Calculation of Liquid-Disordered/Liquid-Ordered Line Tension from Pairwise Lipid Interactions.

The energy penalty for bilayer phase domain interfaces, line tension, is an important quantity for describing the phase domain size transition from the nanometer scale to the micrometer scale and larger. We connected pairwise lipid interaction energies in ternary lipid mixtures with experimentally measured line tensions by using the compositional differences between coexisting liquid-disordered (Ld) and liquid-ordered (Lo) phases known from phase diagrams. Using a mean-field theory model, we developed a computational procedure to map out Ld + Lo phase boundaries and thermodynamic tielines based on a set of pairwise interaction energies. We find that experimentally measured Ld/Lo line tension can be effectively modeled by the sum of pairwise interactions at the interface. This result indicates that pairwise lipid interactions make a major contribution to line tension.

Crosslinking a lipid raft component triggers liquid ordered-liquid disordered phase separation in model plasma membranes.

The mechanisms by which a cell uses and adapts its functional membrane organization are poorly understood and are the subject of ongoing investigation and discussion. Here, we study one proposed mechanism: the crosslinking of membrane components. In immune cell signaling (and other membrane-associated processes), a small change in the clustering of specific membrane proteins can lead to large-scale reorganizations that involve numerous other membrane components. We have investigated the large-scale physical effect of crosslinking a minor membrane component, the ganglioside GM1, in simple lipid models of the plasma membrane containing sphingomyelin, cholesterol, and phosphatidylcholine. We observe that crosslinking GM1 can cause uniform membranes to phase-separate into large, coexistent liquid ordered and liquid disordered membrane domains. We also find that this lipid separation causes a dramatic redistribution of a transmembrane peptide, consistent with a raft model of membrane organization. These experiments demonstrate a mechanism that could contribute to the effects of crosslinking observed in cellular processes: Domains induced by clustering a small number of proteins or lipids might rapidly reorganize many other membrane proteins.

Ternary phase diagram of dipalmitoyl-PC/dilauroyl-PC/cholesterol: nanoscopic domain formation driven by cholesterol.

A ternary phase diagram is proposed for the hydrated lamellar lipid mixture dipalmitoylphosphatidylcholine/dilauroylphosphatidylcholine/cholesterol (DPPC/DLPC/cholesterol) at room temperature. The entire composition space has been thoroughly mapped by complementary experimental techniques, revealing interesting phase behavior that has not been previously described. Confocal fluorescence microscopy shows a regime of coexisting DPPC-rich ordered and DLPC-rich fluid lamellar phases, having an upper boundary at apparently constant cholesterol mole fraction chi(chol) approximately 0.16. Fluorescence resonance energy transfer experiments confirm the identification and extent of this two-phase regime and, furthermore, reveal a 1-phase regime between chi(chol) approximately 0.16 and 0.25, consisting of ordered and fluid nanoscopic domains. Dipyrene-PC excimer/monomer measurements confirm the new regime between chi(chol) approximately 0.16 and 0.25 and also show that rigidly ordered phases seem to disappear around chi(chol) approximately 0.25. This study should be considered as a step toward a more complete understanding of lateral heterogeneity within biomembranes. Cholesterol may play a role in domain separation on the nanometer scale.

Characterization of lipid bilayer phases by confocal microscopy and fluorescence correlation spectroscopy.

We report the application of confocal imaging and fluorescence correlation spectroscopy (FCS) to characterize chemically well-defined lipid bilayer models for biomembranes. Giant unilamellar vesicles of dilauroyl phosphatidylcholine/dipalmitoyl phosphatidylcholine (DLPC/DPPC)/cholesterol were imaged by confocal fluorescence microscopy with two fluorescent probes, 1, 1'-dieicosanyl-3,3,3',3'-tetramethylindocarbocyanine perchlorate (DiI-C(20)) and 2-(4,4-difluoro-5,7-dimethyl-4-bora-3a, 4a-diaza-s-indacene-3-pentanoyl)-1-hexadecanoyl-sn-glycero-3 -phosphoc holine (Bodipy-PC). Phase separation was visualized by differential probe partition into the coexisting phases. Three-dimensional image reconstructions of confocal z-scans through giant unilamellar vesicles reveal the anisotropic morphology of coexisting phase domains on the surface of these vesicles with full two-dimensional resolution. This method demonstrates by direct visualization the exact superposition of like phase domains in apposing monolayers, thus answering a long-standing open question. Cholesterol was found to induce a marked change in the phase boundary shapes of the coexisting phase domains. To further characterize the phases, the translational diffusion coefficient, D(T), of the DiI-C(20) was measured by FCS. D(T) values at approximately 25 degrees C ranged from approximately 3 x 10(-8) cm(2)/s in the fluid phase, to approximately 2 x 10(-9) cm(2)/s in high-cholesterol-content phases, to approximately 2 x 10(-10) cm(2)/s in the spatially ordered phases that coexist with fluid phases. In favorable cases, FCS could distinguish two different values of D(T) in a region of two-phase coexistence on a single vesicle.

