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Apolipoprotein (apo) A-I-containing nascent HDL particles produced by the ATP binding cassette transporter A1 have different sizes and compositions. To understand the molecular basis for this heterogeneity, the HDL particles produced by apoA-I-mediated solubilization of phospholipid (PL)/free (unesterified) cholesterol (FC) bilayer membranes in cell and cell-free systems are compared. Incubation of apoA-I with ATP binding cassette transporter A1-expressing baby hamster kidney cells leads to formation of two populations of FC-containing discoidal nascent HDL particles. The larger 11-nm diameter particles are highly FC-enriched (FC/PL = 1.2/1 mol/mol) relative to the smaller 8 nm particles and the cell plasma membrane (FC/PL = 0.4/1). ApoA-I-mediated spontaneous solubilization of either multilamellar or unilamellar vesicles made of a membrane-PL mixture and FC yields discoidal HDL particles with diameters in the range 9-17 nm and, as found with the cell system, the larger particles are relatively enriched in FC despite the fact that all particles are created by solubilization of a common FC/PL membrane domain. The size-dependent distribution of FC among HDL particles is due to varying amounts of PL being sequestered in a boundary layer by interaction with apoA-I at the disc edge. The presence of a relatively large boundary layer in smaller discoidal HDL promotes preferential distribution of phosphatidylserine to such particles. However, phosphatidylcholine and sphingomyelin which are the primary PL constituents of nascent HDL do not exhibit selective incorporation into HDL discs of different sizes. This understanding of the mechanisms responsible for the heterogeneity in lipid composition of nascent HDL particles may provide a basis for selecting subspecies with preferred cardio-protective properties.

A number of naturally occurring mutations of apolipoprotein (apo) A-I, the major protein of HDL, are known to be associated with hereditary amyloidosis and atherosclerosis. Here, we examined the effects of the G26R point mutation in apoA-I (apoA-I(Iowa)) on the structure, stability, and aggregation propensity to form amyloid fibril of full-length apoA-I and the N-terminal fragment of apoA-I. Circular dichroism and fluorescence measurements demonstrated that the G26R mutation destabilizes the N-terminal helix bundle domain of full-length protein, leading to increased hydrophobic surface exposure, whereas it has no effect on the initial structure of the N-terminal 1-83 fragment, which is predominantly a random coil structure. Upon incubation for extended periods at neutral pH, the N-terminal 1-83 variants undergo a conformational change to β-sheet-rich structure with a great increase in thioflavin T fluorescence, whereas no structural change is observed in full-length proteins. Comparison of fibril-forming propensity among substituted mutants at Gly-26 position of 1-83 fragments demonstrated that the G26R mutation enhances the nucleation step of fibril formation, whereas G26K and G26E mutations have small or inhibiting effects on the formation of fibrils. These fibrils of the 1-83 variants have long and straight morphology as revealed by atomic force microscopy and exhibited significant toxicity with HEK293 cells. Our results indicate dual critical roles of the arginine residue at position 26 in apoA-I(Iowa): destabilization of the N-terminal helix bundle structure in full-length protein and enhancement of amyloid fibril formation by the N-terminal 1-83 fragment.

The principal protein of high density lipoprotein (HDL), apolipoprotein (apo) A-I, in the lipid-free state contains two tertiary structure domains comprising an N-terminal helix bundle and a less organized C-terminal domain. It is not known how the properties of these domains modulate the formation and size distribution of apoA-I-containing nascent HDL particles created by ATP-binding cassette transporter A1 (ABCA1)-mediated efflux of cellular phospholipid and cholesterol. To address this issue, proteins corresponding to the two domains of human apoA-I (residues 1-189 and 190-243) and mouse apoA-I (residues 1-186 and 187-240) together with some human/mouse domain hybrids were examined for their abilities to form HDL particles when incubated with either ABCA1-expressing cells or phospholipid multilamellar vesicles. Incubation of human apoA-I with cells gave rise to two sizes of HDL particles (hydrodynamic diameter, 8 and 10 nm), and removal or disruption of the C-terminal domain eliminated the formation of the smaller particle. Variations in apoA-I domain structure and physical properties exerted similar effects on the rates of formation and sizes of HDL particles created by either spontaneous solubilization of phospholipid multilamellar vesicles or the ABCA1-mediated efflux of cellular lipids. It follows that the sizes of nascent HDL particles are determined at the point at which cellular phospholipid and cholesterol are solubilized by apoA-I; apparently, this is the rate-determining step in the overall ABCA1-mediated cellular lipid efflux process. The stability of the apoA-I N-terminal helix bundle domain and the hydrophobicity of the C-terminal domain are important determinants of both nascent HDL particle size and their rate of formation.

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.

The interaction of apolipoprotein E (apoE) with cell-surface heparan sulfate proteoglycans is an important step in the uptake of lipoprotein remnants by the liver. ApoE interacts predominantly with heparin through the N-terminal binding site spanning the residues around 136-150. In this work, surface plasmon resonance analysis was employed to investigate how amphipathic alpha-helix properties and basic residue organization in this region modulate binding of apoE to heparin. The apoE/heparin interaction involves a two-step process; apoE initially binds to heparin with fast association and dissociation rates, followed by a step exhibiting much slower kinetics. Circular dichroism and surface plasmon resonance experiments using a disulfide-linked mutant, in which opening of the N-terminal helix bundle was prevented, demonstrated that there is no major secondary or tertiary structural change in apoE upon heparin binding. Mutations of Lys-146, a key residue for the heparin interaction, greatly reduced the favorable free energy of binding of the first step without affecting the second step, suggesting that electrostatic interaction is involved in the first binding step. Although lipid-free apoE2 tended to bind less than apoE3 and apoE4, there were no significant differences in rate and equilibrium constants of binding among the apoE isoforms in the lipidated state. Discoidal apoE3-phospholipid complexes using a substitution mutant (K143R/K146R) showed similar binding affinity to wild type apoE3, indicating that basic residue specificity is not required for the effective binding of apoE to heparin, unlike its binding to the low density lipoprotein receptor. In addition, disruption of the alpha-helix structure in the apoE heparin binding region led to an increased favorable free energy of binding in the second step, suggesting that hydrophobic interactions contribute to the second binding step. Based on these results, it seems that cell-surface heparan sulfate proteoglycan localizes apoE-enriched remnant lipoproteins to the vicinity of receptors by fast association and dissociation.

The influence of apolipoprotein (apo) A-I structure on ABCA1-mediated efflux of cellular unesterified (free) cholesterol (FC) and phospholipid (PL) is not well understood. To address this issue, we used a series of apoA-I mutants to examine the contributions of various domains in the molecule to ABCA1-mediated FC and PL efflux from mouse J774 macrophages and human skin fibroblasts. Irrespective of the cell type, deletion or disruption of the C-terminal lipid-binding domain of apoA-I drastically reduced the FC and PL efflux ( approximately 90%), indicating that the C-terminal amphipathic alpha-helix is required for high affinity microsolubilization of FC and PL. Deletion in the N-terminal region of apoA-I also reduced the lipid efflux ( approximately 30%) and increased the K(m) about 2-fold compared with wild type apoA-I, whereas deletion of the central domain (Delta123-166) had no effect on either K(m) or V(max). These results indicate that ABCA1-mediated lipid efflux is relatively insensitive to the organization of the apoA-I N-terminal helix-bundle domain. Alterations in apoA-I structure caused parallel changes in its ability to bind to a PL bilayer and to induce efflux of FC and PL. Overall, these results are consistent with a two-step model for ABCA1-mediated lipid efflux. In the first step, apoA-I binds to ABCA1 and hydrophobic alpha-helices in the C-terminal domain of apoA-I insert into the region of the perturbed PL bilayer created by the PL transport activity of ABCA1, thereby allowing the second step of lipidation of apoA-I and formation of nascent high density lipoprotein particles to occur.

