Supramolecular Polymerizations

Supramolecular Polymerizations Supramolecular Polymerizations

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522 A. Ciferri Figure 14. (a) Disk-shaped, three blades molecule prepared by Meijer and coworkers [4] with side chains having polar, nonpolar, chiral, achiral character. [32, 33] (b) Formation of a helical assembly when the blades assume a propeller-like conformation. [100] (c) Schematic representation of the transition from dispersed disks to partially ordered and to fully ordered columns. [76] (i Am. Chem. Soc. 2000 and 2001.) mation of long columns was shown to occur in very dilute solution in hexane (10 –6 m), and a large association constant (10 8 m –1 ) was reported. [32] It was suggested that such an aggregation reflects the formation of helical columns through a cooperative process attributed to a conformational transition from flat to propeller shape for the blades of each disk, resulting in a maximization of interaction for the chiral helical assembly (Figure 14b). [100] Experimental data for the more polar molecules in dilute butanol (2.4610 –4 m) [33] revealed a sequence of two association steps upon temperature changes. The postulated process is schematized in Figure 14c: starting with an isotropic dispersion of disks, a decrease in the temperature causes the formation of low-DP achiral aggregates stabilized by non-cooperative interaction, followed at a lower critical temperature by the cooperative formation of helical columns with DP attaining the 1000 range. [76] The theoretical description of the processes described above was formulated by van der Schoot and coworkers. [76] The occurrence of the two regimes was described in terms of the cooperativity parameter r. The situation r =1is equivalent to the binding of unimers into disordered aggregates (i.e. MSOA), while r s 1 describes the subsequent cooperative formation of ordered aggregates by a HG mechanism. Essentially, the treatment is a generalization of the Zimm-Bragg and the Oosawa theories (Kh A K) without necessarily specifying a detailed molecular model and a critical nucleus. With respect to Oosawa’s treatment that focused on the critical concentration C* (cf. Figure 4c), Figure 15. (a) Deoxyguanosine, its oligomers, and folic acid. Their assembly in tetrameric disks. [36] (b) Variation of the number of stacked tetrameric disks with folate concentration in (1) pure H2O and (2) 1 m NaCl at 308 C. The vertical broken line indicates the I e H transition (replotted using data taken from ref. [26] ). the van der Schoot treatment emphasizes the fractions of aggregated material and helical bonds as a function of both temperature and concentration. Rigidity and excluded volume effects are not introduced and, therefore, liquid crystallinity does not direct the aggregation of the stacks. 5.3.3 Supermolecules. Tubular Assemblies The formation of disk-like supermolecules from two or more complementary components was discussed by several authors. [2, 34–36, 43, 44] Disk-like supermolecules often show liquid-crystalline behavior even though the separate components do not. Moreover, the discotic supermolecules can form columnar stacks in the melt and in solution just as the molecular discotics discussed above do. The relative contributions of MSOA, HG and SLC mechanisms have not always been characterized adequately. Gottarelli et al. [35, 36] have investigated the most interesting assembly of the nucleotide deoxyguanosine, its oligomers and alkaline folates (Figure 15a). These compounds form hydrogen-bonded disk-like tetramers in solution and are able to assemble in columnar stacks of discrete length and DP. Small-angle neutron scattering techniques were used to determine the length of the aggregates in water and in salt solutions. The critical concentrations for the appearance of the nematic (cholesteric) and the hexagonal phases were determined by means of X-ray diffraction. Selected data for the deoxyguanosine dimer (d(GpG); Figure 15a) and the folate is