Maximum solubility of cholesterol in phosphatidylcholine and phosphatidylethanolamine bilayers.

In any lipid bilayer membrane, there is an upper limit on the cholesterol concentration that can be accommodated within the bilayer structure; excess cholesterol will precipitate as crystals of pure cholesterol monohydrate. This cholesterol solubility limit is a well-defined quantity. It is a first-order phase boundary in the phospholipid/cholesterol phase diagram. There are many different solubility limits in the literature, but no clear picture has emerged that can unify the disparate results. We have studied the effects that different sample preparation methods can have on the apparent experimental solubility limit. We find that artifactual demixing of cholesterol can occur during conventional sample preparation and that this demixed cholesterol may produce artifactual cholesterol crystals. Therefore, phospholipid/cholesterol suspensions which are prepared by conventional methods may manifest variable, falsely low cholesterol solubility limits. We have developed two novel preparative methods which are specifically designed to prevent demixing during sample preparation. For detection of the cholesterol crystals, X-ray diffraction has proven to be quantitative and highly sensitive. Experiments based on these methods yield reproducible and precise cholesterol solubility limits: 66 mol% for phosphatidylcholine (PC) bilayers and 51 mol% for phosphatidylethanolamine (PE) bilayers. We present evidence that these are true, equilibrium values. In contrast to the dramatic headgroup effect (PC vs. PE), acyl chain variations had no effect on the cholesterol solubility limit in four different PC/cholesterol mixtures.

A novel strategy for the preparation of liposomes: rapid solvent exchange.

During the preparation of multi-component model membranes, a primary consideration is that compositional homogeneity should prevail throughout the suspension. Some conventional sample preparation methods pass the lipid mixture through an intermediary, solvent-free state. This is an ordered, solid state and may favor the demixing of membrane components. A new preparative method has been developed which is specifically designed to avoid this intermediary state. This novel strategy is called rapid solvent exchange (RSE) and entails the direct transfer of lipid mixtures between organic solvent and aqueous buffer. RSE liposomes require no more than a minute to prepare and manifest considerable entrapment volumes with a high fraction of external surface area. In phospholipid/cholesterol mixtures of high cholesterol content, suspensions prepared by more conventional methods reveal evidence of artifactual demixing, whereas samples prepared by rapid solvent exchange do not. The principles which may lead to artifactual demixing during conventional sample preparation are discussed.

A microscopic interaction model of maximum solubility of cholesterol in lipid bilayers.

We recently reported the equilibrium maximum solubility of cholesterol in a lipid bilayer, chi*chol, to be 0.66 in four different phosphatidylcholines, and 0.51 in a phosphatidylethanolamine (Huang, J.,J.T. Buboltz, and G. W. Feigenson. 1999. Biochim. Biophys. Acta. in press). Here we present a model of cholesterol-phospholipid mixing that explains these observed values of chi*chol. Monte Carlo simulations show that pairwise-additivity of nearest-neighbor interactions is inadequate to describe all the chi*chol values. Instead, if cholesterol multibody interactions are assigned highly unfavorable energy, then jumps occur in cholesterol chemical potential that lead to its precipitation from the bilayer. Cholesterol precipitation is most likely to occur near three discrete values of cholesterol mole fraction, 0.50, 0.57, and 0.67, which correspond to cholesterol/phospholipid mole ratios of 1/1, 4/3, and 2/1, respectively. At these solubility limits, where cholesterol chemical potential jumps, the cholesterol-phospholipid bilayer mixture forms highly regular lipid distributions in order to minimize cholesterol-cholesterol contacts. This treatment shows that dramatic structural and thermodynamic changes can occur at particular cholesterol mole fractions without any stoichiometric complex formation. The physical origin of the unfavorable cholesterol multibody interaction is explained by an "umbrella model": in a bilayer, nonpolar cholesterol relies on polar phospholipid headgroup coverage to avoid the unfavorable free energy of cholesterol contact with water. Thus, at high cholesterol mole fraction, this unfavorable free energy, not any favorable cholesterol-phospholipid interaction, dominates the mixing behavior. This physical origin also explains the "cholesterol condensing effect" and the increase in acyl chain order parameter in cholesterol-phospholipid mixtures.

