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<strong>Journal</strong> <strong>of</strong><br />

<strong>Materials</strong> <strong>Chemistry</strong><br />

Cite this: J. Mater. Chem., 2011, 21, 3838<br />

www.rsc.org/materials<br />

A citrate sol–gel method to synthesize Li 2 ZrO 3 nanocrystals with improved<br />

CO 2 capture properties<br />

Qiang Xiao, Yefeng Liu, Yijun Zhong and Weidong Zhu*<br />

Received 28th September 2010, Accepted 17th December 2010<br />

DOI: 10.1039/c0jm03243c<br />

<strong>PAPER</strong><br />

Li 2 ZrO 3 nanocrystals with improved CO 2 capture properties were synthesized by a citrate sol–gel<br />

method. The morphology and structure <strong>of</strong> the synthesized Li 2 ZrO 3 samples were characterized in detail<br />

by SEM, TEM, and XRD techniques. The CO 2 capture–regeneration properties <strong>of</strong> these nanocrystals<br />

were investigated by thermogravimetric analysis (TGA) over a wide range <strong>of</strong> temperatures and <strong>of</strong> CO 2<br />

partial pressures. The nanosized Li 2 ZrO 3 crystallites with a tetragonal phase exhibit a better CO 2<br />

capture performance than reported sorbents, exhibiting a faster uptake and a higher, nearly<br />

stoichiometric adsorption capacity (26 wt.%). Furthermore, the adsorbent shows a good stability,<br />

confirmed by capture–regeneration cycles. Based on these excellent properties, application in sorptionenhanced<br />

reaction process (SERP) is anticipated.<br />

Introduction<br />

Recently, hydrogen has gained considerable interest as a potential<br />

alternative fuel for zero-emission vehicles, and by 2005,<br />

about 55% <strong>of</strong> all hydrogen was produced globally from natural<br />

gas, i.e. via steam–methane reforming (SMR) and water–gas shift<br />

(WGS) reaction. 1 The endothermic SMR reaction is generally<br />

carried out in a catalytic (Ni/Al 2 O 3 ) reactor at temperatures<br />

ranging from 1023 to 1173 K, the effluent gas is then cooled and<br />

fed to another catalytic (Fe or Cu/Al 2 O 3 ) reactor for the<br />

exothermic WGS reaction, and finally a multicolumn pressure<br />

swing adsorption (PSA) process containing 4–12 adsorption beds<br />

is usually applied to produce pure hydrogen. 2 The aforementioned<br />

process has been the dominant technology utilized for H 2<br />

production for many years. However, the high-temperature<br />

operation <strong>of</strong> the SMR reactor, the catalyst deactivation due to<br />

coking, the use <strong>of</strong> special high-temperature steel for the<br />

construction <strong>of</strong> the SMR reactor, the requirement <strong>of</strong> large<br />

interstage heat recovery systems, and the complex design <strong>of</strong> the<br />

multicolumn H 2 -PSA system significantly raise the capital cost <strong>of</strong><br />

H 2 production. 3<br />

A process configuration based on a hybrid reaction/adsorption<br />

system, the so-called sorption-enhanced reaction process<br />

(SERP), has been developed by Air Products in the 1990s as an<br />

alternative technology for the industrial production <strong>of</strong> pure<br />

hydrogen. 3,4 When the SERP concept is applied to SMR and<br />

WGS reactions for the production <strong>of</strong> pure hydrogen, an adsorbent<br />

(admixture with the catalyst in the reactor) selectively<br />

Key Laboratory <strong>of</strong> the Ministry <strong>of</strong> Education for Advanced Catalysis<br />

<strong>Materials</strong>, Institute <strong>of</strong> Physical <strong>Chemistry</strong>, Zhejiang Normal University,<br />

