New approach to study fast and slow motions in lipid bilayers: application to dimyristoylphosphatidylcholine-cholesterol interactions.

Natural abundance 13C solid-state nuclear magnetic resonance spectroscopy was used to investigate the effect of the incorporation of cholesterol on the dynamics of dimyristoylphosphatidylcholine (DMPC) bilayers in the liquid-crystalline phase. In particular, the use of a combination of the cross-polarization and magic angle spinning techniques allows one to obtain very high resolution spectra from which can be distinguished several resonances attributed to the polar head group, the glycerol backbone, and the acyl chains of the lipid molecule. To examine both the fast and slow motions of the lipid bilayers, 1H spin-lattice relaxation times as well as proton and carbon spin-lattice relaxation times in the rotating frame were measured for each resolved resonance of DMPC. The use of the newly developed ramped-amplitude cross-polarization technique results in a significant increase in the stability of the cross-polarization conditions, especially for molecular groups undergoing rapid motions. The combination of T1 and T1 rho measurements indicates that the presence of cholesterol significantly decreases the rate and/or amplitude of both the high and low frequency motions in the DMPC bilayers. This effect is particularly important for the lipid acyl chains and the glycerol backbone region.     

Low-frequency motion in membranes. The effect of cholesterol and proteins

Nuclear magnetic resonance (NMR) relaxation techniques have been used to study the effect of lipid-protein interactions on the dynamics of membrane lipids. Proton enhanced (PE) 13C-NMR measurements are reported for the methylene chain resonances in red blood cell membranes and their lipid extracts. For comparison similar measurements have been made of phospholipid dispersions containing cholesterol and the polypeptide gramicidin A+. It is found that the spin-lattice relaxation time in the rotating reference frame (T1 rho) is far more sensitive to protein, gramicidin A+ or cholesterol content than is the laboratory frame relaxation time (T1). Based on this data it is concluded that the addition of the second component to a lipid bilayer produces a low-frequency motion in the region of 10(5) to 10(7) Hz within the membrane lipid. The T1 rho for the superimposed resonance peaks derived from all parts of the phospholipid chain are all influenced in the same manner suggesting that the low frequency motion involves collective movements of large segments of the hydrocarbon chain. Because of the molecular co-operativity implied in this type of motion and the greater sensitivity of T1 rho to the effects of lipid-protein interactions generally, it is proposed that these low-frequency perturbations are felt at a greater distance from the protein than those at higher frequencies which dominate T1.     

2H NMR investigation of the organization and dynamics of polyisoprenols in membranes

The polyisoprenols (PIs) dolichol and undecaprenol function as chemical carriers of glycosyl residues in the membrane-directed synthesis of glycoconjugates in prokaryotic and eukaryotic cells. The molecular details of how these lipid cofactors function is unknown. Presented here are results of deuterium NMR investigations of site specifically 2H-labeled PIs incorporated into model membranes. To complement previous omega-terminal PI labeling schemes, a simple synthesis of head group 2H-labeled PIs is presented in which a PI alcohol is esterified with deuterated acetyl chloride. The 2H-labeled PIs, when incorporated into multilamellar membranes composed of phosphatidylcholine, gave rise to 2H NMR powder patterns interpretable in terms of quadrupole splittings (delta vQ) and spin-lattice relaxation times (T1s). Pure isomers of head group 2H-labeled geraniol (C10) and solanesol (C45) gave rise to single splittings while farnesol (C15) gave rise to two sets of splittings due to cis-trans isomerization at the polar terminal double bond. Membranes containing C45 solanesol exhibited a large isotropic component, indicative of limited partitioning of this poly trans PI into the membrane. T1 measurements revealed high rates of motion for PIs relative to cholesterol in similar membrane hosts and revealed correlation times close to the fatty acyl methyl termini in phosphatidylcholine. The smaller PIs showed higher rates of motion but the T1s of head and tail labels were similar. These data indicate that both ends of the esterified PI molecules see similar environments, probably in the bilayer interior, and suggest that the esterified PIs studied here do not appear to adopt a conventional head group-at-interface orientation of lipids within the bilayer.     

