Two-dimensional diffusion of amphiphiles in phospholipid monolayers at the air-water interface.

Steady-state and time-resolved fluorescence spectroscopy has been used to examine lateral diffusion in dipalmitoyl-L-alpha-phosphatidylcholine (DPPC) and dimyristoyl-L-alpha-phosphatidylcholine (DMPC) monolayers at the air-water interface, by studying the fluorescence quenching of a pyrene-labeled phospholipid (pyrene-DPPE) by two amphiphilic quenchers. Steady-state fluorescence measurements revealed pyrene-DPPE to be homogeneously distributed in the DMPC lipid matrix for all measured surface pressures and only in the liquid-expanded (LE) phase of the DPPC monolayer. Time-resolved fluorescence decays for pyrene-DPPE in DMPC and DPPC (LE phase) in the absence of quencher were best described by a single-exponential function, also suggesting a homogeneous distribution of pyrene-DPPE within the monolayer films. Addition of quencher to the monolayer film produced nonexponential decay behavior, which is adequately described by the continuum theory of diffusion-controlled quenching in a two-dimensional environment. Steady-state fluorescence measurements yielded lateral diffusion coefficients significantly larger than those obtained from time-resolved data. The difference in these values was ascribed to the influence of static quenching in the case of the steady-state measurements. The lateral diffusion coefficients obtained in the DMPC monolayers were found to decrease with increasing surface pressure, reflecting a decrease in monolayer fluidity with compression.     

Penetration of an emulsion surface by cholesteryl ester transfer protein

Quenching of the intrinsic fluorescence of cholesteryl ester transfer protein (CETP) by spin labelled fatty acids (5-NS and 16-NS) was investigated to determine the degree to which the protein penetrated the phospholipid monolayer surface of a lipid emulsion. When bound to the phospholipid surface approximately 50% of the fluorophores of the transfer protein were accessible to quenching by 5-NS whose nitroxy group locates near the monolayer surface. On the other hand, only 22% of the fluorophores of CETP were accessible to quenching by 16-NS whose nitroxy group locates deeper in the surface monolayer. Quenching of the CETP fluorescence by an aqueous phase quencher (acrylamide) shows that the protein undergoes a conformational change on binding which increases the proportion of the tryptophan residues exposed to the aqueous phase. The results indicate that CETP does not penetrate the lipid surface to a significant degree. Received: 29 March 1996 / Accepted: 30 May 1996     

Incorporation of a synthetic mitochondrial signal peptide into charged and uncharged phospholipid monolayers

The interaction of the chemically synthesized 25-residue signal peptide of subunit IV of yeast cytochrome c oxidase with synthetic and natural phospholipids was studied by using a monolayer technique. Incorporation of the peptide into phospholipid monolayers was measured as surface area increase at constant surface pressure. The peptide was readily soluble in aqueous buffer, yet spontaneously inserted from an aqueous subphase into phospholipid monolayers up to limiting pressures of 30-40 mN/m. The incorporation of the positively charged peptide was strongly enhanced by the presence of negatively charged phospholipids. The molecular area of the signal peptide in monolayers was determined with a 14C-labeled signal peptide and was 560 +/- 170 A2. This is consistent with a 25-residue alpha-helical peptide incorporating with its long axis parallel to the plane of the monolayer. Incorporation isotherms into synthetic phosphatidylcholine and phosphatidylglycerol monolayers at different charge densities were analyzed in terms of a simple incorporation/binding model, involving partitioning of the peptide into the monolayer and an in-plane binding reaction of the negatively charged phospholipids to the partitioned peptide.     

Surface-active properties of vasoactive intestinal peptide*

The purpose of this study was to determine whether human vasoactive intestinal peptide (VIP) aggregates in aqueous solution and, if so, whether the peptide interacts with a biomimetic phospholipid monolayer and increases surface pressure. Using a custom-made Teflon trough containing HEPES buffer (pH 7.4) at room temperature and a surface tensiometer, we found that the critical micellar concentration (CMC) of VIP is 0.4 microM. Surface pressure of a dipalmitoylphosphatidylcholine (DPPC) monolayer spread over the HEPES buffer declined significantly over 120 min because of phospholipid decomposition. However, injection of VIP at concentrations above CMC into the subphase of the monolayer elicited a significant concentration-dependent increase in surface pressure that persisted for 120 min (P < 0.05). Unlike VIP, injection of [(8)Arg]-vasopressin at an equimolar concentration only prevented the time-dependent decline in DPPC monolayer surface pressure. Taken together, these data indicate that human VIP aggregates in aqueous solution and expresses surface-active properties at physiological concentrations in vitro. We suggest that these attributes could have a role in modulating the bioactive effects of the peptide in vivo.     