Partitioning of a fluorescent phospholipid between fluid bilayers: dependence on host lipid acyl chains.

The partition coefficient Kp was measured for a headgroup-labeled phospholipid (12:0,12:0)-N-(7-nitrobenz-2-oxa-1,3-diazol-4-yl)-PE (12-NBD-PE), equilibrated between LUV of a series of phosphatidylcholines (PC). Fluorescence resonance energy transfer between the 12-NBD-PE and a headgroup-rhodamine-labeled PE was used to find the equilibrium concentration of the 12-NBD-PE in the different LUV. Reliable equilibrium concentrations were obtained by monitoring the approach to equilibrium starting from a concentration below and from a concentration above the ultimate values. Using (16:0,18:1delta9)-PC as the reference lipid, Kp ranged from a high value of 1.65 favoring (16:0,18:1delta9)-PC over (16:1delta9,16:1delta9)-PC, to a low value of 0.90, favoring (22:1delta13,22:1delta13)-PC over (16:0,18:1delta9)-PC. The Kp values enabled calculation of the acyl chain contribution to the excess free energy of mixing for (12:0,12:0) acyl chains at infinite dilution in the L alpha phase of PC having acyl chains of (16:0,18:1delta9), (16:1delta9,16:1delta9), (18:1delta9,18:1delta9), (18:1delta6,18:1delta6), (20:1delta11,20:1delta11), and (22:1delta13,22:1delta13). (14:1delta9,14:1delta9)-PC was found to transfer so rapidly between LUV as to preclude reliable Kp measurement.

Regulatory mechanisms of the acrosome reaction revealed by multiview microscopy of single starfish sperm.

The acrosome reaction in many animals is a coupled reaction involving an exocytotic step and a dramatic change in cell shape. It has been proposed that these morphological changes are regulated by intracellular ions such as Ca2+ and H+. We report here simultaneous visualization, under a multiview microscope, of intracellular free Ca2+ concentration ([Ca2+]i), intracellular pH (pHi), and morphological changes in a single starfish sperm (Asterina pectinifera). [Ca2+]i and pHi were monitored with the fluorescent probes indo-1 and SNARF-1, respectively. The acrosome reaction was induced with ionomycin. After the introduction of ionomycin in the medium, [Ca2+]i increased gradually and reached a plateau in approximately 30 s. The fusion of the acrosomal vacuole took place abruptly before the plateau, during the rising phase. Although the speed of the [Ca2+]i increase varied among the many sperm tested, exocytosis in all cases occurred at the same [Ca2+]i of approximately 2 microM (estimated using the dissociation constant of indo-1 for Ca2+ of 1.1 microM). This result suggests that the exocytotic mechanism in starfish sperm responds to [Ca2+]i rapidly, with a reaction time of the order of one second or less. Unlike the change in [Ca2+]i, an abrupt increase in pHi was observed immediately after exocytosis, suggesting the presence of a proton mobilizing system that is triggered by exocytosis. The rapid increase in pHi coincided with the formation of the acrosomal rod and the beginning of vigorous movement of the flagellum, both of which have been proposed to be pHi dependent. The exocytotic event itself was visualized with the fluorescent membrane probe RH292. The membrane of the acrosomal vacuole, concealed from the external medium in an unreacted sperm, was seen to fuse with the plasma membrane.

Detection of phase separation in fluid phosphatidylserine/phosphatidylcholine mixtures.

The nonideal mixing of 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphoserine, (16:0, 18:1)PS, and 1,2-didodecenoyl-sn-glycero-3-phosphocholine, (12:1, 12:1)PC, in fluid lamellar model membranes was studied by measuring binding of aqueous Ca2+ ions and by x-ray diffraction. A region of two-phase coexistence was found by invariance of the aqueous concentration and by the appearance of two sets of lamellar spacings. The phases were identified as fluid from the diffuse x-ray diffraction in the wide-angle region. The width of the two-phase coexistence region was greater at higher ionic strength. In 800 mM KCl, the phase boundaries were at PS mole fraction 0.5 and 0.8. In 100 mM KCl, the phase boundaries were at PS mole fraction 0.52 and 0.62. Monte Carlo simulations of the lateral distributions of these PS/PC mixtures show pronounced clustering of the lipids.