321004 Jinhua, P. R. <strong>of</strong> China. E-mail: weidongzhu@zjnu.cn; Fax: +86<br />

579 82282932; Tel: +86 579 82282932<br />

removes in situ CO 2 produced from the reactions and the<br />

adsorbent is periodically regenerated using the principle <strong>of</strong><br />

temperature swing adsorption (TSA), resulting in a higher<br />

conversion <strong>of</strong> the reactant methane at relatively lower temperatures.<br />

Inherently, the purification requirements for the desired<br />

product H 2 can be dramatically reduced or even eliminated. In<br />

order to achieve this objective, it is crucial to find an efficient<br />

adsorbent that can adsorb CO 2 rapidly with high adsorption<br />

capacity at the reaction temperatures.<br />

Many solid adsorbents, mainly CaO- and MgO-based materials,<br />

have been used for the in situ removal <strong>of</strong> CO 2 produced<br />

from SMR and WGS reactions in order to enhance H 2 production.<br />

1,5,6 However, the use <strong>of</strong> this type <strong>of</strong> adsorbent encounters<br />

some obstacles such as very slow CO 2 capture–regeneration rate,<br />

requirement <strong>of</strong> high temperature for regeneration, poor<br />

mechanical stability due to a large volume expansion after CO 2<br />

adsorption, and dramatic reduction <strong>of</strong> CO 2 adsorption efficiency<br />

in terms <strong>of</strong> uptake rate and capacity in the presence <strong>of</strong> steam.<br />

Recently, Li-containing materials, such as lithium zirconate<br />

(Li 2 ZrO 3 ), have been reported to be promising candidates with<br />

high CO 2 capture capacity, high stability, and ease <strong>of</strong> regeneration.<br />

7,8 Nakagawa and Ohashi 7,9 have reported that Li 2 ZrO 3 can<br />

react with CO 2 in a temperature range from 723 to 873 K, based<br />

on the following reaction:<br />

Li 2 ZrO 3(s) +CO 2(g) % Li 2 CO 3(s) + ZrO 2(s) (1)<br />

From eqn (1), the stoichiometric adsorption capacity <strong>of</strong> CO 2 is<br />

up to 28.7 wt.%. Furthermore, the volume increase <strong>of</strong> a Li 2 ZrO 3<br />

particle after the saturated adsorption <strong>of</strong> CO 2 is only 34%, much<br />

less than when CaO or MgO is used as adsorbent, 7 implying<br />

a comparably higher mechanical stability when the adsorbent is<br />

admixed with the catalyst in the reactor. Additionally, the<br />

3838 | J. Mater. Chem., 2011, 21, 3838–3842 This journal is ª The Royal Society <strong>of</strong> <strong>Chemistry</strong> 2011


temperature for the regeneration <strong>of</strong> CO 2 -adsorbed Li 2 ZrO 3 is<br />

much lower, and the presence <strong>of</strong> steam can improve the CO 2<br />

capture properties <strong>of</strong> Li 2 ZrO 3 . 10 These merits <strong>of</strong> Li 2 ZrO 3 lead to<br />

its applicability as an adsorbent for the in situ removal <strong>of</strong> CO 2<br />

produced from SMR and WGS reactions to enhance H 2<br />

productivity. 9<br />

Various solid-state synthetic methods have been used to<br />

prepare Li 2 ZrO 3 powder. 7,11 In a solid-state process, starting<br />

materials, usually ZrO 2 and Li 2 CO 3 , are mechanically mixed and<br />

heated at high temperatures for a long time. Consequently, sintering<br />

at high temperatures results in large particle sizes <strong>of</strong> the<br />

resulting Li 2 ZrO 3 . Meanwhile, the sublimation <strong>of</strong> Li 2 O cannot<br />

be avoided due to high-temperature calcination. These aspects<br />

lead to poor CO 2 adsorption properties <strong>of</strong> the Li 2 ZrO 3 powder<br />

prepared by the solid-state method. Nair et al. 11 pointed out that<br />

the smaller the size <strong>of</strong> Li 2 ZrO 3 particles, the faster their CO 2<br />

uptake. In addition, Lin’s group 12,13 proposed a ‘double-shell’<br />

model for CO 2 adsorption in Li 2 ZrO 3 , which indicates that<br />

Li 2 ZrO 3 <strong>of</strong> a smaller particle size shows a faster CO 2 uptake.<br />

