American Chemical Society. [256]<br />
Combination of distinct metal-ions, which are closely related in coordination chemistry<br />
and have similar effective ionic radii (rion), like Cu 2+ (73 pm) / Zn 2+ (74 pm) couple [257] for<br />
instance, within single MOF has been reported for several structural types. [131, 255, 258] In<br />
fact, partial substitution of Cu 2+ by Zn 2+ and some other metals of 3d-row, namely Co, Fe<br />
and Mn, in HKUST-1 ([Cu3(BTC)2]n, BTC = benzene-1,3,5-tricarboxylate) has been recently<br />
reported (Figure 5.1). [133, 256] Curiously, in later case doping with second metal caused<br />
enhanced selective sorption of O2 vs N2. [256, 259] What is more challenging however, is to<br />
take benefits of solid solution approach to introduce more distinct metals of 4d- [134] or 5drow<br />
[260] as framework-nodes. In particular, metals of the platinum group are highly<br />
attractive as catalytic- / strong sorption-centers. Besides, square planar coordination is
124 Chapter 5<br />
preferred like Cu 2+ . [261-263],[264] Still, due to kinetic reasons, these metal ions are difficult to<br />
be crystallized within 3D structures [263-264] and, therefore, almost neglected in MOF<br />
field. [265] Reports on MOFs featuring Pd-Pd, Pd-M PW nodes could not be even found.<br />
Figure 5.2. (a) Structural and (b) schematic representations of the synthesis of the cuboctahedral<br />
bimetallic MOPs. Reproduced from J. M. Teo, C. J. Coghlan, J. D. Evans, E. Tsivion, M. Head-Gordon,<br />
C. J. Sumby and C. J. Doonan, Chem. Commun., 2016, 52, 276-279, with permission of The Royal<br />
Society of Chemistry. [264]<br />
Recent years the study of Ru-based MOFs has been mainly focused on the synthesis of Ruanalogues<br />
of HKUST-1, which were successfully obtained in our group. [82, 198] Following<br />
the previous studies, in this work the attention was turned also to palladium, which is well<br />
known to facilitate dissociation of molecular hydrogen (spill-over effect). [266-268]<br />
Furthermore, bimetallic Pd/M-paddlewheel (PW) complexes have been lately found to be<br />
promising economical catalysts in the intramolecular benzylic C-H amination. [269]<br />
Interestingly, to date immobilization of Pd-nanoparticles [270-273] and decoration of MOFs<br />
interior with Pd-complexes [274-275] have been investigated a lot. Moreover, porous Pd 2+ -<br />
M 2+ (M = Cu, Ni, Zn) metal-organic polyhedra have been very recently described (Figure<br />
5.2). [264] Regardless obvious interest, studies on integration of palladium as a framework<br />
node into a MOF are, however, in its infancy. [265, 276-277] Hence, considering its structural<br />
peculiarities (i.e., PW SBUs and CUSs) [35] and primary experimentally studies on [Cu3-<br />
xRux(BTC)2]n including Ru 3+ (rion = 68 pm), [257] it would be of interest to choose<br />
[Cu3(BTC)2]n (Cu-BTC) as a matrix for in-framework incorporation of Pd 2+ (rion = 86
Chapter 5 125<br />
pm) [257] via solid solution approach. However, a rigorous exclusion of reducing conditions<br />
during MOF synthesis is difficult. Even technical activation may cause reduction at some<br />
metal sites due to decarboxylation. [250] Therefore, the standard protocol for HKUST-1<br />
synthesis is, intentionally, not changed in this stage.<br />
On the other hand, loading of Pd 0 NPs onto MOF is widely investigated as gas<br />
adsorbents [273, 278-279] and catalysts in hydrogenation, [271-273, 280-281] cross coupling [272, 282]<br />
reaction and so on. [283] To note, one of the most common approaches to obtain Pd 0 @MOFs<br />
is using H2 to reduce Pd 2+ -precursor loading MOFs that are prepared via solution<br />
impregnation by soluble Pd 2+ species. In some cases, trace amount of Pd 2+ can be still<br />
observed after reduction. [282] Actually, according to the concept of post-synthetic metalion<br />
exchange, [117, 121, 284-285] Pd 2+ substitution in the metal nodes of MOFs could probably<br />
happen under this impregnation. Interestingly, the discrimination between the two Pdsites<br />
(from extra-framework loading or in-framework incorporation) is disregarded to<br />
some extent in the current literatures. Given both facts, herein an appropriate one-pot<br />
synthesis has been selected to study MOFs with simultaneous introduction of both Pd 2+ -<br />
nodes and Pd 0 NPs in one step and test their catalytic activity.
126 Chapter 5<br />
5.2 Preparation and Structure of the Cu/Pd-BTC_1-3<br />
Pd@[Cu3-xPdx(BTC)2]n (Cu/Pd-BTC_1-3) materials have been synthesized under<br />
solvothermal conditions by mixing corresponding metal salts (Pd(OOCCH3)2 and<br />
Cu(NO3)2·3H2O) with H3BTC directly in the starting reactions (see Chapter 7 on<br />
experimental details). All Cu/Pd-BTC_1-3 samples (both as-synthesized and dried<br />
phases) are crystalline solids and isostructural with the parent Cu-BTC (Figures 5.3 and<br />
5.4), indicating the preserved structure integrity after the Pd-sites introduction. Recorded<br />
Figure 5.3. PXRD patterns of the activated Pd@[Cu 3-X Pd x (BTC) 2 ] n (Cu/Pd-BTC_1-3) in<br />
comparison with the activated non-doped Cu-BTC. The vertical dash lines correspond to the peak<br />
position of the (111) planes of the face-centered cubic (fcc) Pd-structure.<br />
PXRD patterns and accordingly calculated cell parameters of Cu/Pd-BTC_1-3 match very<br />
well with the respective simulated data of the reported [Cu3(BTC)2]n single-crystal<br />
structure [35] (Figure 5.5, Table 5.1). Remarkably, intensity of the reflections at ca. 6.67,<br />
9.40 and 13.34° (2θ) assigned to the (200), (220) and (400) planes, respectively, varies<br />
(Figure 5.3). This indicates certain changes of electronic density compared to the nondoped<br />
Cu-analogue (Cu-BTC). The main contribution to the reflection of the (200) and<br />
(220) planes is due to the metal-nodes (Figure 5.6). Hence, such difference in intensities<br />
should primary stem from the partial substitution of Cu 2+ by Pd 2+ within the M2-<br />
paddlewheel units of MOFs. Thus, it indicates Pd 2+ framework incorporation. Considering<br />
the presence of Pd NPs in the discussed Cu/Pd-BTC_1-3, small reflections at 40.02°<br />
resulting from (111) planes of the face-centered cubic structure of Pd [286] are observed
Chapter 5 127<br />
(Figure 5.3). This is probably due to the rather small particle size of these Pd NPs and,<br />
therefore, hard to be detected by PXRD technique. Finally, it should be pointed out, that<br />
employing equal molar amounts of Cu- and Pd-salts or only Pd-precursor in the starting<br />
reaction mixtures, formation of only metal/metal-oxide products has been observed<br />
(Figures 7.25 and 7.26).<br />
Figure 5.4. PXRD patterns of the as-synthesized Pd@[Cu 3-X Pd x (BTC) 2 ] n in comparison with<br />
simulated patterns of the non-doped Cu-BTC.<br />
Table 5.1. Calculated cell parameters of the Cu/Pd-BTC_1-3 (TOPAS academic software and<br />
Pawley method [287] have been employed) in comparison with that obtained from the single crystal<br />
data of the reported [Cu 3 (BTC) 2 ] n . [35]<br />
Sample a (Å) V (Å 3 ) Space group R wp R exp<br />
[Cu 3 (BTC) 2 ] [35] n 26.343 18280 Fm-3m - -<br />
Cu/Pd-BTC_1 26.308 18208 Fm-3m 6.018 4.79<br />
Cu/Pd-BTC_2 26.305 18203 Fm-3m 6.618 5.17<br />
Cu/Pd-BTC_3 26.293 18178 Fm-3m 7.201 6.09
128 Chapter 5<br />
Figure 5.5. Pawley Fits of the samples Cu/Pd-BTC_1-3. Blue, olive and magenta lines represent<br />
the fitted patterns of Cu/Pd-BTC_1, 2 and 3, respectively. Black ticks - theoretical positions of the<br />
Bragg reflections; black crosses - the experimental data; violet lines - the difference between fitted<br />
and measured patterns.
Chapter 5 129<br />
Figure 5.6. Crystal structure of the Cu-HKSUT-1 ([Cu 3 (BTC) 2 ] n ) viewed along the plane (200) (a),<br />
plane (220) (b )and plane (222) (c).
130 Chapter 5<br />
5.3 Compositional characterization and sorption properties of the prepared<br />
Cu/Pd-BTC_1-3<br />
AAS analysis of the activated Cu/Pd-BTC_1-3 solids confirms quantitative incorporation<br />
of palladium. Thus, the Pd-contents and Pd : Cu ratios in the final Cu/Pd-BTC_1-3 samples<br />
remain almost unchanged with respect to the taken feeding ratios of the metal-precursors<br />
(Table 5.2). Further, SEM-EDX elemental mapping demonstrates quite homogeneous<br />
Cu/Pd distribution within obtained Cu/Pd-BTC solids (Figure 5.7).<br />
Table 5.2. Feeding and observed contents of Pd in respect to the total metal amount in Pd@[Cu 3-<br />
xPd x (BTC) 2 ] n (Cu/Pd-BTC_1-3). The incorporation Pd-percentages were calculated based on the<br />
AAS results.<br />
Sample feeding (molar%) obtained (molar%) obtained wt%<br />
Cu/Pd-BTC_1 10 9 3.9<br />
Cu/Pd-BTC_2 15 14 6.2<br />
Cu/Pd-BTC_3 20 20 9.2<br />
Figure 5.7. EDX elemental mapping of the Cu/Pd-BTC_3 solid (red – Cu; green – Pd).<br />
Incorporation of Pd 2+ into the framework as well as the Pd 0 NPs loading has been<br />
subsequently corroborated by high-resolution XPS. Figure 5.8 shows the Pd 3d core-level<br />
spectra of the Cu/Pd-BTC_1 and Cu/Pd-BTC_3 (representative samples with relatively<br />
low and high Pd-contents). Three Pd 3d doublets (3d5/2 and 3d3/2) are resolved in the<br />
deconvoluted spectra. The doublet located at 337.9 and 343.2 eV (Pd2) is characteristic<br />
for Pd 2+ species (Table 5.3). [288-289] In addition, the higher binding energies observed at<br />
338.9 and 344.2 eV for Pd1 reveal the presence of an electronically modified Pd 2+ species.<br />
Moreover, we could unambiguously rule out an assignment of both Pd 2+ species to PdO
Chapter 5 131<br />
NPs, as no typical O 1s peak at about 530 eV has been detected in the corresponding<br />
spectra, which showed only one O 1s peak at 531.8 eV originating from the carboxylate (-<br />
COO) groups in the frameworks. Therefore, both found Pd 2+ species (Pd1 and Pd2) very<br />
likely are associated with the formation of Pd-Pd and Cu-Pd framework-nodes. The<br />
doublet at ca. 335.8 and 341.0 eV is attributed to metallic Pd 0 species (Pd3), indicating the<br />
existence of Pd metallic NPs in these samples. Besides, the amount of Pd 0 NPs in the total<br />
Pd species (Pd 2+ and Pd 0 ) increases (from 33 % for Cu/Pd-BTC_1 to 44 % for Cu/Pd-<br />
BTC_3) along with the doping increase of Pd(II) acetate. TEM characterization has not<br />
been performed because of the beam sensitivity of HKUST-1, which does not allow<br />
characterization of the "pristine" Pd@[Cu3-xPdx(BTC)2]n sample as well.<br />
Figure 5.8. Pd 3d region of the deconvoluted XP spectra of the activated solids Cu/Pd-BTC_1 and<br />