Detection of coexisting fluid phospholipid phases by equilibrium Ca2+ binding: peptide-poor L alpha and peptide-rich HII phase coexistence in gramicidin A'/phospholipid dispersions.

The isothermal phase behavior of three gramicidin A'/phospholipid mixtures was investigated by an equilibrium Ca(2+)-binding technique. The phospholipid component was 1,2-dioleoyl-sn-glycero-3-phosphoserine (DOPS), 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphoserine (POPS), or POPS/1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC) at a constant mole ratio of 1/4. The bulk aqueous free Ca2+ concentration, [Ca2+]*f, in equilibrium with one or two gramicidin A'/phospholipid fluid phases and a small amount of the Ca (phosphatidylserine)2 gel phase, was measured as a function of composition at 20 degrees C by use of chromophoric high-affinity Ca2+ chelators. The coexistence of two gramicidin A'/phospholipid fluid phases was detected by an invariance in [Ca2+]*f over the range of compositions throughout which the two phases coexist. The compositions of the two coexisting phases are determined by the compositions at which the invariance in [Ca2+]*f begins and ends. With each of the gramicidin A'/phospholipid mixtures, we estimate that the composition of the gramicidin-poor phase is 0.03-0.04 mole fraction gramicidin A' and the composition of the gramicidin-rich phase is 0.13-0.14 mole fraction gramicidin A'. Characterization of these phases by low-angle X-ray diffraction revealed that, in each case, the gramicidin-poor phase is an L alpha phase and the gramicidin-rich phase is an HII phase. The isothermal phase behavior of gramicidin A'/POPC mixtures at approximately 23 degrees C, as determined by low-angle X-ray diffraction, was found to be similar to that of the other gramicidin A'/phospholipid mixtures.(ABSTRACT TRUNCATED AT 250 WORDS)

Partitioning of gramicidin A' between coexisting fluid and gel phospholipid phases.

The partitioning behavior of gramicidin A' was investigated in four binary phospholipid mixtures with coexisting fluid and gel phases. The ratio of the equilibrium peptide concentration in the fluid phase to that in the gel phase (i.e., the partition coefficient, Kp) was determined by analysis of the quenching of gramicidin A' tryptophanyl fluorescence by a spin-labeled phosphatidylcholine. The partition coefficient was used as a measure of the relative solubility of gramicidin A' in the four types of gel phases analyzed. The composition of the gel phase was entirely Ca(dioleoylphosphatidylserine)2 (Ca(di18:1-PS)2), or was rich in either distearoylphosphatidylcholine (di18:0-PC), dipalmitoylphosphatidylcholine (di16:0-PC), or dimyristoylphosphatidylcholine (di14:0-PC). Except in the last case, the gel phase was depleted of gramicidin A': Kp approximately 30 when the gel phase was Ca(di18:1-PS)2 or di18:0-PC-rich, Kp approximately 10 when the gel phase was di16:0-PC-rich, and Kp approximately 1 when the gel phase was di14:0-PC-rich. The hydrophobic mismatch between the length of gramicidin A' and the length of the phospholipid acyl chains in the bulk gel phase is greatest with di18:1-PS and di18:0-PC, intermediate with di16:0-PC, and least with di14:0-PC. The Kp measurements presented here are consistent with increasing solubility of gramicidin A' in the gel phase with decreasing hydrophobic mismatch.

Monte Carlo simulation of lipid mixtures: finding phase separation.

The nonideal mixing of phosphatidylserine (PS) and phosphatidylcholine (PC) binary lipid mixtures was studied by computer simulation based on a model wherein the excess energy of mixing is divided between an electrostatic term and one adjustable term delta Em that includes all other nonideal interactions. The lateral distribution of the lipids and the energy of the mixtures were obtained by using Kawasaki relaxation in a canonical ensemble. The Gibbs free energies were calculated by Kirkwood's coupling parameter method. The simulation results are strongly dependent on simulation size for sizes smaller than about 1000 lipids. Nonideal interaction between lipids can result in large scale separation of lipid phases of different composition at reasonable delta Em values as well as clustering of like lipids. In plots of total Gibbs free energy of mixing versus PS mole fraction in PS/PC, the boundaries of the two phase region could be accurately determined. The electrostatic interaction influences cluster size and shape, and also the composition of phases in the two-phase region.