Dielectric relaxation in lecithin/cholesterol/water-mixtures

The dielectric spectrum of aqueous solutions of dimyristoyl-l-3-phosphatidylcholine and dipalmitoyl-l-3-phosphatidylcholine with admixed cholesterol has been determined by means of a pulse reflection method which was used to measure the complex permittivity of the solutions as a function of frequency between 100 kHz and 50 MHz. Measurements have been performed at various concentrations of cholesterol in dependence of temperature around the crystal-line/liquid-crystalline phase transition temperature of the solutions.The measured dielectric spectra are treated in terms of a Debye-function. The dielectric relaxation strength and the relaxation time decrease distinctly with increasing cholesterol concentration. In addition, the data are treated on the basis of a theoretical solution model in order to allow for conclusions concerning the lecithin head group motion in the lipid bilayer surface. One important result is that increasing cholesterol concentration affects the interaction of the lecithin head groups and increases their mobility. These effects already occur at small concentrations of cholesterol.     

Dynamics of the phosphate group in phospholipid bilayers. A 31P angular dependent nuclear spin relaxation time study.

To understand 31P relaxation processes and hence molecular dynamics in the phospholipid multilayer it is important to measure the dependence of the 31P spin-lattice relaxation time on as many variables as the physical system allows. Such measurements of the 31P spin-lattice relaxation rate have been reported both as a function of Larmor frequency and temperature for egg phosphatidylcholine liposomes (Milburn, M.P., and K.R. Jeffrey. 1987. Biophys. J. 52:791-799). In principle, the spin-lattice relaxation rate in an anisotropic environment such as a bilayer will be a function of the angle between the bilayer normal and the magnetic field. However, the measurement of this angular dependence has not been possible because the rapid (on the time-scale of the spin-lattice relaxation rate) diffusion of the lipid molecules over the curved surface of the liposome average this dependence (Milburn, M.P., and K.R. Jeffrey. 1987. Biophys. J. 52:791-799; Brown, M.F., and J.H. Davis. 1981. Chem. Phys. Lett. 79:431-435). This paper reports the results of the measurement of the 31P spin-lattice relaxation rate as a function of this angle, beta', (the angle between the bilayer normal and the external magnetic field) using samples oriented between glass plates. These measurements were made at high field (145.7 MHz) where the spin-lattice relaxation processes are dominated by the chemical shielding interaction (Milburn, M.P., and K.R. Jeffrey. 1987. Biophys. J. 52:791-799). A model of molecular motion that includes a fast axially symmetric rotation of the phosphate group (tau i approximately 10(-9) s) and a wobble of the head group tilt with respect to this rotation axis has been used to describe both the angular dependence of the spin-lattice relaxation and the spectral anisotropy.(ABSTRACT TRUNCATED AT 250 WORDS)     

NMR-relaxation in hydrated collagen from the spotted dogfish]

Collagen samples from dog-fish egg case at different water content were studied by the 1H NMR relaxation method. The dependences of the proton spin-lattice and spin-spin relaxation rates on the concentration of water in hydrated native collagen were measured. The fractions of water protons of different mobility and their corresponding spin-spin and spin-lattice relaxation rates were determined in a multi-phase model of water protons in natural biopolymer-water systems. The correlation times were calculated as the characteristics of molecular motion in hydrated collagens with different content of absorbed water. The results obtained were compared with literature data of pulse NMR studies of molecular mobility in other collagen fibers.     

Proton magnetic relaxation studies of mixed phosphatidylcholine/fatty acid and mixed phosphatidylcholine bimolecular bilayers.

