Immuno-electron cryo-microscopy imaging reveals a looped topology of apoB at the surface of human LDL

A single copy of apoB is the sole protein component of human LDL. ApoB is crucial for LDL particle stabilization and is the ligand for LDL receptor, through which cholesterol is delivered to cells. Dysregulation of the pathways of LDL metabolism is well documented in the pathophysiology of atherosclerosis. However, an understanding of the structure of LDL and apoB underlying these biological processes remains limited. In this study, we derived a 22 Å-resolution three-dimensional (3D) density map of LDL using cryo-electron microscopy and image reconstruction, which showed a backbone of high-density regions that encircle the LDL particle. Additional high-density belts complemented this backbone high density to enclose the edge of the LDL particle. Image reconstructions of monoclonal antibody-labeled LDL located six epitopes in five putative domains of apoB in 3D. Epitopes in the LDL receptor binding domain were located on one side of the LDL particle, and epitopes in the N-terminal and C-terminal domains of apoB were in close proximity at the front side of the particle. Such image information revealed a looped topology of apoB on the LDL surface and demonstrated the active role of apoB in maintaining the shape of the LDL particle.     

Human LDL core cholesterol ester packing: three-dimensional image reconstruction and SAXS simulation studies

Human LDL undergoes a reversible thermal order-disorder phase transition associated with the cholesterol ester packing in the lipid core. Structural changes associated with this phase transition have been shown to affect the resistance of LDL to oxidation in vitro studies. Previous electron cryo-microscopy studies have provided image evidence that the cholesterol ester is packed in three flat layers in the core at temperatures below the phase transition. To study changes in lipid packing, overall structure and particle morphology in three dimensions (3D) subsequent to the phase transition, we cryo-preserved human LDL at a temperature above phase transition (53°C) and examined the sample by electron microscopy and image reconstruction. The LDL frozen from 53°C adopted a different morphology. The central density layer was disrupted and the outer two layers formed a "disrupted shell"-shaped density, located concentrically underneath the surface density of the LDL particle. Simulation of the small angle X-ray scattering curves and comparison with published data suggested that this disrupted shell organization represents an intermediate state in the transition from isotropic to layered packing of the lipid. Thus, the results revealed, with 3D images, the lipid packing in the dynamic process of the LDL lipid-core phase transition.     

Cryoelectron microscopy of low density lipoprotein in vitreous ice.

In this report, images of low density lipoprotein (LDL) in vitreous ice at approximately 30 A resolution are presented. These images show that LDL is a quasi-spherical particle, approximately 220-240 A in diameter, with a region of low density (lipid) surrounded by a ring (in projection) of high density believed to represent apolipoprotein B-100. This ring is seen to be composed of four or five (depending on view) large regions of high density material that may represent protein superdomains. Analysis of LDL images obtained at slightly higher magnification reveals that areas of somewhat lower density connect these regions, in some cases crossing the projectional interiors of the LDL particles. Preliminary image analysis of LDL covalently labeled at Cys3734 and Cys4190 with 1.4-nm Nanogold clusters demonstrates that this methodology will provide an important site-specific marker in studies designed to map the organization of apoB at the surface of LDL.     

Molecular packing of high-density and low-density lipoprotein surface lipids and apolipoprotein A-I binding

The surface pressure (pi)-molecular area (A) isotherms for monolayers of human high-density lipoprotein (HDL3) and low-density lipoprotein (LDL) phospholipids and of mixed monolayers of these phospholipids with cholesterol spread at the air-water interface were used to deduce the likely molecular packing at the surfaces of HDL3 and LDL particles. LDL phospholipids form more condensed monolayers than HDL3 phospholipids; for example, the molecular areas of LDL and HDL3 phospholipids at pi = 10 dyn/cm are 88 and 75 A2/molecule, respectively. The closer packing in the LDL phospholipids monolayer can be attributed to the higher contents of saturated phosphatidylcholines and sphingomyelin relative to HDL3. Cholesterol condenses both HDL3 and LDL phospholipid monolayers but has a greater condensing effect on the LDL phospholipid monolayer. The pi-A isotherms for mixed monolayer of HDL3 phospholipid/cholesterol and LDL phospholipid/cholesterol at stoichiometries similar to those at the surfaces of lipoprotein particles suggest that the monolayer at the surface of the LDL particle is significantly more condensed than that at the surface of the HDL3 particle. The closer lateral packing in LDL is due to at least three factors: (1) the difference in phospholipid composition; (2) the higher unesterified cholesterol content in LDL; and (3) a stronger interaction between cholesterol and LDL phospholipids relative to HDL3 phospholipids. The influence of lipid molecular packing on the affinity of human apolipoprotein A-I (apo A-I) for HDL3 and LDL surface lipids was evaluated by monitoring the adsorption of 14C-methylated apo A-I to monolayers of these lipids spread at various initial surface pressures (pi i).(ABSTRACT TRUNCATED AT 250 WORDS)     