Nonideal mixing of phosphatidylserine and phosphatidylcholine in the fluid lamellar phase.

The mixing of phosphatidylserine (PS) and phosphatidylcholine (PC) in fluid bilayer model membranes was studied by measuring binding of aqueous Ca2+ ions. The measured [Ca2+]aq was used to derive the activity coefficient for PS, gamma PS, in the lipid mixture. For (16:0, 18:1) PS in binary mixtures with either (16:0, 18:1)PC, (14:1, 14:1)PC, or (18:1, 18:1)PC, gamma PS > 1; i.e., mixing is nonideal, with PS and PC clustered rather than randomly distributed, despite the electrostatic repulsion between PS headgroups. To understand better this mixing behavior, Monte Carlo simulations of the PS/PC distributions were performed, using Kawasaki relaxation. The excess energy was divided into an electrostatic term Uel and one adjustable term including all other nonideal energy contributions, delta Em. Uel was calculated using a discrete charge theory. Kirkwood's coupling parameter method was used to calculate the excess free energy of mixing, delta GEmix, hence In gamma PS,calc. The values of In gamma PS,calc were equalized by adjusting delta Em in order to find the simulated PS/PC distribution that corresponded to the experimental results. We were thus able to compare the smeared charge calculation of [Ca2+]surf with a calculation ("masked evaluation method") that recognized clustering of the negatively charged PS: clustering was found to have a modest effect on [Ca2+]surf, relative to the smeared charge model. Even though both PS and PC tend to cluster, the long-range nature of the electrostatic repulsion reduces the extent of PS clustering at low PS mole fraction compared to PC clustering at an equivalent low PC mole fraction.

Thermodynamics of mixing of phosphatidylserine/phosphatidylcholine from measurements of high-affinity calcium binding.

A simple model system is described that allows measurement of equilibrium Ca2+ binding to multilamellar vesicle mixtures of palmitoyloleoylphosphatidylserine (P,O-PS) and dimyristoleoylphosphatidylcholine (MO,MO-PC). The constraint of the chemical equilibrium among aqueous Ca2+, hydrated P,O-PS/MO,MO-PC, and Ca(PS)2, together with measurements of the Ca2+ concentration in equilibrium with defined PS/PC ratios, enables the determination of the thermodynamic activity of the lipids. The activity coefficient of dilute P,O-PS in PC is analyzed in terms of the partial molal free energy to transfer P,O-PS from an environment of PS to an environment of PC. This study of P,O-PS/MO,MO-PC, by comparison with the earlier study of P,O-PS/P,O-PC [Feigensen, G.W. (1989) Biochemistry 20, 1270-1278], reveals that the excess partial molal free energy to transfer P,O-PS from P,O-PS to P,O-PC is -0.7 kcal mol-1. This free energy change arises in part from the favorable transfer of the negatively charged phosphoserine headgroup from an environment of negative charges to an environment of zwitterions. The contribution of acyl chain mismatch to the partial molal free energy to transfer P,O-PS from P,O-PS to MO,MO-PC is found to be approximately +0.7 kcal mol-1. This value is much larger than that of the excess partial molal free energy of mixing in isotropic solutions of linear hydrocarbons that differ in chain length or unsaturation.

Fluorescence quenching in model membranes: phospholipid acyl chain distributions around small fluorophores.

Fluorescence quenching in lipid bilayers is treated by a new approach based on calculation of the probability distribution of quenching and nonquenching acyl chains around a fluorophore. The effect of acyl lattice site dependence (i.e., correlations of phospholipid sister chain occupancy of neighbor sites) was modeled by use of Monte Carlo simulations of acyl chain occupancy. This explicit accounting of site occupancy correlation was found to fit observed quenching behavior better than did a model wherein phospholipid quenchers are considered to be independent. A key aspect of this approach is to evaluate the rate for quenching in a bilayer composed of pure quenching lipid. In order to evaluate this quenching rate, and also to provide a strong test of the calculated probability distributions, we synthesized lipids with both acyl chains labeled with a quenching moiety (Br or nitroxide), as well as the more usual single-chain quenchers. The fluorescence of tryptophan octyl ester (TOE), and of the 1,6-diphenyl-1,3,5-hexatriene (DPH) derivatives trimethylammonium-DPH (TMA-DPH) and 1-lauroyl-2-(DPH-propionyl)phosphatidylcholine (DPH-PC), was examined. We obtained consistent results with all the fluorophores and quenchers indicating that up to 18 neighboring acyl sites can contribute to quenching, corresponding to two shells of acyl sites on a hexagonal lattice. Calculated discrete distributions of fluorescence intensities were converted into fluorescence lifetimes and compared with Gaussian and Lorentzian continuous lifetime distributions. The fluorescence quenching theory presented here may be used to explain quantitatively the heterogeneity of fluorophore environments in multicomponent membranes.

