Effect of hydrostatic pressure on the bilayer phase behavior of symmetric and asymmetric phospholipids with the same total chain length

The bilayer phase transitions of palmitoylstearoyl-phosphatidylcholine (PSPC), diheptadecanoyl-PC (C17PC) and stearoylpalmitoyl-PC (SPPC) which have the same total carbon numbers in the two acyl chains were observed by differential scanning calorimetry and high-pressure optical method. As the temperature increased, these bilayers exhibited four phases of the subgel (L_c), lamellar gel (L_β′), ripple gel (P_β′) and liquid crystal (L_α), in turn. The L_c phase was observed only in the first heating scan after cold storage. The temperatures of the phase transitions were almost linearly elevated by applying pressure. The temperature-pressure phase diagrams and the thermodynamic quantities associated with the phase transitions were compared among the lipid bilayers. For all the bilayers studied, the pressure-induced interdigitated gel (L_βI) phase appeared above the critical interdigitation pressure (CIP) between the L_β′ and P_β′ phases. The CIPs for the PSPC, C17PC and SPPC bilayers were found to be 50.6, 79.1 and 93.0 MPa, respectively. Contribution of two acyl chains to thermodynamic properties for the phase transitions of asymmetric PSPC and SPPC bilayers was not even. The sn-2 acyl chain lengths of asymmetric PCs governed primarily the bilayer properties. The fluorescence spectra of Prodan in lipid bilayers showed the emission maxima characteristic of bilayer phases, which were dependent on the location of Prodan in the bilayers. Second derivative of fluorescent spectrum exhibited the original emission spectrum of Prodan to be composed of the distribution of Prodan into multiple locations in the lipid bilayer. The F″₄₉₇/F″₄₃₀ value, a ratio of second derivative of fluorescence intensity at 497 nm to that at 430 nm, is decisive evidence whether bilayer interdigitation will occur. With respect to the L_β′/L_βI phase transition in the SPPC bilayer, the emission maximum of Prodan exhibited the narrow-range red-shift from 441 to 449 nm, indicating that the L_βI phase in the SPPC bilayer has a less polar “pocket” formed by a space between uneven terminal methyl ends of the sn-1 and sn-2 chains, in which the Prodan molecule remains stably.     

Effects of hydrostatic pressure on bilayer phase behavior and dynamics of dilauroylphosphatidylcholine.

Deuterium nuclear magnetic resonance spectroscopy was used to study the thermotropic phase behavior of dilauroylphosphatidylcholine (DLPC) bilayers at pressures up to 221 MPa. Pressure was found to separate the liquid crystal to gel transition from the gel to ordered crystalline phase transition. The jump in chain order observed on cooling through the transition into the gel phase was found to be small and thus consistent with the trend in longer chain saturated diacyl phosphatidylcholines. On cooling, DLPC was observed to enter an unusual state above the transition into the gel phase. This unusual state displayed fluid-like conformational order but short transverse relaxation times. It was found to be much better pronounced and to span a broader temperature range at elevated pressure than at lower pressures. Transverse relaxation measurements of deuterons on the chain alpha-carbons revealed a substantial slowing of molecular motions within the temperature range of the unusual fluid phase. The observation of such a phase at high pressure appears to be consistent with recent reports of an unusual fluid phase, Lx, in DLPC at ambient pressure.     

Dependence of the bilayer to hexagonal phase transition on amphiphile chain length