High resolution proton spin-lattice relaxation times (T1), spin-spin relaxation times (T2) and resonance linewidths were measured above the gel-to-liquid crystal transition temperature (Tm), in phosphatidylcholine bilayers possessing various degrees of intramolecular motional anisotrophy at the level of various alkyl chain proton groups. The experiments were designed to test the hypothesis that coupled trans-gauche isomerizations along the chains can be responsible for the anisotropic motion of phosphatidylcholine proton groups in bilayer membranes (Horwitz, A.F., Horsley, W.J. and Klein, M.O. (1972) Proc. Natl. Acad. Sci. U.S. 69,500). Systematic series of structural perturbations of the bilayer were achieved in mixed phosphatidylcholine/fatty acid and in mixed phosphatidylcholine bilayers where the degree of motional anisotrophy of the chains' proton groups was gradually reduced by progressively increasing the chain length disparity of the two components. The systematic T1 and T2 variations observed were interterpreted on the basis of the Woessner's treatment for computing the relaxation times of a spin pair reorienting randomly about an axis which, in turn, tumbles randomly (Woessner, D.E. (1962) J. Chem. Phys. 36, 1). The results confirmed in a qualitative sense the original hypothesis made by Horwitz et al. The time-averaged structural interpretations suggested by the mangetic relaxation studies are in agreement with low-angle X-ray diffraction results obtained below Tm. In addition, the T1 values evaluated at various temperatures in dipalmitoyl phosphatidylcholine vesicles incorporated with either 2H-labeled or unlabeled palmitic acid chains indicated that the average intermolecular contribution to the spin-lattice relaxation rate of the proton groups of the phosphatidylcholine chains appears comparable to the intramolecular term at temperatures moderately higher than Tm, but becomes less and less important as the temperature is further increased above the thermal transition.     

Electron and proton magnetic resonance studies of the effect of rhodopsin incorporation on molecular motion in dimyristoylphosphatidylcholine bilayers

The effect of rhodopsin incorporation on molecular motion in L-α-dimyristoylphosphatidylcholine (DMPC) bilayers is analyzed with nitroxide ESR and proton NMR techniques. A partial, binary phase diagram for DMPC-rhodopsin is constructed by studying the partitioning of 2,2,6,6-tetramethylpiperidine-1-oxyl (Tempo) between polar and hydrophobic domains as a function of temperature and system composition. Proton NMR spin-lattice relaxation measurements show that rhodopsin is associated with a domain of approx. 50 DMPC molecules which have reduced choline methyl mobilities. ESR studies, utilizing nitroxide-labeled fatty acid probes, indicate that rhodopsin immobilizes the outer half of the hydrophobic region in rhodopsin containing DMPC bilayers. Additional ESR studies, involving a nitroxide label placed in the middle of the membrane, as well as proton chain methyl spin-lattice relaxation measurements, indicate only slight rhodopsin-induced immobilization in the central part of the membrane.     

Constant-pressure molecular dynamics investigation of cholesterol effects in a dipalmitoylphosphatidylcholine bilayer.

We report a 1.4-ns constant-pressure molecular dynamics simulation of cholesterol at 12.5 mol% in a dipalmitoylphosphatidylcholine (DPPC) bilayer at 50 degrees C and compare the results to our previous simulation of a pure DPPC bilayer. The interlamellar spacing was increased by 2.5 A in the cholesterol-containing bilayer, consistent with x-ray diffraction results, whereas the bilayer thickness was increased by only 1 A. The bilayer/water interface was more abrupt because the lipid headgroups lie flatter to fill spaces left by the cholesterol molecules. This leads to less compensation by the lipid headgroups of the oriented water contribution to the membrane dipole potential and could explain the experimentally observed increase in the magnitude of the dipole potential by cholesterol. Our calculations suggested that 12.5 mol% cholesterol does not significantly affect the conformations and packing of the hydrocarbon chains and produces only a slight reduction in the empty free volume. However, cholesterol has a significant influence on the subnanosecond time scale lipid dynamics: the diffusion constant for the center-of-mass "rattling" motion was reduced by a factor of 3, and the reorientational motion of the methylene groups was slowed along the entire length of the hydrocarbon chains.     