Eutectic mixed monolayers in equilibrium with phospholipid-bilayers and triolein-liquid phase.

Triolein (TO) and phospholipids (egg yolk phosphatidylcholine, egg yolk phosphatidylethanolamine, and bovine brain phosphatidylserine) had low mutual solubilities and separated into the TO-liquid phase and phospholipid-bilayers. Spreading pressures of the TO-phospholipid mixture (i.e., surface pressures of the mixed monolayer in equilibrium with the phase-separating lipid mixture) at the air/saline interface were independent of the lipid composition. On the other hand, collapse pressures of the mixed monolayer of TO and phospholipid (i.e., surface pressures of the mixed monolayer in equilibrium with the TO-liquid phase) at the interface changed with the monolayer composition and were lower than the spreading pressure. The experimental data indicated the spreading and collapse pressures as offering a phase diagram for the presence of equilibrium between the mixed monolayer, the phospholipid-bilayers and the TO-liquid phase. The diagram showed that TO and the phospholipids were miscible in the mixed monolayer, forming an eutectic mixed monolayer. When the mixed monolayer initially had the eutectic composition, no collapse of the monolayer was detected until the surface pressure reached the value of the spreading pressure. No specific complex between TO and the phospholipid is required to explain the stability and collapse of the mixed monolayers. The bulk immiscibility of the lipids elucidated by the spreading pressure-measurements, immediately leads to the phase behaviors observed.     

Surface diffusion in human serum lipoproteins

From the viscosity dependence of the 31P NMR signals, the diffusion coefficients DT of phospholipid molecules in the surface monolayer of HDL, LDL and VLDL have been determined. DT for HDL3 and HDL2 are found to be 2.3 X 10(-8) cm2/s and 1.8 X 10(-8) cm2/s, respectively. These values are similar to values reported for diffusion of phospholipid molecules in phospholipid bilayers above the gel to liquid crystalline phase transition temperature. Viscosity dependence of [16,16,16-2H3]phosphatidylcholine incorporated into HDL2 yielded a value similar to that determined by 31P (DT = 1.9 X 10(-8) cm2/s). Slower diffusion coefficients were measured for LDL2 and VLDL. VLDL had a value DT = 9.1 X 10(-9) cm2/s. The diffusion coefficient for LDL2 was 1.4 X 10(-9) cm2/s. Thus, diffusion of phospholipids in LDL2 is a full order of magnitude slower at 25 degrees C than diffusion of phospholipids in the HDLs.     

Lateral diffusion in substrate-supported lipid monolayers as a function of ambient relative humidity

We analyzed the influence of water activity on the lateral self-diffusion of supported phospholipid monolayers. Lipid monolayer membranes were supported by polysaccharide cushions (chitosan and agarose), or glass. A simple diffusion model was derived, based on activated diffusion with an activation energy, E(a), which depends on the hydration state of the lipid headgroup. A crucial assumption of the derived model is that E(a) can be calculated assuming an exponential decay of the humidity-dependent disjoining pressure in the monolayer/substrate interface with respect to the equilibrium separation distance. A plot of ln(D) against ln(p(0)/p), where D is the measured diffusion coefficient and p(0) and p are the partial water pressures at saturation and at a particular relative humidity, respectively, was observed to be linear in all cases (i.e., for differing lipids, lateral monolayer pressures, temperatures, and substrates), in accordance with the above-mentioned diffusion model. No indications for humidity-induced first-order phase transitions in the supported phospholipid monolayers were found. Many biological processes such as vesicle fusion and recognition processes involve dehydration/hydration cycles, and it can be expected that the water activity significantly affects the kinetics of these processes in a manner similar to that examined in the present work.     

