Mixed-chain phosphatidylcholine bilayers: structure and properties

Abstract

Calorimetric and X-ray diffraction data are reported for two series of saturated mixed-chain phosphatidylcholines (PCs), 18:0/n:0-PC and n:0/18:0-PC, where the sn-1 and sn-2 fatty acyl chains on the glycerol backbone are systematically varied by two methylene groups from 18:0 to 10:0 (n = 18,16, 14, 12, or 10). Fully hydrated PCs wre annealed at -4.degree. C and their multilamellar dispersions characterized by differential scanning calorimetry and X-ray diffraction. All mixed-chain PCs form low-temperture "crystalline" bilayer phases following low-temperature incubation, except 18:0/10:0-PC. The subtransition temperature (Ts) shifts toward the main (chain melting) transition temperature (Tm) as the sn-1 or sn-2 fatty acyl chain is reduced in length; for the shorter chain PCs (18:0/12:0-PC, 12:0/18:0-PC, and 10:0/18:0-PC), Ts is 1-2.degree. C greater than Tm, and the subtransition enthalpy (.DELTA.Hs) is much greater than for the longer acyl chain PCs. Tm decreases with acyl chain length for both series of PCs except 18:0/10:0-PC, while for the positional isomers, n:0/18:0-PC and 18:0/n:0-PC, Tm is higher for the isomer with the longer acyl chain in the sn-2 position of the glycerol backbone. The conversion from the crystalline bilayer Lc phase to the liquid-crystalline L.alpha. phase with melted hydrocarbon chains occurs through a series of phase changes which are chain length dependent. For example, 18:0/18:0-PC undergoes the phase changes Lc .fwdarw. L.beta.'' .fwdarw. P.beta.'' .fwdarw. L.alpha., while the shorter chain PC, 10:0/18:0-PC, is directly transformed from the Lc phase to the L.alpha. phase. However, normalized enthalpy and entropy data suggest that the overall thermodynamic change, Lc .fwdarw. L.alpha., is essentially chain length independent. On cooling, the conversion to the Lc phases occurs via bilayer gel phases, L.beta.'', for the longer chain PCs or through triple-chain interdigitated bilayer gel phases, L.beta.*, for the shorter chain PC 18:0/12:0-PC and possibly 10:0/18:0-PC. Molecular models indicate that the bilayer gel phases for the more asymmetric PC series, 18:0/n:0-PC, must undergo progressive interdigitation with chain length reduction to maintain maximum chain-chain interaction. The L.beta.* phase of 18:0/10:0-PC is the most stable structure for this PC below Tm. The formation and stability of the triple-chain structures can be rationalized from molecular models.