In order to prepare Li 2 ZrO 3 with a fine particle size, a liquidphase<br />

method was proposed by Yi and Eriksen. 14 A dramatic<br />

improvement <strong>of</strong> CO 2 adsorption efficiency in the Li 2 ZrO 3<br />

particles prepared by the liquid-phase method was observed,<br />

yielding a higher capacity and about ten times faster uptake.<br />

Later, Chen and coworkers 15,16 reported a modified liquid-phase<br />

method to prepare nanocrystalline Li 2 ZrO 3 , in which soluble Zr<br />

and Li compounds were used as raw materials to obtain<br />

a complex solution containing Zr and Li precursors with<br />

appropriate amounts, and then the solution was spray dried to<br />

form Li 2 ZrO 3 powder. After calcination, the obtained nanocrystalline<br />

Li 2 ZrO 3 showed a better uptake for CO 2 under the<br />

applied conditions.<br />

Although Li 2 ZrO 3 prepared by the liquid-phase method exhibits<br />

a faster uptake, compared to those synthesized by the solid-state<br />

method, the uptake <strong>of</strong> CO 2 is still slow, especially for the case at<br />

CO 2 partial pressures below 0.5 bar. Furthermore, the adsorption<br />

<strong>of</strong> CO 2 hardly reaches its stoichiometric adsorption capacity. It<br />

should be noted that in the liquid-phase procedure soluble Li and<br />

Zr salts are dissolved together, followed by evaporation <strong>of</strong> the<br />

solvent to form a solid mixture containing Li and Zr species.<br />

Differences in the solubility <strong>of</strong> each component would result in<br />

a heterogeneous distribution <strong>of</strong> Li and Zr species. Consequently,<br />

the heterogeneity <strong>of</strong> their spatial distribution would bring forth an<br />

incomplete formation <strong>of</strong> the Li 2 ZrO 3 phase after calcination.<br />

Therefore, the Li 2 ZrO 3 adsorbents prepared by this liquid-phase<br />

method could not possess the desired CO 2 capture properties.<br />

The citrate sol–gel method was first proposed by Pechini 17 for<br />

preparing ABO 3 -perovskite type powders. The typical synthesis<br />

procedure is described as follows: metallic ions and citrate form<br />

complex anions at first and then a sol forms by the polymerization<br />

<strong>of</strong> citrate in glycol. After the evaporation <strong>of</strong> solvent, a gel<br />

comes into being, during which multi-metallic components are<br />

confined in the gel net. After the removal <strong>of</strong> the organic gel by<br />

calcination, a fine powder <strong>of</strong> desired stoichiometric composition<br />

can be obtained. Subsequently, Choy and Han 18 developed<br />

a modified citrate sol–gel method, in which water was used<br />

instead <strong>of</strong> glycol. The citrate sol–gel method is now a common<br />

approach for the synthesis <strong>of</strong> ABO 3 -type nanocrystals. Although<br />

the synthesis <strong>of</strong> ABO 3 -type powders such as Pb(Zr,Ti)O 3 oxides<br />

etc. via the citrate (or modified) sol–gel method has been intensively<br />

investigated, the synthesis <strong>of</strong> Li 2 ZrO 3 nanocrystals via this<br />

method is rarely reported.<br />

In the present work, a citrate sol–gel method has been used to<br />

synthesize Li 2 ZrO 3 nanocrystals. The CO 2 capture–regeneration<br />

properties <strong>of</strong> the synthesized nanocrystals have been investigated<br />

over a wide range <strong>of</strong> CO 2 pressures at different temperatures by<br />