Several series of amphiphiles of increasing chain length were tested for their abilities to modify the L alpha-HII transition of dielaidoylphosphatidylethanolamine using differential scanning calorimetry. Acylcarnitines, alkyl sulfates, alkylsulfobetaines, and phosphatidylcholines, with chain lengths between about 6 and 12 carbon atoms, show an increasing capacity to raise the L alpha-HII phase transition temperature of phosphatidylethanolamine. This is ascribed to increased partitioning of the added amphiphile from water into the membrane as the chain length increases. Alkyl sulfates and alkyltrimethylammonium bromides have diminished capacities to raise the L alpha-HII transition temperature as the chain length is increased from 12 to 16. This is caused by an increase in the hydrophobic portion of the amphiphile leading to a change in the intrinsic radius of curvature and a decrease in the hydrocarbon packing constraints in the HII phase relative to the shorter chain amphiphiles. The L alpha-HII transition temperature of phosphatidylethanolamine with acylcarnitines of chain length 14-20 carbon atoms, alkylsulfobetaines above 14 carbon atoms, and phosphatidylcholines with acyl groups having above 10 carbon atoms is relatively insensitive to chain length. We suggest that this is caused by a balance between increasing hydrocarbon volume promoting the HII phase through decreased intrinsic radius of curvature and greater relief of hydrocarbon packing constraints vs greater intermolecular interactions favoring the more condensed L alpha phase. This latter effect is more important for amphiphiles with large headgroups which can pack more efficiently in the L alpha phase. The phosphatidylcholines show a gradual decrease in bilayer stabilization between 10 and 22 carbon atoms.(ABSTRACT TRUNCATED AT 250 WORDS)     

Mixing behavior of symmetric chain length and mixed chain length phosphatidylcholines in two-component multilamellar bilayers: evidence for gel and liquid-crystalline phase immiscibility

The mixing behavior of symmetric chain length and mixed chain length phosphatidylcholines in two-component multilamellar bilayers has been investigated by high-sensitivity differential scanning calorimetry. Phase diagrams have been constructed for two-component bilayers composed of C(18)C(18)PC and either C(18)C(16)PC, C(18)C(14)PC, C(18)C(12)PC, or C(18)C(10)PC. It is found that C(18)C(18)PC-C(18)C(16)PC and C(18)C(18)PC-C(18)C(14)PC mixed bilayers exhibit complete miscibility of the components in both the gel and liquid-crystalline phases. Whereas this mixing is observed to be nearly ideal for the C(18)C(18)PC-C(18)C(16)PC binary system, the intermixing of the lipids is highly nonideal in the gel phase of the C(18)C(18)PC-C(18)C(14)PC binary mixture. The C(18)C(18)PC-C(18)C(12)PC and C(18)C(18)PC-C(18)C(10)PC mixed bilayers are characterized by partial immiscibility of the phosphatidylcholine components in the bilayer gel phase. Over a large compositional range, these bilayers appear to consist of phase-separated regions of interdigitated and noninterdigitated gel phases. In addition, the C(18)C(18)PC-C(18)C(10)PC two-component bilayer displays a limited region of liquid-liquid immiscibility in the liquid-crystalline bilayer phase. The phase separation of the mixed chain length phosphatidylcholines revealed in these mixed bilayers may represent a three-dimensional phase separation of the lipid components where the phosphatidylcholines are both laterally separated within the plane of the bilayer and conformationally coupled across the bilayer. Such phase-separated domains could have profound effects on membrane structure and function if they were to occur in biological membranes.     

Thermotropic and barotropic phase transitions in bilayer membranes of ether-linked phospholipids with varying alkyl chain lengths

