Effect of phosphatidylethanolamine on the properties of phospholipid-apolipoprotein complexes

Plasma high density lipoproteins (HDL) are synthesized in intestinal mucosal cells and hepatocytes and are secreted into the blood. Factors influencing the structure and function of these HDL, such as lipid and protein composition, are poorly understood. It appears, however, that intracellular, discoidal HDL are enriched, relative to plasma HDL, in phosphatidylethanolamine (PE), a phospholipid known to generate unusual, nonbilayer structures of putative physiological significance. Although incubation of dimyristoylphosphatidylcholine (DMPC) with apolipoprotein A-I at the gel-liquid crystalline phase transition temperature results in the spontaneous formation of lipid-protein complexes, the presence of proportionately small amounts of PE prevents the formation of such complexes, suggesting that PE profoundly alters the phase properties of the phospholipid bilayers. However, by using a detergent-mediated method for the formation of PE-rich model nascent HDL from phospholipids and apolipoprotein A-I, lipid-protein complexes containing as much as 75% DLPE could be formed, thus demonstrating that the presence of PE causes a kinetic, rather than a thermodynamic, barrier to spontaneous complex formation. The products contained a DLPE:DMPC molar ratio similar to that of the initial incubation mixture; however, as the mole percentage of DLPE increased, the products became less heterogeneous, the buoyant density of the products increased, and the Stokes diameter of the products decreased. Similar results were obtained when dimyristoylphosphatidylethanolamine (DMPE) and dipalmitoylphosphatidylethanolamine (DPPE) were employed in lieu of DLPE. Electron microscopy of complexes containing DLPE and DMPC at a 1:1 molar ratio showed that these particles possessed a discoidal, bilayer morphology similar to that seen with complexes containing only phosphatidylcholine.(ABSTRACT TRUNCATED AT 250 WORDS)     

Structural studies of apolipoprotein A-I/phosphatidylcholine recombinants by high-field proton NMR, nondenaturing gradient gel electrophoresis, and electron microscopy

Complexes formed between apolipoprotein A-I (apo A-I) and dimyristoylphosphatidylcholine (DMPC) or egg phosphatidylcholine have been studied by high-field 1H NMR, nondenaturing gradient gel electrophoresis, electron microscopy, and gel filtration chromatography. Emphasis has been placed on an analysis of the particle size distribution within the micellar complexes produced at lipid/protein molar ratios of 40-700. As determined by electron microscopy and gel filtration of DMPC/apo A-I complexes, the size of the discoidal micelles produced appears to increase uniformly with an increasing lipid/protein ratio. By electron microscopy, the diameters of isolated DMPC/apo A-I discoidal micelles range from approximately 89 A at a 40 molar ratio to 205 A at a 700 molar ratio. Analysis of the micellar complexes by 1H NMR shows that concomitant with the increase in size is the progressive downfield shift of the choline N-methyl proton resonance of the complex which is observed from 3.245 to 3.267 ppm over the above molar ratio range. The relationship between chemical shift and micelle size is most simply interpreted as arising from a weighted averaging of two lipid environments--lipid-lipid and lipid-protein. In contrast to the above interpretation of the gel filtration experiments on DMPC/apo A-I complexes, nondenaturing gradient gel electrophoresis analysis of particle size distribution leads to an unexpected observation: as the DMPC/apo A-I ratio increases, discrete complexes of increasing size are formed in an apparently quantized manner.(ABSTRACT TRUNCATED AT 250 WORDS)     

Reconstitution of apolipoprotein A-I from human high density lipoprotein with bovine brain sphingomyelin

Reconstitution of apolipoprotein A-I was found to occur readily with bovine brain sphingomyelin (BBSM), with a maximum rate occurring at a temperature of 28 degrees C, a temperature approximating the phase transition temperature for this naturally occurring phospholipid. At BBSM:A-I weight ratios of 7.5:1 or less, a single recombinant product was observed which contained three A-I molecules per particle, which had a BBSM:A-I molar ratio of 360 to 1 and which appeared in the electron microscope as a discoidal complex with a thickness of 68 A and a diameter of 217 A. By these criteria, as well as by gel filtration, this product appears very similar to that obtained by recombination of A-I with phosphatidylcholine at elevated ratios of phospholipid/protein. No evidence was found for the existence of any BBSM:A-I complexes comparable to the smaller lecithin:A-I complex containing 200-250 mol of phospholipid and two A-I molecules per complex which has been previously reported. At BBSM:A-I ratios of 15:1 (w/w), a new type of complex was observed which was discoidal by electron microscopy but possessed a larger diameter (390 A) and higher phospholipid:protein molar ratio (535:1) than has been observed previously for recombinant complexes. The BBSM:A-I complexes were found to be significantly more resistant to denaturation by guanidine hydrochloride than the dimyristoyl phosphatidylcholine:A-I recombinant complexes. It is concluded that the mechanisms of interaction between apolipoprotein A-I and either bovine brain sphingomyelin or phosphatidylcholines are similar, but that the nature of the protein-lipid interactions with BBSM are such as to produce larger and more stable complexes than are observed with the phosphatidylcholines.     