The apolipoprotein A-I mimetic peptide 4F (Ac-DWFKAFYDKVAEKFKEAF-NH(2)), with four Phe residues on the nonpolar face of the amphipathic alpha-helix, is strongly anti-inflammatory, whereas two 3F analogs (3F(3) and 3F(14)) are not. To understand how changes in helix nonpolar face structure affect function, two additional 3F analogs, Ac-DKLKAFYDKVFEWAKEAF-NH(2) (3F-1) and Ac-DKWKAVYDKFAEAFKEFL-NH(2) (3F-2), were designed using the same amino acid composition as 3F(3) and 3F(14). The aromatic residues in 3F-1 and 3F-2 are near the polar-nonpolar interface and at the center of the nonpolar face of the helix, respectively. Like 4F, but in contrast to 3F(3) and 3F(14), these peptides effectively inhibited lytic peptide-induced hemolysis, oxidized phospholipid-induced monocyte chemotaxis, and scavenged lipid hydroperoxides from low density lipoprotein. High pressure liquid chromatography retention times and monolayer exclusion pressures indicated that there is no direct correlation of peptide function with lipid affinity. Fluorescence studies suggested that, although the peptides bind phospholipids similarly, the Trp residue in 4F, 3F-1, and 3F-2 is less motionally restricted than in 3F(3) and 3F(14). Based on these results and molecular modeling studies, we propose that the arrangement of aromatic residues in class A amphipathic helical molecules regulates entry of reactive oxygen species into peptide-phospholipid complexes, thereby reducing the extent of monocyte chemotaxis, an important step in atherosclerosis.

Apolipoprotein (apo) A-I is thought to undergo a conformational change during lipid association that results in the transition of random coil to alpha-helix. Using a series of deletion mutants lacking different regions along the molecule, we examined the contribution of alpha-helix formation in apoA-I to the binding to egg phosphatidylcholine (PC) small unilamellar vesicles (SUV). Binding isotherms determined by gel filtration showed that apoA-I binds to SUV with high affinity and deletions in the C-terminal region markedly decrease the affinity. Circular dichroism measurements demonstrated that binding to SUV led to an increase in alpha-helix content, but the helix content was somewhat less than in reconstituted discoidal PC.apoA-I complexes for all apoA-I variants, suggesting that the helical structure of apoA-I on SUV is different from that in discs. Isothermal titration calorimetry showed that the binding of apoA-I to SUV is accompanied by a large exothermic heat and deletions in the C-terminal regions greatly decrease the heat. Analysis of the rate of release of heat on binding, as well as the kinetics of quenching of tryptophan fluorescence by brominated PC, indicated that the opening of the N-terminal helix bundle is a rate-limiting step in apoA-I binding to the SUV surface. Significantly, the correlation of thermodynamic parameters of binding with the increase in the number of helical residues revealed that the contribution of alpha-helix formation upon lipid binding to the enthalpy and the free energy of the binding of apoA-I is -1.1 and -0.04 kcal/mol per residue, respectively. These results indicate that alpha-helix formation, especially in the C-terminal regions, provides the energetic source for high affinity binding of apoA-I to lipids.

Human apolipoprotein E (apoE) mediates high affinity binding to the low density lipoprotein receptor when present on a lipidated complex. In the absence of lipid, however, apoE does not bind the receptor. Whereas the x-ray structure of lipid-free apoE3 N-terminal (NT) domain is known, the structural organization of its lipid-associated, receptor-active conformation is poorly understood. To study the organization of apoE amphipathic alpha-helices in a lipid-associated state, single tryptophan-containing apoE3 variants were employed in fluorescence quenching studies. The relative positions of the Trp residues with respect to the phospholipid component of apoE/lipid particles were established from the degree of quenching by phospholipids bearing nitroxide groups at various positions along their fatty acyl chains. Four apoE3-NT variants bearing Trp reporter groups at positions 141, 148, 155, or 162 within helix 4 and two apoE3 variants containing single Trp at positions 257 or 264 in the C-terminal (CT) domain, were reconstituted into phospholipid-containing discoidal complexes. Parallax analysis revealed that each engineered Trp residue in helix 4 of apoE3-NT, as well as those in the CT domain of apoE, localized approximately 5 A from the center of the bilayer. Circular dichroism studies revealed that lipid association induces additional helix formation in apoE. Protease protection assays suggest the flexible loop segment between the NT and CT domains may transition from unstructured to helix upon lipid association. Taken together, these data support a model wherein the alpha-helices in the receptor-binding region and the CT domain of apoE align perpendicular to the fatty acyl chains of the phospholipid bilayer. In this alignment, the residues of helix 4 are arrayed in a positively charged, curved helical segment for optimal receptor interaction.

Scavenger receptor (SR)-BI catalyzes the selective uptake of cholesteryl ester (CE) from high density lipoprotein (HDL) by a two-step process that involves the following: 1) binding of HDL to the receptor and 2) diffusion of the CE molecules into the cell plasma membrane. We examined the effects of the size of discoidal HDL particles containing wild-type (WT) apoA-I on selective uptake of CE and efflux of cellular free (unesterified) cholesterol (FC) from COS-7 cells expressing SR-BI to determine the following: 1) the influence of apoA-I conformation on the lipid transfer process, and 2) the contribution of receptor binding-dependent processes to the overall efflux of cellular FC. Large (10 nm diameter) reconstituted HDL bound to SR-BI better (B(max) approximately 420 versus 220 ng of apoA-I/mg cell protein), delivered more CE, and promoted more FC efflux than small ( approximately 8 nm) particles. When normalized to the number of reconstituted HDL particles bound to the receptor, the efficiencies of either CE uptake or FC efflux with these particles were the same indicating that altering the conformation of WT apoA-I modulates binding to the receptor (step 1) but does not change the efficiency of the subsequent lipid transfer (step 2); this implies that binding induces an optimal alignment of the WT apoA-I.SR-BI complex so that the efficiency of lipid transfer is always the same. FC efflux to HDL is affected both by binding of HDL to SR-BI and by the ability of the receptor to perturb the packing of FC molecules in the cell plasma membrane.

The mechanism of formation of high density lipoprotein (HDL) particles by the action of ATP-binding cassette transporter A1 (ABCA1) is not defined completely. To address this issue, we monitored efflux to apoA-I of phosphatidylcholine (PC), sphingomyelin (SM), and unesterified (free) cholesterol (FC) from J774 macrophages, in which ABCA1 is up-regulated, and investigated the nature of the particles formed. The various apoA-I/lipid particles appearing in the extracellular medium were separated by gel filtration chromatography. The presence of apoA-I in the extracellular medium led to the simultaneous formation of more than one type of poorly lipidated apoA-I-containing particle: there were 9- and 12-nm diameter particles containing approximately 3:1 and 1:1 phospholipid/FC (mol/mol), respectively, which were present together with 6-nm monomeric apoA-I. Removal of the C-terminal alpha-helix (residues 223-243) of apoA-I reduced phospholipid and FC efflux and prevented formation of the 9- and 12-nm HDL particles; the apoA-I variant formed larger particles that eluted in the void volume. FC loading of the J774 cells also led to the formation of larger apoA-I-containing particles that were highly enriched in FC. Besides creating HDL particles, ABCA1 mediated release of larger (20-450-nm diameter) FC-rich particles that were not involved in HDL formation and that are probably membrane vesicles. These particles contained 1:1 PC/SM in contrast to the HDL particles, which contained 2:1 PC/SM. This is consistent with lipid raft and non-raft plasma membrane domains being involved primarily in ABCA1-mediated vesicle release and nascent HDL formation, respectively.