Peripheral protein adsorption to lipid-water interfaces: the free area theory

In fluid monolayers approaching collapse, phospholipids and their complexes with diacylglycerols hinder adsorption to the monolayer of the amphipathic protein, colipase. Herein, a statistical, free-area model, analogous to that used to analyze two-dimensional lipid diffusion, is developed to describe regulation by lipids of the initial rate of protein adsorption from the bulk aqueous phase to the lipid-water interface. It is successfully applied to rate data for colipase adsorption to phospholipid alone and yields realistic values of the two model parameters; the phospholipid excluded area and the critical free surface area required to initiate adsorption. The model is further developed and applied to analyze colipase adsorption rates to mixed monolayers of phospholipid and phospholipid-diacylglycerol complexes. The results are consistent with complexes being stably associated over the physiologically relevant range of lipid packing densities and being randomly distributed with uncomplexed phospholipid molecules. Thus, complexes should form in fluid regions of cellular membranes at sites of diacylglycerol generation. If so, by analogy with the behavior of colipase, increasing diacylglycerol may not trigger translocation of some amphipathic peripheral proteins until its abundance locally exceeds its mole fraction in complexes with membrane phospholipids.     

Atomic force microscopy studies of functional and dysfunctional pulmonary surfactant films, II: albumin-inhibited pulmonary surfactant films and the effect of SP-A

Pulmonary surfactant (PS) dysfunction because of the leakage of serum proteins into the alveolar space could be an operative pathogenesis in acute respiratory distress syndrome. Albumin-inhibited PS is a commonly used in vitro model for studying surfactant abnormality in acute respiratory distress syndrome. However, the mechanism by which PS is inhibited by albumin remains controversial. This study investigated the film organization of albumin-inhibited bovine lipid extract surfactant (BLES) with and without surfactant protein A (SP-A), using atomic force microscopy. The BLES and albumin (1:4 w/w) were cospread at an air-water interface from aqueous media. Cospreading minimized the adsorption barrier for phospholipid vesicles imposed by preadsorbed albumin molecules, i.e., inhibition because of competitive adsorption. Atomic force microscopy revealed distinct variations in film organization, persisting up to 40 mN/m, compared with pure BLES monolayers. Fluorescence confocal microscopy confirmed that albumin remained within the liquid-expanded phase of the monolayer at surface pressures higher than the equilibrium surface pressure of albumin. The remaining albumin mixed with the BLES monolayer so as to increase film compressibility. Such an inhibitory effect could not be relieved by repeated compression-expansion cycles or by adding surfactant protein A. These experimental data indicate a new mechanism of surfactant inhibition by serum proteins, complementing the traditional competitive adsorption mechanism.     

A theoretical model for lipid monolayer phase transitions.

We present a theoretical model for the liquid-expanded to liquid-condensed phase transition observed in many phospholipid monolayer films. The total two-dimensional pressure in the model is the sum of the hydrocarbon chain pressure and the surface pressure. The hydrocarbon chain pressure is calculated in an exteded version of a model published earlier. The surface pressure results from a lowering of the surface tension in the monolayer over that of pure water, thus producing a force on a Langmuir float. When these two contributions are added, pi/A isotherms are obtained which have slope discontinuities very similar to those observed experimentally. The results indicate that a successful model for lipid phase behavior must consider the interactions between head groups and water as well as cooperative hydrocarbon chain melting.     

Incorporation of surface tension into molecular dynamics simulation of an interface: a fluid phase lipid bilayer membrane.

In this paper we report on the molecular dynamics simulation of a fluid phase hydrated dimyristoylphosphatidylcholine bilayer. The initial configuration of the lipid was the x-ray crystal structure. A distinctive feature of this simulation is that, upon heating the system, the fluid phase emerged from parameters, initial conditions, and boundary conditions determined independently of the collective properties of the fluid phase. The initial conditions did not include chain disorder characteristic of the fluid phase. The partial charges on the lipids were determined by ab initio self-consistent field calculations and required no adjustment to produce a fluid phase. The boundary conditions were constant pressure and temperature. Thus the membrane was not explicitly required to assume an area/phospholipid molecule thought to be characteristic of the fluid phase, as is the case in constant volume simulations. Normal to the membrane plane, the pressure was 1 atmosphere, corresponding to the normal laboratory situation. Parallel to the membrane plane a negative pressure of -100 atmospheres was applied, derived from the measured surface tension of a monolayer at an air-water interface. The measured features of the computed membrane are generally in close agreement with experiment. Our results confirm the concept that, for appropriately matched temperature and surface pressure, a monolayer is a close approximation to one-half of a bilayer. Our results suggest that the surface area per phospholipid molecule for fluid phosphatidylcholine bilayer membranes is smaller than has generally been assumed in computational studies at constant volume. Our results confirm that the basis of the measured dipole potential is primarily water orientations and also suggest the presence of potential barriers for the movement of positive charges across the water-headgroup interfacial region of the phospholipid.     