Transformation of large discoidal complexes of apolipoprotein A-I and phosphatidylcholine by lecithin-cholesterol acyltransferase

Using a cholate-dialysis recombination procedure, complexes of apolipoprotein A-I and synthetic phosphatidylcholine (1-palmitoyl-2-oleoylphosphatidylcholine (POPC) or dioleoylphosphatidylcholine (DOPC] were prepared in mixtures at a relatively high molar ratio of 150:1 phosphatidylcholine/apolipoprotein A-I. Particle size distribution analysis by gradient gel electrophoresis of the recombinant mixtures indicated the presence of a series of discrete complexes that included species migrating at RF values observed for discoidal particles in nascent high-density lipoproteins (HDL) in plasma of lecithin-cholesterol acyltransferase-deficient subjects. One of these complex species, designated complex class 6, formed with either phosphatidylcholine, was isolated by gel filtration and characterized at follows: discoidal shape (mean diameter 20.8 nm (POPC) and 19.0 nm (DOPC]; molar ratio, phosphatidylcholine/apolipoprotein A-I, 155:1 (POPC) and 130:1 (DOPC); and both containing 4 molecules of apolipoprotein A-I per particle. Incubation of class 6 complexes with lecithin-cholesterol acyltransferase (EC 2.3.1.43) and a source of unesterified cholesterol (low-density lipoprotein (LDL] was shown by electron microscopy to result in a progressive transformation of the discoidal particles (0 h) to deformable (2.5 h) and to spherical particles (24 h). The spherical particles (diameter 13.6 nm (POPC) and 12.5 nm (DOPC) exhibit sizes at the upper boundary of the interval defining the human plasma (HDL2b)gge (12.9-9.8 nm). The spherical particles contain a cholesteryl ester core that reaches a limiting molar ratio of approx. 50-55:1 cholesteryl ester/apolipoprotein A-I. The deformable particles assume a rectangular shape under negative staining and, relative to the 24-h spherical product, are enriched in phosphatidylcholine. Chemical crosslinking (by dimethyl suberimidate) of the isolated transformation products shows the 24-h spherical particle to contain predominantly 4 apolipoprotein A-I molecules; products produced after intermediate periods of time appear to contain species with 3 and 4 apolipoproteins per particle. Our in vitro studies indicate a potential pathway in the origins of large, apolipoprotein A-I-containing plasma HDL particles. The deformable species observed during transformation were similar in size and shape to particles observed in interstitial fluid.     

Mechanism of ATP-binding cassette transporter A1-mediated cellular lipid efflux to apolipoprotein A-I and formation of high density lipoprotein particles

The ATP-binding cassette transporter A1 (ABCA1) plays a critical role in the biogenesis of high density lipoprotein (HDL) particles and in mediating cellular cholesterol efflux. The mechanism by which ABCA1 achieves these effects is not established, despite extensive investigation. Here, we present a model that explains the essential features, especially the effects of ABCA1 activity in inducing apolipoprotein (apo) A-I binding to cells and the compositions of the discoidal HDL particles that are produced. The apo A-I/ABCA1 reaction scheme involves three steps. First, there is binding of a small regulatory pool of apo A-I to ABCA1, thereby enhancing net phospholipid translocation to the plasma membrane exofacial leaflet; this leads to unequal lateral packing densities in the two leaflets of the phospholipid bilayer. Second, the resultant membrane strain is relieved by bending and by creation of exovesiculated lipid domains. The formation of highly curved membrane surface promotes high affinity binding of apo A-I to these domains. Third, this pool of bound apo A-I spontaneously solubilizes the exovesiculated domain to create discoidal nascent HDL particles. These particles contain two, three, or four molecules of apo A-I and a complement of membrane phospholipid classes together with some cholesterol. A key feature of this mechanism is that membrane bending induced by ABCA1 lipid translocase activity creates the conditions required for nascent HDL assembly by apo A-I. Overall, this mechanism is consistent with the known properties of ABCA1 and apo A-I and reconciles many of the apparently discrepant findings in the literature.     