ApoE exists as three common isoforms, apoE2, apoE3, and apoE4; apoE2 and apoE3 preferentially bind to high density lipoproteins, whereas apoE4 prefers very low density lipoproteins (VLDL). To understand the molecular basis for the different lipoprotein distributions of these isoforms in human plasma, we examined the lipid-binding properties of the apoE isoforms and some mutants using lipid emulsions. With both large (120 nm) and small (35 nm) emulsion particles, the binding affinity of apoE4 was much higher than that of apoE2 and apoE3, whereas the maximal binding capacities were similar among the three isoforms. The 22-kDa N-terminal fragment of apoE4 displayed a much higher binding capacity than did apoE2 and apoE3. The apoE4(E255A) mutant, which has no electrostatic interaction between Arg61 and Glu255, showed binding behavior similar to that of apoE3, indicating that N- and C-terminal domain interaction in apoE4 is responsible for its high affinity for lipid. In addition, the apoE3(P267A) mutant, which is postulated to contain a long alpha-helix in the C-terminal domain, had significantly decreased binding capacities for both sizes of emulsion particle, suggesting that the apoE4 preference for VLDL is not due to a stabilized long alpha-helical structure. Isothermal titration calorimetry measurements showed that there is no significant difference in thermodynamic parameters for emulsion binding among the apoE isoforms. However, fluorescence measurements of 8-anilino-1-naphthalenesulfonic acid binding to apoE indicated that apoE4 has more exposed hydrophobic surface compared with apoE3 mainly due to the different tertiary organization of the C-terminal domain. The less organized structure in the C-terminal domain of apoE4 leads to the higher affinity for lipid, contributing to its preferential association with VLDL. In fact, we found that apoE4 binds to VLDL with higher affinity compared with apoE3.

Detailed structural information on human exchangeable apolipoproteins (apo) is required to understand their functions in lipid transport. Using a series of deletion mutants that progressively lacked different regions along the molecule, we probed the structural organization of lipid-free human apoA-I and the role of different domains in lipid binding, making comparisons to apoE, which is a member of the same gene family and known to have two structural domains. Measurements of alpha-helix content by CD in conjunction with tryptophan and 8-anilino-1-naphthalenesulfonic acid fluorescence data demonstrated that deletion of the amino-terminal or central regions disrupts the tertiary organization, whereas deletion of the carboxyl terminus has no effect on stability and induces a more cooperative structure. These data are consistent with the lipid-free apoA-I molecule being organized into two structural domains similar to apoE; the amino-terminal and central parts form a helix bundle, whereas the carboxyl-terminal alpha-helices form a separate, less organized structure. The binding of the apoA-I variants to lipid emulsions is modulated by reorganization of the helix bundle structure, because the rate of release of heat on binding is inversely correlated with the stability of the helix bundle. Based on these observations, we propose that there is a two-step mechanism for lipid binding of apoA-I: apoA-I initially binds to a lipid surface through amphipathic alpha-helices in the carboxyl-terminal domain, followed by opening of the helix bundle in the amino-terminal domain. Because apoE behaves similarly, this mechanism is probably a general feature for lipid interaction of other exchangeable apolipoproteins, such as apoA-IV.

Apolipoprotein (apo) E mediates lipoprotein remnant clearance via interaction with cell-surface heparan sulfate proteoglycans. Both the 22-kDa N-terminal domain and 10-kDa C-terminal domain of apoE contain a heparin binding site; the N-terminal site overlaps with the low density lipoprotein receptor binding region and the C-terminal site is undefined. To understand the molecular details of the apoE-heparin interaction, we defined the microenvironments of all 12 lysine residues in intact apoE3 and examined their relative contributions to heparin binding. Nuclear magnetic resonance measurements showed that, in apoE3-dimyristoyl phosphatidylcholine discs, Lys-143 and -146 in the N-terminal domain and Lys-233 in the C-terminal domain have unusually low pK(a) values, indicating high positive electrostatic potential around these residues. Binding experiments using heparin-Sepharose gel demonstrated that the lipid-free 10-kDa fragment interacted strongly with heparin and a point mutation K233Q largely abolished the binding, indicating that Lys-233 is involved in heparin binding and that an unusually basic lysine microenvironment is critical for the interaction with heparin. With lipidated apoE3, it is confirmed that the Lys-233 site is completely masked and the N-terminal site mediates heparin binding. In addition, mutations of the two heparin binding sites in intact apoE3 demonstrated the dominant role of the N-terminal site in the heparin binding of apoE even in the lipid-free state. These results suggest that apoE interacts predominately with cell-surface heparan sulfate proteoglycans through the N-terminal binding site. However, Lys-233 may be involved in the binding of apoE to certain cell-surface sites, such as the protein core of biglycan.

This study elucidates the factors underlying the enhancement in efflux of human fibroblast unesterified cholesterol and phospholipid (PL) by lipid-free apolipoprotein (apo) A-I that is induced by cholesterol enrichment of the cells. Doubling the unesterified cholesterol content of the plasma membrane by incubation for 24 h with low density lipoprotein and lipid/cholesterol dispersions increases the pools of PL and cholesterol available for removal by apoA-I from about 0.8-5%; the initial rates of mass release of cholesterol and PL are both increased about 6-fold. Expression of the ATP binding cassette transporter A1 (ABCA1) is critical for this increased efflux of lipids, and cholesterol loading of the fibroblasts over 24 h increases ABCA1 mRNA about 12-fold. The presence of more ABCA1 and cholesterol in the plasma membrane results in a 2-fold increase in the level of specific binding of apoA-I to the cells with no change in binding affinity. Characterization of the species released from either control or cholesterol-enriched cells indicates that the plasma membrane domains from which lipids are removed are cholesterol-enriched with respect to the average plasma membrane composition. Cholesterol enrichment of fibroblasts also affects PL synthesis, and this leads to enhanced release of phosphatidylcholine (PC) relative to sphingomyelin (SM); the ratios of PC to SM solubilized from control and cholesterol-enriched fibroblasts are approximately 2/1 and 5/1, respectively. Biosynthesis of PC is critical for this preferential release of PC and the enhanced cholesterol efflux because inhibition of PC synthesis by choline depletion reduces cholesterol efflux from cholesterol-enriched cells. Overall, it is clear that enrichment of fibroblasts with unesterified cholesterol enhances efflux of cholesterol and PL to apoA-I because of three effects, 1) increased PC biosynthesis, 2) increased PC transport via ABCA1, and 3) increased cholesterol in the plasma membrane.

Scavenger receptor (SR)-BI is the first molecularly defined receptor for high density lipoprotein (HDL) and it can mediate the selective uptake of cholesteryl ester into cells. To elucidate the molecular mechanisms by which SR-BI facilitates lipid uptake, we examined the connection between lipid donor particle binding and lipid uptake using kidney COS-7 cells transiently transfected with SR-BI. We systematically compared the uptake of [(3)H]cholesteryl oleoyl ether (CE) and [(14)C]sphingomyelin (SM) from apolipoprotein (apo) A-I-containing reconstituted HDL (rHDL) particles and apo-free lipid donor particles. Although both types of lipid donor could bind to SR-BI, only apo-containing lipid donors exhibited preferential delivery of CE over SM (i.e. nonstoichiometric lipid uptake). In contrast, apo-free lipid donor particles (phospholipid unilamellar vesicles, lipid emulsion particles) gave rise to stoichiometric lipid uptake due to interaction with SR-BI. This apparent whole particle uptake was not due to endocytosis, but rather fusion of the lipid components of the lipid donor with the cell plasma membrane; this process is perhaps mediated by a fusogenic motif in the extracellular domain of SR-BI. The interaction of apoA-I with SR-BI not only prevents fusion of the lipid donor with the plasma membrane but also allows the optimal selective lipid uptake. A comparison of rHDL particles containing apoA-I and apoE-3 showed that while both particles bound equally well to SR-BI, the apoA-I particle gave approximately 2-fold greater CE selective uptake. Catabolism of all major HDL lipids can occur via SR-BI with the relative selective uptake rate constants for CE, free cholesterol, triglycerides (triolein), and phosphatidylcholine being 1, 1.6, 0.7, and 0.2, respectively. It follows that a putative nonpolar channel created by SR-BI between the bound HDL particle and the cell plasma membrane is better able to accommodate the uptake of neutral lipids (e.g. cholesterol) relative to polar phospholipids.

