Spherical High-density Lipoprotein Research Articles

Determination of the Dynamic Structures of Nacent Discoidal High-Density Lipoprotein (HDL) Bound to Lecithin Cholesterol Acyltransferase (LCAT) and Paraoxonase 1 (PON1)

The relative levels of plasma cholesterol in different lipoproteins are the major indicator for CVD and related diseases. Nascent discoidal HDL particles, which are then converted to spherical mature HDL by lecithin-cholesterol acyltransferase (LCAT), are integral in reverse cholesterol transport. Detailed knowledge of HDL structure is key to understanding its molecular mechanisms, including how Paraoxynase 1 (PON1) associates with the phospholipid surface of HDL helping prevent oxidation. Despite public interest in HDL structure related function, their highly dynamic nature has prevented precise structural determinations for nearly half a century. Here, we used our recently developed individual particle electron tomography (IPET) technique to study each individual complex of HDL-LCAT. The 3D reconstructions show, i) LCAT associates with HDL along a proposed mobile region of the apoA-1 backbone (res ∼122-142), where both monomers overlap antiparallel along the discoidal edge of HDL; ii) PON1 interacts with HDL through its hydrophobic tail, which binds into the phospholipid surface, and loosely associates with apoA-1. The structure provides novel information for modeling nascent discoidal HDL and further reveals the first view of HDL structural dynamics in three-dimensions. This result will benefit public knowledge and pharmaceutical drug design to control plasma HDL cholesterol level.

Abstract 18311: Lipid Composition of Gold Nanoparticle-Templated High-Density Lipoprotein Analogs Dictates Cholesterol Efflux Function

Background: Reverse cholesterol transport, the process by which cholesterol is effluxed from cells to high-density lipoproteins (HDL) and is delivered to the liver for clearance, is a promising pathway to augment for treatment of atherosclerosis. Though structure-function relationships between nascent, discoidal HDL and cholesterol efflux have been well studied, how the lipid composition of spherical HDL species, which varies in pathophysiological conditions, impacts their ability to mediate cholesterol efflux has not been investigated. Methods and Results: Spherical gold nanoparticles (5 nm) were used to synthesize spherical HDL analogs (HDL-NP) by adding ApoAI protein and various lipids to the particle surface. With this strategy a panel of HDL-NP varying in lipid content was generated. HDL-NP designs tested include: dipalmitylphosphatidylcholine (DPPC, saturated fatty acid), dioleoylphosphatidylcholine (DOPC, unsaturated fatty acid), sphingomyelin, lysophosphatidylcholine (LPC), and mixtures thereof. All of these lipids are found in natural HDL. After characterizing the purified HDL-NP, these HDL-NP designs were tested in the cellular reverse cholesterol transport assay using J774 mouse macrophages. These studies demonstrate that all HDL-NP designs mediate more efflux than equimolar amounts of ApoAI protein control, and further demonstrate that HDL-NP designs incorporating unsaturated phospholipid (DOPC), sphingomyelin, and LPC--each of which can increase disorder in the lipid membrane and thus give rise to opportunity for cholesterol to intercalate and bind--enhance cholesterol efflux compared to the saturated phospholipid (DPPC) design. Conclusion: In summary, these results demonstrate that lipid content of HDL-NP,analogs of spherical HDL, dictates cholesterol efflux function, a finding which sheds light on the functional importance of lipid content variation seen in mature, spherical HDL species.

Biomarkers associated with high-density lipoproteins in atherosclerotic kidney disease