Refining Lipoprotein Assessment in Diabetes: Apolipoprotein B Makes Sense

ObjectiveTo summarize the data that support the measurement of apolipoprotein B as an accurate reflection of low-density lipoprotein (LDL) particle number and an easily adapted parameter in clinical practice.MethodsStudy findings are reviewed and a flow chart is provided to guide lipid assessment in patients with dyslipidemia.ResultsCurrent treatment guidelines for lipid management emphasize LDL cholesterol as the primary treatment target in patients at high risk of cardiovascular events. However, LDL cholesterol is a poor surrogate for LDL particle number, particularly in patients with altered LDL composition, such as those with insulin resistance, metabolic syndrome, and type 2 diabetes. Direct measurement of LDL particle number or size is not practical because of methodology and cost considerations. A suggested alternative target in patients with hypertriglyceridemia is non–high-density lipoprotein (HDL) cholesterol. Abundant evidence suggests that even non-HDL cholesterol is an inadequate approximation of the LDL particle number in such patients. The flow chart emphasizes the need to continue achieving the well-established LDL-cholesterol goal, while also considering apolipoprotein B measurement in those with hypertriglyceridemia, rather than relying on the less accurate surrogate of non-HDL cholesterol, when targeting therapy in such patients.ConclusionPresented evidence supports the measurement of apolipoprotein B as a more accurate reflection of LDL particle number than non-HDL cholesterol, and it is an easily adapted parameter in clinical practice. (Endocr Pract. 2009;15:370-376)     

NMR studies of pig low- and high-density serum lipoproteins. Molecular motions and morphology.

1. NMR spectra of porcine high- and low density lipoproteins (d 1.120--1.210 and 1.019--1.070, respectively) and their extracted lipids were obtained as functions of temperature, frequency and solution viscosity, and from solutions to which paramagnetic species had been added. 2. About one-third of the N(CH3)3 groups in low-density lipoproteins are so immobile that they do not give a sharp resonance at any temperature up to 65 degrees C, unless the particles are disrupted with sodium dodecylsulphate. Most of the protein residues also undergo little segmental motion. 3. A marked restriction of motion of acyl chain terminal CH3 groups suggests that chain interdigitation occurs in low-density lipoprotein. Apart from this, there is a general ordering of the lipids without a decrease in the rate of rotation about bonds, suggesting that the protein organizes the lipids by controlling the molecular packing rather than by direct strong interactions. The lipids are more ordered in low-density than in high-density lipoprotein. 4. All phospholipids with mobile N(CH3)3 groups are at the particle surfaces, in patches separated by protein. In low-density lipoprotein the patches are raised proud of the protein, whereas in high-density lipoproteins the protein and lipid polar groups are coplanar. 5. The high-density lipoprotein results are consistent with literature models for the structure. The low-density lipoprotein results suggest a new model, which is basically a trilayer. The centre consists of a monolayer of phospholipid with tightly-packed polar groups in contact with a protein core. The outer monolayer of phospholipid contains the rest (most) of the protein; the central layer contains the neutral lipid (cholesterol esters and triglycerides), interdigitated into both the inner and outer monolayers. Unesterified cholesterol is distributed through all three layers.     

