The fluid-mosaic model, homeoviscous adaptation, and ionic liquids: dramatic lowering of the melting point by side-chain unsaturation.
The fluid-mosaic model, homeoviscous adaptation, and ionic liquids: dramatic lowering of the melting point by side-chain unsaturation.
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DOI:
10.1002/anie.200906169
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发表时间:
2010-04
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通讯作者:
Samuel M. Murray;R. A. O'brien;Kaila M. Mattson;C. Ceccarelli;R. Sykora;Kevin N. West;James H. Davis-James-H.-Davi
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文献类型:
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作者:
Samuel M. Murray;R. A. O'brien;Kaila M. Mattson;C. Ceccarelli;R. Sykora;Kevin N. West;James H. Davis-James-H.-Davi
Proposed by Singer and Nicolson in 1972,[1] the fluid-mosaic model holds that the phospholipid bilayer is a dynamic twodimensional solvent milieu. Its proper function is closely tied to its “fluidity”, and that is often quantified by reference to the melting point, Tm (increased fluidity corresponds to a lower Tm value). The fluid-mosaic model is highly evocative of the emerging picture of nanoscale structuring in ionic liquids (ILs),[2, 3] and just as the function of phospholipid bilayers is tied to the Tm value, so too is the utility of ILs. Whereas the former often have low Tm values despite being composed of charged species with long aliphatic appendages, the fluidity of ILs generally decreases when progressively longer aliphatic appendages are used.[4] It is a challenge to design imidazolium ILs (the most common IL class) that incorporate progressively more lipophilic structural elements while keeping their melting points below room temperature (Figure 1).[4–9] Indeed, the Tm values of these ILs begin to rise dramatically once an appended N-alkyl group exceeds seven carbon atoms in length. Herein we report that by using an approach modeled on homeoviscous adaptation (HVA),[10] ILs with very long alkyl appendages and very low Tm values can be prepared. This discovery may have significant implications for IL use in enzymatic catalysis, lubricants, heat-transfer fluids, and gas storage and separation, among other applications. Widely accepted as a mechanism by which the melting temperature of cell membranes is modulated, HVA is the incorporation into cell membranes of phospholipids with “kinked” tail structures.[10] It is argued that the packing efficiency of the collective membrane hydrophobic components is diminished by the presence of these phospholipids and that increased fluidity results. A comparison of the Tm value of distearoylphosphatidylcholine with that of dioleylphosphatidylcholine provides a dramatic example of how much impact this seemingly trivial difference can have. The former, with its linear, saturated C18 tails has a Tm value of 588C; the latter, with its “kinked” C18 tails (each of which incorporates a cis-alkenyl group), has a Tm value of À228C. This effect is also at the heart of the Tm difference between the solid triacyl glycerols called fats, and those that are liquid at room temperature known as oils. In both instances, the effect is probably entropic in nature, as in the case of anthracene (“linear”, Tm= 2178C) and phenanthrene (“kinked”, Tm= 998C).[11] Accordingly, we hypothesized that ILs with long, unsaturated, aliphatic tail structures would, like the corresponding phospholipids, have significantly lower Tm values than their counterparts with saturated appendages. To test the validity of our hypothesis by measuring their Tm values, we prepared a series of lipid-inspired ILs in a threestep process from high-purity (99+%) fatty-alcohol mesylates, 1-methylimidazole, NaI, and NaTf2N.[12] Each of the ILs (Scheme 1) had a long alkyl appendage identical to that in a natural fatty acid. Compounds 1, 3, and 8 feature fully saturated C16, C18, and C20 side chains, respectively, and their