Interaction of lipid vesicles with monomolecular layers containing lung surfactant proteins SP-B or SP-C

Pulmonary surfactant contains two families of hydrophobic proteins, SP-B and SP-C. Both proteins are thought to promote the formation of the phospholipid monolayer at the air-fluid interface of the lung. The Wilhelmy plate method was used to study the involvement of SP-B and SP-C in the formation of phospholipid monolayers. The proteins were either present in the phospholipid vesicles which were injected into the subphase or included in a preformed phospholipid monolayer. In agreement with earlier investigators, we found that SP-B and SP-C, present in phospholipid vesicles, were able to induce the formation of a monolayer, as became apparent by an increase in surface pressure. However, when the proteins were present in a preformed phospholipid monolayer (20 mN/m) at similar lipid to protein ratios, the rate of surface pressure increase after injection of pure phospholipid vesicles into the subphase at similar vesicle concentrations was 10 times higher. The process of phospholipid insertion from phospholipid vesicles into the protein-containing monolayers was dependent on (1) the presence of (divalent) cations, (2) the phospholipid concentration in the subphase, (3) the size of the phospholipid vesicles, (4) the protein concentration in the preformed monolayer, and (5) the initial surface pressure at which the monolayers were formed. Both in vesicles and in preformed monolayers, SP-C was less active than SP-B in promoting the formation of a phospholipid monolayer. The use of preformed monolayers containing controlled protein concentrations may allow more detailed studies on the mechanism by which the proteins enhance phospholipid monolayer formation from vesicles.     

Effects of lateral diffusion on the fluorescence anisotropy in hexagonal lipid phases. I. Theory.

It is shown that fluorescence anisotropy from lipidlike probes in the hexagonal HII phase gives information of (a) orientational order parameters, (b) the wobbling diffusion constant, and (c) the hopping diffusion constant of the probe, DH, equals DL/R2, the lateral diffusion constant over the square of the radius of the hexagonal tubes. Here we consider only lipidlike probes having the absorption transition movement and/or the emission transition moment along the long axis of the molecule. Three models are introduced for analysis of time-resolved data: the "WOBHOP," the "reduced WOBHOP," and the "P2P4HOP" model. The fluorescence anisotropy in response to a very short excitation pulse in each of the three models is a constant plus a number of exponentials. The WOBHOP and reduced WOBHOP models have 3 and 2 exponentials, respectively, and both contain four fitting parameters: r0 (the fundamental anisotropy), (P2) (the second rank orientational order parameter), DW (the wobbling diffusion constant), and DH (the hopping diffusion constant). The P2P4HOP model has eight exponentials and five fitting parameters: the four parameters listed above and (P4) (the fourth rank orientational order parameter). Analysis of fluorescence anisotropy data in the hexagonal HII phase using one of these models allows for obtaining the hopping diffusion constant, and, if the lateral diffusion constant is known, the radius of the hexagonal tubes. Substitution of DH = 0 in each of the three models yields an expression for the fluorescence anisotropy that is used in the literature for lamellar (L alpha or L beta) phases. The fluorescence anisotropy in coexisting L alpha/HII phases is discussed.     

A theoretical model for lipid monolayer phase transitions

We present a theoretical model for the liquid-expanded to liquid-condensed phase transition observed in many phospholipid monolayer films. The total two-dimensional pressure in the model is the sum of the hydrocarbon chain pressure and the surface pressure. The hydrocarbon chain pressure is calculated in an extended version of a model published earlier. The surface pressure results from a lowering of the surface tension in the monolayer over that of pure water, thus producing a force on a Langmuir float. When these two contributions are added, $\text{π/A}$ isotherms are obtained which have slope discontinuities very similar to those observed experimentally. These results indicate that a successful model for lipid phase behavior must consider the interactions between head groups and water as well as cooperative hydrocarbon chain melting.     