Apolipoprotein (apo) E contains two structural domains, a 22-kDa (amino acids 1-191) N-terminal domain and a 10-kDa (amino acids 223-299) C-terminal domain. To better understand apoE-lipid interactions on lipoprotein surfaces, we determined the thermodynamic parameters for binding of apoE4 and its 22- and 10-kDa fragments to triolein-egg phosphatidylcholine emulsions using a centrifugation assay and titration calorimetry. In both large (120 nm) and small (35 nm) emulsion particles, the binding affinities decreased in the order 10-kDa fragment approximately 34-kDa intact apoE4 > 22-kDa fragment, whereas the maximal binding capacity of intact apoE4 was much larger than those of the 22- and 10-kDa fragments. These results suggest that at maximal binding, the binding behavior of intact apoE4 is different from that of each fragment and that the N-terminal domain of intact apoE4 does not contact lipid. Isothermal titration calorimetry measurements showed that apoE binding to emulsions was an exothermic process. Binding to large particles is enthalpically driven, and binding to small particles is entropically driven. At a low surface concentration of protein, the binding enthalpy of intact apoE4 (-69 kcal/mol) was approximately equal to the sum of the enthalpies for the 22- and 10-kDa fragments, indicating that both the 22- and 10-kDa fragments interact with lipids. In a saturated condition, however, the binding enthalpy of intact apoE4 (-39 kcal/mol) was less exothermic and rather similar to that of each fragment, supporting the hypothesis that only the C-terminal domain of intact apoE4 binds to lipid. We conclude that the N-terminal four-helix bundle can adopt either open or closed conformations, depending upon the surface concentration of emulsion-bound apoE.

Defective binding of apolipoprotein E (apoE) to heparan sulfate proteoglycans (HSPGs) is associated with increased risk of atherosclerosis due to inefficient clearance of lipoprotein remnants by the liver. The interaction of apoE with HSPGs has also been implicated in the pathogenesis of Alzheimer's disease and may play a role in neuronal repair. To identify which residues in the heparin-binding site of apoE and which structural elements of heparan sulfate interact, we used a variety of approaches, including glycosaminoglycan specificity assays, (13)C nuclear magnetic resonance, and heparin affinity chromatography. The formation of the high affinity complex required Arg-142, Lys-143, Arg-145, Lys-146, and Arg-147 from apoE and N- and 6-O-sulfo groups of the glucosamine units from the heparin fragment. As shown by molecular modeling, using a high affinity binding octasaccharide fragment of heparin, these findings are consistent with a binding mode in which five saccharide residues of fully sulfated heparan sulfate lie in a shallow groove of the alpha-helix that contains the HSPG-binding site (helix 4 of the four-helix bundle of the 22-kDa fragment). This groove is lined with residues Arg-136, Ser-139, His-140, Arg-142, Lys-143, Arg-145, Lys-146, and Arg-147. In the model, all of these residues make direct contact with either the 2-O-sulfo groups of the iduronic acid monosaccharides or the N- and 6-O-sulfo groups of the glucosamine sulfate monosaccharides. This model indicates that apoE has an HSPG-binding site highly complementary to heparan sulfate rich in N- and O-sulfo groups such as that found in the liver and the brain.

Lysines in apolipoprotein (apo) E are key factors in the binding of apoE to the low density lipoprotein receptor, and high affinity binding requires that apoE be associated with lipid. To gain insight into this effect, we examined the microenvironments of the eight lysines in the 22-kDa fragment of apoE3 (residues 1-191) in the lipid-free and lipid-associated states. As shown by (1)H,(13)C heteronuclear single quantum coherence nuclear magnetic resonance, lysine resonances in the lipid-free fragment were poorly resolved over a wide pH range, whereas in apoE3.dimyristoyl phosphatidylcholine (DMPC) discs, the lysine microenvironments and protein conformation were significantly altered. Sequence-specific assignments of the lysine resonances in the spectrum of the lipidated 22-kDa fragment were made. In the lipid-free protein, six lysines could be resolved, and all had pK(a) values above 10. In apoE3.DMPC complexes, however, all eight lysines were resolved, and the pK(a) values were 9.2-11.1. Lys-143 and Lys-146, both in the receptor binding region in helix 4, had unusually low pK(a) values of 9.5 and 9.2, respectively, likely as a result of local increases in positive electrostatic potential with lipid association. Shift reagent experiments with potassium ferricyanide showed that Lys-143 and Lys-146 were much more accessible to the ferricyanide anion in the apoE3.DMPC complex than in the lipid-free state. The angle of the nonpolar face of helix 4 is smaller than the angles of helices 1, 2, and 3, suggesting that helix 4 cannot penetrate as deeply into the DMPC acyl chains at the edge of the complex and that its polar face protrudes from the edge of the disc. This increased exposure and the greater positive electrostatic potential created by interaction with DMPC may explain why lipid association is required for high affinity binding of apoE to the low density lipoprotein receptor.

Scavenger receptor, class B, type I (SR-BI) mediates the selective uptake of high density lipoprotein (HDL) cholesteryl ester without the uptake and degradation of the particle. In transfected cells SR-BI recognizes HDL, low density lipoprotein (LDL) and modified LDL, protein-free lipid vesicles containing anionic phospholipids, and recombinant lipoproteins containing apolipoprotein (apo) A-I, apoA-II, apoE, or apoCIII. The molecular basis for the recognition of such diverse ligands by SR-BI is unknown. We have used direct binding analysis and chemical cross-linking to examine the interaction of murine (m) SR-BI with apoA-I, the major protein of HDL. The results show that apoA-I in apoA-I/palmitoyl-oleoylphosphatidylcholine discs, HDL(3), or in a lipid-free state binds to mSR-BI with high affinity (K(d) congruent with 5-8 microgram/ml). ApoA-I in each of these forms was efficiently cross-linked to cell surface mSR-BI, indicating that direct protein-protein contacts are the predominant feature that drives the interaction between HDL and mSR-BI. When complexed with dimyristoylphosphatidylcholine, the N-terminal and C-terminal CNBr fragments of apoA-I each bound to SR-BI in a saturable, high affinity manner, and each cross-linked efficiently to mSR-BI. Thus, mSR-BI recognizes multiple sites in apoA-I. A model class A amphipathic alpha-helix, 37pA, also showed high affinity binding and cross-linking to mSR-BI. These studies identify the amphipathic alpha-helix as a recognition motif for SR-BI and lead to the hypothesis that mSR-BI interacts with HDL via the amphipathic alpha-helical repeat units of apoA-I. This hypothesis explains the interaction of SR-BI with a wide variety of apolipoproteins via a specific secondary structure, the class A amphipathic alpha-helix, that is a common structural motif in the apolipoproteins of HDL, as well as LDL.

Despite extensive studies and characterizations of the high density lipoprotein-cholesteryl ester (HDL-CE)-selective uptake pathway, the mechanisms by which the hydrophobic CE molecules are transferred from the HDL particle to the plasma membrane have remained elusive, until the discovery that scavenger receptor BI (SR-BI) plays an important role. To elucidate the molecular mechanism, we examined the quantitative relationships between the binding of HDL and the selective uptake of its CE in the murine adrenal Y1-BS1 cell line. A comparison of concentration dependences shows that half-maximal high affinity cell association of HDL occurs at 8.7 +/- 4.7 micrograms/ml and the Km of HDL-CE-selective uptake is 4.5 +/- 1.5 micrograms/ml. These values are similar, and there is a very high correlation between these two processes (r2 = 0.98), suggesting that they are linked. An examination of lipid uptake from reconstituted HDL particles of defined composition and size shows that there is a non-stoichiometric uptake of HDL lipid components, with CE being preferred over the major HDL phospholipids, phosphatidylcholine and sphingomyelin. Comparison of the rates of selective uptake of different classes of phospholipid in this system gives the ranking: phosphatidylserine > phosphatidylcholine approximately phosphatidylinositol > sphingomyelin. The rate of CE-selective uptake from donor particles is proportional to the amount of CE initially present in the particles, suggesting a mechanism in which CE moves down its concentration gradient from HDL particles docked on SR-BI into the cell plasma membrane. The activation energy for CE uptake from either HDL3 or reconstituted HDL is about 9 kcal/mol, indicating that HDL-CE uptake occurs via a non-aqueous pathway. HDL binding to SR-BI allows access of CE molecules to a "channel" formed by the receptor from which water is excluded and along which HDL-CE molecules move down their concentration gradient into the cell plasma membrane.