High-density lipoproteins (HDL) originate as discoidal particles that are rapidly converted by lecithin:cholesterol acyltransferase (LCAT) into the spherical particles that predominate in normal human plasma. Spherical HDL consist of multiple populations of particles that vary widely in size, composition and function. Human population studies have established that high plasma HDL cholesterol levels are associated with a reduced incidence of cardiovascular disease. The mechanistic basis of this relationship is not well understood, but most likely involves a number of the cardioprotective functions of HDL. These include the ability of apolipoprotein (apo) A-I, the main apolipoprotein constituent of HDL, to remove cholesterol from macrophages in the artery wall. HDL also have antioxidant and anti-inflammatory properties that are potentially cardioprotective. Evidence that some of these beneficial properties are compromised in people with diabetes and renal disease is emerging. Persistently elevated plasma glucose levels in people with diabetes and poor glycemic control can lead to irreversible, non-enzymatic glycation of plasma proteins, including apoA-I. Non-enzymatically glycated proteins are also prevalent in people with diabetes and end-stage renal disease who are at high cardiovascular risk. Evidence that non-enzymatically glycated apoA-I inhibits the LCAT reaction and impairs some of the cardioprotective properties of HDL is also emerging. This review is concerned with how non-enzymatic glycation of apoA-I affects the ability of LCAT to convert discoidal HDL into spherical HDL, how it affects cholesterol efflux from macrophages and how it affects the anti-inflammatory and antioxidant properties of HDL.

Conservation of Apolipoprotein A-I’s Central Domain Structural Elements upon Lipid Association on Different High-Density Lipoprotein Subclasses

The antiatherogenic properties of apolipoprotein A-I (apoA-I) are derived, in part, from lipidation-state-dependent structural elements that manifest at different stages of apoA-I's progression from lipid-free protein to spherical high-density lipoprotein (HDL). Previously, we reported the structure of apoA-I's N-terminus on reconstituted HDLs (rHDLs) of different sizes. We have now investigated at the single-residue level the conformational adaptations of three regions in the central domain of apoA-I (residues 119-124, 139-144, and 164-170) upon apoA-I lipid binding and HDL formation. An important function associated with these residues of apoA-I is the activation of lecithin:cholesterol acyltransferase (LCAT), the enzyme responsible for catalyzing HDL maturation. Structural examination was performed by site-directed tryptophan fluorescence and spin-label electron paramagnetic resonance spectroscopies for both the lipid-free protein and rHDL particles 7.8, 8.4, and 9.6 nm in diameter. The two methods provide complementary information about residue side chain mobility and molecular accessibility, as well as the polarity of the local environment at the targeted positions. The modulation of these biophysical parameters yielded new insight into the importance of structural elements in the central domain of apoA-I. In particular, we determined that the loosely lipid-associated structure of residues 134-145 is conserved in all rHDL particles. Truncation of this region completely abolished LCAT activation but did not significantly affect rHDL size, reaffirming the important role of this structural element in HDL function.

Translation of High-Density Lipoprotein Function Into Clinical Practice

High-density lipoproteins (HDLs) represent a spectrum of particles that vary in their physicochemical and functional properties.1 It has been shown in many population studies that the concentration of HDL cholesterol (HDL-C) is inversely related to the risk of having a cardiovascular disease (CVD) event. In this paradigm, HDL-C has been considered to be a marker of the potentially cardioprotective functions of HDL. However, recent studies have suggested that the simple concentration of HDL-C may not always reflect HDL function, with growing evidence that under some circumstances HDL function may be compromised despite high concentrations of HDL-C. The best known of the potentially antiatherogenic functions of HDLs is their ability to promote cholesterol efflux from cells, including that from macrophages in the arterial wall.2 Cellular cholesterol efflux is achieved by several mechanisms. One involves the interaction of phospholipid-depleted and cholesterol-deficient apolipoprotein (apo) A-I complexes (discoidal, pre–β-migrating particles [very small HDL] with the ATP-binding cassette transporter A1 (ABCA1) in a process that results in the formation of a heterogeneous population of nascent HDL particles that are discoidal in shape and contain apoA-I, phospholipids, and free cholesterol. A proportion of the free cholesterol is subsequently esterified by lecithin:cholesterol acyltransferase (LCAT); this enzyme generates a core of cholesteryl esters in a process that converts HDL particles from discoidal, very small, pre-β1-migrating particles into spherical, α-migrating particles (small HDL]).1 The interaction of spherical HDL particles with other active cellular transporters such as ABCG1 and passive diffusion of cellular cholesterol further increase the cholesterol load of HDL. However, it is often unappreciated that peripheral cholesterol efflux contributes <5% of the cholesterol content of HDL.2 Thus, HDL-C is an inadequate surrogate measure for the most heralded of HDL functions. Various HDL subpopulations differ in other antiatherogenic functions that extend beyond macrophage …