Partitioning behavior of indocarbocyanine probes between coexisting gel and fluid phases in model membranes.

Gel-fluid partition coefficients, Kp, were measured for a series of indocarbocyanine dyes in multilamellar lipid vesicles. The dyes examined had alkyl chain lengths from 12 to 22 carbons. Fluorescence quenching by a spin-labeled phosphatidylcholine-enriched fluid phase created a large difference in quantum yield for indocarbocyanine fluorescence between fluid and gel phases, enabling reliable Kp determinations. The values range from Kp = 8 for the 12-carbon chain, favoring a fluid phase over a Ca2-phosphatidylserine rigid phase, to Kp = 0.02 for the 20-carbon chain dye, favoring a distearoylphosphatidylcholine-rich gel phase over the fluid phase.

Calcium ion binding between lipid bilayers: the four-component system of phosphatidylserine, phosphatidylcholine, calcium chloride, and water.

Ca2+ binding between lamellae of phosphatidylserine (PS) and phosphatidylcholine (PC) gives rise to a rigid phase of Ca(PS)2. When aqueous Ca2+, hydrated PS/PC, and Ca(PS)2 coexist at equilibrium, the aqueous Ca2+ concentration is invariant and is characteristic of the PS/PC ratio. This characteristic Ca2+ concentration is 0.040 microM for palmitoyloleoylphosphatidylserine without PC and increases as the inverse square of the PS mole fraction at high PS concentration (Raoult's law) and as the inverse square of the PS mole fraction multiplied by a constant at low PS concentration (Henry's law). For example, for palmitoyloleoylphosphatidylserine/palmitoyloleoylphosphatidylcholi ne = 0.6/0.4 or 0.2/0.8, this characteristic Ca2+ concentration is about 0.1 or about 6 microM, respectively. These observations at constant temperature are summarized in a quaternary phase diagram for the four-component system CaCl2/PS/PC/water.

On the use of partition coefficients to characterize the distribution of fluorescent membrane probes between coexisting gel and fluid lipid phase: an analysis of the partition behavior of 1,6-diphenyl-1,3,5-hexatriene.

The distribution of the fluorescent membrane probe 1,6-diphenyl-1,3,5-hexatriene between coexisting gel and fluid phospholipid phases in multilamellar vesicles has been examined using fluorescence quenching by spin-labeled phosphatidylcholine. For both thermally-induced and Ca2+-induced lipid phase separation, the ratio of probe concentration in the fluid liquid-crystal phase to that in the gel phase is found to be independent of either the probe concentration or the relative amounts of gel and fluid lipid phases, and hence is an equilibrium concentration ratio, or partition coefficient.

Location and ion-binding of membrane-associated valinomycin, a proton nuclear magnetic resonance study.

Valinomycin, incorporated in small unilamellar vesicles of perdeuterated dimyristoylphosphatidylcholine, reveals several well-resolved 1H-NMR resonances. These resonances were used to examine the location, orientation and ion-binding of membrane-bound valinomycin. The order of affinity of membrane-bound valinomycin for cations is Rb+ greater than K+ greater than Cs+ greater than Ba2+, and binding is sensitive to surface change. The exchange between bound and free forms is fast on the NMR time scale. The intrinsic binding constants, extrapolated to zero anion concentration, are similar to those determined in aqueous solution. Rb+ and K+ show 1:1 binding to valinomycin, whereas the stoichiometry of Cs+ and Ba2+ is not certain. Paramagnetic chemical shift reagents and nitroxide spin label relaxation probes were used to study the location and orientation of valinomycin in the membrane. Despite relatively fast exchange of bound cations, the time average location of the cation-free form of valinomycin is deep within the bilayer under the conditions of these experiments. Upon complexation to K+, valinomycin moves closer to the interfacial region.