Packing of cholesterol molecules in human low-density lipoprotein

High-resolution, proton-decoupled 13C nuclear magnetic resonance spectra (90.55 MHz) of human low-density lipoprotein (LDL) have been employed to investigate the physical state of unesterified cholesterol molecules in this particle. Approximately half of the cholesterol molecules in LDL were replaced with [4-13C]cholesterol by exchange from Celite. About two-thirds of the cholesterol molecules contribute to a resonance at delta 41.8 from the C-4 atom. This signal is assigned to cholesterol molecules located at the surface of the LDL particle in a mixed monolayer with phospholipid molecules; the spin-lattice relaxation of the C-4 nucleus of such cholesterol molecules is enhanced by the presence of Mn2+ ions in the aqueous phase. The remaining one-third of the cholesterol molecules are apparently neither associated with phospholipid nor exposed to the aqueous phase; these cholesterol molecules are presumed to be located in the core of the particle. Cholesterol molecules in the two microenvironments are in slow exchange on the NMR time scale but in fast exchange on a biological time scale, so that the cholesterol molecules in LDL behave physiologically as one pool. There is a loss of about 20% of the intensity of the N(CH3)3 resonance from phosphatidylcholine and sphingomyelin molecules in the LDL spectrum; this is attributed to the presence of apolipoprotein B in the surface of LDL particles, which may immobilize some of the phospholipid polar groups. Spin-lattice relaxation time measurements suggest that the fast axial motions of cholesterol molecules in the surface of LDL are the same as in high-density lipoprotein (HDL).(ABSTRACT TRUNCATED AT 250 WORDS)     

Thermal transitions in human very-low-density lipoprotein: fusion, rupture, and dissociation of HDL-like particles

Very-low-density lipoproteins (VLDL) are metabolic precursors of low-density lipoproteins (LDL) and a risk factor for atherosclerosis. Human VLDL are heterogeneous complexes containing a triacylglycerol-rich apolar lipid core and polar surface composed of phospholipids, a nonexchangeable apolipoprotein B, and exchangeable apolipoproteins E and Cs. We report the first stability study of VLDL. Circular dichroism and turbidity data reveal an irreversible heat-induced VLDL transition that involves formation of larger particles and repacking of apolar lipids but no global protein unfolding. Heating rate effect on the melting temperature indicates a kinetically controlled reaction with high activation energy, Ea. Arrhenius analysis of the turbidity data reveals two kinetic phases with Ea = 53 +/- 7 kcal/mol that correspond to distinct morphological transitions observed by electron microscopy. One transition involves VLDL fusion, partial rupture, and dissociation of small spherical particles (d = 7-15 nm), and another involves complete lipoprotein disintegration and lipid coalescence into droplets accompanied by dissociation of apolipoprotein B. The small particles, which are unique to VLDL denaturation, are comparable in size and density to high-density lipoproteins (HDL); they have an apolar lipid core and polar surface composed of exchangeable apolipoproteins (E and possibly Cs) and phospholipids. We conclude that, similar to HDL and LDL, VLDL are stabilized by kinetic barriers that prevent particle fusion and rupture and decelerate spontaneous interconversion among lipoprotein classes and subclasses. In addition to fusion, VLDL disruption involves transient formation of HDL-like particles that may mimic protein exchange among VLDL and HDL pools in plasma.     

LDL particle subspecies are distinct in their capacity to mediate free cholesterol efflux via the SR-BI/Cla-1 receptor

The human scavenger receptor SR-BI/Cla-1 promotes efflux of free cholesterol from cells to both high-density and low-density lipoproteins (HDL, LDL). SR-BI/Cla-1-mediated cholesterol efflux to HDL is dependent on particle size, lipid content and apolipoprotein conformation; in contrast, the capacity of LDL subspecies to accept cellular cholesterol via this receptor is indeterminate. Cholesterol efflux assays were performed with CHO cells stably transfected with Cla-1 cDNA. Expression of Cla-1 in CHO cells induced elevation in total cholesterol efflux to plasma, LDL and HDL. Such Cla-1-specific efflux was abrogated by addition of anti-Cla-1 antibody. LDL were fractionated into five subspecies either on the basis of hydrated density or size. Among LDL subfractions, small dense LDL (sdLDL) were 1.5-to 3-fold less active acceptors for Cla-1-mediated cellular cholesterol efflux. Equally, sdLDL markedly reduced Cla-1-specific cholesterol efflux to large buoyant LDL in a dose-dependent manner. Conversely, sdLDL did not influence efflux to HDL(2). These findings provide evidence that LDL particles are heterogeneous in their capacity to promote Cla-1-mediated cholesterol efflux. Relative to HDL(2), large buoyant LDL may constitute physiologically-relevant acceptors for cholesterol efflux via Cla-1.     