Mode of assembly of amphipathic helical segments in model high-density lipoproteins

The structure of discoidal apo A-I-phospholipid complexes, representing the metabolic precursors of mature high-density lipoprotein particles, was studied by a combination of both a theoretical and an experimental approach. The secondary structure of the complex was determined by circular dichroic measurements, while the relative orientation of the apo A-I helical segments and of the phospholipid acyl chains was determined by ATR infrared measurements. Fluorescence energy transfer between the tryptophan residues of apo A-I and fluorescent phospholipid probes yielded an estimation of the relative topography of the lipid and apolipoprotein components in discoidal and spherical particles. The theoretical approach consisted of the identification of the helical segments in various apo A-I species. These segments were then oriented at a lipid/water interface by minimization of their hydrophobic and hydrophilic transfer energies. The calculation of the hydrophobicity profiles along the axis of the helices leads to the identification of specific interactions between pairs of helices. The helices were further assembled together with the phospholipids by computer modelling, enabling an estimation of the dimensions of the complex. The combination of the experimental and theoretical results yielded a model for discoidal apolipoprotein-phospholipid complexes, in which the amphipathic helical segments are oriented along the edges of the discs. Such a model can be extended to the conversion of these complexes into mature spherical HDL, through the formation of a cholesteryl ester core.     

Novel changes in discoidal high density lipoprotein morphology: a molecular dynamics study

ApoA-I is a uniquely flexible lipid-scavenging protein capable of incorporating phospholipids into stable particles. Here we report molecular dynamics simulations on a series of progressively smaller discoidal high density lipoprotein particles produced by incremental removal of palmitoyloleoylphosphatidylcholine via four different pathways. The starting model contained 160 palmitoyloleoylphosphatidylcholines and a belt of two antiparallel amphipathic helical lipid-associating domains of apolipoprotein (apo) A-I. The results are particularly compelling. After a few nanoseconds of molecular dynamics simulation, independent of the starting particle and method of size reduction, all simulated double belts of the four lipidated apoA-I particles have helical domains that impressively approximate the x-ray crystal structure of lipid-free apoA-I, particularly between residues 88 and 186. These results provide atomic resolution models for two of the particles produced by in vitro reconstitution of nascent high density lipoprotein particles. These particles, measuring 95 angstroms and 78 angstroms by nondenaturing gradient gel electrophoresis, correspond in composition and in size/shape (by negative stain electron microscopy) to the simulated particles with molar ratios of 100:2 and 50:2, respectively. The lipids of the 100:2 particle family form minimal surfaces at their monolayer-monolayer interface, whereas the 50:2 particle family displays a lipid pocket capable of binding a dynamic range of phospholipid molecules.     

Reaction of lecithin: cholesterol acyltransferase with micellar substrates. Effect of particle sizes

Micellar, discoidal complexes were prepared from L-alpha-dipalmitoylphosphatidylcholine (DPPC) or egg phosphatidylcholine (egg-PC), cholesterol, and human apolipoprotein A-I by the cholate dialysis method. Reaction mixtures containing from 70:7:1 to 500:50:1, PC/cholesterol/apolipoprotein A-I (mol/mol) were fractionated by gel-filtration into various complex fractions. The isolated DPPC complexes ranged in size from 103 to 380 A in diameter, and in composition from 70:7:1 to 470:45:1, PC/cholesterol/apolipoprotein A-I (mol/mol), respectively. In contrast, the isolated egg-PC complexes only ranged in size from 105 to 214 A in diameter, and in composition from 65:5:1 to 153:17:1, PC/cholesterol/apolipoprotein A-I (mol/mol), respectively. Measurements of fluorescence wavelength maxima and fluorescence polarization of tryptophan residues of apolipoprotein A-I, in both series of complexes, revealed uniform spectral properties for all the egg-PC containing complexes. The DPPC complexes, on the other hand, had maxima in the fluorescence parameters for complexes with diameters around 200 A. When reacted with purified human lecithin:cholesterol acyltransferase, either at constant apolipoprotein A-I or at constant lipid concentration, all egg-PC complexes had very similar reaction rates, but the DPPC complex series exhibited major differences in reactivity. Minima in reaction rates occurred for DPPC complexes around 200 A in diameter, and optimal rates were observed with the small discoidal complexes (110 A in diameter). These reaction rates correlate well with the apolipoprotein A-I fluorescence properties and indicate that the apolipoprotein structure, reflected at the interface with phosphatidylcholine, may be the most important factor in determining complex reactivity with lecithin:cholesterol acyltransferase.     