Molecular simulation of rapid translocation of cholesterol, diacylglycerol, and ceramide in model raft and nonraft membranes

The translocation of lipids across membranes (flip-flop) is an important biological process. Slow exchange on a physiological timescale allows the creation of asymmetric distributions of lipids across cellular membranes. The location of lipids and their rate of exchange have important biological consequences, especially for lipids involved in cellular signaling. We investigated the translocation of cholesterol, ceramide, and diacylglycerol in two model bilayers using molecular dynamics simulations. We estimate half times for flip-flop for cholesterol, diacylglycerol, and ceramide of 20 μs, 30 μs, and 10 ms in a POPC bilayer, compared with approximately 30 min, 30 ms, and 30 s in a model raft bilayer (1:1:1 PSM, POPC, and cholesterol). Cholesterol has a large (54 kJ/mol) free energy of exchange between the POPC and raft bilayer, and therefore, it strongly prefers the more ordered and rigid raft bilayer over the more liquid POPC bilayer. Ceramide and diacylglycerol have relatively small free energies of exchange, suggesting nearly equal preference for both bilayers. This unexpected result may have implications for ceramide and diacylglycerol signaling and membrane localization.     

Anisotropic 2H-nuclear magnetic resonance spin-lattice relaxation in cerebroside- and phospholipid-cholesterol bilayer membranes.

The axially symmetric powder pattern 2H-nuclear magnetic resonance (NMR) lineshapes observed in the liquid crystalline phase of pure lipid or lipid/cholesterol bilayers are essentially invariant to temperature, or, equivalently, to variations in the correlation times characterizing C-2H bond reorientations. In either of these melted phases, where correlation times for C-2H bond motions are shorter than 10(-7) s, information on the molecular dynamics of the saturated hydrocarbon chain would be difficult to obtain using lineshape analyses alone, and one must resort to other methods, such as the measurement of 2H spin-lattice relaxation rates, in order to obtain dynamic information. In pure lipid bilayers, the full power of the spin-lattice relaxation technique has yet to be realized, since an important piece of information, namely the orientation dependence of the 2H spin-lattice relaxation rates is usually lost due to orientational averaging of T1 by rapid lateral diffusion. Under more favorable circumstances, such as those encountered in the lipid/cholesterol mixtures of this study, the effects of orientational averaging by lateral diffusion are nullified, due to either a marked reduction (by at least an order of magnitude) in the diffusion rate, or a marked increase in the radii of curvature of the liposomes. In either case, the angular dependence of 2H spin-lattice relaxation is accessible to experimental study, and can be used to test models of molecular dynamics in these systems. Simulations of the partially recovered lineshapes indicate that the observed T1 anisotropies are consistent with large amplitude molecular reorientation of the C-2H bond among a finite number of sites.(ABSTRACT TRUNCATED AT 250 WORDS)     

Disparate molecular dynamics of plasmenylcholine and phosphatidylcholine bilayers

The molecular dynamics of binary dispersions of plasmenylcholine/cholesterol and phosphatidylcholine/cholesterol were quantified by electron spin resonance (ESR) and deuterium magnetic resonance (2H NMR) spectroscopy. The order parameter of both 5-doxylstearate (5DS) and 16-doxylstearate (16DS) was larger in vesicles comprised of plasmenylcholine in comparison to phosphatidylcholine at all temperatures studied (e.g., S = 0.592 vs. 0.487 for 5DS and 0.107 vs. 0.099 for 16DS, respectively, at 38 degrees C). Similarly, the order parameter of plasmenylcholine vesicles was larger than that of phosphatidylcholine vesicles utilizing either spin-labeled phosphatidylcholine or spin-labeled plasmenylcholine as probes of molecular motion. The ratio of the low-field to the midfield peak height in ESR spectra of 16-doxylstearate containing moieties (i.e., spin-labeled plasmenylcholine and phosphatidylcholine) was lower in plasmenylcholine vesicles (0.93 +/- 0.01) in comparison to phosphatidylcholine vesicles (1.03 +/- 0.01). 2H NMR spectroscopy demonstrated that the order parameter of plasmenylcholine was greater than that of phosphatidylcholine for one of the two diastereotopic deuterons located at the C-2 carbon of the sn-2 fatty acyl chain. The spin-lattice relaxation times for deuterated plasmenylcholine and phosphatidylcholine in binary mixtures containing 0-50 mol % cholesterol varied nonmonotonically as a function of cholesterol concentration and were different for each phospholipid subclass. Taken together, the results indicate that the vinyl ether linkage in the proximal portion of the sn-1 aliphatic chain of plasmenylcholine has substantial effects on the molecular dynamics of membrane bilayers both locally and at sites spatially distant from the covalent alteration.     