Structure‐based mechanism for the adaptation of apolipoprotein A‐I to the changing lipid load in Good Cholesterol

High‐density lipoproteins (HDL) and their main protein, apoA‐I, remove excess cell cholesterol and protect against atherosclerosis. Heterogeneity and large size of HDL (8–12 nm) hamper their high‐resolution structural studies. Low‐resolution studies showed that two apoA‐I molecules form an antiparallel α‐helical double belt around an HDL particle. High‐resolution structure of the C‐terminally truncated apoA‐I solved by Mei and Atkinson provides tremendous new insights into HDL structure‐function. It enables us to propose apoA‐I conformations on the small, midsize and large HDL and validate them by comparison with extensive biophysical data. We postulate that the central “constant” half of the double belt is structurally conserved while the N‐and C‐terminal “variable” half re‐arranges upon HDL growth. This includes sequential unhinging of the N‐terminal bundle around two flexible Gly‐containing regions to elongate the belt, along with concerted swing motion of the double belt around G65‐P66 and G185‐G186 hinges that are aligned on various‐size particles, to confer 2D surface curvature to spherical HDL. Our ensemble reconciles several existing HDL models and helps provide a structural framework for understanding functional interactions with ~60 other HDL‐associated proteins and, ultimately, to improve cardioprotective function of HDL. This work was supported by NIH grants HL026355 and GM067260.

Interactions of Apolipoprotein A-I with High-Density Lipoprotein Particles

Although the partitioning of apolipoprotein A-I (apoA-I) molecules in plasma between high-density lipoprotein (HDL)-bound and -unbound states is an integral part of HDL metabolism, the factors that control binding of apoA-I to HDL particles are poorly understood. To address this gap in knowledge, we investigated how the properties of the apoA-I tertiary structure domains and surface characteristics of spherical HDL particles influence apoA-I binding. The abilities of 14C-labeled human and mouse apoA-I variants to associate with human HDL and lipid emulsion particles were determined using ultracentrifugation to separate free and bound protein. The binding of human apoA-I (243 amino acids) to HDL is largely mediated by its relatively hydrophobic C-terminal domain; the isolated N-terminal helix bundle domain (residues 1–190) binds poorly. Mouse apoA-I, which has a relatively polar C-terminal domain, binds to human HDL to approximately half the level of human apoA-I. The HDL binding abilities of apoA-I variants correlate strongly with their abilities to associate with phospholipid (PL)-stabilized emulsion particles, consistent with apoA-I–PL interactions at the particle surface being important. When equal amounts of HDL2 and HDL3 are present, all of the apoA-I variants partition preferentially to HDL3. Fluorescence polarization measurements using Laurdan-labeled HDL2 and HDL3 indicate that PL molecular packing is looser on the more negatively charged HDL3 particle surface, which promotes apoA-I binding. Overall, it is clear that both apoA-I structural features, especially the hydrophobicity of the C-terminal domain, and HDL surface characteristics such as the availability of free space influence the ability of apoA-I to associate with HDL particles.

Pharmacokinetics and atherosclerotic lesions targeting effects of tanshinone IIA discoidal and spherical biomimetic high density lipoproteins

High density lipoproteins (HDL) have been successfully reconstructed to deliver a large number of lipophilic drugs. Here, discoidal and spherical recombinant HDL loaded with cardiovascular drug tanshinone IIA (TA) were constructed (TA-d-rHDL and TA-s-rHDL), respectively. And next their in vitro physiochemical and biomimetic properties were characterized. Furthermore, pharmacokinetics, atherosclerotic lesions targeting effects and antiatherogenic efficacies were elaborately performed and compared in atherosclerotic New Zealand White (NZW) rabbits. In vitro characterizations results showed that both TA-d-rHDL and TA-s-rHDL had nano-size diameter, high entrapment efficiency (EE) and drug-loading capacity (DL). Additionally, similar to their native counterparts, TA-d-rHDL maintained remodeling behaviors induced by lecithin cholesterol acyltransferase (LCAT), and TA leaked during remodeling behaviors. Pharmacokinetic studies manifested that both TA-d-rHDL and TA-s-rHDL markedly improved pharmacokinetic behaviors of TA in vivo. Ex vivo imaging demonstrated that both d-rHDL and s-rHDL bound more avidly to atherosclerotic lesions than to normal vessel walls, and s-rHDL had better targeting effect than d-rHDL. Pharmacodynamic tests illustrated that both TA-d-rHDL and TA-s-rHDL had much stronger antiatherogenic efficacies than conventional TA nanostructured lipid carriers (TA-NLC), TA liposomes (TA-L) and commercially available preparation Sulfotanshinone Sodium Injection (SSI). Moreover, TA-s-rHDL had more potent antiatherogenic efficacies than TA-d-rHDL. Collectively our studies indicated that rHDL could be exploited as potential delivery vehicles of TA targeting atherosclerotic lesions as well as synergistically improving efficacies, especially for s-rHDL.