3. Figure is provided by Dr. Y. Wang.
132 Chapter 5<br />
Table 5.3. The assignment of binding energies as well as the determined molar fraction of Pd 2+<br />
and Pd 0 in Cu/Pd-BTC_1 and _3.<br />
Sample<br />
Binding energy, eV<br />
Molar fraction (%)<br />
Assignment<br />
Pd 3d 3/2 Pd 3d 5/2 Pd 2+ : (Pd 2+ +Pd 0 ) Pd 0 : (Pd 2+ +Pd 0 )<br />
Cu/Pd-BTC_1<br />
Cu/Pd-BTC_3<br />
344.2 338.9 Pd 2+ (Pd1)<br />
343.2 337.9 Pd 2+ (Pd2)<br />
340.9 335.6 Pd (Pd3)<br />
344.2 338.9 Pd 2+ (Pd1)<br />
343.2 337.9 Pd 2+ (Pd2)<br />
341.2 335.9 Pd (Pd3)<br />
67 33<br />
56 44<br />
Figure 5.9. IR spectra of the activated samples Cu/Pd-BTC_1-3 in comparison with the parent<br />
Cu-BTC as well as H 3 BTC and Pd-acetate.<br />
Furthermore, any vibrations stemming neither from the non-reacted H3BTC linker nor<br />
used metal-precursors (i.e., acetate-, nitrate-groups) could be revealed in the FT-IR
Chapter 5 133<br />
spectra of all prepared Cu/Pd-BTC solids (Figure 5.9). Moreover, 1 H-NMR spectra of the<br />
digested Cu/Pd-BTC_1-3 samples show presence of only BTC-linker (Figure 5.10). Thus,<br />
absence of the resonances at about 1.9 ppm stemming from the acetate protons fully<br />
supports IR results ruling out any residuals of the employed starting Pd-reactant. Hence,<br />
the presence of Pd 2+ -sites should originate from the in-framework nodes rather than Pd 2+ -<br />
precursor loading.<br />
Figure 5.10. 1 H-NMR spectra of the digested activated Cu/Pd-BTC_1-3 samples. The vertical dash<br />
line stands for the position where the peak of CH 3 -protons from the acetic acid commonly appears.<br />
TGA suggests that thermal stability of the obtained Cu/Pd-BTC_1-3 solids is fully<br />
preserved (in comparison with the parent Cu-BTC) [35] with the decomposition<br />
temperatures close to 300 °C (Figure 5.11). The N2 (77 K) sorption isotherms recorded<br />
for obtained samples reveal type I isotherm (Figure 5.12), confirming their permanent<br />
microporosity. Brunauer-Emmett-Teller (BET) surface area of Cu/Pd-BTC_1 and _2<br />
increase a little in comparison with parent Cu-BTC (prepared under similar conditions)<br />
(Table 5.4), indicating that the presence of Pd 2+ incorporation as metal nodes in the
134 Chapter 5<br />
framework are dominant. When it turns to Cu/Pd-BTC_3, the increasing of Pd 0 NPs<br />
species results in a slight lower BET surface area in comparison with the others samples.<br />
Figure 5.11. TG curves of the prepared Pd-doped solids Cu/Pd-BTC_1-3 in comparison with the<br />
“non-doped” material Cu-BTC.<br />
Table 5.4. BET surface area (S BET ) of Cu/Pd-BTC_1-3 in comparison with the “non-doped” Cu-<br />
BTC.<br />
Sample S BET (m 2 /g) S BET (m 2 /mmol)<br />
Cu-BTC 1561 944<br />
Cu/Pd-BTC_1 (9 mol% of Pd) 1594 982<br />
Cu/Pd-BTC_2 (14 mol% of Pd) 1750 1090<br />
Cu/Pd-BTC_3 (20 mol% of Pd) 1112 700
Chapter 5 135<br />
Figure 5.12. N 2 sorption isotherms collected at 77 K for the non-doped [Cu 3 (BTC) 2 ] n (Cu-BTC) and<br />
Pd-doped solids Pd@[Cu 3-x Pd x (BTC) 2 ] n (Cu/Pd-BTC_1-3).
136 Chapter 5<br />
5.4 Synthesis, compositional characterization and sorption properties of Cu/Pd-<br />
BTC_4<br />
Before the further investigation on catalytic reaction, it is important to prepare analogous<br />
samples featuring dominant extra-framework Pd 0 NPs loading as well. As known from the<br />
earlier experiments, employing higher Pd(II) acetate (more than 20%) in the starting<br />
reaction mixture, will only lead to the formation of metal/metal-oxide products.<br />
Interestingly, PdCl2 exhibits a rather distinct coordination mode with Pd(II) acetate. [290-<br />
292] Besides, longer reaction time in solvothermal conditions could facilitate the creation<br />
of Pd NPs to some extent. Thus, it is expected that higher Pd 0 NPs dispersion can be<br />
reached in Cu/Pd-BTC_4 by altering the Pd-precursor to PdCl2 and extending the reaction<br />
time.<br />
Figure 5.13. PXRD patterns of the as-synthesized (_as) and activated (_ht) Cu/Pd-BTC_4 in<br />
comparison with the patterns simulated from the single crystal XRD data of the reported<br />
[Cu 3 (BTC) 2 ] n (Cu-BTC_sim). [35]
Chapter 5 137<br />
The phase purity and good crystallinity of Cu/Pd-BTC_4 have been proved by the<br />
comparison of the PXRD patterns (Figures 5.13) before and after activation with those<br />
simulated from the single crystal XRD data of the reported [Cu3(BTC)2]n (Cu-BTC_sim). [35]<br />
Notably, the PXRD patterns of the Cu/Pd-BTC_4 sample display higher relative intensity<br />
of the (222) reflection, which is different with the intensity of that in the parent Cu-BTC.<br />
This suggests certain electronic modification on the metal nodes in the framework (e.g.<br />
Pd 2+ substitution of Cu 2+ -sites). However, the presence of Pd NPs could not be precisely<br />
determined by PXRD. No apparent reflections at 40.02 and 46.59 °originating from (111)<br />
and (200) planes of the face-centered cubic structure of Pd are found in the PXRD patterns<br />
of the Cu/Pd-BTC_4. [286] This can be due to the rather small particle size of NPs.<br />
Cu/Pd-BTC_4<br />
Cu-BTC<br />
H 3<br />
BTC<br />
4000 3500 3000 2500 2000 1500 1000 500<br />
wavenumber, cm -1<br />
Figure 5.14. IR spectra of the Cu/Pd-BTC_4 solid in comparison with the parent Cu-BTC and the<br />
starting linker H 3 BTC.<br />
In addition, no vibrations stemming from the non-reacted H3BTC linker or employed<br />
metal-precursors (i.e. nitrate groups) could be observed in the FT-IR spectra of the
138 Chapter 5<br />
obtained Pd-doped solid (Figure 5.14), indicating the absence of nitrate from the<br />
employed for the synthesis of Cu/Pd-BTC_4 Cu-salt. The absence of Cl - in the Cu/Pd-<br />
BTC_4 sample is hard to rule out based only on the IR and 1 H-NMR data. Further<br />
characterizations, namely SEM-EDX and XPS, will addresses this issue.<br />
Figure 5.15. SEM images of the Cu/Pd-BTC samples.<br />
Figure 5.16. EDX elemental mapping of the Cu/Pd-btc_4. Red: Cu-mapping; green: Pd-mapping.<br />
Curiously, SEM image of the sample Cu/Pd-BTC_4 displays that its particles have welldefined<br />
octahedral shape and are visibly bigger (ca. 20 μm) compared to the other solid<br />
(Cu/Pd-BTC_3) (Figure 5.15). Thus, variation of the Pd-precursor apparently influences<br />
extent of palladium inclusion and morphology of the Cu/Pd-MOF particles (as also<br />
reflected in the PXRD, Figures 5.13): Pd(II) acetate favors quantitative palladium<br />
incorporation (samples Cu/Pd-BTC_1-3), while PdCl2 somehow decelerates MOF growth,<br />
leading therefore to larger crystals (sample Cu/Pd-BTC_4). SEM-EDX mapping of the<br />
Cu/Pd-BTC_4 solid shows the homogeneous distribution of Pd and Cu in the particles of<br />
framework (Figure 5.16). In addition, the formation of some Pd species where there is no<br />
contribution of Cu has also been observed. These Pd species could be assigned to Pd-Pd<br />
PWs or just Pd NPs. Due to the beam stability of Cu/Pd-BTC under high electron voltage,
Chapter 5 139<br />
it is hard to distinguish these two possibility. To note, no Cl Kα peak could be observed in<br />
the EDX spectrum of the Cu/Pd-BTC_4 (Figures 5.17), suggesting absence (at least in high<br />
concentration) of Cl - or PdCl2.<br />
Figure 5.17. EDX spectrum of the sample Cu/Pd-btc_4 with the assignments of Cl Kα and Cl Kβ<br />
(green lines).<br />
Deconvoluted XP spectra from the Pd 3d region scan has been gathered for the sample<br />
Cu/Pd-BTC_4 (Figure 5.18). In addition to the Pd 3d doublet (Pd 3d3/2 and Pd 3d5/2) of<br />
Pd 2+ at 343.6 and 338.4 eV as well as 342.4 and 337.2 eV (Table 5.5), [288-289] another<br />
doublet appears at 340.9 and 335.7 eV, which can be attributed to Pd 0 in metallic<br />
palladium. Compared with Cu/Pd-BTC_1-3, this sample reveals dominant Pd 0 than in<br />
case of Cu/Pd-BTC_1-3. The concentration of Pd 0 is determined to amount to 70 %.<br />
Likewise, in Cu/Pd-BTC_1-3, only the O 1s peak at 531.8 eV stemming from COO- has<br />
been revealed. Hence, the presence of PdO can be ruled out due to the absence of<br />
corresponding O 1s peak at about 530 eV. Moreover, the peak of Cl 2p in the survey scan<br />
of Cu/Pd-BTC_4 cannot be observed (Figure 5.19), which together with SEM result<br />
proves that the Pd 2+ in the solid is attributed from Pd 2+ /M 2+ -node in the framework rather<br />
than Pd 2+ -precursor or PdO loading on the framework.
140 Chapter 5<br />
Figure 5.18. Deconvoluted XP spectra of the Cu/Pd-BTC_ 4 in the Pd 3d region. Figure is provided<br />
by Dr. Y. Wang.<br />
Figure 5.19. XPS survey scan of the activated sample Cu/Pd-BTC_4. Figure is provided by P. Guo.
weight loss, %<br />
Chapter 5 141<br />
Table 5.5. The assignment of binding energies as well as the determined molar fraction of Pd 2+<br />
and Pd 0 in Cu/Pd-BTC_4.<br />
sample<br />
Molar fraction (%)<br />
Binding energy, eV<br />
Assignment<br />
Pd 3d 3/2 Pd 3d 5/2 Pd 2+ : (Pd 2+ +Pd 0 ) Pd 0 : (Pd 2+ +Pd 0 )<br />
Cu/Pd-BTC_4<br />
343.6 338.4 Pd 2+ (Pd1)<br />
342.4 337.2 Pd 2+ (Pd2)<br />
340.9 335.7 Pd 0 (Pd3)<br />
30 70<br />
100<br />
90<br />
80<br />
Cu-BTC<br />
Cu/Pd-BTC_3<br />
Cu/Pd-BTC_4<br />
70<br />
60<br />
50<br />
40<br />
100 200 300 400 500 600<br />
T, C<br />
Figure 5.20. TG curves of the activated Cu/Pd-BTC_4 and _5 solids in comparison with the parent<br />
Cu-BTC and Cu/Pd-BTC_3.<br />
In order to gain information on the quantitative incorporation of palladium, AAS analysis<br />
of the activated Cu/Pd-BTC_4 solids has been performed. Thus, with respect to the taken<br />
feeding ratios of the metal-precursors (20%), amount of the incorporated Pd in Cu/Pd-<br />
BTC_4 sample is 12%, which is a little lower than that in Cu/Pd-BTC_3 (20%). TGA of the<br />
Cu/Pd-BTC_4 (Figure 5.20) demonstrates the preserved thermal stability after palladium<br />
introduction and show the framework decomposition after 300 °C. Interestingly, N2
V, cm 3 /g<br />
142 Chapter 5<br />
sorption isotherms recorded at 77K for Cu/Pd-BTC_4 sample show type I isotherms<br />
(Figure 5.21), suggesting the microporosity. This is in analogy to other Cu/Pd-BTC<br />
samples described above. The higher BET surface area of Cu/Pd-BTC_4 (Table 5.6) than<br />
Cu/Pd-BTC_1-3 points to external Pd-NPs rather than included particles into the volumes<br />
of the framework. Besides, from the above described better crystallinity revealed in PXRD<br />
patterns as well as the well-shaped of the particles in SEM image, it is not surprised that<br />
this sample prepared from PdCl2 exhibit higher SBET.<br />
500<br />
450<br />
400<br />
350<br />
300<br />
250<br />
200<br />
150<br />
100<br />
50<br />
/ Cu-BTC<br />
/ Cu/Pd-BTC_3<br />
/ Cu/Pd-BTC_4<br />
0<br />
0.0 0.2 0.4 0.6 0.8 1.0<br />
relative pressure, p/p 0<br />
Figure 5.21. N 2 sorption isotherms collected at 77 K for the non-doped [Cu 3 (BTC) 2 ] n (Cu-BTC) and<br />
solids [Cu 3-x Pd x (BTC) 2 ] n (Cu/Pd-BTC_3-4).<br />
Table 5.6. BET surface areas calculated from N 2 sorption isotherms (77 K) of Cu/Pd-BTC samples<br />
in comparison with the parent Cu-BTC.<br />
Sample<br />
BET surface area (m 2 /g)<br />
Cu-BTC 1561<br />
Cu/Pd-BTC_3 1112<br />
Cu/Pd-BTC_4 2000
Chapter 5 143<br />
5.5 Catalytic test reaction<br />
Both Pd 2+ -containing MOF ([Pd(2-pymo)2]n, 2-pymo = 2-pyrimidinolate) [276-277, 293] and<br />
Pd 0 @MOF [272-273, 281-282] have been reported as good reusable catalysts in typical<br />
palladium-catalyzed reactions such as Suzuki C–C couplings and hydrogenation. Owing to<br />
both Pd 0 NPs and potential Pd 2+ -CUS (that should be available after thermal treatment<br />
and specifically promote H2 splitting) in obtained Pd-doped Cu/Pd-BTC materials, it was<br />
of interest to test their catalytic activity.<br />
Figure 5.22. Concentration of PNP as a function of time for non-doped Cu-BTC and Pd containing<br />
Cu/Pd-BTC_1-4 as catalysts in the aqueous-phase hydrogenation of PNP with NaBH 4 to PAP. The<br />
insert shows the initial reaction rate for Cu/Pd-BTC_1-4 normalized to the amount of Pd in the<br />
catalyst, respectively. Reaction conditions: c PNP = 0.18 mmol dm −3 , c NaBH4 = 0.60 mmol dm −3 , T =<br />
298 K, stirring speed = 1300 min −1 , m catalyst = 5.0 mg, ambient pressure. Figure is provided by Z.<br />
Chen.<br />
As a test reaction, the aqueous-phase hydrogenation of PNP to PAP using NaBH4 as a<br />
reducing agent has been chosen. It can be conducted at room temperature and ambient<br />
pressure within reaction times < 10 min using a simple on-line UV-Vis spectroscopy to<br />
monitor the progress of the reaction. [281, 294-295] The concentration of PNP as a function of
144 Chapter 5<br />
time as well as the initial reaction rate normalized to the amount of Pd in the catalyst for<br />
Cu/Pd-BTC_1-4 are depicted in Figure 5.22. Before addition of the solid catalyst, i.e.,<br />
within the first 0.5 min of the experiment, no PNP conversion was observed. Complete<br />
conversion of PNP to PAP was reached within 2 min of reaction time using Cu/Pd-BTC_1-<br />
4, whereas the conversion of PNP remained incomplete for the Pd-free Cu-BTC. This<br />
incomplete conversion is known for catalysts with low activity and results from<br />
unproductive NaBH4 decomposition to hydrogen. [294] Evidently, the Pd-containing Cu-<br />
BTC catalysts are significantly more active than the Pd-free Cu-BTC. Interestingly, the<br />
initial reaction rate related to the Pd amount for Cu/Pd-BTC_1 and 2 (i.e., 4.0×10 -3 and<br />
2.0×10 -3 dm -3 min -1 ) is significantly higher than that achieved over a metallic Pd catalyst<br />
supported on an Al-containing mesocellular silica foam (1.0×10 -3 dm -3 min -1 ) under the<br />
same reaction conditions. [296] Note that the activity of Cu/Pd-BTC_1 and 2 is so high that<br />
the difference in their catalytic activity cannot be distinguished under the reaction<br />
conditions used.<br />
Figure 5.23. PXRD patterns of the sample with 14% of Pd-doping after the hydrogenation of PNP<br />
to PAP (Cu/Pd-BTC_2_cat) in comparison with that one before the reaction (Cu/Pd-BTC_2). The<br />
diamond symbol represents the reflection position of Cu 2 O, which could be present due to the<br />
reduction by NaBH 4 .