Molecular motion and order in oriented lipid multibilayer membranes evaluated by simulations of spin label ESR spectra. Effects of temperature, cholesterol and magnetic field.

A simulation method to interpret electron spin resonance (ESR) of spin labelled amphiphilic molecules in oriented phosphatidylcholine multibilayers in terms of a restricted motional model is presented. Order and motion of the cholestane spin label (3-spiro-doxyl-5alpha-cholestane) incorporated into egg yolk phosphatidylcholine, dipalmitoylphosphatidylcholine and dimyristoylphosphatidylcholine, pure and in mixture with cholesterol, were studied at various temperatures. With egg yolk phosphatidylcholine identical sets of motional parameters were obtained from simulations of ESR spectra obtained at three microwave frequencies (X-, K- and Q-band). With dipalmitoylphosphatidylcholine and dimyristoylphosphatidylcholine analyses of the spectra show that phase transitions occur in samples containing up to 30 mol % cholesterol. The activation energy for the motion of the spin label is about three times larger above than below the phase transition, indicating a more collective motion in the lipid crystalline state than in the gel state. In the liquid crystalline state the activation energy is larger in the pure phosphatidylcholines than with cholesterol added. Additions of cholesterol to egg phosphatidylcholine induces a higher molecular order but does not appreciably affect correlation times. This is in contrast to dipalmitoylphosphatidylcholine where both order and correlation times are affected by the presence of cholesterol. The activation energies follow the same order as the transition temperatures: dipalmitoylphosphatidylcholine greater than dimyristoylphosphatidylcholine greater than egg yokd phosphatidylcholine, suggesting a similar order of the cooperativity of the motion of the lipid molecules. Magnetic field-induced effects on egg phosphatidylcholine multibilayers were found at Q-band measurements above 40 degrees C. The cholestane spin label mimics order and motion of cholesterol molecule incorporated into the lipid bilayers. This reflects order and motion of the portions of the lipid molecules on the same depth of the bilayer as the rigid steroid portions of the intercalated molecules.     

Structure and dynamics of sphingomyelin bilayer: insight gained through systematic comparison to phosphatidylcholine

Sphingomyelin, one of the main lipid components of biological membranes, is actively involved in various cellular processes such as protein trafficking and signal transduction. In particular, specific lateral domains enriched in sphingomyelin and cholesterol have been proposed to play an important functional role in biomembranes, although their precise characteristics have remained unclear. A thorough understanding of the functional role of membranes requires detailed knowledge of their individual lipid components. Here, we employ molecular dynamics simulations to conduct a systematic comparison of a palmitoylsphingomyelin (PSM, 16:0-SM) bilayer with a membrane that comprises dipalmitoylphosphatidylcholine (DPPC) above the main phase transition temperature. We clarify atomic-scale properties that are specific to sphingomyelin due to its sphingosine moiety, and further discuss their implications for SM-rich membranes. We find that PSM bilayers, and in particular the dynamics of PSM systems, are distinctly different from those of a DPPC bilayer. When compared with DPPC, the strong hydrogen bonding properties characteristic to PSM are observed to lead to considerable structural changes in the polar headgroup and interface regions. The strong ordering of PSM acyl chains and specific ordering effects in the vicinity of a PSM-water interface reflect this issue clearly. The sphingosine moiety and related hydrogen bonding further play a crucial role in the dynamics of PSM bilayers, as most dynamic properties, such as lateral and rotational diffusion, are strongly suppressed. This is most evident in the rotational motion characterized by spin-lattice relaxation times and the decay of hydrogen bond autocorrelation functions that are expected to be important in complexation of SM with other lipids in many-component bilayers. A thorough understanding of SM bilayers would greatly benefit from nuclear magnetic resonance experiments for acyl chain ordering and dynamics, allowing full comparison of these simulations to experiments.     