Lipid-free apolipoprotein (apo) A-I contributes to the reverse transport of cholesterol from the periphery to the liver by solubilizing plasma membrane phospholipid and cholesterol. The features of the apolipoprotein required for this process are not understood and are addressed in the current study. Membrane microsolubilization of human fibroblasts is not specific for apo A-I; unlipidated apos A-II, C, and E incubated with the fibroblast monolayers at a saturating concentration of 50 micrograms/ml are all able to release cholesterol and phospholipid similarly. To determine the properties of the apolipoprotein that drive the process, apo A-I peptides spanning the entire sequence of the protein were utilized; the peptides correspond to the 11- and 22-residue amphipathic alpha-helical segments, as well as adjacent combinations of the helices. Of the 20 helical peptides examined, only peptides representing the N-and C-terminal portions of the protein had the ability to solubilize phospholipid and cholesterol. Cholesterol efflux to the most effective peptides, 44-65 and 209-241, was approximately 50 and 70%, respectively, of that to intact apo A-I. Deletion mutants of apo E and apo A-I were constructed that have reduced lipid binding affinities as compared with the intact molecule. The proteins, apo A-I (Delta222-243), apo A-I (Delta190-243), apo E3 (Delta192-299) and apo E4 (Delta192-299) all exhibited a decreased ability to remove cellular cholesterol and phospholipid. These decreases correlated with the reduced ability of these proteins to penetrate into a phospholipid monomolecular film. Overall, the results indicate that insertion of amphipathic alpha-helices between the plasma membrane phospholipid molecules is a required step in the mechanism of apolipoprotein-mediated cellular lipid efflux. Therefore the lipid binding ability of the apolipoprotein is critical for efficient membrane microsolubilization.

The role of HDL and its major protein constituent, apolipoprotein (apo) A-I, in promoting the removal of excess cholesterol from cultured cells has been well established; however, the mechanisms by which this occurs are not completely understood. To address the effects of apoA-I modification on cellular unesterified (free) cholesterol (FC) efflux, three recombinant human apoA-I deletion mutants and plasma apoA-I were combined with 1-palmitoyl-2-oleoyl phosphatidylcholine (POPC) and FC to make reconstituted high density lipoprotein (rHDL) discoidal complexes. These particles were characterized structurally and for their efficiency as acceptors of mouse L-cell fibroblast cholesterol. The deletion mutant proteins lacked NH2-terminal (apoA-I (Delta44-126)), central (apoA-I (Delta139-170)), or COOH-terminal (apoA-I (Delta190-243)) domains of apoA-I. The three deletion mutants all displayed lipid-binding abilities and formed discoidal complexes that were similar in major diameter (13.2 +/- 1.5 nm) to those formed by human apoA-I when reconstituted at a 100:5:1 (POPC:FC:protein) mole ratio. Gel filtration profiles indicated unreacted protein in the preparation made with apoA-I (Delta190-243), which is consistent with the COOH terminus portion of apoA-I being an important determinant of lipid binding. Measurements of the percent alpha-helix content of the proteins, as well as the number of protein molecules per rHDL particle, gave an indication of the arrangement of the deletion mutant proteins in the discoidal complexes. The rHDL particles containing the deletion mutants had more molecules of protein present than particles containing intact apoA-I, to the extent that a similar number of helical segments was incorporated into each of the discoidal species. Comparison of the experimentally determined number of helical segments with an estimate of the available space indicated that the deletion mutant proteins are probably more loosely arranged than apoA-I around the edge of the rHDL. The abilities of the complexes to remove radiolabeled FC were compared in experiments using cultured mouse L-cell fibroblasts. All four discoidal complexes displayed similar abilities to remove FC from the plasma membrane of L-cells when compared at an acceptor concentration of 50 microg of phospholipid/ml. Thus, none of the deletions imposed in this study notably altered the ability of the rHDL particles to participate in cellular FC efflux. These results suggest that efficient apoA-I-mediated FC efflux requires the presence of amphipathic alpha-helical segments but is not dependent on specific helical segments.

Alterations in high density lipoprotein (HDL) composition that occur in dyslipidemic states may modulate a number of events involved in cholesterol homeostasis. To elucidate the details of how HDL-core composition can affect the molecular structure of different kinds of HDL particles, the conformation and stability of apoA-I have been investigated in homogeneous recombinant HDL particles (LpA-I) containing palmitoyloleoyl phosphatidylcholine (POPC), triolein (TG), and/or cholesteryl linoleate (CE). In a discoidal particle containing two molecules of apoA-I and 85 molecules of POPC, apoA-I exhibits an alpha-helix content of 70% and a free energy of stability of its alpha-helical segments (delta G0D) of 2.2 kcal/mol. Inclusion of eight molecules of TG into the complex significantly reduces the alpha-helix content and stability of apoA-I, whereas inclusion of four molecules of CE into the complex has an opposite effect in that the alpha-helix content is significantly reduced and the stability of the remaining alpha-helical structure of apoA-I is increased. Neutral lipids have a different effect on apoA-I conformation in spherical LpA-I particles. In a sonicated-spherical LpA-I particle containing two molecules of apoA-I and 70 molecules of POPC, apoA-I exhibits an alpha-helix content of about 60% and a delta G0D of 1.2 kcal/mol apoA-I. Inclusion of either 10 molecules of TG or six molecules of CE into such a particle increases both the alpha-helix content and stability of apoA-I. Increasing the CE/TG ratio in LpA-I particles that contain both neutral lipids enhances the stability of the alpha-helical segments. ApoA-I molecules tend to dissociate and cause particle instability when delta G0D for the lipid-bound alpha-helices is less than that for helices in the lipid-free state. The stabilities of both discoidal and spherical LpA-I particles are relatively low when the only neutral lipid present is TG but the particle stability is enhanced by the presence of CE molecules. Such dissociation of apoA-I molecules from LpA-I particles that have a low CE/TG ratio would be promoted in the hypertriglyceridemic state in vivo.

Several subspecies of human high density lipoprotein (HDL) have been shown to exist, and particle size is one parameter that can be used to distinguish them. Recently, a small HDL subspecies has been described that may be a particularly efficient acceptor of peripheral cell unesterified (free) cholesterol (FC). To address the effects of particle size on the ability of HDL to remove FC from cells, homogeneous, well defined HDL particles were reconstituted (rHDL) that varied in particle diameter within the size range of human HDL particles (7-13 nm). The abilities of each of these particles to remove cellular FC from mouse L-cells and rat Fu5AH hepatoma cells were compared on the basis of their phospholipid (PL) content as well as on a per particle basis. The effect of particle size was also examined using small unilamellar vesicles (SUV) of 25 nm in diameter and large unilamellar vesicles (LUVs) of 70-180 nm in diameter. The SUV were prepared by sonication, and the LUVs were prepared by extrusion techniques. The FC efflux efficiency of these particles (in order of decreasing efficiency) was: rHDL > SUV > LUV when compared on the basis of acceptor PL content across a range of concentrations (i.e. at a given PL concentration for these three acceptor classes, smaller particles were more efficient). The FC efflux differences between the rHDL and the vesicles were not due to the absence of apolipoprotein in the vesicles. No difference was detected among the rHDL of varying size, nor was a difference detected among the LUVs of varying size when compared on the basis of PL content. When the FC efflux data for rHDL and LUVs were normalized on the basis of the number of acceptor particles present at a given PL concentration, a correlation was found between acceptor particle radius and the ability to accept cellular FC with larger particles being the most efficient. However, the dependence of the rate of FC efflux on acceptor particle size was not quantitatively the same within the rHDL and LUV classes of acceptor particles. The dependence of FC efflux on acceptor particle size may reflect differing abilities of the variously sized acceptor particles to access the region very close to the cell plasma membrane where most of the FC removal is expected to occur.