Chapter 5 145<br />
Surprisingly, the normalized initial reaction rate decreases with increasing overall Pd<br />
content from 4×10 -3 dm -3 min -1 for Cu/Pd-BTC_1 to 1.0×10 -3 dm -3 min -1 for Cu/Pd-BTC_3,<br />
respectively (insert in Figure 5.22). This can be explained by considering the decreasing<br />
concentration of Pd 2+ species with increasing Pd content from Cu/Pd-BTC_1 to Cu/Pd-<br />
BTC_3 as observed by XPS (Table S3). Especially, Cu/Pd-BTC_4 containing the lowest<br />
concentration of Pd 2+ species (70%) display the lowest initial reaction rate in comparison<br />
with the other three Cu/Pd-BTC samples. It may, therefore, be concluded that Pd 2+<br />
species in the catalyst are catalytically active and that they are dominantly responsible for<br />
the observed high catalytic activity. Moreover, it has been reported that Pd 2+ can act as<br />
active metal sites in olefin hydrogenations. [276-277, 293] To note, PXRD patterns of the<br />
Cu/Pd-BTC samples before and after reaction indicate that the structure of the<br />
framework stays unchanged (Figure 5.23). Finally, according to the ICP-OES analysis of<br />
the solution after reaction (Cu/Pd-BTC_2 as selective catalysts), leaching of palladium is<br />
negligible (i.e., 0.01mg/L), indicating the stability of the used MOF catalysts as well as the<br />
heterogeneous nature of the catalytic reaction.
146 Chapter 5<br />
5.6 Conclusions<br />
In summary, via one-pot synthesis crystalline porous Pd@[Cu3-xPdx(BTC)2]n MOFs with<br />
various doping levels of Pd have been successfully obtained. On the basis of entire<br />
experimental data, structural incorporation of Pd 2+ serving as frameworks-nodes (within<br />
Cu-Pd or/and Pd-Pd paddlewheels) as well as Pd 0 NPs dispersion in the framework of<br />
HKUST-1 are concluded. To best of our knowledge, it is the singular case of MOFs bearing<br />
both Pd 2+ -paddlewheels and Pd NPs known so far. Curiously, certain dependency of the<br />
crystals morphology of Cu/Pd-BTC and extent of relative ratio of Pd-NPs and Pd 2+ -nodes<br />
on the employed Pd-precursors could be traced. Moreover, distinct Pd sites, especially<br />
Pd 2+ /M-CUS considerably enhances MOFs performance in the aqueous-phase<br />
hydrogenation of PNP to PAP comparing to the “Pd-free” Cu-BTC catalysts, which affords<br />
a perspective way to tune their catalytic activity. Furthermore, a synthesis of HKUST-1<br />
analogs excluding Pd 0 formation and featuring exclusive Pd 2+ /Cu 2+ mixed-metal PWs<br />
would lead to highly active catalysts.
6 Summary and Outlook<br />
Among all MOF’s features, one of the most important and interesting characteristics is the<br />
presence of coordinatively unsaturated metal sites (CUS). Due to much stronger affinity<br />
of many “bare” metal-ions towards some gases (e.g. H2, CO2, CH4) and organic molecules,<br />
design of CUSs within MOFs has been a key factor in enhancing MOFs performance in a<br />
variety of applications such as gas storage, gas selectivity and catalysis.<br />
HKUST-1 ([Cu3(BTC)2]n, Cu-BTC) represents one of the well-known and investigated<br />
MOFs where removal of the coordinated water molecules and, thus, generation of CUSs<br />
could be easily achieved upon heating under vacuum. Moreover, [Ru3(BTC)2Yy]n (Ru-<br />
BTC), which is mixed-valence ruthenium structural analog of HKUST-1, has been<br />
elaborated. Interestingly, this ruthenium MOF exhibits sufficient chemical as well as<br />
thermal stability, and offers rich photo/redox chemistry. Hence, in this dissertation Cuand<br />
Ru-MOFs of [M3(BTC)2Yy]n family (M = Cu, Ru, Mo, Cr, Ni, Fe; x = 0 or 1.5, respectively)<br />
have been chosen as candidates to study the modification of MOF’s local structures (via<br />
modification of CUSs, defects engineering, for instance) and its impact on their properties.<br />
First of all, controlled secondary building units approach (CSA) has been employed to<br />
study the (optimized) formation of isostructural Ru II,II and Ru II,III analogs of HKUST-1.<br />
Notably, compared to the Cu-BTC, the composition and local structure of the Ru-BTC<br />
([Ru3(BTC)2Yy]n·G g) turn to be more complex due to the mixed-valence oxidation state of<br />
Ru-centers. The last requires presence of additional counter-ions X from the employed<br />
Ru-SBUs to compensate the charge of [Ru2] 5+ PW units. Besides, some crucial synthetic<br />
parameters like solvents mixture (H2O: AcOH = 1:0.05) lead to the presence of residual<br />
acetic acid/acetate (as counter-ions X, guest molecules/species G or both) in the final<br />
frameworks. By utilizing distinct Ru II,III -SBUs (either [Ru2 II,III (OOCR)4X] or<br />
[Ru2 II,III (OOCCH3)4]A) with various nature of counter-ions X and A and alkyl groups -R, the<br />
local environment of the metal sites in the obtained isostructural MOF solids could be<br />
tuned to a certain extent. Thus, employment of the [Ru2 II,III (OOCCH3)4]A (where A is a<br />
weakly coordinating anion) instead of [Ru2 II,III (OOCR)4X] (where X is a strongly
148 Chapter 6<br />
coordinating anion), facilitates to decrease the amount of coordinated counter-ions in the<br />
framework of Ru II,III -BTC. Additionally, solvent exchange procedure is another way to<br />
remove residual AcO(H), which is occluded within the framework’s pores or strongly<br />
coordinated to the Ru-sites. Furthermore, the usage of the mono-valence Ru II,II -SBU<br />
([Ru2 II,II (OOCCH3)4]) without any counter-ions has turned to be an optimized way to<br />
prepare highly porous Ru II,II -BTC MOF featuring more accessible Ru-CUSs in comparison<br />
with its mixed-valence Ru II,III -BTC variant.<br />
Secondly, modification of the metal PWs in [M3(BTC)2Yy]n has been accomplished by inframework<br />
incorporation of a scope of di-topic isophthalate (ip) defect generating linkers<br />
DLs (5-X-ip, X = OH, H, NH2 or Br). Remarkably, two kinds of structural defects have been<br />
found in the obtained crystalline and isostructural DEMOFs. One type (A) represents<br />
modified PW nodes featuring reduced metal sites, while the other one (type B) is<br />
associated with the missing PW nodes. In fact, the abundances of these two defect types<br />
depend on the choice of the functional group X in the DLs, doping level of DL as well as the<br />
chosen MOF matrix (i.e., Cu-BTC or Ru-BTC). Moreover, the defects of type A and B in Ru-<br />
DEMOFs seem to play a key role in sorption of small molecules (i.e., CO2, CO, H2) and<br />
catalytic activity (i.e., in ethylene dimerization and Paal-Knorr reaction). Thus,<br />
investigations performed on the Ru-DEMOF and Cu-DEMOF solid solutions have shown<br />
rather a complex picture. Still, the studies on the defects characterization have pave up<br />
the way to more deep understanding of the nature of created defects and defects<br />
engineering in MOFs in general.<br />
Apart from the mixed-linker solid solution approach, mixing of distinct metal-ions via onepot<br />
synthesis has also been utilized to successfully obtain Pd-doped solids Pd@[Cu3-<br />
xPdx(BTC)2]n. To note, simultaneously structural incorporation of palladium within Pd-Pd<br />
and/or Pd-Cu PWs as framework-nodes and Pd nanoparticles (NPs) dispersion has been<br />
achieved for the first time. Interestingly, employing prepared Pd-doped Cu/Pd-BTC as<br />
catalysts revealed their enhanced activity (in comparison with the intact Cu-BTC), namely<br />
in aqueous-phase hydrogenation of p-nitrophenol (PNP) to p-aminophenol (PAP) using<br />
NaBH4 as a hydrogen source. Furthermore, the stability and heterogeneous nature of the<br />
catalysts have been confirmed.<br />
All in all, the studies presented in this dissertation provide a deep insight into the<br />
formation and structure of the complex Ru-BTC. Moreover, creation of various types of<br />
structural defects has been gained and analyzed in its defects-engineered variants (Ru-
Chapter 6 149<br />
DEMOFs). These results are essential for further studies on elaboration of the related<br />
DEMOFs. For example, one may avoid many complications by means of employing Ru II,II<br />
SBUs (instead of mixed-valence Ru II,III -SBUs) to form respectively Ru II,II -MOF, which could<br />
by subsequently used as a matrix for defects engineering. From the other side, the doping<br />
of Pd 2+ into less “complicated” Cu-BTC (because of more substitution labile Cu 2+<br />
precursors) has open a way to exploit more functionality of the resulting MOFs. What<br />
more challenging is, to strictly exclude any reducing parameters during synthesis and<br />
prepare a Pd 0 free Pd 2+ /Cu 2+ mixed-metal analog of HKUST-1. Due to the specific<br />
palladium features (like ability to split H2, etc.), this mixed-metal Cu/Pd-BTC materials<br />
including the defect engineering should hold huge promises for many applications. For<br />
instance, gas sorption (e.g. hydrogen uptake), conductivity (TCNQ loading on Cu/Pd-BTC<br />
to modify the electron density at the metal sites, TCNQ = tetracyanoquinodimethane),<br />
catalysis (e.g. using Cu/Pd-BTC as catalysts in alcohol oxidation, cross coupling reaction,<br />
etc.) are topics worth being studied. Last but not the least, phase pure mixed-component<br />
MOFs, structural analogs of HKUST-1, incorporating both Zn 2+ and Cu 2+ ions, H3BTC and<br />
5-nitroisophthalic acid defect linker have been obtained as well (See chapter 7.5).<br />
However, MOFs with only quite low concentration of the incorporated Zn 2+ (about 3%)<br />
have been obtained during this initial study. In a long run, such combination of mixedmetal<br />
and defect linker within single-phased framework could also be very attractive for<br />
advanced properties owing to the more factors (“tuning keys”) influencing modification<br />
on the metal sites.