thermogravimetric analysis (TGA).<br />

Experimental<br />

Chemicals<br />

Zirconium oxynitrate [ZrO(NO 3 ) 2 $2H 2 O] was purchased from<br />

Tianjin Guangfu Fine Chemical Research Institute. Lithium<br />

nitrate (LiNO 3 ) was purchased from Shanghai Shanpu Chemical<br />

Co., Ltd. Citric acid (CA, C 6 H 8 O 7 $H 2 O) and urea [CO(NH 2 ) 2 ]<br />

were purchased from Shantou Xilong Chemical Factory. All the<br />

reagents were analytical grade and used as received without<br />

further purification. The deionized water was obtained from<br />

Millipore Milli-QÒ ultrapure water purification systems with<br />

a resistivity greater than 18.2 MU.<br />

Syntheses<br />

In a typical citrate sol–gel synthesis, 2.67 g ZrO(NO 3 ) 2 $2H 2 O,<br />

1.38 g LiNO 3 , 6.30 g CA, and 3.00 g urea were dissolved in 46 ml<br />

deionized water. The solution was heated to 343 K and aged for 6<br />

h with stirring and then was exposed to air to evaporate the<br />

solvent until a gel was formed. The resulting gel was dried at 393<br />

K in an oven overnight, and the formed solid is referred to as the<br />

as-obtained sample. The as-obtained powder was put into<br />

a dense alumina crucible in a furnace box where the temperature<br />

was first increased to 673 K at a rate <strong>of</strong> 1 K min :1 and then<br />

maintained at 673 K in stagnant air for 2 h. Afterwards the<br />

temperature was further increased to 923 K at a rate <strong>of</strong> 1 K min :1<br />

and maintained for 6 h. After being cooled down to room<br />

temperature, the final white powder was obtained.<br />

For comparison, Li 2 ZrO 3 particles were synthesized by<br />

coprecipitation and liquid-phase methods. In a coprecipitation<br />

synthesis, the dose and addition order <strong>of</strong> the raw materials and<br />

the heat treatment that followed were the same as those in the<br />

sol–gel synthesis, except that no citric acid was used. In a liquidphase<br />

method, neither citric acid nor urea was used. The samples<br />

prepared by the citrate sol–gel, coprecipitation, and liquid-phase<br />

methods are referred to as LZ-sg, LZ-co, and LZ-lp, respectively.<br />

Characterization<br />

The X-ray diffraction patterns were recorded on a Philips<br />

PW3040/60 diffractometer using CuKa radiation (l ¼ 1.54 A).<br />

The scans were recorded in the 2q range between 10 and 90 with<br />

a step width <strong>of</strong> 0.03 . The average crystallite size <strong>of</strong> powder was<br />

calculated using Scherrer’s equation from the width <strong>of</strong> the<br />

reflection peak located at 2q ¼ 42.3 . Silicon standard, Si, was<br />

used as reference material to determine the instrumental line<br />

broadening.<br />

The scanning electron microscope (SEM) observations were<br />

performed on a Hitachi S-4800 apparatus equipped with a field<br />

emission gun. The acceleration voltage was set to 5 kV. The<br />

This journal is ª The Royal Society <strong>of</strong> <strong>Chemistry</strong> 2011 J. Mater. Chem., 2011, 21, 3838–3842 | 3839


sample was stuck on the observation platform and sprayed with<br />

gold vapor under high vacuum for about 20 s. The transmission<br />

electron microscopy (TEM) observations were carried out on<br />

a Philips Tecnai F20 transmission electron microscope working<br />

at 200 kV. The sample was diluted in ethanol to give a 1 : 5<br />

volume ratio, and sonicated for 10 min. The ethanol slurry was<br />

then dripped onto a Cu grid covered with a thin film <strong>of</strong> carbon.<br />