The plasma cholesteryl ester transfer protein (CETP) mediates the transfer of neutral lipids between lipoproteins and is associated with high density lipoproteins (HDL). To understand the mechanism of interaction of CETP with HDL, we studied the binding of pure recombinant CETP to 1-palmitoyl-2-oleoylphosphatidylcholine (POPC)/apoA-I discoidal particles. Separating bound from free CETP using native gradient gel electrophoresis, complexes of CETP with 10-nm hydrodynamic diameter discoidal particles migrated with a diameter of 12-16 nm, compared with approximately 7.5 nm for CETP. At lower ratios of CETP to discs, CETP bound to discs without displacement of apoA-I. CETP alone was unable to generate discoidal complexes. Cross-linking and fluorescence resonance energy transfer experiments indicated that CETP bound to discs as monomers. Cross-linking of CETP to apoA-I in discs suggested proximity of apoA-I and CETP. By negative-stain electron microscopy, discoidal complexes containing CETP and CETP monoclonal antibody showed localization of antibody molecules to the disc edge, suggesting that CETP was bound to the disc edge. The binding of CETP to discs of different composition or size was studied. Discs (10-nm Stokes diameter) prepared with either apoA-I or apoA-II had a similar Kd (120 nM). Inclusion of 1 mol % cholesteryl oleate, 5 mol % cholesterol, or 6 mol % phosphatidylinositol increased the binding affinity of CETP 3-10 times (20-30 nM). In comparison, plasma HDL3 had a Kd of approximately 450 nM. For POPC/apoA-I discs, 10-nm discs bound CETP with much higher affinity than smaller 7.8-nm discs (Kd = 1-2 microM). 7.7-nm hydrodynamic diameter POPC/apoA-I spherical particles containing either triolein or cholesteryl oleate in their core bound CETP with higher affinity (Kd = 50-100 nM) than 7.8-nm POPC/apoA-I discs. Thus, CETP appears to bind to the perimeter of discoidal particles, possibly in a process in which flexible segments in apoA-I or apoA-II accommodate CETP at the disc edge. The binding of CETP to HDL is markedly influenced by overall particle size and shape and by lipid composition, and the increased binding affinity for cholesterol- and cholesteryl ester-containing discs suggests a higher affinity of CETP for nascent than mature HDL.

High density lipoprotein (HDL) phospholipid (PL) fatty acyl chain composition has been proposed to affect the ability of HDL to participate in the first step of reverse cholesterol transport. To examine the effects of PL fatty acid chain length and degree of unsaturation in this process, reconstituted HDL (rHDL) particles were made with human apolipoprotein (apo) A-I and PL containing fatty acid chains from 14 to 18 carbons in length, which were either fully saturated or unsaturated in one or both chains. These particles were characterized structurally and for their ability to promote free (unesterified) cholesterol (FC) efflux from cells growing in culture. The discoidal rHDL particles were homogeneous and exhibited similar hydrodynamic diameters (10.4 +/- 1.0 nm) indicating that apoA-I forms similarly sized discs with a variety of PL. Measurements of particle surface charge, apoA-I alpha-helix content, and conformational stability indicated that the conformation of apoA-I varies among the particles. These conformational effects on apoA-I are consistent with the PL fluidity influencing the interaction between the amphipathic alpha-helical segments and PL acyl chains. Differential scanning calorimetry demonstrated that the physical state of the rHDL PL at 37 degrees C varied according to acyl chain length and degree of unsaturation; the FC efflux efficiencies for particles with PL in either the gel or liquid crystal states were determined. The ability of the rHDL to accept cellular FC depended on the physical state of the PL in the rHDL. Liquid crystal PL formed the most efficient FC acceptor particles exhibiting a maximal efflux velocity (Vmax) of 12-14% release of total cellular FC per h. Gel-phase PL formed inefficient rHDL acceptors with a Vmax of about 3%/h. A similar hierarchy of FC efflux efficiency was noted when either mouse L-cells or rat Fu5AH hepatoma cells were used as the FC donors. Furthermore, this hierarchy was found to be due to the characteristics of the PL and not due to variable apoA-I conformation because protein-free, small unilamellar vesicles made with the same PL exhibited similar relative efflux capabilities. Generally, the ability of a given rHDL particle to accept cellular FC was related to rHDL PL acyl chain length and degree of unsaturation; decreases in PL acyl chain length and increases in chain unsaturation tended to result in more efficient FC acceptor particles.(ABSTRACT TRUNCATED AT 400 WORDS)

Exchangeable apolipoproteins possess tandem repeating units of class A amphipathic helical segments and many of them are linked together by proline residues. To understand the optimal arrangement of the amphipathic helixes for lipid association, we have studied the interactions of three model class A amphipathic helical peptides with lipids. The three peptides are: 37pA, a dimer of 18A (DWLKAFYDKVAEKLKEAF) linked together by a Pro (18A-Pro-18A); 37aA, a dimer of 18A linked together by an Ala (18A-Ala-18A); and 36A, a dimer of 18A without any linker residue (18A-18A). Circular dichroism (CD) spectra showed that the peptides are predominantly alpha-helical in aqueous and lipid environments. Temperature dependent CD studies indicated that in buffer helix stability decreases in the order 36A > 37aA > 37pA; however, in the presence of dimyristoyl phosphatidylcholine (DMPC), the above order is reversed. The retention times of the peptides on a C18 reversed-phase high performance liquid chromatography column decreased in the order 36A > 37aA > 37pA, consistent with the lengths of the nonpolar faces of the alpha-helixes being in the same order; the retention time of the parent 18A was shorter than 37pA. While 37pA adsorbed to egg phosphatidylcholine monolayers most strongly, the degree and rate of association of 36A were significantly lower. Differential scanning calorimetry indicated that, while 37pA was most effective in reducing the enthalpy of the gel to liquid-crystalline phase transition of DMPC multilamellar vesicles, 36A was least effective; 36A was even less effective than 18A. Fluorescence quenching experiments with iodide and acrylamide indicated that, in the presence of DMPC, Trp residues in 36A are most exposed to the quenchers while in 37pA they are least exposed. In the presence of DMPC, shielding of Trp in 18A from the quenchers was more than that observed with Trp residues in 36A. The results of this study suggest that the arrangement of tandem repeating amphipathic helical units which results in the formation of a class A amphipathic helix with a nonpolar face longer than five or six turns reduces the ability of the helix to associate with phospholipid.

The influence of apolipoprotein conformation on the ability of high density lipoprotein (HDL) to remove cellular free cholesterol (FC) has not been studied in detail. To address the effects of amphipathic alpha-helix structure on cellular FC efflux, three class A helical peptides and apolipoprotein (apo) AI were complexed to dimyristoyl phosphatidylcholine (DMPC) to make discoidal complexes that were used as acceptors of cell cholesterol. The peptides consisted of an 18-amino acid, amphipathic, alpha-helical peptide with the sequence DWLKAFYDKVAEKLKEAF (18A), a dimer of 18A covalently linked by a proline residue (37pA), and acetyl-18A-amide (Ac-18A-NH2) that has a higher alpha-helix content than the unblocked 18A molecule. The three peptides strongly mimic the lipid-binding characteristics of the amphipathic segments of apolipoproteins and form discoidal complexes with DMPC that are similar in diameter (11-12 nm) to those formed by human apoAI when reconstituted at a 2.5:1 (w:w) phospholipid to protein ratio. The abilities of these complexes to remove radiolabeled FC were compared in experiments using cultured mouse L-cell fibroblasts; efflux of FC from both the plasma membrane and the lysosomal pools was examined. For each of the acceptors, the removal of cholesterol from the plasma membrane and lysosomal pools was equally efficient. All four discoidal complexes were equally efficient cell membrane FC acceptors when compared at saturating acceptor concentrations of > 200 micrograms of DMPC/ml of medium. However, at the same lipid concentration, protein-free DMPC small unilamellar vesicles (SUV) were significantly less efficient. The initial rates of FC removal from cells at saturating concentrations of acceptor particles (Vmax) were 12, 10, 10, and 11% per h, respectively, for the complexes containing either 18A, Ac-18A-NH2, 37pA, or apoAI, but only 1% cellular FC per h for the DMPC SUV. The 10-fold higher Vmax for the apoprotein/peptide-containing acceptors was likely due to a reversible interaction of apoprotein or peptide with the plasma membrane that changed the lipid packing characteristics in such a way as to increase the rate of FC desorption from the cell surface. This interaction required amphipathic alpha-helical segments, but it was not affected by the length, number, or lipid-binding affinity of the helices. Furthermore, the efflux efficiency was not dependent on the amino acid sequence of the helical segments which suggests that this interaction is not mediated by a specific cell surface binding site.(ABSTRACT TRUNCATED AT 400 WORDS)