The bilayer phase transitions of a series of ether-linked phospholipids, 1,2-dialkylphosphatidylcholines containing linear saturated alkyl chain (C_n = 12, 14, 16 and 18), were observed by differential scanning calorimetry (DSC) under ambient pressure and light-transmittance measurements under high pressure. The thermodynamic quantities of the pre- and main-transitions for the ether-linked PC bilayer membranes were calculated and compared with those of a series of ester-linked PCs, 1,2-diacylphosphatidylcholines. The thermodynamic quantities of the main transition for the ether-linked PC bilayers showed distinct dependence on alkyl-chain length and were slightly different from those of the ester-linked PC bilayers. From the comparison of thermodynamic quantities for the main transition between both PC bilayers, we revealed that the attractive interaction in the gel phase for the ether-linked PC bilayers is weaker than that for the ester-linked PC bilayers. Regarding the pretransition, although changes in enthalpy and entropy for both PC bilayers were comparable to each other, the volume changes of the ether-linked PC bilayers roughly doubled those of the ester-linked PC bilayers. The larger volume change results from the smallest partial molar volume of the ether-linked PC molecule in the interdigitated gel phase. Further, we constructed the temperature-pressure phase diagrams for the ether-linked PC bilayers by using the phase-transition data. The region of the interdigitated gel phase in the phase diagrams was extended by applying pressure and by increasing the alkyl-chain length of the molecule. Comparing the phase diagrams with those for the ester-linked PC bilayers, it was proved that the phase behavior of the ester-linked PC bilayers under high temperature and pressure is almost equivalent to that of the ether-linked PC bilayers in the vicinity of ambient pressure.     

Thermotropic and barotropic phase transitions in bilayer membranes of ether-linked phospholipids with varying alkyl chain lengths

The bilayer phase transitions of a series of ether-linked phospholipids, 1,2-dialkylphosphatidylcholines containing linear saturated alkyl chain (C(n)=12, 14, 16 and 18), were observed by differential scanning calorimetry (DSC) under ambient pressure and light-transmittance measurements under high pressure. The thermodynamic quantities of the pre- and main-transitions for the ether-linked PC bilayer membranes were calculated and compared with those of a series of ester-linked PCs, 1,2-diacylphosphatidylcholines. The thermodynamic quantities of the main transition for the ether-linked PC bilayers showed distinct dependence on alkyl-chain length and were slightly different from those of the ester-linked PC bilayers. From the comparison of thermodynamic quantities for the main transition between both PC bilayers, we revealed that the attractive interaction in the gel phase for the ether-linked PC bilayers is weaker than that for the ester-linked PC bilayers. Regarding the pretransition, although changes in enthalpy and entropy for both PC bilayers were comparable to each other, the volume changes of the ether-linked PC bilayers roughly doubled those of the ester-linked PC bilayers. The larger volume change results from the smallest partial molar volume of the ether-linked PC molecule in the interdigitated gel phase. Further, we constructed the temperature-pressure phase diagrams for the ether-linked PC bilayers by using the phase-transition data. The region of the interdigitated gel phase in the phase diagrams was extended by applying pressure and by increasing the alkyl-chain length of the molecule. Comparing the phase diagrams with those for the ester-linked PC bilayers, it was proved that the phase behavior of the ester-linked PC bilayers under high temperature and pressure is almost equivalent to that of the ether-linked PC bilayers in the vicinity of ambient pressure.     

Effect of headgroup type on the miscibility of homologous phospholipids with different acyl chain lengths in hydrated bilayer

The miscibility of homologous phosphatidylcholines with different acyl chain lengths in hydrated bilayer was examined through the binary phase diagram constructed by differential scanning calorimetry. By analyzing the phase diagram according to a thermodynamic model based on the Bragg-Williams approximation to evaluate the excess free energy of mixing, the non-ideality parameter of mixing, rho(0), was estimated, which allows one to interpret the mixing behavior of the two lipid components in terms of the difference in the pair-interaction energies between like-pairs and mixed-pairs formed in the mixture. By summarizing the rho(0) values obtained previously for other classes of phospholipids, it was found that rho(0) increases in the order of phosphatidylglycerol (PG) approximately phosphatidylcholine (PC) < phosphatidylethanolamine (PE) < phosphatidic acid (PA). Since the difference in the pair-interaction energies is considered to be determined by the relative contribution of inter-headgroup interaction to the overall intermolecular interaction, this sequence of rho(0) value suggests that the headgroup interaction in hydrated bilayer increases in the order of PA < PE < PC approximately PG.     