The TGA-DTA experiments with ca. 15 mg <strong>of</strong> the as-obtained<br />

samples were carried out on a NETZSCH STA449 thermogravimetric<br />

analyzer with a heating rate <strong>of</strong> 20 K min :1 in an air flow<br />

<strong>of</strong> 40 ml min :1 .<br />

CO 2 adsorption<br />

The adsorption <strong>of</strong> CO 2 in the synthesized Li 2 ZrO 3 nanocrystals<br />

was studied on a thermogravimetric analyzer (NETZSCH<br />

STA449). The sample cell (a dense alumina crucible pot) was<br />

loaded with ca. 15 mg <strong>of</strong> adsorbent. Prior to the CO 2 adsorption<br />

experiments, the adsorbent was heated up to the desired<br />

temperature (823 K or 773 K) at a rate <strong>of</strong> 10 K min :1 in<br />

a nitrogen flow <strong>of</strong> 40 ml min :1 , during which the adsorbed<br />

impurities in the sample were removed. Then, the N 2 flow was<br />

switched to a mixture flow containing CO 2 and N 2 or to a pure<br />

CO 2 flow for adsorption, all at 1 bar. The partial pressure <strong>of</strong> CO 2<br />

was determined by its fraction <strong>of</strong> the total feed flow rate and the<br />

total pressure. The total feed flow was always set at 40 ml min :1 .<br />

The adsorption <strong>of</strong> CO 2 was carried out for 60 min, referred to as<br />

period I. Afterwards, the feed gas stream was switched to a pure<br />

N 2 flow <strong>of</strong> 40 ml min :1 and the temperature was raised at a rate <strong>of</strong><br />

10 K min :1 to 923 K, maintaining this temperature for 50 min.<br />

This desorption (regeneration) process lasted 60 min, referred to<br />

as period II. The combined period I and period II is defined as<br />

one adsorption–desorption (capture–regeneration) cycle. To<br />

correct for the weight change caused by the change in the density<br />

<strong>of</strong> the gas phase, blank experiments were performed. In a blank<br />

experiment the TGA response was measured with the empty<br />

dense alumina crucible pot used.<br />

Results and discussion<br />

The as-obtained sample prepared via the citrate sol–gel method<br />

contains a large amount <strong>of</strong> organic species. As shown in the TGA<br />

curve (Fig. 1), a decrease <strong>of</strong> 85% by weight can be seen in the<br />

range from 298 to 1123 K. The whole weight loss process can be<br />

divided into two stages. The first with a weight loss <strong>of</strong> 55%<br />

accompanied with a broad endothermic peak at temperatures<br />

between 298 and 533 K should be attributed to the desorption or<br />

decomposition <strong>of</strong> the organic species, partially from the citrate<br />

precursor. 19 The second stage with a weight loss <strong>of</strong> ca. 30% starts<br />

at 673 K and an exothermic peak around 847 K can be observed<br />

in the DTA curve, corresponding to the drastic combustion <strong>of</strong><br />

the organic species in the sample. The weight stays constant at<br />

temperatures over 923 K, which is much lower than those (ca.<br />

1273 K) required for preparing Li 2 ZrO 3 powder via the solidstate<br />

reaction method. 7<br />

The adsorption and desorption pr<strong>of</strong>ile <strong>of</strong> CO 2 in the Li 2 ZrO 3<br />

adsorbent prepared via the citrate sol–gel method is shown as<br />

curve a in Fig. 2. At 823 K and a CO 2 partial pressure <strong>of</strong> 0.5 bar,<br />

the uptake <strong>of</strong> CO 2 reaches 26 wt.% within 20 min, which is about<br />

90% <strong>of</strong> the stoichiometric adsorption capacity <strong>of</strong> CO 2 in Li 2 ZrO 3<br />