The conformation of apolipoprotein A-I in discoidal and spherical recombinant high density lipoprotein particles. 13C NMR studies of lysine ionization behavior.

To elucidate the molecular details of how high density lipoprotein (HDL) microstructure affects the conformation of apolipoprotein (apo) A-I in various classes of HDL particles, apoA-I structure in homogeneous recombinant HDL (rHDL) complexes containing palmitoyl-oleoyl phosphatidylcholine (POPC) and cholesteryl oleate has been investigated by NMR spectroscopy of [13C]lysine-labeled apoA-I. All Lys residues in rHDL apoA-I were labeled with 13C by reductive methylation, and then their ionization behavior was characterized by 13C NMR spectroscopy. Four discoidal particles were prepared to contain from 64 to 256 molecules of POPC and 2 molecules of apoA-I; their major diameters ranged from 9.3 to 12.1 nm. (13CH3)2-Lys resonances from apoA-I in discoidal complexes exhibit six distinct chemical shifts at pH 10. The various Lys have pKa values ranging from 8.3 to 10.5, indicating that they exist in different microenvironments. More than 80% of the Lys residues in small (9.3 nm) discoidal particles titrate at a significantly lower pH than in the large (12.1 nm) discoidal particles. This indicates that apoA-I has a different conformation on the differently size discs. Two spherical particles were prepared with POPC:cholesteryl oleate:apoA-I molar stoichiometries of 56:16:2 and 232:84:4 and diameters of 7.4 and 12.6 nm, respectively. On spherical rHDL, apoA-I (13CH3)2-Lys resonances exhibit five distinct chemical shifts at pH 10. The titration behavior of apoA-I Lys residues is the same in small and large spherical particles, indicating that apoA-I conformation is similar on the two particles. The Lys microenvironments indicate that the conformation of apoA-I in discoidal complexes is dependent on particle size and that these conformations are substantially different from that of apoA-I on spherical complexes. Lys microenvironments in discoidal complexes differ from that of spherical complexes by 4 to 5 ysines which titrate with relatively low pKa values on discs. This reflects apparent differences in conformation in the NH2-terminal one-third of apoA-I on discs and spheres.     

Reaction of lecithin:cholesterol acyltransferase with micellar complexes of apolipoprotein A-I and phosphatidylcholine, containing variable amounts of cholesterol

In a continued investigation of lecithin:cholesterol acyltransferase reaction with micellar, discoidal complexes of phosphatidylcholine (PC) . cholesterol . apolipoprotein A-I (apo-A-I), we prepared well defined complexes with variable free cholesterol contents and examined their reactivity with purified enzyme. The complexes, prepared by the sodium cholate dialysis method, were fractionated into "small" and "large" classes by gel filtration of the reaction mixtures through a Bio-Gel A-5m column. The small complexes had egg-PC/cholesterol/apo-A-I molar ratios from 68:14:1 to 80:1:1, discoidal shapes with diameters around 114 (+/- 13) A and widths of 42 A by electron microscopy, and Stokes radii from 47 to 49 A corresponding to molecular weights near 2 X 10(5). The corresponding properties of the large complexes, isolated from samples with higher cholesterol contents, were egg-PC/cholesterol/apo-A-I molar ratios from 84:26:1 to 96:17:1, diameters of 161 (+/- 20) A, widths of 43 A, Stokes radii around 80 A, and estimated molecular weights in the vicinity of 5 X 10(5). Both types of complexes, when adjusted to equal apo-A-I concentrations, gave essentially identical initial reaction velocities with purified lecithin:cholesterol acyltransferase over a wide range of cholesterol concentrations (from 2 X 10(-7) to 4 X 10(-4) M), PC/cholesterol molar ratios (from 3:1 to 12:1), and quite different lipid fluidity conditions as detected by diphenylhexatriene fluorescence polarization. When complexes were adjusted to a constant cholesterol concentration, the initial velocities of the lecithin:cholesterol acyltransferase reaction followed Michaelis-Menten kinetics relative to the apo-A-I concentrations. Arrhenius plots of initial reaction rates for various complexes with variable cholesterol content and fluidity, measured at constant apo-A-I concentrations, gave identical temperature dependences with an average activation energy of 18.0 kcal/mol. These results strongly suggest that the cholesterol esterification on high density lipoprotein particles does not depend on their unesterified-cholesterol contents, PC/unesterified-cholesterol molar ratios, nor on the fluidity of their lipid domains.     