Crystal structure of Δ(185-243)ApoA-I suggests a mechanistic framework for the protein adaptation to the changing lipid load in good cholesterol: from flatland to sphereland via double belt, belt buckle, double hairpin and trefoil/tetrafoil.

Apolipoprotein A-I (apoA-I) is the major protein of plasma high-density lipoproteins (HDLs), macromolecular assemblies of proteins and lipids that remove cell cholesterol and protect against atherosclerosis. HDL heterogeneity, large size (7.7-12 nm), and ability to exchange proteins have prevented high-resolution structural analysis. Low-resolution studies showed that two apoA-I molecules form an antiparallel α-helical "double belt" around an HDL particle. The atomic-resolution structure of the C-terminal truncated lipid-free Δ(185-243)apoA-I, determined recently by Mei and Atkinson, provides unprecedented new insights into HDL structure-function. It allows us to propose a molecular mechanism for the adaptation of the full-length protein to increasing lipid load during cholesterol transport. ApoA-I conformations on small, midsize, and large HDLs are proposed based on the tandem α-helical repeats and the crystal structure of Δ(185-243)apoA-I and are validated by comparison with extensive biophysical data reported by many groups. In our models, the central half of the double belt ("constant" segment 66-184) is structurally conserved while the N- and C-terminal half ("variable" segments 1-65 and 185-243) rearranges upon HDL growth. This includes incremental unhinging of the N-terminal bundle around two flexible regions containing G39 and G65 to elongate the belt, along with concerted swing motion of the double belt around G65-P66 and G185-G186 hinges that are aligned on various-size particles, to confer two-dimensional surface curvature to spherical HDLs. The proposed conformational ensemble integrates and improves several existing HDL models. It helps provide a structural framework necessary to understand functional interactions with over 60 other HDL-associated proteins and, ultimately, improve the cardioprotective function of HDL.

Harnessing a Physiologic Mechanism for siRNA Delivery With Mimetic Lipoprotein Particles

Therapeutics based on RNA interference (RNAi) have emerged as a potential new class of drugs for treating human disease by silencing the target messenger RNA (mRNA), thereby reducing levels of the corresponding pathogenic protein. The major challenge for RNAi therapeutics is the development of safe delivery vehicles for small interfering RNAs (siRNAs). We previously showed that cholesterol-conjugated siRNAs (chol-siRNA) associate with plasma lipoprotein particles and distribute primarily to the liver after systemic administration to mice. We further demonstrated enhancement of silencing by administration of chol-siRNA pre-associated with isolated high-density lipoprotein (HDL) or low-density lipoprotein (LDL). In this study, we investigated mimetic lipoprotein particle prepared from recombinant apolipoprotein A1 (apoA) and apolipoprotein E3 (apoE) as a delivery vehicle for chol-siRNAs. We show that apoE-containing particle (E-lip) is highly effective in functional delivery of chol-siRNA to mouse liver. E-lip delivery was found to be considerably more potent than apoA-containing particle (A-lip). Furthermore, E-lip–mediated delivery was not significantly affected by high endogenous levels of plasma LDL. These results demonstrate that E-lip has substantial potential as delivery vehicles for lipophilic conjugates of siRNAs.