7 Experimental Section<br />
In this Chapter various experimental and analytical procedures are given. In the first part,<br />
general analytical procedures and methods broadly used for characterization of the<br />
prepared MOF materials in this work are provided. In the second part, synthetic<br />
procedures as well as supplementary analytical details are described for each Chapter.<br />
7.1 General methods<br />
7.1.1 X-ray Diffraction (XRD)<br />
Powder XRD (PXRD) for all the bulk as-synthesized samples and most of the activated<br />
samples were performed by Dr. M. Tu, S. Wannapaiboon, and W. Zhang on an X’ Pert PRO<br />
PANalytical equipment (Bragg–Brentano geometry with automatic divergence slits,<br />
position sensitive detector, continuous mode, room temperature, Cu-Kα radiation(λ =<br />
1.54178 Å), Ni-filter, in the range of 2θ = 5–50, step size 0.01). Activated sample were<br />
prepared on a silicon wafer in an Ar-filled glovebox right before the measurement starts.<br />
For the measurement of activated samples (Ru-DEMOFs series 1 and 3), the data were<br />
collected by W. Zhang with the assistance of Dr. C. Sternemann, A. Schneemann, and S.<br />
Wannapaiboon at beam line BL9 of the synchrotron radiation facility DELTA at a<br />
wavelength of 0.4592 Å using a two-dimensional MAR345 image plate detector. The<br />
sample was filled into standard capillaries (0.5-mm diameter) in an Ar-filled glovebox and<br />
measured. The data were integrated using the program package Fit2D [297] and<br />
transformed to the CuKα radiation used for all other PXRD measurements on reported<br />
materials for the convenient comparison. PXRD of some other activated samples were<br />
collected by Dr. K. Khaletskaya, C. Rösler, and I. Schwedler in a D8-Advance Bruker AXS<br />
diffractometer with CuKα radiation at 25 °C (Göbel mirror; θ–2θscan; 2θ= 5–50°; step size<br />
= 0.0142 (2θ); position sensitive detector; α-Al2O3 as external standard. The sample was<br />
filled into 0.7 mm diameter standard capillaries in an Ar-filled glovebox and measured in<br />
Debye-Scherrer geometry. All the data were interpreted/analyzed by W. Zhang.
Chapter 7 151<br />
Single crystal XRD data for Ru-SBU were collected on an Oxford Supernova with Atlas<br />
detector (Cu-Kα 1.54184 Å) by Dr. K. Freitag and M. Winter. The crystals were coated with<br />
a perfluoropolyether, collected with a glass fiber loop under a microscope and mounted<br />
in the nitrogen cold gas stream of the diffractometer. For the air-sensitive crystals, they<br />
were transferred from a Schlenk tube in an argon stream onto a specimen holder with<br />
perfluoro-polyalkylether before being picked up with the glass fiber loop. The structural<br />
solution and refinement were done M. Winter and W. Zhang (with the assistance of, Dr. A.<br />
Puls, and Dr. S. Henke) using the program suite Olex2 [298] with the executables SHELXS97<br />
and SHELXL97. [299] For refinement the full-matrix least squares on F2 method was<br />
employed. All non-hydrogen atoms were refined anisotropically while the hydrogen<br />
atoms were calculated and refined with isotropic character.<br />
7.1.2 FT-IR spectroscopy<br />
Conventional FTIR spectra were collected by W. Zhang on a Bruker Alpha FTIR instrument<br />
in the ATR geometry with a diamond ATR unit in the range 400–4000 cm -1 inside a<br />
LABStar MB 10 compact MBraun glove-box (argon atmosphere).<br />
Ultra High Vacuum (UHV) FT-IR measurements were performed using a novel UHV-FTIRS<br />
apparatus (state‐of‐the‐art vacuum IR spectrometer (Bruker, VERTEX 80v) coupled to a<br />
novel UHV system (Prevac)) [300] by our collaboration partners, M. Kauer and P. Guo (the<br />
group of Dr. Y. Wang,) in the Laboratory of Industrial Chemistry (Prof. Dr. M. Muhler),<br />
Ruhr‐University Bochum. The sample transfer to the instrument, data acquisition and<br />
interpretation were carried out by M. Kauer and P. Guo. The discussion of the selected<br />
data and the experimental/synthetic work documented in the thesis were done by W.<br />
Zhang. The powder samples were first pressed into a stainless steel grid (0.5 x 0.5 cm)<br />
covered by gold and then mounted on a sample holder, which was specially designed for<br />
the FTIR transmission measurements under UHV conditions. The grid was cleaned by<br />
heating up to 850 K to remove all contaminants formed on it during preparation. The base<br />
pressure in the measurement chamber was 5 x 10 -11 mbar. The optical path inside the IR<br />
spectrometer and the space between the spectrometer and UHV chamber were also<br />
evacuated to avoid atmospheric moisture adsorption resulting in a high sensitivity and<br />
stability. The MOF samples were cleaned in the UHV chamber by heating to 500 K in order<br />
to remove the contaminants involved during synthesis and all the adsorbed species such
152 Chapter 7<br />
as water and hydroxyl groups. Prior to each exposure, a spectrum of the clean sample was<br />
recorded to be as a background reference. The exposure of the sample to CO and CO2 was<br />
carried out by backfilling the measurement chamber through a leak valve. All UHV-FTIR<br />
spectra were collected with 512 scans at a resolution of 4 cm -1 in transmission mode. The<br />
figures below show the UHV-FTIR apparatus (Figure 7.1) and the schematic<br />
representation of the whole optical path of the IR beam in both reflection and<br />
transmission geometries (Figure 7.2).<br />
Figure 7.1. The UHV‐FTIRS apparatus in (a) perspective view and (b) top view. The labeled<br />
components are: (1) load‐lock, (2) distribution, (3) magazine, (4) measurement (FTIR) chambers,<br />
(5) sample manipulator, (6) vacuum FTIR spectrometer, (7) preparation chamber (planned).<br />
Reprinted with permission from Y. Wang, A. Glenz, M. Muhler, C. Wöll, Rev. Sci. Instrum. 2009, 80,<br />
113108‐6, with the permission of AIP Publishing. [300]
Chapter 7 153<br />
Figure 7.2. Schematic representation of different types of IR measurements: (a) reflectionabsorption<br />
at grazing incidence, (b) transmission. Reprinted with permission from Y. Wang, A.<br />
Glenz, M. Muhler, C. Wöll, Rev. Sci. Instrum. 2009, 80, 113108‐6, with the permission of AIP<br />
Publishing. [300]<br />
7.1.3 Nuclear Magnetic Resonance (NMR) Spectroscopy<br />
Liquid phase 1 H-NMR spectra for the digested activated MOFs were measured and<br />
analyzed by W. Zhang on a Bruker Avance DPX-200 spectrometer at 293 K using TMS as
154 Chapter 7<br />
internal standards and normalizing the signals to the DMSO-d6 signal. The samples were<br />
digested in 0.5 ml DMSO-d6 and 0.1 ml DCl (38 wt %)/D2O(99 %) in a NMR tube. Spectra<br />
for Ru-(DE)MOFs were collected with 512 scans and for the other samples with 128 scans.<br />
7.1.4 Thermogravimetric analyses (TGA)<br />
The thermogravimetric analyses (TGA) data were collected and analyzed by W. Zhang<br />
using a TG/DSC NETZSCH STA 409 PC instrument at a heating rate of 5 K min -1 in a<br />
temperature range from 30–600 °C at atmospheric pressure under flowing N2 (N2<br />
,99.999%; gas flow, 20 ml min -1 ). The sample weight is in a range of 7-12 mg. Activated<br />
sample was filled in a crucible with a vial in an Ar-filled glove-box and immediately used<br />
for the measurement.<br />
7.1.5 Scanning Electron Microscopy (SEM) and Energy-dispersive X-ray<br />
spectroscopy (EDX)<br />
SEM images and EDX mapping were recorded from an FEI ESEM Dual Beam TM Quanta 3D<br />
FEG microscope by Dr. K. Khaletskaya and S. Cwik. In order to increase the conductivity<br />
of MOF samples, they were coated with gold by Dr. R. Neuser prior to being loaded in the<br />
instrument. Sample preparation for the SEM measurement and analysis were done by W.<br />
Zhang.<br />
7.1.6 Transmission electron microscope (TEM) and EDX<br />
Bright filed transmission electron microscope (BFTEM) images and EDX spectra for the<br />
composition determination of Ru-DEMOFs were recorded on a Tecnai G 2 F20 equipped<br />
with a Schottky field emission gun operated at an acceleration voltage of 200 kV by Dr. C.<br />
Wiktor at the department of Mechanical Engineering, Ruhr-University Bochum. Data<br />
analysis was done by W. Zhang.<br />
7.1.7 Elemental Analysis / Atomic absorption spectroscopic (AAS)<br />
EA / AAS analysis data for Ru-(DE)MOFs were obtained from the Mikroanalytisches<br />
Laboratorium Kolbe in Mülheim an der Ruhr (http://www.mikro-lab.de/index.html).<br />
Samples were filled into finger schlenks in an Ar-filled glove-box by W. Zhang and
Chapter 7 155<br />
measured under Ar. Atomic absorption spectroscopic (AAS) analysis for mixed-metal<br />
materials to determine Cu, and Pd contents were performed in the Microanalytical<br />
Laboratory of the Department of Analytical Chemistry at the Ruhr‐University Bochum by<br />
K. Bartholomäus. An AAS apparatus by Vario of type 6 (1998) was employed. Data<br />
interpretation was done by W. Zhang.<br />
7.1.8 Gas Sorption<br />
Experiments on sorption of CO2 (298 K) and H2 (77 K) as well as CO (298K) was performed<br />
with assistance of D. J. Xiao and D. Reed (the group of Prof. J. R. Long) at the Department<br />
of Chemistry in the University of California, Berkeley (USA). Part of the N2 sorption data<br />
were collected and interpreted by N. Arshadi at the laboratory of Industrial Chemistry<br />
department (Prof. Dr. M. Muhler) using a Quantachrome Autosorp-1 MP instrument. Most<br />
of N2 sorption data were collected and analyzed by W. Zhang.<br />
CO adsorption (298 K) and the majority of N2 (99.999%) sorption (77 K) measurements<br />
were performed using a Micromeritics 3Flex instrument. The N2 sorption isotherms of Ru-<br />
DEMOFs with defect 5-NH2-ip linker (3a-3d) samples were collected using a<br />
Quantachrome Autosorp-1 MP instrument, optimized protocols and N2 of 99.9995 %<br />
purity. Sorption isotherms of CO2 (298 K) and H2 (77 K) were conducted on a<br />
Micromeritics ASAP 2020 gas adsorption analyzer. The sample cells were cooled with a<br />
liquid nitrogen bath (77 K) or a liquid argon bath (87 K). For room temperature<br />
measurements (298 K) the sample cells were tempered in a water bath.<br />
Calculation of specific surface area and the isosteric heat of adsorption<br />
A method generated from BET theory, which was developed by Brunauer, Emmett, and<br />
Teller in 1938 as an extension of Langmuirs monolayer adsorption to a very simple model<br />
of multilayer physisorption, is commonly employed to calculate the specific surface area<br />
of a porous solid. This area value is usually determined from the data of physisorption<br />
nitrogen isotherms recorded at 77 K.<br />
The BET theory can be derived similarly to the Langmuir theory, but with the<br />
consideration of multilayered gas molecule adsorption, where it is not required for a layer<br />
to be completed before an upper layer formation starts. For the development of the BET<br />
method five assumptions have been made: i) The sample surface is homogeneous; ii)
156 Chapter 7<br />
Uppermost layer is in equilibrium with vapor phase. iii) The heat of adsorption at all sites<br />
is constant and equal to the heat of condensation from the second layer on; iv) There is no<br />
lateral interactions between molecules. v) At saturation pressure, the number of layers<br />
has infinite thickness. Hence, the BET equation could be derived:<br />
p<br />
n a (p 0 − p) = 1<br />
n a m C<br />
+<br />
(C − 1)<br />
n m a C<br />
Here n a is the amount adsorbed, p is the pressure, p0 is the saturation pressure of the<br />
adsorbed gas at a given temperature, n m<br />
a<br />
is the monolayer capacity and C an empirical<br />
constant. The value of C can be associated to the magnitude of adsorbent-adsorbate<br />
interactions. This equation is an adsorption isotherm and can be plotted as a BET plot<br />
where 1/[n a (p0/p-1)] is the y-axis and p/p0 on the x-axis. The linear relationship of the<br />
BET plot is kept only in a pressure region of p/p0= 0.05 - 0.30. For microporous materials<br />
such as MOFs, a even smaller pressure range (p/p0 = 0.02 - 0.10) is usually applied.<br />