Determining the membrane topology of peptides by fluorescence quenching

Determination of the topology of peptides in membranes is important for characterizing and understanding the interactions of peptides with membranes. We describe a method that uses fluorescence quenching arising from resonance energy transfer ("FRET") for determining the topology of the tryptophan residues of peptides partitioned into phospholipid bilayer vesicles. This is accomplished through the use of a novel lyso-phospholipid quencher (lysoMC), N-(7-hydroxyl-4-methylcoumarin-3-acetyl)-1-palmitoyl-2-hydroxy-sn-gly cero-3-phosphoethanolamine. The design principle was to anchor the methylcoumarin quencher in the membrane interface by attaching it to the headgroup of lyso-phosphoethanolamine. We show that lysoMC can be incorporated readily into large unilamellar phospholipid vesicles to yield either symmetrically (both leaflets) or asymmetrically (outer leaflet only) labeled bilayers. LysoMC quenches the fluorescence of membrane-bound tryptophan by the F?rster mechanism with an apparent R(0) that is comparable to the thickness of the hydrocarbon core of a lipid bilayer (approximately 25 A). Consequently, the methylcoumarin acceptor predominantly quenches tryptophans that reside in the same monolayer as the probe. The topology of a peptide's tryptophan in membranes can be determined by comparing the quenching in symmetric and asymmetric lysoMC-labeled vesicles. Because it is essential to know that asymmetrically incorporated lysoMC remains so under all conditions, we also developed a second type of FRET experiment for assessing the rate of transbilayer diffusion (flip-flop) of lysoMC. Except in the presence of pore-forming peptides, there was no measurable flip-flop of lysoMC, indicating that asymmetric distributions of quencher are stable. We used these methods to show that N-acetyl-tryptophan-octylamide and tryptophan-octylester rapidly equilibrate across phosphatidylcholine (POPC) and phosphatidylglycerol (POPG) bilayers, while four amphipathic model peptides remain exclusively on the outer monolayer. The topology of the amphipathic peptide melittin bound to POPC could not be determined because it induced rapid flip-flop of lysoMC. Interestingly, melittin did not induce lysoMC flip-flop in POPG vesicles and was found to remain stably on the external monolayer.     

Comparative structural studies of Vpu peptides in phospholipid monolayers by x-ray scattering

Vpu is an 81-residue HIV-1 accessory protein, its transmembrane and cytoplasmic domains each responsible for one of its two functions. Langmuir monolayers of phospholipid incorporating a membrane protein with a unidirectional vectorial orientation, on a semiinfinite aqueous subphase, provide one "membranelike" environment for the protein. The cytoplasmic domain's interaction with the surface of the phospholipid monolayer in determining the tertiary structure of the peptide within the monolayer was investigated, employing a comparative structural study of Vpu with its submolecular fragments Tm and TmCy truncated to different extents in the cytoplasmic domain, via synchrotron x-ray scattering utilizing a new method of analysis. Localizations of the transmembrane and cytoplasmic domains within the monolayer profile structure were similar for all three proteins, the hydrophobic transmembrane helix within the hydrocarbon chain region tilted with respect to the monolayer plane and the helices of the cytoplasmic domains lying on the surface of the headgroups parallel to the monolayer plane. The thickness of the hydrocarbon chain region, determined by the tilt of the hydrocarbon chains and transmembrane domain with respect to the monolayer plane, was slightly different for Tm, TmCy, and Vpu systematically with protein/lipid mole ratio. Localization of the helices in the cytoplasmic domains of the three proteins relative to the headgroups depends on their extents and amphipathicities. Thus, the interaction of the cytoplasmic domain of Vpu on the surface may affect the tilt of the transmembrane helix within the hydrocarbon chain region in determining its tertiary structure in the membrane.     

Behavior of human apolipoprotein E in aqueous solutions and at interfaces

Human plasma apolipoprotein E (apo-E) strongly self-associates to form a stable tetramer in an aqueous solution at pH 7.4 containing 0.15 M NaCl. Tetramerized apo-E is abundant in alpha-helical conformation with an asymmetric molecular shape. Apo-E forms a stable monolayer at the air-water interface with a collapse pressure of 14 dynes/cm and with a limiting molecular area of 21 A2/amino acid. Under low surface pressure (less than 0.5 dyne/cm), it behaves as a monomer at the interface. It binds reversibly to the surface of phosphatidylcholine-coated triolein particles with a diameter of 26 nm from the aqueous phase in which most of the molecules are tetramerized. An apparent dissociation constant (Kd), 1.2 X 10(-6) M (monomeric molarity) or 40 mg/l, is substantially larger than those of the other apolipoproteins, while a binding saturation level (N), 0.8 amino acid/surface phospholipid, is equivalent to the N values of those proteins (Tajima, S., Yokoyama, S., and Yamamoto, A. (1983) J. Biol. Chem. 258, 10073-10082). Content of alpha-helix increases slightly when it is transferred from the aqueous phase to the lipid surface. The results are consistent with a model that amphiphilic alpha-helical conformation is responsible both for self-association and surface binding and suggest that apo-E may easily dissociate from the lipoprotein surface to form a self-associated soluble tetramer.     