(28.7 wt.%). Additionally, the desorption in flowing N 2 is also<br />

fast and the complete desorption takes less than 20 min. To<br />

illustrate the role <strong>of</strong> citric acid in the synthesis <strong>of</strong> Li 2 ZrO 3 , two<br />

samples without the use <strong>of</strong> citric acid have been synthesized for<br />

comparison. The adsorption and desorption pr<strong>of</strong>iles <strong>of</strong> CO 2 in<br />

these two samples are also shown in Fig. 2. The Li 2 ZrO 3 sample<br />

prepared by the liquid-phase method, i.e. LZ-lp, displays the<br />

lowest CO 2 uptake rate under the investigated conditions, see<br />

curve c in Fig. 2. Although the Li 2 ZrO 3 sample prepared by the<br />

coprecipitation method, i.e. LZ-co, shows some improved CO 2<br />

capture properties in comparison with LZ-lp, its CO 2 uptake is<br />

still slower, compared to that in the Li 2 ZrO 3 sample prepared by<br />

the sol–gel method, i.e. LZ-sg. These results clearly show that<br />

LZ-sg has the best CO 2 capture properties.<br />

It has been reported that the crystallite phase <strong>of</strong> Li 2 ZrO 3 can<br />

have a great influence on CO 2 capture properties. 11 Fig. 3 shows the<br />

XRD patterns <strong>of</strong> the Li 2 ZrO 3 samples prepared by the aforementioned<br />

three methods, indicating that both tetragonal and<br />

monoclinic crystallite phases are present in all samples. However,<br />

as shown in Fig. 3, the crystallite phase <strong>of</strong> LZ-sg is mainly<br />

tetragonal. Nair et al. 11 reported that Li 2 ZrO 3 crystallites with<br />

a tetragonal phase showed better CO 2 -capture properties in terms<br />

<strong>of</strong> uptake rate than those with a monoclinic phase. The current<br />

results are in agreement with this observation from the literature.<br />

Fig. 1 TGA and DTA curves <strong>of</strong> the as-obtained sample synthesized via<br />

the citrate sol–gel method with a heating rate <strong>of</strong> 20 K min :1 in an air flow<br />

<strong>of</strong> 40 ml min :1 .<br />

Fig. 2 Adsorption and desorption pr<strong>of</strong>iles <strong>of</strong> CO 2 for three different<br />

Li 2 ZrO 3 samples. (a) LZ-sg, (b) LZ-co, (c) LZ-lp; (I) adsorption at 823 K<br />

and a CO 2 partial pressure <strong>of</strong> 0.5 bar, (II) desorption by heating (10 K<br />

min :1 ) to 923 K in a pure N 2 flow <strong>of</strong> 40 ml min :1 .<br />

3840 | J. Mater. Chem., 2011, 21, 3838–3842 This journal is ª The Royal Society <strong>of</strong> <strong>Chemistry</strong> 2011


Fig. 3 XRD patterns <strong>of</strong> three different Li 2 ZrO 3 samples. (a) LZ-sg, (b)<br />

LZ-co, (c) LZ-lp.<br />

The uptake rate <strong>of</strong> CO 2 should be also related to the crystallite<br />

size <strong>of</strong> Li 2 ZrO 3 . The crystallite sizes <strong>of</strong> the three different<br />

samples, estimated from the XRD data using Scherrer’s equation,<br />

are 17, 26, and 34 nm for LZ-sg, LZ-co, and LZ-lp,<br />

respectively. It is logical from an engineering point <strong>of</strong> view that<br />

the smaller the size <strong>of</strong> Li 2 ZrO 3 crystals, the faster the CO 2 uptake<br />

in case <strong>of</strong> a diffusion limited process.<br />

The stability <strong>of</strong> an adsorbent is crucial when applied to the in<br />

situ removal <strong>of</strong> CO 2 produced in some reactions such as steam–<br />

methane reforming (SMR) and water–gas shift (WGS) reaction<br />

to enhance hydrogen production as well as in the separation <strong>of</strong><br />

