Pressure locking of the subgel phase of hydrated dipalmitoyl phosphatidylcholine bilayers: a Raman spectroscopic study

Iodothyronine-phospholipid interactions in the lipid gel phase probed by Raman spectral markers

A better understanding of the structural effects induced by thyroid hormones in model membranes is attained by Raman spectroscopy. The interactions of T3 and T4 with multilamellar vesicles of dipalmytoylphosphatidylcholine (DPPC) in the gel phase are characterized by analyzing the spectral behavior of the C-H and C-C stretching vibrations of the acyl chains. The spectra evidence an increase in the relative number of gauche conformation, which indicates the hormones are able to penetrate into the hydrophobic region of the bilayer and partially alter the lipid structure. In addition, the density packing of the acyl chains appears increased and the rotational mobility of the terminal methylene groups is slightly reduced in the iodothyronine/DPPC mixtures. These effects are interpreted in terms of the transition to an interdigitated phase due to the hormone incorporation to the membrane. The polar heads of the lipids also interact with the hormone, as evidenced by the PO2(-) symmetric stretching band.

Detecting phase transitions in phosphatidylcholine vesicles by Raman microscopy and self-modeling curve resolution

The study of phospholipid phase transitions is important for understanding drug- and protein-membrane interactions as well as other phenomena such as trans-membrane diffusion and vesicle fusion. A temperature-controlled stage on a confocal Raman microscope has allowed phase transitions in optically trapped phospholipid vesicles to be monitored. Raman spectra were acquired and analyzed using self-modeling curve resolution, a multivariate statistical analysis technique. This method revealed the subtle spectral changes indicative of sub- and pretransitions and main transitions in vesicles composed of 1,2-dipalmitoyl-sn-glycero-3-phosphocholine (DPPC). The Raman scattering results were compared to differential scanning calorimetry (DSC) experiments and found to be in good agreement. This method of observing lipid phase transition profiles requires little sample preparation and a minimal amount of lipid (<or=0.1 nmol) for an experiment. The conformational changes of the phospholipid molecules occurring during phase transitions are elucidated from the Raman spectroscopy results. The evolution of chain decoupling, rotational disorder, and gauche defects in the lipid acyl chains as a function of temperature is described.

Comparison of the effects of NaCl on the thermotropic behaviour of sn-1' and sn-3' stereoisomers of 1,2-dimyristoyl-sn-glycero-3-phosphatidylglycerol

The phase behaviour of liposomes of 1,2-dimyristoyl-sn-glycero-3-phosphatidyl-sn-1'-glycerol (1'-DMPG) and the corresponding sn-3' stereoisomer (3'-DMPG) were studied by DSC as a function of NaCl concentration. The melting of the metastable gel phase to the liquid-crystalline phase was similar for both lipids. However, in the presence of salt and at 6 degrees C (T less than Tp) the gel phase of both stereoisomers of DMPG was shown to be metastable and a new phase nominated here as the highly crystalline phase was formed as the stable state. However, significant differences in the formation and melting of the highly crystalline phase were evident between the two polar headgroup stereoisomers. For 3'-DMPG in the presence of 300 mM NaCl the melting enthalpy of this phase is approx. 82 kJ/mol and the transition temperature about 11 degrees higher (at 33.6 degrees C) than for the gel to liquid-crystalline phase transition (25 kJ/mol at 23.0 degrees C). In the presence of 0.15-1.2 M NaCl at 6 to 10 degrees C the formation of the highly crystalline phase of 3'-DMPG is complete within 2 to 5 days, increasing [NaCl] facilitates the rate. For a 1:1 mixture of 1'- and 3'-DMPG the formation of the highly crystalline phase requires several weeks and melts at about 20 degrees higher than the gel phase (at approx. 40 degrees C). For 1'-DMPG partial conversion into the highly crystalline phase requires several months. For 3'-DMPG several intermediate phases appeared as endothermic peaks between the main phase transition temperature and the melting temperature of the highly crystalline phase. In contrast, for 1'-DMPG and the 1:1 mixture the subgel phase appears to be the only metastable intermediate phase. Different monovalent cations differ in their effect on the metastable behaviour.

Scanning calorimetry reveals a new phase transition in L-alpha-dipalmitoylphosphatidylcholine

We report a new phase transition in fully hydrated dispersions of dipalmitoylphosphatidylcholine (DPPC). This new transition, called the sub-subtransition, exhibits a transition enthalpy of 0.25 kcal/mol with a Tm at 6.8 degrees C. Unlike the subtransition, no extended low temperature incubation is required to observe the sub-subtransition. This new sub-subgel (SGII) phase may be a precursor to the subgel (SGI) phase, and this discovery is discussed in relation to the current knowledge regarding the polymorphic gel phases of both ester- and ether-linked lipids with identical acyl chains.

Pressure studies on two hydrated phospholipids--1,2-dimyristoyl-phosphatidylcholine and 1,2-dipalmitoyl-phosphatidylcholine

We present results of studies on the effect of pressure on phase transitions in 1,2-dimyristoyl-phosphatidylcholine (DMPC) and 1,2-dipalmitoyl-phosphatidylcholine (DPPC) dispersed in excess water. The P-T diagram of hydrated DMPC shows a Gel III-Gel II-Gel I triple point at 3.5 kbar, 41 degrees C, the Gel III phase being obtained by annealing the sample at high pressure for several hours. In the case of DPPC, a pressure induced phase (X) appears between the Gel II and Gel I phases at approximately 0.93 kbar. With increasing pressure the temperature range of the X phase increases at the expense of that of the Gel I phase until finally at 2.87 kbar, the latter is completely suppressed. The P-T diagram of water-rich DPPC thus has 2 triple points, the Gel II-X-Gel I triple point at 0.93 kbar, 42.5 degrees C and the X-Gel I-liquid crystal triple point at 2.87 kbar, 98.5 degrees C. A pressure induced Gel III-Gel II transition is also observed in DPPC in the pressure range of 1.7-3 kbar.