Subsequently, the monolayer capacity n m<br />
a<br />
can be derived from the slope of the BET plot.<br />
Consequently, the specific surface area SBET can be calculated from the following equation:<br />
SBET = n m a N A a m /m<br />
p<br />
p 0<br />
where NA is the Avogadro constant and am is molecular cross-section area occupied by a<br />
single adsorbate molecule in the complete monolayer and m the mass of adsorbent. Still,<br />
we should note that the BET theory is developed on basis of the oversimplified model. In<br />
fact, SBET is greatly affected by the nature of the adsorbent as well as the strength of<br />
adsorbate-adsorbent interactions. Microporous solids including MOFs, the pore surface of<br />
which are rather heterogeneous, the above mentioned assumptions are not valid. The<br />
obtained value of the BET surface area (SBET) can be widely used to compare the porosity<br />
of different porous materials and should not be considered as a precise absolute value.<br />
The adsorption isotherms of H2 adsorption at 77 K and 87 K were independently fit with<br />
triple site Langmuir model<br />
n = q sat,Ab A p<br />
1 + b A p + q sat,Bb B p<br />
1 + b B p + q sat,Cb C p<br />
1 + b C p<br />
where n is the molar loading of adsorbate (mmol/g), qsat is the saturation loading of site<br />
A/B/C (mmol/g), b is the Langmuir parameter for A/B/C (bar -1 ), and p the pressure(bar).<br />
After the triple-site Langmuir fits, the exact pressures correspond to the same amount
Chapter 7 157<br />
adsorbed at different temperatures can be plotted. Subsequently, the Clausius−Clapeyron<br />
equation,<br />
−Q st = RT 2 ( ∂lnp<br />
∂T ) n<br />
was used to calculated the isosteric heats of adsorption(-Qst) as a function of the amount<br />
of H2 adsorbed (n). -Qst is a value represent for the average binding energy of an adorbate<br />
at specific surface coverage.<br />
7.1.9 X-ray absorption near edge structure (XANES)<br />
Data acquisition and analysis for XANES were done at beam line BL8 of the synchrotron<br />
radiation facility DELTA by W. Zhang with the assistance of R. Wagner (and A.<br />
Schneemann).<br />
Simplified theory behind XANES<br />
XANES, also known as near edge X-ray absorption fine structure (NEXAFS), is a kind of<br />
absorption spectroscopy showing the features in the X-ray absorption spectra (XAS) of<br />
condensed matter because of the photoabsorption cross section for electronic transitions<br />
from an atomic core level to final states in the energy region of 50-100 eV above the<br />
selected atomic core level ionization energy. X-rays are ionizing electromagnetic radiation<br />
which afford sufficient energy to excite a core electron of an atom to an excited state (an<br />
empty below the ionization threshold), or to the continuum which is above the ionization<br />
threshold. A core hole is the space that a core electron occupied before it absorbs an X-ray<br />
photon and ejected from its core shell. Subsequently, another atomic electron drops down<br />
in to fill the core hole and release energies either through Auger electron ejection or X-ray<br />
Fluorescence.<br />
When the energy of X-ray radiation is scanning through the binding energy region of a<br />
core shell, there will be a sudden appearance of absorption increase, corresponding to<br />
absorption of the X-ray photon by a specific type of core electrons (eg. 1s, 2s, 2p electrons,<br />
etc.). This gives rise to a so-called absorption edge (K, L, M edge, etc.) in the XAS spectrum<br />
due to its vertical appearance. The binding energies of different core electrons are distinct.<br />
Atoms with a higher oxidation state need more energetic X-ray to excite its core level due
158 Chapter 7<br />
to the more tightly bound electron states. Consequently, the absorption edge energy<br />
increases along with the increase of oxidation-state of the absorption site.<br />
Sample measurements details<br />
The collection of XANES spectra was performed at the Ru-K edge (22117 eV) using a Si<br />
(311) monochromator at Beamline BL8 of the synchrotron radiation facility DELTA, TU<br />
Dortmund. The samples were filled into 1 mm caplillaries in an inert Ar atmosphere glovebox<br />
before the measurement. The set-up was acquired using 15cm Ionchamber filled with<br />
Ar as I0, a 15 cm Ionchamber filled with Xe as I1 and a 30 cm Ionchamber filled with Xe as<br />
I2. Approx 30 mm above the sample was the PIN-Diode capturing a relatively wide solid<br />
angle of fluorescence radiation. The energy was calibrated by measuring a metallic Ru foil<br />
as reference simultaneously to each sample scan. The data processing and analysis were<br />
done using the program ATHENA. [301]<br />
7.1.10 X-ray photoelectron spectroscopy (XPS)<br />
XPS spectra were recorded and analyzed by our collaboration partners, P. Guo and Dr. Y.<br />
Wang in the Laboratory of Industrial Chemistry (Prof. Dr. M. Muhler), Ruhr‐University<br />
Bochum. The discussion of the selected data was done by W. Zhang.<br />
XPS measurements were performed in a UHV setup equipped with a high-resolution<br />
Gammadata-Scienta SES 2002 analyzer. A monochromatic Al Kα X-ray source (energy<br />
1486.6 eV) was used as incident radiation. The analyzer slit width was set at 0.3 mm and<br />
the pass energy was fixed at 200 eV for all the measurements. The overall energy<br />
resolution was better than 0.5 eV. A flood gun was used to compensate for the charging<br />
effects. All spectra reported here are calibrated to the C 1s corelevel binding energy at 285<br />
eV. The XP spectra were deconvoluted using the CASA XPS program with a mixed Gaussian<br />
−Lorentzian function and Shirley background subtraction.<br />
7.1.11 High Performance Liquid Chromatography (HPLC)<br />
HPLC measurements to determine the ratio of the organic components were conducted<br />
by Dr. H. B. Albada and M. Strack at the Chair of Inorganic Chemistry I-Bioinorganic<br />
Chemistry (Prof. Dr. N. Metzler-Nolte), Ruhr‐University Bochum.<br />
Experimental setup:
Chapter 7 159<br />
Buffers: A: water/MeCN/TFA – 95/5/0.1 (%, v/v/v); B: MeCN/water/TFA – 95/5/0.1 (%,<br />
v/v/v)<br />
Gradient: start with 100 % A for 5 min; then in 15 min to 75 % B (i.e. 5 %/min); steady at<br />
75 % B for 2.5 min; drop to 100 % A in 5 min (i.e. 20 %/min); steady at 100 % A for 2.5<br />
min.<br />
Column: Prontosil, RP C18‐AQ, with pre‐column; dimensions: 250 x 4.6 mm (length x<br />
internal diameter), particle size: 5 μm; pore diameter: 120 Å (Knauer, Batch No. 2362,<br />
Column SN: CG 108, 25VF184PSJ).<br />
Detection: λ = 254 nm.<br />
Equipment: HPLC‐runs were performed on a Knauer HPLC‐machine.<br />
7.1.12 Catalytic studies<br />
Catalytical tests for Paal-Knorr reaction in Chapter 4 were performed in collaboration<br />
with the group of Prof. A. Corma, in particular by K. Epp (TU Munich) and Dr. F. X. Llabrés<br />
i Xamena, in the Institute of Chemical Technologies (Instituto de Tecnología Química, ITQ),<br />
Polytechnical University of Valencia (Spain). Ethylene dimerization in Chapter 4 was<br />
carried out by W. Zhang with the assistance of M. Gonzalez (the group of Prof. J. R. Long)<br />
in the department of Chemistry, University of California, Berkeley (US). Catalytic reaction<br />
for the hydrogenation of PNP to PAP in Chapter 5 was performed by Z. Chen and M. Al-<br />
Naji (Group of Prof. R. Gläser) in the institute of Chemical Technology, University of<br />
Leipzig. Data for the catalysis was analyzed by W. Zhang with the assistance of these<br />
collaborators.<br />
Gas Chromatography measurements for monitoring the product of Paal-Knorr reaction<br />
were performed on an Agilent Technologies 7890A with FID (Flame Ionization Detector)<br />
using a capillary column HP-5 (5% phenylmethylpolysiloxane) of 30 m length and 0.32<br />
mm internal diameter as well as BP20(WAX) of 15 m length and 0.32 mm internal<br />
diameter as another column. Thereby, the products were measured in high dilution using<br />
volatile organic solvents (usually ethanol or acetone).
160 Chapter 7<br />
7.2 Experimental data on chapter 3<br />
All chemicals (RuCl3·xH2O, LiCl, AgSO4, NaBPh4, AgBF4, pivalic acid, benzene-1, 3, 5-<br />
tricarboxylic acid (H3BTC)) and all solvents (CH3COOH, H2O, CH3OH, EtOH, acetic<br />
anhydride, acetone and hexane) were used as commercially received unless otherwise<br />
noted. Tetrahydrofuran (THF) used in the synthesis of SBU-c was catalytically dried,<br />
deoxygenated, and saturated with argon using an automatic solvent purification system<br />
from MBraun.<br />
7.2.1 Synthesis of the ruthenium precursors ([Ru2(OOCR)4X] and<br />
[Ru2(OOCCH3)4]A)<br />
Scheme 7.1. Preparation of the Ru-SBUs (SBU-a to SBU-d) used for MOF syntheses.<br />
[Ru2(OOCCH3)4Cl] (SBU-a)<br />
This compound was prepared using the method reported in the literature with slight<br />
modification. [202] RuCl3·xH2O (0.5 g, 2 mmol) and LiCl (0.5 g, 11.9 mmol) were mixed in<br />
one flask. Then glacial acetic acid (17.5 ml) and acetic anhydride (3.5 ml) were added.<br />
Subsequently, the mixture was refluxed for 24 h. The resulting red-brown precipitate was<br />
collected, washed several times with acetone, and dried under ambient conditions first<br />
and then under dynamic vacuum for at least 4 h (Yield: 0.33 g).
Chapter 7 161<br />
Figure 7.3. PXRD patterns of [Ru 2 (OOCCH 3 ) 4 Cl] SBU-a in comparison with the simulated patterns<br />
reported. [203]<br />
Figure 7.4. Acid-digested (DCl) 1 H-NMR spectrum of [Ru 2 (OOCCH 3 ) 4 Cl] (SBU-a) in the solvent of<br />
DMSO-d 6 .
162 Chapter 7<br />
[Ru2(OOCC(CH3)3)4(H2O)Cl](CH3OH) (SBU-b)<br />
The synthesis was carried out according to the literature. [201] SBU-a (0.3 g, 0.63 mmol)<br />
was dissolved in 60 ml solution of the H2O : CH3OH (1 : 1) mixture. Later, pivalic acid (0.39<br />
g, 3.79 mmol) was added and the resulting mixture was refluxed. The reaction was<br />
finished after 5 hours, when the solution turned to a red-brown color. This solution was<br />
cooled down and left to stay overnight. As a result, red-brown crystals precipitated. The<br />
final product was collected and washed twice with hexane (Yield: 0.37 g).<br />
Figure 7.5. Schematic description of the molecular structure of SBU-b in the solid state obtained<br />
by single crystal structure analysis. Note the half occupied Cl and half occupied O positions at the<br />
apical position of Ru coordination sphere. The oxygen atoms of the methanol molecule in the<br />
asymmetric unit (solvate) were split into two parts due to disorder. Circle with cross: Ru; circle<br />
shaded: Cl; circle shaded bottom right to top left: O; circle with blank: C. Single crystals of SBU-b<br />
were measured at low temperature (101K) while in the literature reference at 295K. The carbon<br />
atoms in CMe 3 were refined isotropically as well as the centrosymmetric structural model with<br />
partial occupation of Cl and O water as in the reference. [201] However, the measurement in the lower<br />
temperature reported here tends to be of better quality.
Chapter 7 163<br />
Table 7.1. Cell parameters of [Ru 2 (OOCC(CH 3 ) 3 ) 4 (H 2 O)Cl](CH 3 OH) (SBU-b) obtained from single<br />
crystal X-ray diffraction and reported in the literature. [201]<br />
Obtained Literature [201]<br />
Cell<br />
parameters<br />
a = 9.256(4)Å,<br />
b = 9.383(4) Å,<br />
c = 9.605(4) Å;<br />
α = 73.712(4)°,<br />
β = 83.681(4)°,<br />
γ = 73.585(4)°;<br />
V = 767.65(6)Å 3<br />
a = 9.353(3)Å,<br />
b = 9.469(6) Å,<br />
c = 9.804(4) Å;<br />
α = 72.57(4)°,<br />
β = 83.21(3)°,<br />
γ = 73.88(4)°;<br />
V = 795.3(7) Å 3<br />
Figure 7.6. Acid-digested (DCl) 1 H-NMR spectrum of [Ru 2 (OOCC(CH 3 ) 3 ) 4 (H 2 O)Cl](CH 3 OH) (SBUb)<br />
in the solvent of DMSO-d 6 .
164 Chapter 7<br />
Figure 7.7. The PXRD patterns of [Ru 2 (OOCC(CH 3 ) 3 ) 4 (H 2 O)Cl](CH 3 OH) (SBU-b) measured at<br />
different states (immediately after synthesis, one day later and two days later). From the PXRD<br />
patterns, we can infer that when the single crystal stays at room temperature for a while, it will<br />
lose the solvents gradually, which leads to the disappearance of certain reflexes.