The influence of dioxan on the bilayer and monolayer phase transition of phospholipids

The influence of 1.4.-dioxan on the bilayer phase transition of various phospholipids was studied by differential scanning calorimetry and turbidity measurements. The addition of 1.4.-dioxan to lipid bilayers decreases the transition temperature T_m increases the transition enthalpy of the transition. The cooperativity of the transition is unaffected. The phospholipid monolayer transition from the liquid-condensed to the liquid-expanded phase was measured by recording area versus temperature curves at constant surface pressure (isobars). The monolayer transition temperature at constant surface pressure is increased when 1.4.-dioxan is added to the subphase. The change in molecular area becomes larger. A comparison of monolayer isobars on water and water/dioxan as subphase at constant surface tension rather than surface pressure leads to a decrease of the transition temperature on water/dioxan as subphase. This decrease as well as the larger change in molecular area at the monolayer transition can be correlated to the decrease in T_m and the increase in the transition enthalpy of the corresponding bilayer system. 1.4.-Dioxan seems to accumulate at the lipid head group/water interface, thus lowering the tension of the bilayer membrane. This cyclic ether can be used for altering the characteristics of bilayer membranes without disturbing the lipid chain organization.     

Effect of ceramide acyl chain length on skin permeability and thermotropic phase behavior of model stratum corneum lipid membranes

Stratum corneum ceramides play an essential role in the barrier properties of skin. However, their structure-activity relationships are poorly understood. We investigated the effects of acyl chain length in the non-hydroxy acyl sphingosine type (NS) ceramides on the skin permeability and their thermotropic phase behavior. Neither the long- to medium-chain ceramides (8-24 C) nor free sphingosine produced any changes of the skin barrier function. In contrast, the short-chain ceramides decreased skin electrical impedance and increased skin permeability for two marker drugs, theophylline and indomethacin, with maxima in the 4-6C acyl ceramides. The thermotropic phase behavior of pure ceramides and model stratum corneum lipid membranes composed of ceramide/lignoceric acid/cholesterol/cholesterol sulfate was studied by differential scanning calorimetry and infrared spectroscopy. Differences in thermotropic phase behavior of these lipids were found: those ceramides that had the greatest impact on the skin barrier properties displayed the lowest phase transitions and formed the least dense model stratum corneum lipid membranes at 32°C. In conclusion, the long hydrophobic chains in the NS-type ceramides are essential for maintaining the skin barrier function. However, this ability is not shared by their short-chain counterparts despite their having the same polar head structure and hydrogen bonding ability.     

Effect of a hydrostatic pleural pressure gradient on mechanical behavior of lung lobes

Using 133Xe, the vertical distribution of regional volume (Vr) was measured in three regions of excised canine lobes both in air and when completely submerged in saline at 40, 60, 70, and 80% lobar vital capacity (VC). The estimated pleural pressure gradient, derived from values of Vr, distance between regions, and the lobar pressure-volume (PV) curve, underestimated the true gradient by 45%. Conversely, the gradient of Vr was substantially less than predicted. From the mean depth of each region below the waterline, pleural, and hence transpulmonary, pressure (PL) was computed. The values of Vr-PL for each region at 40, 60, and 80% lung volume (VL) were related to the lobar PV curve. Slopes of lines joining initial VL-PL points on the lobar PV curve to corresponding Vr-PL points in submerged lobes represent an effective regional compliance of a lobe undergoing deformation. With one exception this was less than the corresponding homogeneous compliance, indicating a stiffening of the lobe during deformation. Slopes of lines joining Vr-PL points of each region at the three lobar volumes represent effective regional compliance of a deformed lobe undergoing volume change. This was not significantly different from the homogeneous compliance. However, effective compliance can only be an approximate indicator of the forces required for a given volume change due to the inadequacy of PL to represent the unequal stress components induced by lobe deformation.     