Characterization of discoidal complexes of phosphatidylcholine, apolipoprotein A-I and cholesterol by gradient gel electrophoresis

Complexes of egg yolk phosphatidylcholine and apolipoprotein A-I were prepared by a detergent (sodium cholate)-dialysis method and characterized by gradient gel electrophoresis, gel filtration, electron microscopy and chemical analysis. Multicomponent electrophoretic patterns were obtained indicating formation of at least eight classes of discoidal complexes. The relative contribution of the different classes to the electrophoretic pattern was a function of the molar ratio of phosphatidylcholine:apolipoprotein A-I in the interaction mixture. Molar ratios of phosphatidylcholine:apolipoprotein A-I in isolated complexes were strongly and positively correlated with disc diameter obtained by electron microscopy. Incorporation of unesterified cholesterol into phosphatidylcholine/apolipoprotein A-I interaction mixtures also resulted in formation of unique complexes but with considerably different particle size distributions relative to those observed in the absence of cholesterol. One common consequence of cholesterol incorporation into interaction mixtures of 87.5:1 and 150:1 molar ratio of phosphatidylcholine:apolipoprotein A-I was the disappearance of a major complex class with diameter of 10.8 nm and the appearance of a major component with diameter of approximately 8.8 nm. Electrophoretic patterns of cholesterol-containing complexes showed a strong similarity to patterns recently published for high density lipoproteins from plasma of lecithin:cholesterol acyltransferase-deficient subjects, suggesting that the complexes formed in vitro by the detergent-dialysis method may serve as appropriate models for investigation of the origins of the HDL particle size distribution.     

Defined apolipoprotein A-I conformations in reconstituted high density lipoprotein discs

We prepared and isolated defined, reconstituted high density lipoprotein (r-HDL) particles containing apolipoprotein A-I (apoA-I), palmitoyloleoylphosphatidylcholine, and cholesterol. The initial r-HDL were prepared by the sodium cholate method, then part of the preparation was depleted of phospholipid by exposure to LDL, and the resulting, stable r-HDL species were isolated by gel filtration. The isolated r-HDL were characterized in terms of their size, alpha-helix content, and the conformation of apoA-I as reported by the fluorescence properties of the tryptophan residues. Then the relative reactivity of the r-HDL with lecithin cholesterol acyltransferase was assessed. The isolated, discoidal r-HDL contained 2 and 3 apoA-I molecules/particle, and had 77 and 109 A diameters, respectively. Their spectral properties were essentially identical and were distinct from the larger particles in the class of r-HDL with 2 apoA-I molecules/particle (particles with diameters of 86 and 96 A). In addition, the reactivity of the 77 and 109 A particles with pure lecithin cholesterol acyltransferase was similar and about 10-fold lower than for the 86 and 96 A particles. We conclude that the stable, limiting r-HDL particles in each class (77 and 109 A) can arise from the larger particles of the same class by depletion of phospholipids. These limiting particles have very similar apoA-I conformations, with decreased alpha-helix contents and compact protein regions, that are very poor in activating lecithin cholesterol acyltransferase. Based on these results, we propose a model to explain the origin of the different classes and subclasses of the discoidal r-HDL particles.     

Formation of spherical, reconstituted high density lipoproteins containing both apolipoproteins A-I and A-II is mediated by lecithin:cholesterol acyltransferase

