Chiral hexa- and nonamethylene-bridged bis(L-Leu-oxalamide) gelators: the first oxalamide gels containing aggregates with a chiral morphology.

Chiral amino acid- and amino alcohol-oxalamides are well-known as versatile and efficient gelators of various lipophilic and polar organic solvents and water. To further explore the capacity of the amino acid/oxalamide structural fragment as a gelation-generating motif, the dioxalamide dimethyl esters 1(6)Me and 1(9)Me, and dicarboxylic acid 2(6)OH/2(9)OH derivatives containing flexible methylene bridges with odd (9; n=7) and even (6; n=4) numbers of methylene groups were prepared. Their self-assembly motifs and gelation properties were studied by using a number of methods (FTIR, (1)H NMR spectroscopy, CD, TEM, DSC, XRPD, molecular modeling, MMFF94, and DFT). In contrast to the previously studied chiral bis(amino acid or amino alcohol) oxalamide gelators, in which no chiral morphology was ever observed in the gels, the conformationally more flexible 1(6)Me, 1(9)Me, 2(6)OH, and 2(9)OH provide gelators that are capable of forming diverse aggregates of achiral and chiral morphologies, such as helical fibers, twisted tapes, nanotubules, straight fibers, and tapes, in some cases coexisting in the same gel sample. It is shown that the differential scanning calorimetry (DSC)-determined gelation enthalpies could not be correlated with gelator and solvent clogP values. Spectroscopic results show that intermolecular hydrogen-bonding between the oxalamide units provides the major and self-assembly directing intermolecular interaction in the aggregates. Molecular modeling studies reveal that molecular flexibility of gelators due to the presence of the polymethylene bridges gives three conformations (zz, p1, and p2) close in energy, which could form oxalamide hydrogen-bonded layers. The aggregates of the p1 and p2 conformations tend to twist due to steric repulsion between neighboring iBu groups at chiral centers. The X-ray powder diffraction (XRPD) results of 1(6)Me and 1(9)Me, xerogels prove the formation of p1 and p2 gel aggregates, respectively. The latter results explain the formation of gel aggregates with chiral morphology and also the simultaneous presence of aggregates of diverse morphology in the same gel system.