Evidence that apoB-100 of low-density lipoproteins is a novelsrc-related protein kinase

Protein-tyrosine kinases of signal transduction pathways occur and function intracellularly. In contrast, the low-density lipoprotein (LDL) particle circulates in plasma, where its function is to solubilize and transport lipid. Recently, several reports showed that LDL may have a role in signal transduction. We have identified a region in the apoB-100 primary structure which shows similarity to Src-homology-1 (SH1) domains, the kinase region of protein-tyrosine kinases. Results obtained in protein kinase assays of highly purified LDL showed that only the apoB-100 was phosphorylated, suggesting that apoB-100 has the capacity to undergo autophosphorylation like known protein-tyrosine kinases. Phosphorylation was not observed for any other apolipoprotein in LDL or for any component of high-density lipoprotein and lipoprotein [a]. Our results suggest that apoB-100 may be a novel and functional member of thesrc protein kinase family.     

Evidence that apoB-100 of low-density lipoproteins is a novelsrc-related protein kinase

Protein-tyrosine kinases of signal transduction pathways occur and function intracellularly. In contrast, the low-density lipoprotein (LDL) particle circulates in plasma, where its function is to solubilize and transport lipid. Recently, several reports showed that LDL may have a role in signal transduction. We have identified a region in the apoB-100 primary structure which shows similarity to Src-homology-1 (SH1) domains, the kinase region of protein-tyrosine kinases. Results obtained in protein kinase assays of highly purified LDL showed that only the apoB-100 was phosphorylated, suggesting that apoB-100 has the capacity to undergo autophosphorylation like known protein-tyrosine kinases. Phosphorylation was not observed for any other apolipoprotein in LDL or for any component of high-density lipoprotein and lipoprotein [a]. Our results suggest that apoB-100 may be a novel and functional member of thesrc protein kinase family.     

Modification of human low-density lipoprotein by the lipid peroxidation product 4-hydroxynonenal

The effects of the lipid peroxidation product 4-hydroxynonenal on freshly prepared human low-density lipoprotein (LDL) were studied. At a fixed LDL concentration (5.7 mg/ml) the amount of 4-hydroxynonenal incorporated into the LDL increased with increasing aldehyde concentration from 28-30 (0.2 mM) to 140 (1 mM) mol per mol LDL, whereas at a fixed aldehyde concentration (0.2 mM) its incorporation into LDL decreased with increasing LDL concentration from 48 (1 mg LDL/ml) to 26 (12 mg LDL/ml) mol 4-hydroxynonenal bound per mol LDL. Of the total hydroxynonenal taken up 78% was bound to the protein and 21% to the lipid moiety; the remaining 1% was dissolved as free aldehyde in the lipid fraction. Amino acid analysis of the apolipoprotein B revealed that 4-hydroxynonenal attacks mainly the lysine and tyrosine residues and to a lesser extent also serine, histidine and cysteine. Treatment of LDL with 4-hydroxynonenal results in a concentration-dependent increase of the negative charge of the LDL particle as evidenced by its increased electrophoretic mobility. Moreover, 4-hydroxynonenal treatment leads to a partial conversion of the apolipoprotein B-100 into higher molecular weight forms most probably apolipoproteins B-126 and B-151. Compared to malonaldehyde, 4-hydroxynonenal exhibits a much higher capacity to modify LDL and it is therefore believed that this aldehyde is a more likely candidate for being responsible for LDL modification under in vivo lipid peroxidation conditions.     

Conversion of human low density lipoprotein into a very low density lipoprotein-like particle in vitro.