Chapter 7 165<br />
[Ru2(OOCCH3)4(THF)2]BF4 (SBU-c)<br />
The compound was synthesized under Ar using the method reported in the literature. [200]<br />
SBU-a (100 mg, 0.211 mmol) and AgBF4 (42 mg, 0.211 mmol) were stirred in dry THF (4<br />
ml) with the protection of tin foil at room temperature. A red solution and white<br />
precipitate of AgCl was obtained after 24 h. The solution was filtered and the precipitate<br />
was washed several times with THF until colorless. All the filtrates were collected<br />
together, and the volume was reduced (ca. 4 times) in vacuum and the product was<br />
obtained (Yield: 108 mg).<br />
Figure 7.8. Acid-digested (DCl) liquid 1 H-NMR spectrum of SBU-c (solvent: DMSO-d 6 ).
166 Chapter 7<br />
[Ru2(OOCCH3)4(H2O)2]BPh4 (SBU-d)<br />
This precursor was synthesized in accordance to the literature procedure. [199] SBU-a (0.48<br />
g, 1.0 mmol) and AgSO4 (0.17 g, 0.5 mmol) were stirred in 20 ml of water at 40 °C. A white<br />
powder (AgCl) precipitated after 10 min and was filtered off. The resulting brown solution<br />
was cooled down to 0 °C, and then the aqueous solution of NaBPh4 (0.4 g, 1.2 mmol) was<br />
added drop-wise while stirring. The orange-brown product precipitated immediately.<br />
Subsequently, it was filtered and washed with cold water three times (Yield: 0.64 g). The<br />
final product was dried in vacuum at room temperature and stored in a fridge.<br />
Figure 7.9. 1 H-NMR spectrum of SBU-d (solvent: DMSO-d 6 ).<br />
[Ru2(OOCCH3)4] (SBU-e)<br />
The precursor SBU-e was obtained according to the reported method. [206-207] RuCl3·xH2O<br />
(4 g) together with 20mg PtO2 were put into a Fischer-Porter bottle in an argon-filled<br />
glove-box. Then 50 mg degassed methanol was added. After the whole system was<br />
degassed, the reactor was pressurized with ca. 2 atm hydrogen. The solution was stirred<br />
for 3 hours until it was deep blue. Subsequently, the solution was filtered under argon into<br />
50 ml degassed methanol which contain 4.7 g Li acetate. After heating under reflux for 18
Chapter 7 167<br />
hours, a deep red brown solution and an orange-brown microcrystalline product were<br />
resulted. The hot solution was filtered and the obtained solid was washed with methanol<br />
(3 x 20 ml). The product was then dried at 80°C under vacuum as a brown powder. m.p.<br />
276 °C.<br />
Scheme 7.2. Synthesis procedure of Ru 2 (OOCCH 3 ) 4 (SBU-e).<br />
Figure 7.10. IR spectra of [Ru 2 II,II (OOCCH 3 ) 4 ] (SBU-e) in comparison with [Ru 2 II,III (OOCCH 3 ) 4 Cl]<br />
(SBU-a). The vertical dash line represents the position of vibrations originated from ν as (COO) and<br />
ν s (COO) in [Ru 2 II,II (OOCCH 3 ) 4 ].
168 Chapter 7<br />
[Ru2(OOCCH3)4](THF)2<br />
Single crystal of [Ru2(OOCCH3)4](THF)2 was obtained in accordance to the reported<br />
procedure. [207] In particular, the sample of [Ru2(OOCCH3)4] was dissolved into<br />
tetrahydrofuran (THF) at 74 °C (oil bath) for 10 min with stirring. Subsequently, the stir<br />
was stopped and the solution was slowly cooled down (10 °C/30 min) to room<br />
temperature in a slow stream of Ar. The solution was then stored in a freezer at -20 °C<br />
overnight giving brown crystals.<br />
Table 7.2. Cell parameters of single crystal [Ru II,II 2 (OOCCH 3 ) 4 ](THF) 2 . Single crystal structure was<br />
not given due to the formation of twin crystal.<br />
obtained literature [207]<br />
a = 14.3787 Å, b = 9.6279 Å,<br />
c = 15.4351 Å; α = 90.000°,<br />
β = 90.000°, γ = 90.000°;<br />
V = 2134.5Å 3<br />
c = 14.606(3)Å a = 9.598(2)Å,<br />
b = 15.803(3)Å; α = 90.00°,<br />
β = 90.00°, γ = 90.00°;<br />
V = 2215.4Å 3<br />
7.2.2 Synthesis of Ru-MOFs [Ru3(BTC)2Xx]·Gg<br />
Scheme 7.3. Syntheses scheme of Ru-MOFs (1-4) employing various SBUs. Reaction Conditions<br />
for 1: CH 3 COOH, H 2 O, 160 °C, 72h; 2: CH 3 COOH, H 2 O, 160 °C, 168h; 3: CH 3 COOH, H 2 O, 160 °C, 72h;<br />
4: CH 3 COOH, H 2 O, 120 °C, 72h.
Chapter 7 169<br />
[Ru3(BTC)2Cl(AcO)0.5]n·(AcOH)1.5(H3BTC)0.1(H2O)4 (1_ex)<br />
This sample was obtained according to the method reported by Kozachuk et al. [82] A<br />
sample of SBU-a (170 mg, 0.36 mmol) and H3BTC (101 mg, 0.48 mmol) were placed in a<br />
20 ml Teflon vessel, and 4 ml of H2O and 0.7 ml of CH3COOH were subsequently added.<br />
The vessel was sealed in an autoclave and kept in a preheated oven at 160 °C for 72 h. The<br />
crude product was filtered and washed several times with distilled water and dried under<br />
ambient conditions (Yield: 171 mg). The obtained powder was further activated by<br />
heating at 150 °C for 24 h under dynamic vacuum (ca. 10 -3 mbar).<br />
[Ru3(BTC)2Cl1.2(OH)0.3]n·(H3BTC)0.15(AcOH)2.4(PivOH)0.45 (2_ex)<br />
The sample was prepared in accordance to the reported procedure. [83] A sample of SBUb<br />
(270 mg, 0.42 mmol) and H3BTC (120 mg, 0.57 mmol) were placed in a Teflon vessel,<br />
and then 6 ml of H2O and 0.1 ml of CH3COOH were added. The vessel was sealed in an<br />
autoclave and kept in the preheated oven at 160 °C for 120 h. As a result, a powdered<br />
product was obtained. It was filtered, washed several times with ethanol and dried at<br />
ambient temperature first (Yield: 223 mg). The sample was activated by heating under<br />
dynamic vacuum (ca. 10 -3 mbar) at 150 °C for 24 h.<br />
[Ru3(BTC)2F0.7(OH)0.8]n·(AcOH)1.5(H3BTC)0.2 (3_ex)<br />
A sample of SBU-c (241 mg, 0.36 mmol) and H3BTC (101 mg, 0.48 mmol) were mixed in a<br />
20 ml Teflon vessel with 4 ml of H2O and 0.7 ml of CH3COOH. The vessel was subsequently<br />
sealed in an autoclave and placed in the preheated oven at 160 °C for 72 h. The final brown<br />
product was collected, washed several times with distilled water, and dried under<br />
ambient conditions first (Yield: 265 mg). The sample was further activated by heating at<br />
150 °C for 24 h under dynamic vacuum (ca. 10 -3 mbar).
170 Chapter 7<br />
[Ru3(BTC)2(OH)1.5]n·(H3BTC)0.8(AcOH)1.4(H2O)3 (4_ex)<br />
A sample of SBU-d (286 mg, 0.36 mmol) and H3BTC (101 mg, 0.48 mmol), 4 ml of H2O and<br />
0.7 ml of CH3COOH were mixed in a Teflon vessel. The vessel was subsequently sealed in<br />
an autoclave and placed in the preheated oven at 120 °C for 72 h. The final product was<br />
filtered, washed several times with distilled water, and dried under ambient conditions<br />
first (Yield: 191 mg). The material was further activated by heating at 150 °C for 24 h<br />
under dynamic vacuum (ca. 10 -3 mbar).<br />
Figure 7.11. 1 H-NMR spectra of 4 (before solvent exchange) and 4-ex (after solvent exchange) in<br />
comparison with NaBPh 4 .
Chapter 7 171<br />
Figure 7.12. PXRD patterns of the materials obtained from different solvents with a small amount<br />
of acetic acid or without acetic acid as component in the solvent mixture at the same conditions<br />
(160 °C, 72h, solvothermal, starting with SBU-a and H 3 BTC) in comparison with SBU-a and Ru-<br />
MOF 1. a) 4 ml diglyme and 4 drops HCl, b) 4 ml H 2 O and 0.7 ml HCOOH, c) 4 ml H 2 O and 0.7 ml<br />
CF 3 COOH, d) 4 ml diglyme, e) 4 ml H 2 O and 4 drops HCl; f) pH = 1.89 solution of H 2 O and CF 3 COOH,<br />
10 ml (note: the same pH value with the literature; [82] formula: 4ml H 2 O and 0.7ml CH 3 COOH); g)<br />
pH = 1.89 solution of H 2 O and CF 3 COOH, 24 ml; h) pH = 1.89 solution of H 2 O and CF 3 COOH, 4.7 ml;<br />
i) pH = 1.89 solution of H 2 O and HCl, 4.7 ml; j). 12 ml H 2 O and 161 μl CH 3 COOH (pH = 2.47; note<br />
the same pH value with the literature [83] formula: 12ml H 2 O and 161 μl CH 3 COOH). Note: CF 3 COOH<br />
was employed to trace the incorporation of the carboxylic acid by the CF 3 -group.
172 Chapter 7<br />
[Ru3(BTC)2]n∙(AcOH)2.3 (5)<br />
The preparation of Ru-MOF 5 was similar with Ru-MOF 1 using SBU-e (158 mg, 0.36<br />
mmol) and H3BTC (101 mg. 0.48 mmol) with degassed water and AcOH. All the degassed<br />
reactant was then mixed in a Teflon vessel sitting in a schlenk flask under Argon<br />
atomosphere. The vessel was subsequently quickly sealed in an autoclave and placed in<br />
the preheated oven at 160 °C for 72 h. The crude product was filtered and washed several<br />
times with degassed distilled water and dried under vacuum. Further activation of the<br />
powder was performed by heating at 150 °C for 24 h under dynamic vacuum (ca. 10 -3<br />
mbar).<br />
Figure 7.13. 1 H-NMR spectra of the sample 5 ([Ru 3 (C 9 H 3 O 6 ) 2 ] n·(CH 3 COOH) 2.3 ) digested in<br />
DCl/DMSO-d 6 mixture.
Chapter 7 173<br />
7.3 Experimental data on chapter 4<br />
Ruthenium SBU precursor [Ru2(OOCCH3)4Cl]n [202] as well as the parent single-linker Ru-<br />
MOF [82, 198] were prepared following procedures previously described in the literature and<br />
in Chapter 7.2. All other reagents were available commercially and used without further<br />
purification. Before further manipulations, all activated samples were stored in a glovebox<br />
under inert Ar atmosphere.<br />
7.3.1 Synthesis of Ru-DEMOF samples (1a-1d, 2a-2d, 3a-3d, 4a-4c)<br />
[Ru3(BTC)2-x(5-X-ip)xXy]n (X = counter ion; 0.1 ≤ x ≤ 1; 0 ≤ y ≤ 1.5). The samples were<br />
synthesized according to the reported method [138] applying the so-called controlled SBU<br />
approach. The mixtures of parent linker (1,3,5-benzenetricarboxylic acid, i.e. H3BTC) and<br />
defective linker (5-X-isophthalic acid, i.e. 5-X-ip, X = OH (1), H (2), NH2 (3) and Br (4),<br />
respectively) combined with 1.5 molar equivalents of [Ru2(OOCCH3)4Cl]n (0.36 mmol,170<br />
mg) were placed in the 20 ml Teflon vessels. Subsequently, 4 ml of HPLC grade water and<br />
0.7 ml of glacial acetic acid were added. The molar ratios and amounts of the linkers used<br />
in the starting materials are listed in the Table 7.3. The Teflon reaction vessels were then<br />
placed in the Teflon-lined stainless steel autoclaves. The autoclaves were further sealed<br />
and placed into the pre-heated oven at 433 K for 72 h. Afterwards the autoclaves were<br />
taken out and cooled down at room temperature. The resulting powder products were<br />
collected by centrifugation. Afterwards, they were soaked into HPLC grade water (ca. 20<br />
ml) and the solvent was refreshed by the same water amount every 24 hours for 3 times.<br />
Finally, the solvent was removed and collected powders were dried under air at room<br />
temperature. The activation of the solids was performed by heating at 423 K for 24 h<br />
under dynamic vacuum (ca. 10 -3 mbar).