Several subspecies of human high density lipoprotein (HDL) exist, and particle surface charge is one parameter that can be used to distinguish them. For instance, pre-beta HDL has a lower negative surface charge than the bulk of plasma HDL resulting in slower migration when subjected to electrophoresis in an agarose gel at pH 8.6. The molecular basis for the variations in HDL particle surface charge have been established in this work. Quantitative analysis of electrophoretic mobilities in agarose gels indicates that the surface potentials of reconstituted pre-beta HDL and alpha-HDL3 are -7.6 and -11.4 mV, respectively. The difference of 3.8 mV corresponds to an apparent 1e more net negative charge on alpha-migrating HDL3. The contributions of the lipid and protein components to the charge of HDL3 were defined using reconstituted particles (rHDL) containing various combinations of HDL3 protein and lipid. The surface potentials of spherical and discoidal rHDL are not affected by the particle apoprotein composition. Thin layer chromatography of the HDL3 phospholipid fraction from five normolipidemic subjects revealed that it consists of approximately 84% phosphatidylcholine, 12% sphingomyelin, and 4% phosphatidylinositol (PI) by weight. PI significantly affects the charge of discoidal rHDL and is responsible for approximately 0.7 mV of the surface potential difference between pre-beta- and alpha-HDL. Reconstitution of spherical complexes containing apolipoprotein AI, palmitoyl-oleoyl phosphatidylcholine, and HDL3 neutral lipid esters showed that particles containing a neutral lipid core migrate to an alpha position in an agarose gel. The change in particle shape accounts for approximately 3 mV of the difference in surface potential between pre-beta and alpha-HDL. Overall, the charge of HDL particles is determined by 1) a direct contribution of negative charge from PI molecules in the surface of the lipoprotein and 2) the conformation of the resident apolipoprotein(s) which is influenced by the presence of neutral lipids and the particle shape. This quantitative understanding of surface charge provides a basis for understanding variations in function of HDL subspecies.

The effects of cholesterol on the conformation and net charge of apoA-I have been investigated in homogeneous recombinant high density lipoprotein (HDL) particles. ApoA-I charge and structure in discoidal recombinant HDL complexes containing palmitoyloleoylphosphatidylcholine and cholesterol have been quantitated by guanidine HCl denaturation, circular dichroism, electrokinetic analysis, and NMR spectroscopy of [13C]lysine-labeled apoA-I. In a discoidal particle containing 2 molecules of apoA-I and 160 molecules of palmitoyloleoylphosphatidylcholine, apoA-I exhibits an alpha-helix content of 75%, and the particle has a net negative surface charge of -5.2e/mol of apoA-I at pH 8.6. Addition of 2 molecules of cholesterol to this complex has no significant effect upon particle size, but slightly decreases the net charge (-5.0e) and alpha-helix content (68%) of apoA-I and enhances the stability of the helical segments, as reflected by an increase in the free energy of unfolding from 2.9 to 3.5 kcal/mol. In contrast, increasing the cholesterol content to 20 molecules/particle progressively increases particle size and apoA-I net negative charge (-6.1e), and there is a concomitant reduction in the free energy of stabilization of the alpha-helical structure in apoA-I to 2.2 kcal/mol. (13CH3)2-Lys resonances from apoA-I in discoidal recombinant HDL exhibit six chemical shifts at pH 10; these peaks originate from dimethyl-Lys residues that have pKa values ranging from 8.4 to 10.3. The titration behavior of apoA-I Lys residues is generally similar in the presence and absence of cholesterol, except that 4 Lys residues titrate at a significantly higher pH in the presence of cholesterol. These data are consistent with cholesterol having a direct effect on apoA-I conformation and charge in HDL. Structural changes of this magnitude can affect the interactions between HDL and various plasma proteins and cell surfaces. It is therefore likely that the cholesterol content of HDL plays an important role in regulating the metabolism of this lipoprotein.

Lysine (Lys) residues in apolipoprotein (apo) E are known to be involved in binding of apoE-containing lipoproteins to the low density lipoprotein (LDL) receptor. To examine the microenvironments of the Lys residues of apoE-3 in a variety of lipid-associated states, we have used a high resolution 13C-NMR method in which Lys were reductively methylated with [13C] formaldehyde. Over a wide pH range, the spectrum of apoE in canine HDLc, a spherical lipoprotein particle, exhibited two peaks from Lys epsilon-amino groups. The two pools of Lys in HDLc titrate with pK alpha values of 10.4 ("normal") and 9.3 ("active"). In contrast, eight epsilon-[13CH3]2Lys peaks (delta = 42.5-44.5 parts/million) with pK alpha values ranging from 8.2 to 10.1 and 7.8 to 10.5 were observed at pH 9.5 for human and canine apoE, respectively, in discoidal complexes with dimyristoyl glycerophosphocholine. A single Lys microenvironment was observed for apoE present in a disordered, lipid-free, state in 8 M urea, confirming the fact that the lipid environment is modulating the conformation of apoE. The above data demonstrate that the conformation of apoE, as reflected by the Lys microenvironments, on spherical HDLc particles is different from that on discoidal complexes.

The details of how high density lipoprotein (HDL) microstructure affects the conformation and net charge of apolipoprotein (apo) A-I in various classes of HDL particles have been investigated in homogeneous recombinant HDL (rHDL) particles containing apoA-I, palmitoyl-oleoyl phosphatidylcholine (POPC) and cholesteryl oleate. Isothermal denaturation with guanidine HCl was used to monitor alpha-helix structural stability, whereas electrokinetic analyses and circular dichroism were used to determine particle charge and apoA-I secondary structure, respectively. Electrokinetic analyses show that at pH 8.6 apoA-I has a net negative charge on discoidal (POPC.apoA-I) particles (-5.2 electronic units/mol of apoA-I) which is significantly greater than that of apoA-I either free in solution or on spherical (POPC.cholesteryl oleate.apoA-I) rHDL (approximately -3.5 electronic units). Raising the POPC content (32-128 mol/ml of apoA-I) of discoidal particles 1) increases the particle major diameter from 9.3 to 12.1 nm, 2) increases the alpha-helix content from 62 to 77%, and 3) stabilizes the helical segments by increasing the free energy of unfolding (delta GD degree) from 1.4 to 3.0 kcal/mol of apoA-I. Raising the POPC content (28-58 mol/mol of apoA-I) of spherical particles 1) increases the particle diameter from 7.4 to 12.6 nm, 2) increases the percent alpha-helix from 62 to 69%, and 3) has no significant effect on delta GD degree (2.2 kcal/mol of apoA-I). This study shows that different HDL subspecies maintain particular apoA-I conformations that confer unique charge and structural characteristics on the particles. It is likely that the charge and conformation of apoA-I are critical molecular properties that modulate the metabolism of HDL particles and influence their role in cholesterol transport.

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.