Origins of delays in monolayer kinetics: phospholipase A2 paradigm

The interfacial kinetic paradigm is adopted to model the kinetic behavior of pig pancreatic phospholipase A(2) (PLA2) at the monolayer interface. A short delay of about a minute to the onset of the steady state is observed under all monolayer reaction progress conditions, including the PLA2-catalyzed hydrolysis of didecanoylphosphatidyl-choline (PC10) and -glycerol (PG10) monolayers as analyzed in this paper. This delay is independent of enzyme concentration and surface pressure and is attributed to the equilibration time by stationary diffusion of the enzyme added to the stirred subphase to the monolayer through the intervening unstirred aqueous layer. The longer delays of up to several hours, seen with the PC10 monolayers at >15 mN/m, are influenced by surface pressure as well as enzyme concentration. Virtually all features of the monolayer reaction progress are consistent with the assumption that the product accumulates in the substrate monolayer, although the products alone do not spread as a compressible monolayer. These results rule out models that invoke slow "activation" of PLA2 on the monolayer. The observed steady-state rate on monolayers after the delays is <1% of the rate observed with micellar or vesicles substrates of comparable substrate. Together these results suggest that the monolayer steady-state rate includes contributions from steps other than those of the interfacial turnover cycle. Additional considerations that provide understanding of the pre-steady-state behaviors and other nonideal effects at the surface are also discussed.     

Activation of protein kinase C in lipid monolayers

The potential of lipid monolayers spread at an air-water interface was investigated as a well defined membrane model able to support protein kinase C (PKC) association and activation. PKC association to a mixed phospholipid film (phosphatidylcholine, phosphatidylserine) could be detected by an increase of the monolayer surface pressure. This association was strikingly dependent upon the presence of submicromolar concentrations of Ca2+. The effect of Ca2+ resulted in an increase of the PKC penetration into the lipid core at a given permissive surface pressure as well as in a marked increase of the critical surface pressure (29-38 dynes/cm) above which the enzyme was excluded from the membrane. Inclusion of diacylglycerol or tetradecanoate phorbol acetate (TPA) did not modify the PKC-monolayer association in a detectable manner. PKC associated to the lipid layer exhibited the expected catalytic property and was fully activated when diacylglycerol or TPA was included in the membrane. PKC activity was highly dependent upon the surface pressure of the lipid monolayer, being optimal between 30 and 35 dynes/cm. Study of the compression isotherm of various diacylglycerol structures revealed that all potent PKC agonists exhibited an expanded liquid phase behavior with collapse pressure below 40 dynes/cm, in contrast to weak activators which showed condensed isotherms with high collapse pressure (approximately equal to 60 dynes/cm). These observations showed that the lipid monolayer system is well adapted to the study of the molecular mechanisms involved in the regulation of PKC activity at a model membrane interface. They are in line with the suggestion of a major role of Ca2+ in the association (translocation) of PKC to membrane in living cell and suggest that diacylglycerol (and TPA) might activate membrane-associated PKC through local change in the surrounding lipid phase organization.     

Regulation of cholesteryl oleate and triolein miscibility in monolayers and bilayers

The miscibility of triolein and cholesteryl oleate with 1-palmitoyl-2-oleoyl phosphatidylcholine was studied at the argon-buffer interface. The surface phase behavior of the system was analogous to that for cholesteryl ester-phospholipid mixtures in that both monolayer and double layer surface phases were formed. By considering the bulk properties of cholesteryl oleatetriolein mixtures and the two-dimensional phase rule, the entire system could be described. Double layer properties suggest that it consists of mostly triolein and phospholipid in the layer adjacent to the aqueous phase. The monolayer phase shows the formation of complexes between the neutral lipids and the phospholipid with stoichiometries nearly identical with those reported for bilayers (Hamilton, J. A., Miller, K. W., and Small, D. M. (1983) J. Biol. Chem. 258, 12821-12826). A second complex with a 3:1 stoichiometry is formed between triolein and cholesteryl oleate independently of interactions with phospholipid. Upon interaction with phospholipid, the triolein-cholesteryl oleate complex loses proportionately more area than either lipid alone. Because the area of complexes with phospholipid is constant, overall neutral lipid miscibility in such complexes is enhanced by the cholesteryl oleate-triolein interaction. Thus, our data explain the apparently nonideal mixing of cholesteryl oleate, triolein, and phospholipid in monolayers and in bilayers.