Effect of chain length on coiled-coil stability: decreasing stability with increasing chain length

The de novo design and biophysical characterization of three series of two-stranded alpha-helical coiled coils with different chain lengths are described. Our goal was to examine how increasing chain length would affect protein folding and stability when one or more heptad repeat(s) of K-A-E-A-L-E-G (gabcdef) was inserted into the central region of different coiled-coil host proteins. This heptad was designed to maintain the continuous 3-4 hydrophobic repeat of the coiled-coil host and introduce an Ala and Leu residue in the hydrophobic core at the a and d position, respectively, and a pair of stabilizing interchain ionic i to i' + 5 (g to e') interactions per heptad inserted. The secondary structures of the three series of disulfide-bridged polypeptides were studied by CD spectroscopy and their stabilities determined by chemical and thermal denaturation. The results showed that successive insertions of this heptad systematically decreased the stability of all the coiled coils studied regardless of the overall initial stability of the host coiled coil. These observations are in contrast to the generally accepted implication that the folding and stability of coiled coils are enhanced with increasing chain length. Our results imply that, in these examples where an Ala and Leu hydrophobic residue were introduced into the coiled-coil core per inserted heptad, there was still insufficient stability to overcome unfavorable entropy associated with chain length extension, even though the inserted heptad contained the most stabilizing hydrophobic residue (Leu) at position d and stabilizing ionic attractions.     

Effect of acyl chain structure and bilayer phase state on binding and penetration of a supported lipid bilayer by HPA3

The effect of acyl chain structure and bilayer phase state on binding and penetration by the peptide HPA3 was studied using dual polarisation interferometry. This peptide is an analogue of Hp(2-20) derived from the N-terminus of Helicobacter pylori ribosomal protein L1 (RpL1) which has been shown to have antimicrobial and cell-penetrating properties. The binding of HPA3 to zwitterionic 1,2-dimyristoyl-sn-glycero-3-phosphocholine (DMPC) or 1-palmitolyl-2-oleyl-sn-glycero-3-phosphocholine (POPC) and negatively charged membranes composed of DMPC and 1,2-dimyristoyl-sn-glycero-3-(phosphor-rac-(1-glycerol)) (DMPG) or POPC and 1-palmitolyl-2-oleyl-sn-glycero-3-(phosphor-rac-(1-glycerol)) (POPG) was determined using dual polarisation interferometry (DPI). Mass and birefringence were measured in real time, enabling the creation of birefringence–mass plots for detailed analysis of the changes in lipid bilayer order during the peptide-binding process. HPA3 bound to all four lipids and the binding progressed as a single phase for the saturated gel phase bilayers DMPC and DMPC–DMPG. However, the binding process involved two or more phases, with penetration of the unsaturated fluid phase POPC and POPC–POPG bilayers. Structural changes in the saturated bilayer were partially reversible whereas binding to the unsaturated bilayer resulted in irreversible changes in membrane structure. These results demonstrate that more disordered unsaturated bilayers are more susceptible to further disorganisation and have a lower capacity to recover from peptide-induced structural changes than saturated ordered bilayers. In addition, this study further establishes DPI as powerful tool for analysis of multiphase peptide-insertion processes associated with complex structural changes in the liquid-crystalline membrane.     

High-pressure study on bilayer phase behavior of oleoylmyristoyl- and myristoyloleoyl-phosphatidylcholines