CO 2 from fuel-fired power stations at high temperatures.<br />

Therefore, the stability <strong>of</strong> LZ-sg was investigated by TGA. Fig. 4<br />

shows three CO 2 capture–regeneration cycles, indicating an<br />

excellent stability <strong>of</strong> the Li 2 ZrO 3 crystals prepared by the citrate<br />

sol–gel method. This indicates the potential applicability <strong>of</strong> the<br />

synthesized nanosized Li 2 ZrO 3 crystallites with a tetragonal<br />

phase in the removal <strong>of</strong> CO 2 at high temperatures.<br />

Fig. 5A, B, and C show the morphologies <strong>of</strong> the unused, onecycle<br />

used, and three-cycles used LZ-sg samples by SEM images,<br />

indicating that all the samples consist <strong>of</strong> crystallite agglomerates,<br />

confirmed by the TEM observation, as shown in Fig. 5D.<br />

Additionally, these SEM images give evidence that the particles<br />

do not become larger after CO 2 capture–regeneration cycles,<br />

unlike CaO- or MgO-based adsorbents, in which the particles are<br />

easily enlarged after regeneration at high temperatures, 20 resulting<br />

in the rapidly reduced uptake rate <strong>of</strong> CO 2 . The results from<br />

Fig. 5 SEM images <strong>of</strong> the unused (A), one-cycle used (B), and threecycles<br />

used (C) LZ-sg samples and the TEM image (D) <strong>of</strong> the unused<br />

LZ-sg sample.<br />

Fig. 6 Uptake pr<strong>of</strong>iles <strong>of</strong> CO 2 in LZ-sg at different partial pressures <strong>of</strong><br />

CO 2 and 823 K.<br />

Fig. 5 give an explanation for the stability <strong>of</strong> the Li 2 ZrO 3<br />

prepared by the citrate sol–gel method for CO 2 capture.<br />

The uptake pr<strong>of</strong>iles <strong>of</strong> CO 2 in LZ-sg at different partial pressures<br />

<strong>of</strong> CO 2 are shown in Fig. 6. Obviously, the uptake rate<br />

decreases with decreasing CO 2 pressure at the same temperature.<br />

When the partial pressure <strong>of</strong> CO 2 is below 0.25 bar, the uptake<br />

becomes rather slow and the capacity is not fully reached within<br />

60 min. In addition, almost no uptake takes place at CO 2 pressures<br />

below 0.15 bar, probably due to thermodynamic limitations.<br />

Thus, the uptake rate <strong>of</strong> CO 2 in Li 2 ZrO 3 strongly depends<br />

on CO 2 pressure.<br />

Conclusions<br />

Fig. 4 Three cycles <strong>of</strong> CO 2 capture–regeneration in LZ-sg. (I) adsorption<br />

at 773 K and a CO 2 partial pressure <strong>of</strong> 0.5 bar, (II) regeneration by<br />

heating (10 K min :1 ) to 923 K in a pure N 2 flow <strong>of</strong> 40 mL min :1 .<br />

The citrate sol–gel method has been developed to prepare<br />

Li 2 ZrO 3 nanocrystals that can adsorb 26 wt.% CO 2 within 20<br />

min, which is about 90% <strong>of</strong> the stoichiometric capacity <strong>of</strong> CO 2 in<br />

Li 2 ZrO 3 (28.7 wt.%), at 823 K and CO 2 partial pressures above<br />

0.5 bar. The adsorbent shows a good stability, confirmed by<br />

repeated CO 2 capture–regeneration cycles. The small sol–gel<br />

This journal is ª The Royal Society <strong>of</strong> <strong>Chemistry</strong> 2011 J. Mater. Chem., 2011, 21, 3838–3842 | 3841


synthesized Li 2 ZrO 3 crystallites with a tetragonal phase exhibit<br />

better CO 2 capture–regeneration properties than those prepared<br />

by other synthesis methods. The uptake rate <strong>of</strong> CO 2 decreases<br />