174 Chapter 7<br />
Table 7.3. Feeding molar ratios and amounts of the linkers used in the syntheses of the Ru-<br />
DEMOF samples.<br />
parent linker (H 3 BTC)<br />
defect linker (5-X-ip)<br />
Sample<br />
H 3 BTC : (H 3 BTC + 5-XipH<br />
2 )<br />
mass<br />
(mg)<br />
5-X-ipH 2 : (H 3 BTC + 5-X-ipH 2 )<br />
mass<br />
(mg)<br />
1a 90% 90.8<br />
10% 9<br />
1b 80% 80.7 20% 18<br />
X = OH<br />
1c 70% 71 30% 26<br />
1d 50% 50.5 50% 43.7<br />
2a 90% 90.8<br />
10% 8<br />
2b 80% 80.7 20% 16<br />
X = H<br />
2c 70% 71 30% 24<br />
2d 50% 50.5 50% 40<br />
3a 90% 90.8<br />
10% 8.7<br />
3b 80% 80.7 20% 17.4<br />
X = NH 2<br />
3c 70% 71 30% 26<br />
3d 50% 50.5 50% 43.5<br />
4a 90% 90.8<br />
10% 12<br />
4b 80% 80.7 X = Br<br />
20% 24<br />
4c 70% 71 30% 35.3
Chapter 7 175<br />
Table 7.4. BET surface area (S BET ) values of the Ru-DEMOFs (1a-1d, 2a-2c, 3a-3d, 4a-4c)<br />
compared with the parent Ru-MOF as well as [Cu 3 (BTC) 2 ] n . S BET (m 2 /mmol) of the parent Ru-MOFs<br />
and Ru-DEMOFs 1a, 1c and 1d was converted from the respective measured S BET (m 2 /g) values<br />
according to the proposed composition in Chapter 3 and 4.<br />
Sample S BET , m 2 /g S BET , m 2 /mmol<br />
parent Ru-MOF 1_ex 998 [208] 964<br />
parent Ru-MOF 5 1371 1173<br />
[Cu 3 (BTC) 2 ] n 1734 [83] 1049<br />
1a 1106 1062<br />
1b 1284 -<br />
1c 1302 1232<br />
1d 947 930<br />
2a 1059 -<br />
2b 1023 -<br />
2c 838 -<br />
2d 574 -<br />
3a 1003 -<br />
3b 985 -<br />
3c 975 -<br />
3d 781 -<br />
4a 996 -<br />
4b 847 -<br />
4c 693 -
176 Chapter 7<br />
For comparison of the obtained S BET values for Ru-MOFs with the homologous Cu-MOFs, it might<br />
be more informative using m 2 /mmol units (due to substantial difference in the molecular weight<br />
of Cu and Ru and the presence of guest molecules). Thus, the S BET of the parent Ru-MOF (964<br />
m 2 /mmol) is quite similar to that of a typical reference sample [Cu 3 (BTC) 2 ] n (1049 m 2 /mmol).<br />
More importantly, the S BET of the Ru-DEMOF solids slightly increases in comparison with both<br />
parent analogues. Due to the complexity of the composition (which has been mentioned in the<br />
section 4.2.1.2 of Chapter 4), EA was not performed for the rest Ru-DEMOFs to determine the<br />
unambiguous composition with counter-ions and guest molecules. Hence, S BET values in the unit<br />
of m 2 /mmol were not calculated for them.<br />
Figure 7.14. XPS survey scan of the parent Ru-MOF and Ru-DEMOFs (1a, 1c, 1d, 2a and 2b). 1a,<br />
1c and 1d - 8%, 32% and 37% 5-OH-ip incorporation, respectively; 2a and 2b - 15% and 28% ip<br />
incorporation, respectively. Figure is provided by P. Guo.
Chapter 7 177<br />
7.3.2 Catalytic reactions using Ru-DEMOFs as catalysts<br />
7.3.2.1 Ethylene dimerization<br />
In a typical run (entry 5), 2.1 mg of the activated Ru-MOF 1c was put in a 10 ml steel<br />
reactor followed by adding of 0.81 ml of Et2AlCl (1M in heptane), 2.1 ml of toluene and<br />
0.09 ml of undecane (0.01 M in toluene). After degassing, the reactor was flushed with<br />
C2H4 (800psi) and placed in a pre-heated oil bath at 80 °C with stirring for 2 hours.<br />
Subsequently, the reaction was stopped and the reactor was cooled down at -7 °C in a<br />
mixture of dry ice and ethylene glycol bath. Cold distilled water was added to quench the<br />
reaction. The organic layer kept cold was then quickly analyzed by gas chromatography<br />
(SRI 8610V GC, 60 m x 0.54 mm internal diameter, 5.0 µm MXT-1 capillary columns) using<br />
undecane signal as a reference. In case of no additive, the volume of toluene was changed<br />
to 2.91 ml. Other parameters are the same as entry 5 described above.<br />
7.3.2.2 Paal-Knorr reaction<br />
In a typical run, 5 mg of the activated Ru-MOF/DEMOFs in 0.5 ml of toluene were<br />
introduced into 125 mg (1.1 mmol) of 2,5-hexadione and 95 mg (1 mmol) of aniline and<br />
were stirred at 90 °C for 24h under air. The reaction was followed by taking aliquots every<br />
hour and analyzing the products by GC-MS. The reactions were performed in closed<br />
(pressurize able) reaction vials.<br />
7.3.3 Synthesis of [Cu3(BTC)2]n (Cu-BTC)<br />
[Cu3(BTC)2]n was prepared from a reported method [35] at a litter lower temperature (120<br />
°C). Specifically, Cu(NO3)2∙3H2O (1.8 mmol, 438 mg) and 1, 3, 5-benzentricarboxylic acid<br />
(H3BTC, 1.0 mmol, 210 mg) were put into a Teflon vessel, and a solution of 12 ml H2O:EtOH<br />
(1:1) was added. The vessel was sealed in an autoclave and kept in a preheated oven at<br />
100 °C for 12 h. The crude product was filtered and washed several times with distilled<br />
water and absolute ethanol, respectively. After dried under ambient conditions the<br />
obtained powder (152 mg) was further activated by heating at 120 °C for 24 h under<br />
dynamic vacuum (ca. 10 -3 mbar).
178 Chapter 7<br />
7.3.4 Synthesis of Cu-DEMOF samples (D1-8)<br />
D1<br />
H3BTC (100mg, 0.48 mmol) and ip (80mg, 0.48 mmol) equaling a 1:1 ratio were mixed<br />
with Cu(BF4)2 6H2O (488 mg, 1.4 mmol) and placed into a 20 ml screw jaw. Subsequently<br />
14 ml N,N-Dimethylformamide (DMF) was added. The screw jaw was then sealed and put<br />
into a pre-heated oven at 80 °C for 20 h. The resulting blue powder products were<br />
collected by centrifugation. Afterwards, they were washed by DMF (30 ml x 3), EtOH (30<br />
ml x 3) and acetone (30 ml x 3) subsequently. The final powder was collected and dried<br />
under air at room temperature. The activation of the solids was performed by heating at<br />
170 °C for 24 h under dynamic vacuum (ca. 10 -3 mbar).<br />
Figure 7.15. 1 H-NMR spectra of the acid-digest D1 sample (solvent: DMSO-d 6 , DCl).
Chapter 7 179<br />
D2<br />
This sample was prepared as D1 using 160mg ip (2 molar equivalent to that of H3BTC)<br />
instead. The resulting blue powder products were separated from the solution by<br />
centrifugation. Afterwards, they were washed by DMF(30 ml x 3), EtOH (30 ml x 3) and<br />
acetone (30 ml x 3) subsequently. Finally, the solvent was removed and the powder was<br />
dried under air at room temperature. The activation of the solids was performed by<br />
heating at 170 °C for 24 h under dynamic vacuum (ca. 10 -3 mbar).<br />
Figure 7.16. 1 H-NMR spectra of the acid-digest D2 sample (solvent: DMSO-d 6 , DCl).
180 Chapter 7<br />
D3<br />
The mixture of H3BTC (100mg, 0.48 mmol), ip (80 mg, 0.48 mmol) and Cu(BF4)2 6H2O<br />
(488 mg, 1.4 mmol) was placed into a 50 ml Teflon vessel. Subsequently, 24 ml EtOH was<br />
added. The Teflon reaction vessel was then placed in the Teflon-lined stainless steel<br />
autoclaves. The autoclaves were further sealed and placed into the pre-heated oven at 80<br />
°C for 20 h. Afterwards the autoclaves were taken out and cooled down at room<br />
temperature. The resulting blue powder products were separated from the solution by<br />
centrifugation. Afterwards, they were washed by EtOH (30 ml x 3) and acetone (30 ml x<br />
3) subsequently. Finally, the solvent was removed and the powder was dried under<br />
ambient atmosphere at room temperature. The activation of the solids was performed by<br />
heating at 120 °C for 24 h under dynamic vacuum (ca. 10 -3 mbar).<br />
Figure 7.17. 1 H-NMR spectra of the acid-digest D3 sample (solvent: DMSO-d 6 , DCl).
Chapter 7 181<br />
D4<br />
This sample was prepared as D3 using 160mg ip (2 molar equivalent to that of H3BTC)<br />
instead. The resulting powder products were collected by centrifugation. Afterwards, they<br />
were washed by EtOH (30 ml x 3) and acetone (30 ml x 3) subsequently. Finally, the<br />
solvent was removed and the powder was dried under ambient atmosphere at room<br />
temperature. The activation of the solids was performed by heating at 120 °C for 24 h<br />
under dynamic vacuum (ca. 10 -3 mbar).<br />
Figure 7.18. 1 H-NMR spectra of the acid-digest D4 sample (solvent: DMSO-d 6 , DCl).
182 Chapter 7<br />
D5<br />
This sample was repeated following the reported method. [140] H3BTC (50mg, 0.24 mmol)<br />
and 1 molar equivalent of ip (40mg, 0.24 mmol) combined with Cu(NO3)2·3H2O (171mg,<br />
0.70 mmol) was placed into a 20ml screw jaw. Subsequently, 7 ml DMF and 0.3 ml conc.<br />
HBF4 was added. The screw jaw was then sealed and put into a pre-heated oven at 80 °C<br />
for 20 h. The resulting blue powder products were collected by centrifugation.<br />
Afterwards, they were washed by DMF(30 ml x 3), EtOH (30 ml x 3) and acetone (30 ml x<br />
3) subsequently. The final powder was collected and dried under air at room temperature.<br />
The activation of the solids was performed by heating at 140 °C for 24 h under dynamic<br />
vacuum (ca. 10 -3 mbar).<br />
Figure 7.19. 1 H-NMR spectra of the acid-digest D5 sample (solvent: DMSO-d 6 , DCl).
Chapter 7 183<br />
D6<br />
This sample was obtained as D5 using 80 mg ip instead. [140] The resulting blue powder<br />
products were collected by centrifugation. Afterwards, they were washed by DMF(30 ml<br />
x 3), EtOH (30 ml x 3) and acetone (30 ml x 3) subsequently. The final powder was<br />
collected and dried under ambient atmosphere at room temperature. The activation of the<br />
solids was performed by heating at 140 °C for 24 h under dynamic vacuum (ca. 10 -3 mbar).<br />
Figure 7.20. 1 H-NMR spectra of the acid-digest D6 sample (solvent: DMSO-d 6 , DCl).
184 Chapter 7<br />
The synthesis of D7 and D8 are basically the same as D5 and D6, respectively. The only<br />
difference is that there is no usage of HBF4 during synthesis.<br />
Figure 7.21. 1 H-NMR spectra of the acid-digest D7 sample (solvent: DMSO-d 6 , DCl).<br />
Figure 7.22. 1 H-NMR spectra of the acid-digest D8 sample (solvent: DMSO-d 6 , DCl).
Chapter 7 185<br />
Figure 7.23. PXRD patterns of as-synthesized samples prepared from similar reactant with the<br />
sample D7 and D8 using EtOH instead of DMF (100 °C, 12h) in comparison with patterns<br />
simulated from [Cu 3 (BTC) 2 ] n (Cu-HKUST-1 sim.).
186 Chapter 7<br />
7.4 Experimental data on chapter 5<br />
All chemicals (Cu(NO3)2∙3H2O, Pd(OOCCH3)2, PdCl2, benzene-1,3,5-tricarboxylic acid<br />
(H3BTC), p-nitrophenol (PNP) (99%), Sodium borohydrate (NaBH4) (98%)) and all<br />
solvents (H2O, ethanol, and acetone) were used as commercially received unless<br />
otherwise noted. Before further manipulations, all activated samples were stored in an<br />
Ar-filled glove-box.<br />
7.4.1 Synthesis of [Cu3-XPdx(BTC)2]n<br />
Cu/Pd-BTC_1-3<br />
For Cu/Pd-BTC_1-3, 2.0 mmol of H3BTC (420 mg) was combined with 1.8 molar<br />
equivalents of a mixture of Cu(NO3)2∙3H2O and Pd acetate and then placed into a Teflon<br />
vessel. Subsequently 15ml of H2O/ethanol (1:1) solution was added. The molar<br />
percentage and amount of each metal salts in the total metal source as well as their weight<br />
used in the starting reactant are for Cu/Pd-BTC_1, Cu(NO3)2∙3H2O (90%, 3.24 mmol, 783<br />
mg) / Pd acetate (10%, 0.36 mmol. 80.8 mg); for Cu/Pd-BTC_2, Cu(NO3)2∙3H2O (85%,<br />
3.06 mmol, 739 mg) / Pd acetate (15%, 0.54 mmol. 121.2 mg); for Cu/Pd-BTC_3,<br />
Cu(NO3)2∙3H2O (80%, 2.88 mmol, 696 mg) / Pd acetate (20%, 0.72 mmol. 161.6 mg). The<br />
Teflon vessel was sealed in an autoclave and kept in the oven at 125 °C for 12h. The<br />
resulting power product was collected by filtration and washed several times with<br />
distilled water and acetone, respectively. After dried under ambient conditions the<br />
obtained powder was further activated by heating at 120 °C for 24 h under dynamic<br />
vacuum (ca. 10 -3 mbar).