Apolipoprotein A-II-mediated Conformational Changes of Apolipoprotein A-I in Discoidal High Density Lipoproteins

It is well accepted that HDL has the ability to reduce risks for several chronic diseases. To gain insights into the functional properties of HDL, it is critical to understand the HDL structure in detail. To understand interactions between the two major apolipoproteins (apos), apoA-I and apoA-II in HDL, we generated highly defined benchmark discoidal HDL particles. These particles were reconstituted using a physiologically relevant phospholipid, 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC) incorporating two molecules of apoA-I and one homodimer of apoA-II per particle. We utilized two independent mass spectrometry techniques to study these particles. The techniques are both sensitive to protein conformation and interactions and are namely: 1) hydrogen deuterium exchange combined with mass spectrometry and 2) partial acetylation of lysine residues combined with MS. Comparison of mixed particles with apoA-I only particles of similar diameter revealed that the changes in apoA-I conformation in the presence of apoA-II are confined to apoA-I helices 3-4 and 7-9. We discuss these findings with respect to the relative reactivity of these two particle types toward a major plasma enzyme, lecithin:cholesterol acyltransferase responsible for the HDL maturation process.

Lipid-bound apolipoproteins in tyrosyl radical-oxidized HDL stabilize ABCA1 like lipid-free apolipoprotein A-I

BackgroundATP-binding cassette transporter A1 (ABCA1) mediates the lipidation of exchangeable apolipoproteins, the rate-limiting step in the formation of high density lipoproteins (HDL). We previously demonstrated that HDL oxidized ex vivo by peroxidase-generated tyrosyl radical (tyrosylated HDL, tyrHDL) increases the availability of cellular cholesterol for efflux and reduces the development of atherosclerosis when administered to apolipoprotein E-deficient mice as compared to treatment with control HDL.ResultsIn the current study we determined that tyrHDL requires functional ABCA1 for this enhanced activity. Like lipid-free apolipoprotein A-I (apoA-I), tyrHDL increases total and cell surface ABCA1, inhibits calpain-dependent and -independent proteolysis of ABCA1, and can be bound by cell surface ABCA1 in human skin fibroblasts. Additionally, tyrHDL apoproteins are susceptible to digestion by enteropeptidase like lipid-free apoA-I, but unlike lipid-bound apoA-I on HDL, which is resistant to proteolysis.ConclusionsThese results provide the first evidence that lipid-bound apolipoproteins on the surface of spherical HDL particles can behave like lipid-free apoA-I to increase ABCA1 protein levels and activity.

The Low Resolution Structure of ApoA1 in Spherical High Density Lipoprotein Revealed by Small Angle Neutron Scattering

Spherical high density lipoprotein (sHDL), a key player in reverse cholesterol transport and the most abundant form of HDL, is associated with cardiovascular diseases. Small angle neutron scattering with contrast variation was used to determine the solution structure of protein and lipid components of reconstituted sHDL. Apolipoprotein A1, the major protein of sHDL, forms a hollow structure that cradles a central compact lipid core. Three apoA1 chains are arranged within the low resolution structure of the protein component as one of three possible global architectures: (i) a helical dimer with a hairpin (HdHp), (ii) three hairpins (3Hp), or (iii) an integrated trimer (iT) in which the three apoA1 monomers mutually associate over a portion of the sHDL surface. Cross-linking and mass spectrometry analyses help to discriminate among the three molecular models and are most consistent with the HdHp overall architecture of apoA1 within sHDL.

Structure of Apolipoprotein A-I N Terminus on Nascent High Density Lipoproteins

Apolipoprotein A-I (apoA-I) is the major protein component of high density lipoproteins (HDL) and a critical element of cholesterol metabolism. To better elucidate the role of the apoA-I structure-function in cholesterol metabolism, the conformation of the apoA-I N terminus (residues 6-98) on nascent HDL was examined by electron paramagnetic resonance (EPR) spectroscopic analysis. A series of 93 apoA-I variants bearing single nitroxide spin label at positions 6-98 was reconstituted onto 9.6-nm HDL particles (rHDL). These particles were subjected to EPR spectral analysis, measuring regional flexibility and side chain solvent accessibility. Secondary structure was elucidated from side-chain mobility and molecular accessibility, wherein two major α-helical domains were localized to residues 6-34 and 50-98. We identified an unstructured segment (residues 35-39) and a β-strand (residues 40-49) between the two helices. Residues 14, 19, 34, 37, 41, and 58 were examined by EPR on 7.8, 8.4, and 9.6 nm rHDL to assess the effect of particle size on the N-terminal structure. Residues 14, 19, and 58 showed no significant rHDL size-dependent spectral or accessibility differences, whereas residues 34, 37, and 41 displayed moderate spectral changes along with substantial rHDL size-dependent differences in molecular accessibility. We have elucidated the secondary structure of the N-terminal domain of apoA-I on 9.6 nm rHDL (residues 6-98) and identified residues in this region that are affected by particle size. We conclude that the inter-helical segment (residues 35-49) plays a role in the adaptation of apoA-I to the particle size of HDL.