Specific binding of ethanol to cholesterol in organic solvents

Although ethanol has been reported to affect cholesterol homeostasis in biological membranes, the molecular mechanism of action is unknown. Here, nuclear magnetic resonance (NMR) spectroscopic techniques have been used to investigate possible direct interactions between ethanol and cholesterol in various low dielectric solvents (acetone, methanol, isopropanol, DMF, DMSO, chloroform, and CCl(4)). Measurement of (13)C chemical shifts, spin-lattice and multiplet relaxation times, as well as self-diffusion coefficients, indicates that ethanol interacts weakly, yet specifically, with the HC-OH moiety and the two flanking methylenes in the cyclohexanol ring of cholesterol. This interaction is most strong in the least polar-solvent carbon tetrachloride where the ethanol-cholesterol equilibrium dissociation constant is estimated to be 2 x 10(-3) M. (13)C-NMR spin-lattice relaxation studies allow insight into the geometry of this complex, which is best modeled with the methyl group of ethanol sandwiched between the two methylenes in the cyclohexanol ring and the hydroxyl group of ethanol hydrogen bonded to the hydroxyl group of cholesterol.     

Role of cholesterol flip-flop in oxidized lipid bilayers

We performed a series of molecular dynamics simulations of cholesterol (Chol) in nonoxidized 1-palmitoyl-2-linoleoyl-sn-glycero-3-phosphatidylcholine (PLPC) bilayer and in binary mixtures of PLPC-oxidized-lipid-bilayers with 0–50% Chol concentration and oxidized lipids with hydroperoxide and aldehyde oxidized functional groups. From the 60 unbiased molecular dynamics simulations (total of 161 μs), we found that Chol inhibited pore formation in the aldehyde-containing oxidized lipid bilayers at concentrations greater than 11%. For both pure PLPC bilayer and bilayers with hydroperoxide lipids, no pores were observed at any Chol concentration. Furthermore, increasing cholesterol concentration led to a change of phase state from the liquid-disordered to the liquid-ordered phase. This condensing effect of Chol was observed in all systems. Data analysis shows that the addition of Chol results in an increase in bilayer thickness. Interestingly, we observed Chol flip-flop only in the aldehyde-containing lipid bilayer but neither in the PLPC nor the hydroperoxide bilayers. Umbrella-sampling simulations were performed to calculate the translocation free energies and the Chol flip-flop rates. The results show that Chol’s flip-flop rate depends on the lipid bilayer type, and the highest rate are found in aldehyde bilayers. As the main finding, we shown that Chol stabilizes the oxidized lipid bilayer by confining the distribution of the oxidized functional groups.     

Proton nuclear magnetic resonance investigation of the conformation and dynamics in the synthetic deoxyribonucleic acid decamers d(ATATCGATAT) and d(ATATGCATAT)