We have demonstrated previously that HDL-mediated efflux of plasma membrane cholesterol is independent of specific binding of apolipoproteins to the high density lipoprotein (HDL) receptor in either control or cholesterol-enriched cells (Karlin, J. B., Johnson, W. J., Benedict, C. R., Chacko, G. K., Phillips, M. C., and Rothblat, G. H. (1987) J. Biol. Chem. 262, 12557-12564 and Johnson, W. J., Mahlberg, F. H., Chacko, G. K., Phillips, M. C., and Rothblat, G. H. (1988) J. Biol. Chem. 263, 14099-14106). The present studies were conducted to determine if the process for removal of intracellular (lysosomal) cholesterol is similar to that of membrane cholesterol or if, in contrast, it is selectively regulated by specific apolipoproteins of HDL. For these reasons, we examined the influence of each of the major apolipoproteins of human HDL, apoAI, apoAII, and apoCs on the metabolism of membrane and lysosomal cholesterol in a macrophage foam cell model. We developed an experimental system which allows, for the first time, the simultaneous determination of lysosomal hydrolysis of cholesteryl ester and efflux and esterification of both lysosomal and membrane cholesterol. J774 and elicited mouse peritoneal macrophages were loaded with cholesteryl ester within lysosomes through phagocytosis of sonicated lipid droplets. Membrane and lysosomal pools of cholesterol were differentially radiolabeled. Discoidal complexes of egg phosphatidylcholine and purified apolipoproteins having a similar size and composition were used as cholesterol acceptors. Our results demonstrate that lysosomal hydrolysis of cholesteryl ester is independent of the presence of extracellular acceptors. Lysosomal production of cholesterol stimulates the esterification by acyl-CoA:cholesterol acyltransferase of membrane and lysosomal cholesterol. All the particles tested induce the efflux of both pools of cholesterol at a similar ratio. As efflux is stimulated, esterification by acyl-CoA:cholesterol acyltransferase is reduced. We conclude that none of these apolipoproteins selectively influences the efflux or the esterification of membrane of lysosomal cholesterol. In addition, we observe that particles containing apoAI are the most efficient acceptors, but this effect is not linked to specific binding to the HDL receptor.

Familial defective apoB-100 is a genetic mutation that is characterized by abnormal low density lipoprotein (LDL) and moderate hypercholesterolemia. Heterozygotes for this disorder possess two populations of LDL. One has normal receptor binding, and the other, which can be isolated by monoclonal antibody 19 immunoaffinity chromatography, has almost no binding activity. The mutation that disrupts binding is a Gln for Arg substitution of apoB-100 residue 3500. NMR spectra of LDL containing (13CH3)2Lys residues show that chemically modified Lys exist in two microenvironments. In normal human LDL, there are about 50 Lys with pK 8.9 and 170 Lys with pK 10.5; an upper limit of 10 pK 8.9 Lys may be particularly involved in binding to the LDL receptor. Examination of the mixture of normal LDL and mutant LDL from five patients shows that the latter have fewer pK 8.9 Lys. In purified defective LDL at least seven Lys are redistributed from the active to normal pool. The CD spectra of mutant and normal LDL are identical. Therefore, substitution of Gln for Arg at position 3500 induces a change in local conformation which disrupts the receptor-binding domain of apoB-100.

To further understand the packing of amphipathic alpha-helices of apolipoproteins in serum lipoproteins, we have investigated the interactions with dimyristoyl phosphatidylcholine (DMPC) of a 13C-labeled, 18-residue peptide (18A) which can form an amphipathic alpha-helix. This peptide whose amino acid sequence is DWLKAFYDKVAEKLKEAF has the positive-negative residue clustering typical of the apolipoprotein class of amphipathic helix. 13CH3-alanine was introduced as the 11th residue of 18A so that the 13CH3 group protrudes on the apolar side of the amphipathic helix. [13C]NMR spectra of [13C-Ala11]18A in discoidal complexes with DMPC show three resonances from the Ala-13CH3 group; one originates from 18A in aqueous solution, while those at chemical shifts (delta) of 15.2 and 16.4 ppm are assigned to 18A in the "edge" and "faces," respectively, of the discoidal complex. The proportion of 18A in the faces of the discoidal complex increases as the size of the disk is increased by raising the lipid/peptide ratio. 18A covers the edge of the disk so that the 13CH3-Ala side chain from these molecules is in contact with DMPC acyl chains. [13C-Ala11]18A bound to the surface of an egg PC small unilamellar vesicle gives a single resonance from 18A at delta 16.3 ppm consistent with there being no edge location. Cooling 18A-DMPC disks to 15 degrees C crystallizes the DMPC bilayer and restricts the motion of the 13CH3-Ala group of the 18A molecules. The molecular motions of the side chains of the amphipathic helix are sensitive to their location in the disk and to PC molecular packing.

NMR spectroscopy of 13C-labeled human low density lipoprotein (LDL) has been employed to characterize the lysine (Lys) residues in apo B-100. Reductive methylation with [13C]formaldehyde converts up to two-thirds of the Lys to the dimethylamino derivative; this pool of Lys is exposed at the surface of the LDL particle. The [13C]dimethyl-Lys which are visualized exhibit resonances at chemical shifts of 42.8 and 43.2 ppm (pH 7.6) indicating that they exist in two different microenvironments; this is a reflection of the native conformation of apo B associated with lipid, because the labeled, reduced, and alkylated protein gives a single resonance when dissolved in 7 M guanidine hydrochloride. The pH dependences of the Lys chemical shifts indicate that the two types of Lys titrate with different pK values; "active" Lys have a pK of 8.9, while "normal" Lys have a pK of 10.5. About 53 active Lys and 172 normal Lys are exposed on the surface of LDL with the remaining 132 Lys which are present in the human apo B-100 molecule being buried and unavailable for methylation. Addition of paramagnetic ions indicates that the active and normal Lys have different exposures to the aqueous phase; apparently this is a reflection of folding of the apo B molecule. The relative involvement of active and normal Lys in binding of apo B-100 to the LDL receptor on fibroblasts was explored by measuring the decrease in receptor binding as a function of the degree of methylation of the two types of Lys. Upper limits of 21 active and 31 normal Lys in the entire apo B-100 molecule are involved in the binding of LDL to the receptor. It is likely that these Lys are located in domains of apo B which contain clusters of basic amino acid residues and also bind heparin. If the sequence corresponding to apo B-48 (residues 1-2151) which does not bind to the receptor is excluded, then the above limits are halved; an upper limit of 10 active Lys may be particularly involved in receptor binding.

To study the effect of triglyceride content of low density lipoprotein (LDL) on its physicochemical and biological properties, we have depleted the triglyceride by incubation with hepatic lipase (HL-LDL) and raised the triglyceride by incubation of HL-LDL with very low density lipoprotein and lipoprotein-deficient serum. HL-LDL was taken up by human monocyte-derived macrophages and by human skin fibroblasts at an increased rate compared to untreated LDL. Incubation of the various LDL preparations revealed that cellular LDL degradation as well as LDL-mediated cholesterol esterification were inversely related to the triglyceride content of the LDL preparation. Modification of the triglyceride content of LDL also was associated with changes in the free fatty acid content, but the interaction of the LDL with cells was unaffected by the level of this component. The triglyceride content of LDL was found to be reciprocally related to the number of free lysine amino groups of LDL apolipoprotein B (apoB) which could be labeled with trinitrobenzenesulfonic acid. 13C-Nuclear magnetic resonance (NMR) spectra of native LDL and HL-LDL samples containing [13CH3]2 lysine residues formed by reductive methylation (11-13% modification) showed that the arrangement of apoB lysines is perturbed by the exposure to hepatic lipase. The ratio of labeled lysines with pK 8.9 to those with pK 10.5 exposed on the surface of LDL particles was decreased by about 40% by lipase treatment. These effects are apparently due to changes in local apoB conformation because circular dichroism spectra revealed that the average secondary structure of the entire apoB molecule is the same in native LDL and HL-LDL. The triglyceride content of LDL reciprocally affected its binding to a monoclonal antibody which recognizes epitopes around the LDL receptor binding domain of apoB. The above evidence indicates that modulation of the core triglyceride and possibly also surface phospholipid content of LDL can alter the conformation of apoB on the surface of the particle, thereby influencing the interaction with cell surface LDL receptors.