Morphology and structure of lipoproteins revealed by an optimized negative-staining protocol of electron microscopy

Plasma lipoprotein levels are predictors of risk for coronary artery disease. Lipoprotein structure-function relationships provide important clues that help identify the role of lipoproteins in cardiovascular disease. The compositional and conformational heterogeneity of lipoproteins are major barriers to the identification of their structures, as discovered using traditional approaches. Although electron microscopy (EM) is an alternative approach, conventional negative staining (NS) produces rouleau artifacts. In a previous study of apolipoprotein (apo)E4-containing reconstituted HDL (rHDL) particles, we optimized the NS method in a way that eliminated rouleaux. Here we report that phosphotungstic acid at high buffer salt concentrations plays a key role in rouleau formation. We also validate our protocol for analyzing the major plasma lipoprotein classes HDL, LDL, IDL, and VLDL, as well as homogeneously prepared apoA-I-containing rHDL. High-contrast EM images revealed morphology and detailed structures of lipoproteins, especially apoA-I-containing rHDL, that are amenable to three-dimensional reconstruction by single-particle analysis and electron tomography.

Role of Lipids in Spheroidal High Density Lipoproteins

We study the structure and dynamics of spherical high density lipoprotein (HDL) particles through coarse-grained multi-microsecond molecular dynamics simulations. We simulate both a lipid droplet without the apolipoprotein A-I (apoA-I) and the full HDL particle including two apoA-I molecules surrounding the lipid compartment. The present models are the first ones among computational studies where the size and lipid composition of HDL are realistic, corresponding to human serum HDL. We focus on the role of lipids in HDL structure and dynamics. Particular attention is paid to the assembly of lipids and the influence of lipid-protein interactions on HDL properties. We find that the properties of lipids depend significantly on their location in the particle (core, intermediate region, surface). Unlike the hydrophobic core, the intermediate and surface regions are characterized by prominent conformational lipid order. Yet, not only the conformations but also the dynamics of lipids are found to be distinctly different in the different regions of HDL, highlighting the importance of dynamics in considering the functionalization of HDL. The structure of the lipid droplet close to the HDL-water interface is altered by the presence of apoA-Is, with most prominent changes being observed for cholesterol and polar lipids. For cholesterol, slow trafficking between the surface layer and the regimes underneath is observed. The lipid-protein interactions are strongest for cholesterol, in particular its interaction with hydrophobic residues of apoA-I. Our results reveal that not only hydrophobicity but also conformational entropy of the molecules are the driving forces in the formation of HDL structure. The results provide the first detailed structural model for HDL and its dynamics with and without apoA-I, and indicate how the interplay and competition between entropy and detailed interactions may be used in nanoparticle and drug design through self-assembly.

Effects of cholesterol on thermal stability of discoidal high density lipoproteins

Reverse cholesterol transport in plasma involves variations in HDL cholesterol concentration. To understand physicochemical and functional implications of such variations, we analyzed stability of reconstituted HDL containing human apolipoproteins (apoA-I, apoA-II, or apoC-I), phosphatidylcholines varying in chain length (12-18 carbons) and unsaturation (0 or 1), and 0-35 mol% cholesterol. Lipoprotein heat denaturation was monitored by circular dichroism for protein unfolding/dissociation and by light scattering for particle fusion. We found that cholesterol stabilizes relatively unstable complexes; for example, incorporation of 10-30 mol% cholesterol in apoC-I:dimyristoyl phosphatidylcholine complexes increased their kinetic stability by deltaDeltaG* congruent with 1 kcal/mol. In more stable complexes containing larger proteins and/or longer-chain lipids, incorporation of 10% cholesterol did not significantly alter the disk stability; however, 15% or more cholesterol destabilized the apoA-I-containing complexes and led to vesicle formation. Thus, cholesterol tends to stabilize less stable lipoproteins, apparently by enhancing favorable packing interactions, but in more stable lipoproteins, where such interactions are already highly optimized, the stabilizing effect of cholesterol decreases and, eventually, becomes destabilizing. These results help uncouple the functional roles of particle stability and chain fluidity and suggest that structural disorder in HDL surface, rather than chain fluidity, is an important physicochemical determinant of HDL function.