A variety of one-dimensional proton NMR methods have been used to investigate the properties of two synthetic DNA decamers, d(ATATCGATAT) and d(ATATGCATAT). These results, in conjunction with the results of two-dimensional NMR experiments, permit complete assignment of the base proton resonances. Low-field resonances were assigned by sequential "melting" of the A . T base pairs and by comparison of the spectra of the two decamers. Below 20 degree C spin-lattice relaxation is dominated by through-space dipolar interactions. A substantial isotope effect on the G imino proton relaxation is observed in 75% D2O, confirming the importance of the exchangeable amino protons in the relaxation process. A somewhat smaller isotope effect is observed on the T imino proton relaxation. At elevated temperatures spin-lattice relaxation of the imino protons is due to proton exchange with solvent. Apparent activation energies for exchange vary from 36 kcal/base pair for base pairs (3,8) to 64 kcal/mol for the most interior base pairs (5,6), indicating that disruption of part, or all, of the double helix contributes significantly to the exchange of the imino protons in these decamers. By contrast, single base pair opening events are the major low-temperature pathways for exchange from A X T and G X C base pairs in the more stable higher molecular weight DNA examined in other studies. The temperature dependence of the chemical shifts and line widths of certain aromatic resonances indicates that the interconversion between the helix and coil states is not in fast exchange below the melting temperature, Tm. Within experimental error, no differential melting of base pairs was found in either molecule, and both exhibited melting points Tm = 50-52 degrees C. Spin-spin and spin-lattice relaxation rates of the nonexchangeable protons (TH6, AH8, and AH2) are consistent with values calculated by using an isotropic rotor model with a rotational correlation time of 6 ns and interproton distances appropriate for B-family DNA. The faster decay of AH8 compared with GH8 is attributed to an interaction between the thymine methyl protons and the AH8 protons in adjacent adenines (5'ApT3'). The base protons (AH8, GH8, and TH6) appear to be located close (1.9-2.3 A) to sugar H2',2" protons.(ABSTRACT TRUNCATED AT 400 WORDS)     

Effect of alkyl chain unsaturation and cholesterol intercalation on oxygen transport in membranes: a pulse ESR spin labeling study.

Transport and diffusion of molecular oxygen in phosphatidylcholine (PC)-cholesterol membranes and their molecular mechanism were investigated. A special attention was paid to the molecular interaction involving unsaturated alkyl chains and cholesterol. Oxygen transport was evaluated by monitoring the bimolecular collision rate of molecular oxygen and the lipid-type spin labels, tempocholine phosphatidic acid ester, 5-doxylstearic acid, and 16-doxylstearic acid. The collision rate was determined by measuring the spin-lattice relaxation times (T1's) in the presence and absence of molecular oxygen with long-pulse saturation-recovery ESR techniques. In the absence of cholesterol, incorporation of either a cis or trans double bond at the C9-C10 position of the alkyl chain decreases oxygen transport at all locations in the membrane. The activation energy for the translational diffusion of molecular oxygen in the absence of cholesterol is 3.7-6.5 kcal/mol, which is comparable to the activation energy theoretically estimated for kink migration or C-C bond rotation of alkyl chains [Tr?uble, H. (1971) J. Membr. Biol. 4, 193-208; Pace, R. J., & Chan, S. I. (1982) J. Chem. Phys. 76, 4241-4247]. Intercalation of cholesterol in saturated PC membranes reduces oxygen transport in the headgroup region and the hydrophobic region near the membrane surface but little affects the transport in the central part of the bilayer. In unsaturated PC membranes, intercalation of cholesterol also reduces oxygen transport in and near the headgroup regions. In contrast, it increases oxygen transport in the middle of the bilayer. On the basis of these observations, a model for the mechanism of oxygen transport in the membrane is proposed in which oxygen molecules reside in vacant pockets created by gauche-trans isomerization of alkyl chains and the structural nonconformability of neighboring lipids, unsaturated PC and cholesterol in particular, and oxygen molecules jump from one pocket to the adjacent one or move along with the movement of the pocket itself. The presence of cholesterol decreases oxygen permeability across the membrane in all membranes used in this work in spite of the increase in oxygen transport in the central part of unsaturated PC-cholesterol membranes because cholesterol decreases oxygen transport in and near the headgroup regions, where the major barriers for oxygen permeability are located. Oxygen gradients across the membranes of the cells and the mitochondria are evaluated. Arguments are advanced that oxygen permeation across the protein-rich mitochondrial membranes can be a rate-limiting step for oxygen consumption under hypoxic conditions in vivo.