Supramolecular Polymerizations 523 Table 2. Critical concentration and DP in the isotropic phase for folic acid (selected data taken from ref. [36] ). Sample Solvent C IN % C NH % LISO DPISO a) XISO b) d(GpG) H2O – – 70 15 2.3 d(GpG) H2O +Na + 2.5 18 – – – d(GpG) H2O +K + 1.5 15 – – – folate H2O – 35 2.3 1 0.1 folate H2O +Na + 27 35 2.1 9 0.7 a) L/2.35 Š (4.70 for d(GpG)). b) L/30 Š. collected in Table 2. The deoxyguanosine derivatives generally show larger DPs in isotropic solutions and lower critical concentrations CIN and CNH than the folates. The presence of NA + and, particularly, K + ions enhances the stabilization of the aggregates. In the case of folates in pure H2O, no nematic phase and small DPs were observed. Due to the considerable diameter of the cylinders (D L 30 Š) and the thickness of each disk (L = 2.35 Š), the DP in the isotropic phase is extremely small and the corresponding axial ratio X suggests that thick disks rather than columns are present. Figure 15b illustrates the evolution of DP with concentration covering the range from the isotropic to the hexagonal phase. The smooth dependence DP vs C does not evidence cooperative effects in the case of folates. The largest DP (L30), determined from a 60% (hexagonal) solution, reveals in fact columns of very small geometric anisotropy (X L 2.3). The formation of the mesophase may be promoted by the large excluded volume effect of disks even in the absence of soft interactions. In fact, simulation studies evidenced nematic and columnar phases for solutions of extremely thin disks (0 a L/D a 0.1). [101] Disk-like supermolecules based on dimers of ureidotriazines connected by a 4 H-bond scheme similar (but not identical) to that of the ureidopyrimidone polymers in Figure 7c were reported by Meijer and coworkers. [34] These disks stack in columns with loose positional order and low DP (Figure 16a). Percec and coworkers [44] reported tubular polymeric assemblies of disks composed by six tapered molecules of 12-ABG-15C5 complexed with triflate salt (Figure 16b). The columns assembled into a hexagonal mesophase revealed as by means of Xray diffraction from the undiluted system. Several of the systems described above present a central cavity into which a covalent polymer can be hosted or a flow of ions be achieved (cf. also next section). Of particular interest are nanotubes (Figure 16c) formed by stacking cyclic peptides connected by H-bonds along the columnar axis. [37–41] The chemical design of these flat ring-like peptides was discussed by De Santis and coworkers. [37] Tubes assembled in solution and the contact forces for the dimerization (K L 2.5610 3 m –1 ) are too Figure 16. (a) Monofunctional ureidotriazine disks capable of assembling into columns. [34] (b) Assembly of tapered 12-ABG- 12C5 into disks, formation of a column of stacked disk, hexagonal columnar organization. [44] (c) Nanotubules formed by Hbonded cyclic peptides. [37] (i Am. Chem. Soc. 1994 and 1996.) small for a large DP unless cooperative effects occur. [38] Cyclic b-peptides were also considered. [39] The self assembly of the nanotubules into ion-selective membranes was discussed as well. [40] Unimers of most of the systems considered above were subsequently connected by flexible covalent spacers, producing main-chain or side-chain SPs that should be described more appropriately under class C SPs. The basic ability of the disks to form columnar assemblies was preserved, but the covalent segments produced alterations in the stacking details such as the occurrence of helicity. For instance, a slowly rising helicoidal stack was produced when the crown ether receptor in Figure 16b was replaced by a flexible endo-receptor (nEO- PMA) connected as a side-chain to a poly(methyl acrylate) chain. [42] When the ureidotriazine disks in Figure 16a were main-chain linked through flexible spacers, helical columns and large DPs were observed. [34] Applications. The columnar nematic or hexagonal packing of disk-like molecules and supermolecules could be exploited as a precursor step for the assembly of large, oriented structures modeling natural systems. Electronic mobility due to the p–p interactions along the columnar axis may be useful for electronic and photonic devices. [102] Central cavities could be exploited for the selective hosting of polymer molecules [44] or for ion- [40, 41] selective channels. 5.4 Host/Guest Polymeric Assemblies Covalent polymers can enter a cavity of a columnar assembly or of single ring-like structures. The result is a composite host/guest polymeric assembly exhibiting a