Previous studies have provided detailed information on the formation of spherical high density lipoproteins (HDL) containing apolipoprotein (apo) A-I but no apoA-II (A-I HDL) by an lecithin:cholesterol acyltransferase (LCAT)-mediated process. In this study we have investigated the formation of spherical HDL containing both apoA-I and apoA-II (A-I/A-II HDL). Incubations were carried out containing discoidal A-I reconstituted HDL (rHDL), discoidal A-II rHDL, and low density lipoproteins in the absence or presence of LCAT. After the incubation, the rHDL were reisolated and subjected to immunoaffinity chromatography to determine whether A-I/A-II rHDL were formed. In the absence of LCAT, the majority of the rHDL remained as either A-I rHDL or A-II rHDL, with only a small amount of A-I/A-II rHDL present. By contrast, when LCAT was present, a substantial proportion of the reisolated rHDL were A-I/A-II rHDL. The identity of the particles was confirmed using apoA-I rocket electrophoresis. The formation of the A-I/A-II rHDL was influenced by the relative concentrations of the precursor discoidal A-I and A-II rHDL. The A-I/A-II rHDL included several populations of HDL-sized particles; the predominant population having a Stokes' diameter of 9.9 nm. The particles were spherical in shape and had an electrophoretic mobility slightly slower than that of the alpha-migrating HDL in human plasma. The apoA-I:apoA-II molar ratio of the A-I/A-II rHDL was 0.7:1. Their major lipid constituents were phospholipids, unesterified cholesterol, and cholesteryl esters. The results presented are consistent with LCAT promoting fusion of the A-I rHDL and A-II rHDL to form spherical A-I/A-II rHDL. We suggest that this process may be an important source of A-I/A-II HDL in human plasma.     

Discoidal complexes containing apolipoprotein E and their transformation by lecithin-cholesterol acyltransferase

The primary objectives of this study were to determine whether analogs to native discoidal apolipoprotein (apo)E-containing high-density lipoproteins (HDL) could be prepared in vitro, and if so, whether their conversion by lecithin-cholesterol acyltransferase (LCAT; EC 2.3.1.43) produced particles with properties comparable to those of core-containing, spherical, apoE-containing HDL in human plasma. Complexes composed of apoE and POPC, without and with incorporated unesterified cholesterol, were prepared by the cholate-dialysis technique. Gradient gel electrophoresis showed that these preparations contain discrete species both within (14-40 nm) and outside (10.8-14 nm) the size range of discoidal apoE-containing HDL reported in LCAT deficiency. The isolated complexes were discoidal particles whose size directly correlated with their POPC:apoE molar ratio: increasing this ratio resulted in an increase in larger complexes and a reduction in smaller ones. At all POPC:apoE molar ratios, size profiles included a major peak corresponding to a discoidal complex 14.4 nm long. Preparations with POPC:apoE molar ratios greater than 150:1 contained two distinct groups of complexes, also in the size range of discoidal apoE-containing HDL from patients with LCAT deficiency. Incorporation of unesterified cholesterol into preparations (molar ratio of 0.5:1, unesterified cholesterol:POPC) resulted in component profiles exhibiting a major peak corresponding to a discoidal complex 10.9 nm long. An increase of unesterified cholesterol and POPC (at the 0.5:1 molar ratio) in the initial mixture, increased the proportion of larger complexes in the profile. Incubation of isolated POPC-apoE discoidal complexes (mean sizes, 14.4 and 23.9 nm) with purified LCAT and a source of unesterified cholesterol converted the complexes to spherical, cholesteryl ester-containing products with mean diameters of 11.1 nm and 14.0 nm, corresponding to apoE-containing HDL found in normal plasma. Conversion of smaller cholesterol-containing discoidal complexes (mean size, 10.9 nm) under identical conditions resulted in spherical products 11.3, 13.3, and 14.7 nm across. The mean sizes of these conversion products compared favorably with those (mean diameter, 12.3 nm) of apoE-containing HDL of human plasma. This conversion of cholesterol-containing complexes is accompanied by a shift of some apoE to the LDL particle size interval. Our study indicates that apoE-containing complexes formed by the cholate-dialysis method include species similar to discoidal apoE-containing HDL and that incubation with LCAT converts most of them to spherical core-containing particles in the size range of plasma apoE-containing HDL. Plasma HDL particles containing apoE may arise in part from direct conversion of discoidal apoE-containing HDL by LCAT.     