We investigated the thermotropic and barotropic bilayer phase behavior of 1-myristoyl-2-oleoyl-sn-glycero-3-phosphocholine (MOPC) and 1-oleoyl-2-myristoyl-sn-glycero-3-phosphocholine (OMPC) by means of the differential scanning calorimetry (DSC) and high-pressure light-transmittance technique. Water could be used as a solvent for measurements at high pressures because of the elevation of the transition temperatures above 0 degrees C by pressurization, whereas aqueous 50 wt.% ethylene glycol solution was used mainly for those at low pressures. Only one phase transition was observed in the DSC thermogram of the MOPC bilayer membrane as an endothermic peak, and also observed at high pressures as an abrupt change of the light-transmittance. The transition was assigned as a main transition between the lamellar gel (L(beta)) and liquid-crystalline (L(alpha)) phases on the basis of the values of enthalpy change (DeltaH) and slope of the transition temperature with respect to pressure (dT/dP). The DSC thermogram of the OMPC bilayer membrane similarly showed a single endothermic peak but two kinds of phase transitions were observed at different temperatures in the light-transmittance profile at high pressures. The extrapolation of the lower-temperature transition in the high-pressure range to an ambient pressure coincided with the transition observed in the DSC thermogram. This transition was identified as a transition between the lamellar crystal (L(c)) and L(alpha) (or L(beta)) phases from the DeltaH and dT/dP values. The higher-temperature transition, appearing only at high pressures, was identified as the L(beta)/L(alpha) transition considering the topological resemblance of its temperature-pressure phase diagram as that of the dioleoylphosphatidylcholine bilayer membrane. The phase diagram of the OMPC bilayer membrane demonstrated that the L(beta) phase cannot exist at pressures below ca. 190 MPa while it can exist stably in a finite temperature range at pressures above the pressure.     

Effect of hydrostatic pressure on translational fidelity

We have used the application of hydrostatic pressure to modify the misreading of polyuridylate template. Pressure was used to test ribosomes isolated from Escherichia coli strains containing mutations in the S12 ribosomal protein which lead to streptomycin-resistance and -dependence. The incorporation of phenylalanine into polypeptide, at a given pressure, was found to vary with the source of ribosomes and was found to correlate with S12-dependent changes in rates of incorporation suggesting a role of the S12 ribosomal protein in the pressure effect. Streptomycin partially alleviated the increased pressure-resistance in those cases where control rates of incorporation were found to be stimulated by the addition of streptomycin. In contrast, the misincorporation of isoleucine was substantially more sensitive to pressure application, regardless of ribosome source or the presence of streptomycin. These results suggest that the application of hydrostatic pressure affects at least two distinct ribosomal reactions important to the discrimination of these two amino acids.     

Effect of hydrostatic pressure on starch gelatinisation

Samples of wheat and potato starches, mixed with water to four concentrations were subjected to preselected hydrostatic pressures (in the range 200–1500 MPa) and temperatures. Subsequent examination in a polarising microscope revealed that the effect of high hydrostatic pressure was to lower the gelatinisation temperature. With the exception of the low water content samples, the samples did not appear to be greatly affected in any other way by hydrostatic pressure (as evidenced by staining behaviour, appearance in the polarising microscope and subsequent gelatinisation behaviour at ambient pressure). Reduction in gelatinisation temperature was a non-linear function of pressure, being greatest at high pressure. The effect was also more pronounced at the higher water contents. The significance of these results with respect to thermodynamic models of starch gelatinisation is discussed.     

Effect of hydrostatic pressure on nucleic acids

In comparison to other biomolecules, the effect of hydrostatic pressure on the conformational stability of DNA and RNA has received scant attention. However, the increasing interest in the hydration of biological molecules has resulted in a concomitant increase in the number of investigations of the effect of pressure upon the structure of nucleic acids. In this review, studies concerning the effect of pressure on DNA and RNA oligomers and polymers are presented. The greatest amount of research has been directed at studying the effect of pressure on the stability of the double helix. In general, under most conditions, the helical form of DNA or RNA is stabilized by pressure. The extent of stabilization is small relative to the effect of pressure on other biomolecular systems such as lipid membranes or protein quaternary structure. The absence of a larger pressure effect arises, in part because the state of ionization does not change as a function of the helical state. Initial experiments have also appeared on the effect of pressure upon helix-formation kinetics, B-Z and A-Z equilibria, and DNA topology. Fourier-transform ir spectroscopy of DNA polymers under high pressure has yielded data that showing that pressure does not induce large-scale structural changes.     