<strong>Supramolecular</strong> <strong>Polymerizations</strong> 523<br />

Table 2. Critical concentration and DP in the isotropic phase<br />

for folic acid (selected data taken from ref. [36] ).<br />

Sample Solvent C IN<br />

%<br />

C NH<br />

%<br />

LISO DPISO a) XISO b)<br />

d(GpG) H2O – – 70 15 2.3<br />

d(GpG) H2O +Na + 2.5 18 – – –<br />

d(GpG) H2O +K + 1.5 15 – – –<br />

folate H2O – 35 2.3 1 0.1<br />

folate H2O +Na + 27 35 2.1 9 0.7<br />

a) L/2.35 Š (4.70 for d(GpG)).<br />

b) L/30 Š.<br />

collected in Table 2. The deoxyguanosine derivatives<br />

generally show larger DPs in isotropic solutions and<br />

lower critical concentrations CIN and CNH than the folates.<br />

The presence of NA + and, particularly, K + ions enhances<br />

the stabilization of the aggregates. In the case of folates<br />

in pure H2O, no nematic phase and small DPs were<br />

observed. Due to the considerable diameter of the cylinders<br />

(D L 30 Š) and the thickness of each disk (L = 2.35<br />

Š), the DP in the isotropic phase is extremely small and<br />

the corresponding axial ratio X suggests that thick disks<br />

rather than columns are present. Figure 15b illustrates the<br />

evolution of DP with concentration covering the range<br />

from the isotropic to the hexagonal phase. The smooth<br />

dependence DP vs C does not evidence cooperative<br />

effects in the case of folates. The largest DP (L30), determined<br />

from a 60% (hexagonal) solution, reveals in fact<br />

columns of very small geometric anisotropy (X L 2.3).<br />

The formation of the mesophase may be promoted by the<br />

large excluded volume effect of disks even in the absence<br />

of soft interactions. In fact, simulation studies evidenced<br />

nematic and columnar phases for solutions of extremely<br />

thin disks (0 a L/D a 0.1). [101]<br />

Disk-like supermolecules based on dimers of ureidotriazines<br />

connected by a 4 H-bond scheme similar (but<br />

not identical) to that of the ureidopyrimidone polymers in<br />

Figure 7c were reported by Meijer and coworkers. [34]<br />

These disks stack in columns with loose positional order<br />

and low DP (Figure 16a). Percec and coworkers [44]<br />

reported tubular polymeric assemblies of disks composed<br />

by six tapered molecules of 12-ABG-15C5 complexed<br />

with triflate salt (Figure 16b). The columns assembled<br />

into a hexagonal mesophase revealed as by means of Xray<br />

diffraction from the undiluted system.<br />

Several of the systems described above present a central<br />

cavity into which a covalent polymer can be hosted<br />

or a flow of ions be achieved (cf. also next section). Of<br />

particular interest are nanotubes (Figure 16c) formed by<br />

stacking cyclic peptides connected by H-bonds along the<br />

columnar axis. [37–41] The chemical design of these flat<br />

ring-like peptides was discussed by De Santis and coworkers.<br />

[37] Tubes assembled in solution and the contact<br />

forces for the dimerization (K L 2.5610 3 m –1 ) are too<br />

Figure 16. (a) Monofunctional ureidotriazine disks capable of<br />

assembling into columns. [34] (b) Assembly of tapered 12-ABG-<br />

12C5 into disks, formation of a column of stacked disk, hexagonal<br />

columnar organization. [44] (c) Nanotubules formed by Hbonded<br />

cyclic peptides. [37] (i Am. Chem. Soc. 1994 and 1996.)<br />

small for a large DP unless cooperative effects occur. [38]<br />

Cyclic b-peptides were also considered. [39] The self<br />

assembly of the nanotubules into ion-selective membranes<br />

was discussed as well. [40]<br />

Unimers of most of the systems considered above were<br />

subsequently connected by flexible covalent spacers, producing<br />

main-chain or side-chain SPs that should be<br />

described more appropriately under class C SPs. The<br />

basic ability of the disks to form columnar assemblies<br />

was preserved, but the covalent segments produced<br />

alterations in the stacking details such as the occurrence<br />

of helicity. For instance, a slowly rising helicoidal stack<br />

was produced when the crown ether receptor in Figure<br />

16b was replaced by a flexible endo-receptor (nEO-<br />

PMA) connected as a side-chain to a poly(methyl acrylate)<br />

chain. [42] When the ureidotriazine disks in Figure<br />

16a were main-chain linked through flexible spacers,<br />

helical columns and large DPs were observed. [34]<br />

Applications. The columnar nematic or hexagonal<br />

packing of disk-like molecules and supermolecules could<br />

be exploited as a precursor step for the assembly of large,<br />

oriented structures modeling natural systems. Electronic<br />

mobility due to the p–p interactions along the columnar<br />

axis may be useful for electronic and photonic<br />

devices. [102] Central cavities could be exploited for the<br />

selective hosting of polymer molecules [44] or for ion-<br />

[40, 41]<br />

selective channels.<br />

5.4 Host/Guest Polymeric Assemblies<br />

Covalent polymers can enter a cavity of a columnar<br />

assembly or of single ring-like structures. The result is a<br />

composite host/guest polymeric assembly exhibiting a

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