with decreasing CO 2 pressure, reaching a thermodynamic limit at<br />

around 0.15 bar. The synthesized Li 2 ZrO 3 nanocrystals with<br />

excellent properties for CO 2 capture–regeneration display a good<br />

prospect for application in the in situ removal <strong>of</strong> CO 2 produced<br />

in some reactions such as steam–methane reforming (SMR) and<br />

water–gas shift (WGS) reaction to enhance hydrogen production<br />

as well as in the separation <strong>of</strong> CO 2 from fuel-fired power stations<br />

at high temperatures.<br />

Acknowledgements<br />

The financial supports by the National Basic Research Program<br />

<strong>of</strong> China (2009CB626607) and the Natural Science Foundation<br />

<strong>of</strong> Zhejiang Province, China (R4080084 and Y4090473) are<br />

gratefully acknowledged.<br />

Notes and references<br />

1 K. Schoots, F. Ferioli, G. J. Kramer and B. C. C. van der Zwaan, Int.<br />

J. Hydrogen Energy, 2008, 33, 2630–2645.<br />

2 J. A. Moulijn, M. Makkee and A. van Diepen, Chemical Process<br />

Technology, Wiley, New York, 2001.<br />

3 J. R. Hufton, S. Mayorga and S. Sircar, AIChE J., 1999, 45, 248–256.<br />

4 B. T. Carvill, J. R. Hufton, M. Anand and S. Sircar, AIChE J., 1996,<br />

42, 2765–2772.<br />

5 N. H. Florin and A. T. Harris, Chem. Eng. Sci., 2009, 64, 187–191.<br />

6 C. R. Muller, R. Pacciani, C. D. Bohn, S. A. Scott and J. S. Dennis,<br />

Ind. Eng. Chem. Res., 2009, 48, 10284–10291.<br />

7 K. Nakagawa and T. Ohashi, J. Electrochem. Soc., 1998, 145, 1344–<br />

1346.<br />

8 M. Olivares-Marin, M. Castro-Diaz, T. C. Drage and M. M. Maroto-<br />

Valer, Sep. Purif. Technol., 2010, 73, 415–420.<br />

9 K. Nakagawa and T. Ohashi, Electrochemistry, 1999, 67, 618–621.<br />

10 L. Martinez-DlCruz and H. Pfeiffer, J. Phys. Chem. C, 2010, 114,<br />

9453–9458.<br />

11 B. N. Nair, T. Yamaguchi, H. Kawamura, S. I. Nakao and<br />

K. Nakagawa, J. Am. Ceram. Soc., 2004, 87, 68–74.<br />

12 J. Ida, R. Xiong and Y. S. Lin, Sep. Purif. Technol., 2004, 36, 41–51.<br />

13 R. T. Xiong, J. Ida and Y. S. Lin, Chem. Eng. Sci., 2003, 58, 4377–<br />

4385.<br />

14 K. B. Yi and D. O. Eriksen, Sep. Sci. Technol., 2006, 41, 283–296.<br />

15 E. Ochoa-Fernandez, M. Ronning, T. Grande and D. Chen, Chem.<br />

Mater., 2006, 18, 1383–1385.<br />

16 E. Ochoa-Fernandez, M. Ronning, T. Grande and D. Chen, Chem.<br />

Mater., 2006, 18, 6037–6046.<br />

17 M. P. Pechini, US pat., 3 330 697, 1967.<br />

18 J. H. Choy and Y. S. Han, J. Mater. Chem., 1997, 7, 1815–1820.<br />

19 C. Mao, X. Dong and T. Zeng, Mater. Lett., 2007, 61, 1633–1636.<br />

20 A. Silaban, M. Narcida and D. P. Harrison, Chem. Eng. Commun.,<br />

1996, 146, 149–162.<br />

3842 | J. Mater. Chem., 2011, 21, 3838–3842 This journal is ª The Royal Society <strong>of</strong> <strong>Chemistry</strong> 2011

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