Effect of fatty acid chain length,fatty acid hydroxylation,and various cations on phase behavior of synthetic cerebroside sulfate

Synthetic species of CBS containing palmitic, stearic, lignoceric, D-2-hydroxy palmitic, or D-2-hydroxy stearic acid were prepared and their phase behavior in the presence of a number of mono- and divalent cations was studied by differential scanning calorimetry and the use of fatty acid spin labels. The results showed that both the non-hydroxy fatty acid (NFA) and hydroxy fatty acid (HFA) forms of cerebroside sulfate (CBS) can occur in two different gel states, a metastable state and a lower entropy stable state. The phase behavior is more sensitive to the type and concentration of cation present than in the case with acidic phospholipids. The sensitivity of the transition temperature (T_m) to cation concentration reflects, in part, increased participation of the lipid in intermolecular hydrogen bonding interactions as the negative charge of the sulfate is shielded. The extra hydroxyl group on the HFA also contributes to the intermolecular hydrogen bonding network causing a significant increase in the T_m.The HFA has an even more significant effect in causing inhibition of formation of the stable state. Formation of the stable state is also inhibited by Li⁺ and divalent cations. A similar mechanism may be involved, i.e.; cross-linking of adjacent lipids or increased intermolecular interactions inhibit the molecular rearrangement necessary to form the stable state. This inhibition is counteracted by an increase in fatty acid chain length. The results suggest that the stable state may be interdigitated as a result of the unequal chain length between the sphingosine base and the fatty acid.     

Transbilayer diffusion of phospholipids: dependence on headgroup structure and acyl chain length

The kinetics and thermodynamics of the transmembrane movement (flip-flop) of fluorescent analogs of phosphatidic acid (PA), phosphatidylglycerol (PG), phosphatidylcholine (PC), and phosphatidylethanolamine (PE) were investigated to determine the contributions of headgroup composition and acyl chain length to phospholipid flip-flop. The phospholipid derivatives containing n-octanoic, n-decanoic or n-dodecanoic acid in the sn-1 position and 9-(1-pyrenyl)nonanoic acid in the sn-2 position were incorporated at 3 mol% into sonicated single-bilayer vesicles of 1-palmitoyl-2-oleoyl-sn-glycerol-3-phosphocholine (POPC). The kinetics of diffusion of the pyrene-labeled phospholipids from the outer and inner monolayers of the host vesicles to a large pool of POPC acceptor vesicles were monitored by the time-dependent decrease of pyrene excimer fluorescence. The observed kinetics of transfer were biexponential, with a fast component due to the spontaneous transfer of pyrenyl phospholipids in the outer monolayer of labeled vesicles and a slower component due to diffusion of pyrenyl phospholipid from the inner monolayer of the same vesicles. Intervesicular transfer rates decreased approx. 8-fold for every two carbons added to the first acyl chain. Correspondingly, the free energy of activation for transfer increased approx. 1.3 kcal/mol. With the exception of PE, the intervesicular transfer rates for the different headgroups within a homologous series were nearly the same, with the PC derivative being the fastest. Transfer rates for the PE derivatives were 5-to 7-fold slower than the rates observed for PC. Phospholipid flip-flop, in contrast, was strongly dependent on headgroup composition with a smaller dependence on acyl chain length. At pH 7.4, flip-flop rates increased in the order PC less than PG less than PA less than PE, where the rates for PE were at least 10-times greater than those of the homologous PC derivative. Activation energies for flip-flop were large, and ranged from 38 kcal/mol for the longest acyl chain derivative of PC to 25 kcal/mol for the PE derivatives. Titration of the PA headgroup at pH 4.0 produced an approx. 500-fold increase in the flip-flop rate of PA, while the activation energy decreased 10 kcal/mol. Increasing acyl chain length reduced phospholipid flip-flop rates, with the greatest change observed for the PC analogs, which exhibited an approx. 2-fold decrease in flip-flop rate for every two methylene carbons added to the acyl chain at the sn-1 position.(ABSTRACT TRUNCATED AT 400 WORDS)