Chapter 7 187<br />
Figure 7.24. XPS survey scans of the activated samples Cu/Pd-BTC_1 and 3. Figure is provided<br />
by P. Guo.<br />
Figure 7.25. PXRD patterns of the sample obtained using 50% feeding of Pd(II)-acetate under the<br />
same conditions as [Cu 3-X Pd x (BTC) 2 ] n with 10%, 15% and 20% feeding .
188 Chapter 7<br />
Figure 7.26. PXRD patterns of the sample prepared using only Pd(II)-acetate and H 3 btc under the<br />
same conditions as introduced mixed-metal solids with 10%, 15% and 20% feeding of Pd(II)-<br />
acetate. No Cu-salt was employed.
Chapter 7 189<br />
Cu/Pd-BTC_4<br />
For sample Cu/Pd-BTC_4, 0.48 mmol of H3BTC (101 mg) was combined with 1.5 molar<br />
equivalents of mixture of Cu(NO3)2∙3H2O (80%, 0.58 mmol, 139 mg) / PdCl2 (20%, 0.14<br />
mmol. 25.5 mg) and then placed into a Teflon vessel. Subsequently 6ml of H2O/ethanol<br />
(1:1) solution was added. The Teflon vessel was sealed in an autoclave and kept in the<br />
oven at 90 °C for 16h. The resulting power product was collected by filtration and washed<br />
several times with distilled water and acetone, respectively. After dried under ambient<br />
conditions the obtained powder was further activated by heating at 120 °C for 24 h under<br />
dynamic vacuum (ca. 10 -3 mbar).<br />
Figure 7.27. 1 H-NMR spectra of the acid-digest sample of Cu/Pd-BTC_4 (solvent: DMSO-d 6 , DCl).
190 Chapter 7<br />
7.4.2 Hydrogenation of PNP to PAP<br />
The catalytic aqueous-phase in-situ hydrogenation of PNP to PAP using NaBH4 as a<br />
hydrogen source was carried out in a 100 cm 3 batch reactor at room temperature (298K),<br />
ambient pressure and 1300 min -1 stirring speed. Figure 7.28 depicts the catalytic<br />
experimental setup. In the typical catalytic experiment, 5.0 cm 3 of an aqueous solution of<br />
NaBH4 (0.60 mmol dm −3 ) were added to 45.0 cm 3 of an aqueous solution of PNP (0.18<br />
mmol dm −3 ). The reaction was started by introducing 5.0 mg of the catalyst. PNP<br />
concentration changes were monitored via online UV-vis spectroscopy (AvaSpec-3648,<br />
optical path length: 5 mm) at a wavelength of 400 nm (see Figure 7.29). The initial<br />
reaction rate (r0) was calculated by assuming a zero order reaction from the linear<br />
decrease of PNP concentration after the addition of the catalyst.<br />
Figure 7.28. Experimental setup for aqueous-phase in-situ hydrogenation of PNP to PAP with<br />
NaBH 4 as hydrogen source using an online UV-vis spectrometer. Figure is provided by M. Al-Naji.
Absorbance, a. u.<br />
Chapter 7 191<br />
O 2<br />
N<br />
OH<br />
NaBH 4<br />
catalyst<br />
H 2<br />
N<br />
t reaction<br />
OH<br />
250 300 350 400 450 500<br />
Wavelength, nm<br />
Figure 7.29. UV-vis spectra for increasing reaction time in the aqueous-phase in-situ<br />
hydrogenation of PNP with NaBH 4 to PAP. Figure is provided by M. Al-Naji.
192 Chapter 7<br />
7.5 Supplementary details in Outlook<br />
Synthesis of mixed-component MOF (S1-5, [Cu3-XZnx(BTC)2-y(5-NO2-ip)y]n)<br />
3.6 mmol of a mixture of Cu(NO3)2∙3H2O (80%, 2.88 mmol, 696 mg) and Zn(NO3)2∙6H2O<br />
(20%, 0.72 mmol. 214 mg) was dissolved into a 15 ml solution of H2O/ethanol (1:1) in a<br />
Teflon vessel. Subsequently, mixed-linkers (H3BTC and 5-NO2-ip) in a total molar amount<br />
of 2 mmol (see Table 7.5 for the molar ratio differences for each sample) were added. After<br />
the Teflon vessel was sealed in an autoclave, it was kept in the oven at 125 °C for 12h. The<br />
resulting power product was collected by centrifuge and washed several times with<br />
distilled water and ethanol, respectively. Subsequently, the powder was soaked in the<br />
fresh ethanol for 24 h. After soaking the collected powder was dried under ambient<br />
conditions and further activated by heating at 120 °C for 24 h under dynamic vacuum (ca.<br />
10 -3 mbar).<br />
Table 7.5. Feeding molar ratios and amounts of the linkers used in the syntheses of the S1-5.<br />
samples<br />
H 3 BTC : (H 3 BTC + 5-NO 2 -ipH 2 )<br />
H 3 BTC 5-NO 2 -ipH 2<br />
Mass<br />
(mg)<br />
5-NO 2 -ipH 2 : (H 3 BTC + 5-<br />
NO 2 -ipH 2 )<br />
Mass<br />
(mg)<br />
S1 90% 378 10% 42<br />
S2 80% 336 20% 84<br />
S3 70% 294 30% 127<br />
S4 50% 210 50% 211<br />
S5 0 - 100% 422<br />
Scheme 7.4. Scheme illustration of preparation for mixed-component MOFs.
Chapter 7 193<br />
Figure 7.30. PXRD patterns of activated mixed-component MOFs S1-4 in comparison with parent<br />
Cu-BTC and only Zn-doped Cu/Zn-BTC.<br />
Table 7.6. The feeding molar percentage of Zn 2+ content and defect linker 5-NO 2 -ip during the<br />
synthesis of mixed-component sample S1-4 as well as the obtained values calculated from HPLC<br />
and AAS results.<br />
sample<br />
n(Zn 2+ ): n(Zn 2+ +Cu 2+ )<br />
n(5-NO 2 -ip): n(5-NO 2 -ip + H 3 BTC)<br />
feeding obtained feeding obtained<br />
S1 20% 3% 10% 3%<br />
S2 20% 2% 20% 10%<br />
S3 20% 2% 30% 14%<br />
S4 20% 1% 50% 21%
8 Bibliography<br />
[1] A. J. Ihde, The Development of Modern Chemistry, Harper and Row, 1964.<br />
[2] Y. Shibata, J. Coll. Sci., Imp. Univ. Tokyo 1916, 37, 1-17.<br />
[3] J. C. Bailar, Jr., Preparative Inorg. Reactions 1964, 1, 1-27.<br />
[4] N. G. Connelly, T. Damhus, R. M. Hartshorn, A. T. Hutton, Editors, Nomenclature of<br />
Inorganic Chemistry: IUPAC Recommendations 2005, Royal Society of Chemistry,<br />
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Appendix<br />
List of Publications<br />
Several paragraphs and figures of this thesis have already been published in peerreviewed<br />
journals. These articles are reproduced in part with permission from the related<br />
publishers:<br />
Wenhua Zhang, Olesia Kozachuk, Raghavender Medishetty, Andreas Schneemann,<br />
Ralph Wagner, Kira Khaletskaya, Konstantin Epp, and Roland A. Fischer*. “Controlled<br />
SBU Approaches to Isoreticular Metal-Organic Framework Ruthenium-Analogues of<br />
HKUST-1”, European Journal of Inorganic Chemistry, 2015, 2015, 3913-3920.<br />
Wenhua Zhang, Max Kauer, Olesia Halbherr, Konstantin Epp, Penghu Guo, Miguel I.<br />
Gonzalez, Dianne J. Xiao, Christian Wiktor, Francesc X. LIabrés i Xamena, Christof Wöll,<br />
Yuemin Wang,* Martin Muhler, and Roland A. Fischer*. “Ruthenium Metal-Organic<br />
Frameworks with Different Defect Types: Influence on Porosity, Sorption and Catalytic<br />
Properties”, Chemistry-A European Journal, accepted.<br />
Wenhua Zhang, Zhihao Chen, Majd Al-Naji, Penghu Guo, Stefan Cwik, Olesia Halbherr,<br />
Yuemin Wang, Martin Muhler, Nicole Wilde, Roger Gläser and Roland A. Fischer*.<br />
“Simultaneous introduction of various palladium active sites into MOF via one-pot<br />
synthesis: Pd@[Cu3-xPdx(BTC)2]n”, Dalton Transactions (submitted).<br />
Wenhua Zhang, Kerstin Freitag, Suttipong Wannapaiboon, Roland A. Fischer*.<br />
“Elaboration of a Highly Porous Ru II,II analog of HKUST-1”, Inorganic Chemistry<br />
(submitted).<br />
Wenhua Zhang, Max Kauer, Sebastian Kunze, Stefan Cwik, Yueming Wang, and Roland<br />
A. Fischer*. “Study of synthesis parameters on the defect engineering of HKUST-1”,<br />
European Journal of Inorganic Chemistry (to be submitted).<br />
Zhenlan Fang, Johannes P. Dürholt, Max Kauer, Wenhua Zhang, Charles Lochenie,<br />
Bettina Jee, Bauke Albada, Nils Metzler-Nolte, Andreas Pöppl, Birgit Weber, Martin<br />
Muhler, Yuemin Wang*, Rochus Schmid*, and Roland A. Fischer*. “Structural<br />
Complexity in Metal–Organic Frameworks: Simultaneous Modification of Open Metal<br />
Sites and Hierarchical Porosity by Systematic Doping with Defective Linkers”, Journal<br />
of the American Chemical Society, 2014, 136, 9627-9636.
206 Appendix<br />
List of Presentations<br />
Wenhua Zhang, Max Kauer, Dianne J. Xiao, Ralph Wagner, Konstantin Epp, Olesia<br />
Kozachuk, Yuemin Wang, Roland A. Fischer. “Defect Engineered” mixed valence Ru-<br />
MOFs: study on the influence of defect metal sites.<br />
250th American Chemical Society National Meeting & Exposition<br />
Boston (USA), August 16 - 20, 2015, oral presentation.<br />
Wenhua Zhang, Olesia Kozachuk, Max Kauer, Zhenlan Fang, Yuemin Wang, Roland A.<br />
Fischer. “Defect Engineered” Mixed Valence MOFs.<br />
4th International Conference on Metal-Organic Frameworks and Open Framework<br />
Compounds<br />
Kobe (Japan), September 28 - October 1, 2014, poster presentation.<br />
Wenhua Zhang, Ralph Wagner and Roland A. Fischer. Investigation on the Ru-sites<br />
of the ruthenium Defect-Engineered Metal-Organic Frameworks by XAS.<br />
DELTA user meeting<br />
Dortmund (Germany), November 2015, post presentation.
Appendix 207<br />
Curriculum Vitae<br />
Personal information<br />
Name:<br />
Wenhua Zhang<br />
Date of Birth: 6th Dec. 1987<br />
Place of Birth:<br />
Nationality:<br />
Marital Status<br />
Education<br />
Henan, China<br />
Chinese<br />
unmarried<br />
10. 2012- Present Ruhr-University Bochum, Bochum, Germany<br />
Ph. D. candidate at the Chair of Inorganic Chemistry II<br />
Supervisor: Prof. Roland A. Fischer<br />
06.2015-08.2015 University of California, Berkeley, USA<br />
Visit Scholar in the group of Prof. Jeffrey R. Long at the<br />
Department of Chemistry<br />
09. 2009- 07. 2012 Zhengzhou University, Zhengzhou, China<br />
Master of Science in Inorganic Chemistry, College of Chemistry<br />
and Molecular Engineering<br />
Supervisor: Prof. Guang Yang<br />
Recommended postgraduate candidates exempt from admission<br />
exam<br />
09. 2005- 07. 2009 Zhengzhou University, Zhengzhou, China<br />
Bachelor of Science in Chemistry, Department of Chemistry<br />
Bachelor Thesis Supervisor: Prof. Guang Yang<br />
08. 2001-06. 2005 Yichuan High School, Luoyang, China<br />
Awards and Fellowships<br />
High school education<br />
2012- Present Scholarship from China Scholarship Council (CSC)
208 Appendix<br />
05. 2015 Grant from the RS plus (Ruhr-University Bochum) for the<br />
research (exchange) stay in the group of Prof. Jeffrey. R. Long,<br />
University of California, Berkeley (USA) including the business<br />
trip to ACS fall meeting 2015<br />
02. 2015 Grant from RS Plus (RUB) for PR.INT (International Project) to<br />
invite Dianne J. Xiao from the group of Prof. Jeffrey R. Long to<br />
RUB<br />
07. 2014 Grant from RS Plus (RUB) for funding the business trip to MOF<br />
2014 conference<br />
2009-2012 Scholarship for Outstanding Student of Zhengzhou University