Characterization of nascent HDL particles and microparticles formed by ABCA1-mediated efflux of cellular lipids to apoA-I

The nascent HDL created by ABCA1-mediated efflux of cellular phospholipid (PL) and free (unesterified) cholesterol (FC) to apolipoprotein A-I (apoA-I) has not been defined. To address this issue, we characterized the lipid particles released when J774 mouse macrophages and human skin fibroblasts in which ABCA1 is activated are incubated with human apoA-I. In both cases, three types of nascent HDL containing two, three, or four molecules of apoA-I per particle are formed. With J774 cells, the predominant species have hydrodynamic diameters of approximately 9 and 12 nm. These discoidal HDL particles have different FC contents and PL compositions, and the presence of acidic PL causes them to exhibit alpha-electrophoretic mobility. These results are consistent with ABCA1 located in more than one membrane microenvironment being responsible for the production of the heterogeneous HDL. Activation of ABCA1 also leads to the release of apoA-I-free plasma membrane vesicles (microparticles). These larger, spherical particles released from J774 cells have the same PL composition as the 12 nm HDL and contain CD14 and ganglioside, consistent with their origin being plasma membrane raft domains. The various HDL particles and microparticles are created concurrently, and there is no precursor-product relationship between them. Importantly, a large fraction of the cellular FC effluxed from these cells by ABCA1 is located in microparticles. Collectively, these results show that the products of the apoA-I/ABCA1 interaction include discoidal HDL particles containing different numbers of apoA-I molecules. The cellular PLs and cholesterol incorporated into these nascent HDL particles originate from different cell membrane domains.     

Interaction of the alpha-helices of apolipophorin III with the phospholipid acyl chains in discoidal lipoprotein particles: a fluorescence quenching study.

Quenching of tryptophan fluorescence by nitroxide-labeled phospholipids and nitroxide-labeled fatty acids was used to investigate the lipid-binding domains of apolipophorin III. The location of the Trp residues relative to the lipid bilayer was investigated in discoidal lipoprotein particles made with 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine and five different single-Trp mutants of apoLp-III. A comparison of the quenching efficiencies of phospholipids containing nitroxide groups at the polar head, and at positions 5 and 16 of the sn-2 acyl chain, indicated that the protein is interacting with the acyl chains of the phospholipid along the periphery of the bilayer of the discoidal lipoprotein. N-Bromosuccinimide readily abolished 100% of the fluorescence of all Trp residues in the lipid-bound state. Larger quenching rates were observed for the Trp residues in helices 1, 4, and 5 than for those located in helices 2 and 3, suggesting differences between the interaction of these two groups of helices. However, the extent of Trp fluorescence quenching observed in lipoproteins made with any of the mutants was comparable to that reported for deeply embedded Trp residues, suggesting that all Trp residues interact with the phospholipid acyl chains. This study provides the first experimental evidence of a massive interaction of the alpha-helices of apoLp-III with the phospholipid acyl chains in discoidal lipoproteins. The extent of interaction deduced is consistent with the apolipoprotein adopting a highly extended conformation.     

Interaction of human plasma high-density lipoprotein HDL2b with discoidal complexes of dimyristoylphosphatidylcholine and apolipoprotein A-I

The interaction of HDL2b, a major subclass (d = 1.063 - 1.100 g/ml) of human plasma high-density lipoproteins, with discoidal complexes composed of dimyristoylphosphatidylcholine (DMPC) and apolipoprotein A-I (weight ratio, DMPC/apolipoprotein A-I (2.1 - 2.5:1); dimensions, 10.0 x 4.4 nm) was investigated. Incubation at 37 degrees C for 4.5 h of HDL2b with discoidal complexes resulted in a transfer of DMPC from the discoidal complexes to the HDL2b, a release of lipid-free apolipoprotein A-I from the discoidal complexes during such transfer, and a dissociation of some apolipoprotein A-I from the HDL2b surface. The number of discoidal complexes degraded during interaction with HDL2b depended on the initial molar ratio of HDL2b to discoidal complexes. Approximately one molecule of HDL2b was required for the degradation of one discoidal complex particle, and the degradation process appeared limited by the capacity of the HDL2b for uptake of DMPC. Degradation of discoidal complexes was also observed when human plasma LDL (d = 1.006-1.063 g/ml) was substituted for HDL2b in the interaction mixture.     

Comparative models for human apolipoprotein A-I bound to lipid in discoidal high-density lipoprotein particles