Abstract: S3-6 APOA-I HDL BIOGENESIS AND SITES OF REGULATION

High-density lipoproteins (HDLs) are complexes of proteins (mainly apoA-I and apoA-II) and lipids that remove cholesterol and prevent atherosclerosis. Understanding the distinct properties of the heterogeneous HDL population may aid the development of new diagnostic tools and therapies for atherosclerosis. Mature human HDLs form two major subclasses differing in particle diameter and metabolic properties, HDL2 (large) and HDL3 (small). These subclasses are comprised of HDL(A-I) containing only apoA-I, and HDL(A-I/A-II) containing apoA-I and apoA-II. ApoA-I is strongly cardioprotective, but the function of the smaller, more hydrophobic apoA-II is unclear. ApoA-II is thought to counteract the cardioprotective action of apoA-I by stabilizing HDL particles and inhibiting their remodeling. To test this notion, we performed the first kinetic stability study of human HDL subclasses. The results revealed that the stability of plasma spherical HDL decreases with increasing particle diameter; which may facilitate preferential cholesterol ester uptake from large lipid-loaded HDL2. Surprisingly, size-matched plasma HDL(A-I/A-II) showed comparable or slightly lower stability than HDL(A-I); this is consistent with the destabilization of model discoidal HDL observed upon increasing the A-II to A-I ratio. These results clarify the roles of the particle size and protein composition in HDL remodeling, and help reconcile conflicting reports regarding the role of apoA-II in this remodeling.

Differential Stability of High-density Lipoprotein Subclasses: Effects of Particle Size and Protein Composition

High-density lipoproteins (HDLs) are complexes of proteins (mainly apoA-I and apoA-II) and lipids that remove cholesterol and prevent atherosclerosis. Understanding the distinct properties of the heterogeneous HDL population may aid the development of new diagnostic tools and therapies for atherosclerosis. Mature human HDLs form two major subclasses differing in particle diameter and metabolic properties, HDL 2 (large) and HDL 3 (small). These subclasses are comprised of HDL(A-I) containing only apoA-I, and HDL(A-I/A-II) containing apoA-I and apoA-II. ApoA-I is strongly cardioprotective, but the function of the smaller, more hydrophobic apoA-II is unclear. ApoA-II is thought to counteract the cardioprotective action of apoA-I by stabilizing HDL particles and inhibiting their remodeling. To test this notion, we performed the first kinetic stability study of human HDL subclasses. The results revealed that the stability of plasma spherical HDL decreases with increasing particle diameter; which may facilitate preferential cholesterol ester uptake from large lipid-loaded HDL 2. Surprisingly, size-matched plasma HDL(A-I/A-II) showed comparable or slightly lower stability than HDL(A-I); this is consistent with the destabilization of model discoidal HDL observed upon increasing the A-II to A-I ratio. These results clarify the roles of the particle size and protein composition in HDL remodeling, and help reconcile conflicting reports regarding the role of apoA-II in this remodeling.

Templated Spherical High Density Lipoprotein Nanoparticles

We report the synthesis of high density lipoprotein (HDL) biomimetic nanoparticles capable of binding cholesterol. These structures use a gold nanoparticle core to template the assembly of a mixed phospholipid layer and the adsorption of apolipoprotein A-I. These synthesized structures have the general size and surface composition of natural HDL and, importantly, bind free cholesterol (K(d) = 4 nM). The determination of the K(d) for these particles, with respect to cholesterol complexation, provides a key starting and comparison point for measuring and evaluating the properties of subsequently developed synthetic versions of HDL.