We have constructed a series of models for apolipoprotein A-I (apo A-I) bound to discoidal high-density lipoprotein (HDL) particles, based upon the molecular belt model [Segrest, J. P., et al. (1999) J. Biol. Chem. 274, 31755-31758] and helical hairpin models [Rogers, D. P., et al. (1998) Biochemistry 37, 11714-11725], and compared these with picket fence models [Phillips, J. C., et al. (1997) Biophys. J. 73, 2337-2346]. Molecular belt models for discoidal HDL particles with differing diameters are presented, illustrating that the belt model can explain the discrete changes in HDL particle size observed experimentally. Hairpin models are discussed for the binding of apo A-I to discoidal HDL particles with diameters identical to those for the molecular belt model. Two models are presented for the binding of three monomers of apo A-I to a 150 A diameter discoidal HDL particle. In one model, two monomers of apo A-I bind to the exterior of the HDL particle in an antiparallel belt, with a third monomer of apo A-I bound to the disk in a hairpin conformation. In the second model, all three monomers of apo A-I are bound to the discoidal HDL particle in a hairpin conformation. Previously published experimental data for each model are reviewed, with FRET favoring either the belt or hairpin models over the picket fence models for HDL particles with diameters of 105 A. Naturally occurring mutations appear to favor the belt model for the 105 A particles, while the 150 A HDL particles favor the presence of at least one hairpin.     

Properties of phosphatidylethanolamine-containing phospholipid-apolipoprotein complexes modified by lecithin-cholesterol acyltransferase

The effect of the inclusion of phosphatidylethanolamine (PE), a phospholipid with unusual packing properties, on the substrate properties of protein-lipid complexes toward lecithin-cholesterol acyltransferase (LCAT) has been studied. Recombinant particles of apolipoprotein A-I with dimyristoylphosphatidylcholine (DMPC), dilauroylphosphatidylethanolamine (DLPE) and cholesterol were prepared at a molar ratio of 1:140:14 (A-I/DMPC/cholesterol) or 1:70:70:14 (A-I/DMPC/DLPE/cholesterol); the efficiency of cholesterol incorporation into complexes containing phosphatidylethanolamine was found to be very pH-dependent, with enhanced cholesterol incorporation at elevated pH values. By incubating the complexes with either purified human LCAT or the d greater than 1.21 g/ml fraction of rat serum as a source of LCAT activity, it was found that a high degree of cholesterol esterification could be achieved with either complex; however, the DLPE-containing complex possessed a much smaller Stokes' diameter than the DMPC-only particle despite compositional similarities between these complexes. With respect to particle diameter the DLPE-containing particles behaved more like complexes prepared with egg yolk lecithin than did complexes prepared with DMPC alone. When human LDL was added to the incubations to provide a source of additional cholesterol, the products were markedly different. Concomitant with an increased cholesteryl ester core was an increase in the protein stoichiometry in both types of particles, from 2 to 3 or 4 apo A-I per particle. The proportion of DLPE to DMPC in the products was reduced from 1:1 to 0.3:1, reflecting a preferential hydrolysis of PE by LCAT, and the Stokes' diameters of the DMPC-only and the DLPE-containing complexes were closely similar. We conclude that the presence of elevated proportions of certain phospholipid species may significantly alter both the physical properties of the particles and their substrate properties with regard to reactions with enzymes of lipid metabolism.     

Remodeling of apolipoprotein E-containing spherical reconstituted high density lipoproteins by phospholipid transfer protein

Phospholipid transfer protein (PLTP) transfers phospholipids between HDL and other lipoproteins in plasma. It also remodels spherical, apolipoprotein A-I (apoA-I)-containing HDL into large and small particles in a process involving the dissociation of lipid-free/lipid-poor apoA-I. ApoE is another apolipoprotein that is mostly associated with large, spherical HDL that do not contain apoA-I. Three isoforms of apoE have been identified in human plasma: apoE2, apoE3, and apoE4. This study investigates the remodeling of spherical apoE-containing HDL by PLTP and the ability of PLTP to transfer phospholipids between apoE-containing HDL and phospholipid vesicles. Spherical reconstituted high density lipoproteins (rHDL) containing apoA-I [(A-I)rHDL], apoE2 [(E2)rHDL], apoE3 [(E3)rHDL], or apoE4 [(E4)rHDL] as the sole apolipoprotein were prepared by incubating discoidal rHDL with low density lipoproteins and lecithin:cholesterol acyltransferase. PLTP remodeled the spherical, apoE-containing rHDL into large and small particles without the dissociation of apoE. The PLTP-mediated remodeling of apoE-containing rHDL was more extensive than that of (A-I)rHDL. PLTP transferred phospholipids from small unilamellar vesicles to apoE-containing rHDL in an isoform-dependent manner, but at a rate slower than that for spherical (A-I)rHDL. It is concluded that apoE enhances the capacity of PLTP to remodel HDL but reduces the ability of HDL to participate in PLTP-mediated phospholipid transfers.