The lipid substrate specificity of Manduca sexta lipid transfer particle (LTP) was examined in in vitro lipid transfer assays employing high density lipophorin and human low density lipoprotein (LDL) as donor/acceptor substrates. Unesterified cholesterol was found to exchange spontaneously between these substrate lipoproteins, and the extent of transfer/exchange was not affected by LTP. By contrast, transfer of labeled phosphatidylcholine and cholesteryl ester was dependent on LTP in a concentration-dependent manner. Facilitated phosphatidylcholine transfer occurred at a faster rate than facilitated cholesteryl ester transfer; this observation suggests that either LTP may have an inherent preference for polar lipids or the accessibility of specific lipids in the donor substrate particle influences their rate of transfer. The capacity of LDL to accept exogenous lipid from lipophorin was investigated by increasing the high density lipophorin:LDL ratio in transfer assays. At a 3:1 (protein) ratio in the presence of LTP, LDL became turbid (and aggregated LDL were observed by electron microscopy) indicating LDL has a finite capacity to accept exogenous lipid while maintaining an overall stable structure. When either isolated human non B very low density lipoprotein (VLDL) apoproteins or insect apolipophorin III (apoLp-III) were included in transfer experiments, the sample did not become turbid although lipid transfer proceeded to the same extent as in the absence of added apolipoprotein. The reduction in sample turbidity caused by exogenous apolipoprotein occurred in a concentration-dependent manner, suggesting that these proteins associate with the surface of LDL and stabilize the increment of lipid/water interface created by LTP-mediated net lipid transfer. The association of apolipoprotein with the surface of modified LDL was confirmed by sodium dodecyl sulfate-polyacrylamide gel electrophoresis analysis, and scanning densitometry revealed that apoLp-III bound to the surface of LDL in a 1:14 apoB:apoLp-III molar ratio. Electron microscopy showed that apoLp-III-stabilized modified LDL particles have a larger diameter (29.2 +/- 2.6 nm) than that of control LDL (22.7 +/- 1.9 nm), consistent with the observed changes in particle density, lipid, and apolipoprotein content. Thus LTP-catalyzed vectorial lipid transfer can be used to introduce significant modifications into isolated LDL particles and provides a novel mechanism whereby VLDL-LDL interrelationships can be studied.     

Theoretical model of human apolipoprotein B100 tertiary structure

Low density lipoprotein (LDL) particles are the main cholesterol carriers in human plasma. The organization of the particle, composed of apolar lipids and phospholipid monolayer stabilized by apolipoprotein B100 (apoB), is highly complex and still unknown. ApoB is an extremely large protein (4563 amino acids) and very little is known about its structure. A 3D model of the N-terminal region has been recently proposed and has provided interesting insights about the physico-chemical properties of the protein and putative interaction zones with lipids. In the present article, we propose the first tentative 3D modelling for most remaining residues. All predicted features emerging from the models are confronted with agreement to experimental data available. Using different up-to-date prediction methods, we decomposed the protein into eight domains and predicted 3D structure for each of them. The analysis of hydrophobic patches, polar regions, coupled with functional predictions based on the 3D models, gives new clues to understanding of the functional role of apoB. We suggest precise regions putatively involved in the lipid interactions, and discuss the position of apoB on the LDL particle. Finally, we propose relative organization of the domains, providing a shape quite compatible with the low resolution electron microscopy map.     

Nascent Astrocyte Particles Differ from Lipoproteins in CSF

Abstract: Little is known about lipid transport and metabolism in the brain. As a further step toward understanding the origin and function of CNS lipoproteins, we have characterized by size and density fractionation lipoprotein particles from human CSF and primary cultures of rat astrocytes. The fractions were analyzed for esterified and free cholesterol, triglyceride, phospholipid, albumin, and apolipoproteins (apo) E, AI, AII, and J. As determined by lipid and apolipoprotein profiles, gel electrophoresis, and electron microscopy, nascent astrocyte particles contain little core lipid, are primarily discoidal in shape, and contain apoE and apoJ. In contrast, CSF lipoproteins are the size and density of plasma high-density lipoprotein, contain the core lipid, esterified cholesterol, and are spherical. CSF lipoproteins were heterogeneous in apolipoprotein content with apoE, the most abundant apolipoprotein, localized to the largest particles, apoAI and apoAII localized to progressively smaller particles, and apoJ distributed relatively evenly across particle size. There was substantial loss of protein from both CSF and astrocyte particles after density centrifugation compared with gel-filtration chromatography. The differences between lipoproteins secreted by astrocytes and present in CSF suggest that in addition to delivery of their constituents to cells, lipoprotein particles secreted within the brain by astrocytes may have the potential to participate in cholesterol clearance, developing a core of esterified cholesterol before reaching the CSF. Study of the functional properties of both astrocyte-secreted and CSF lipoproteins isolated by techniques that preserve native particle structure may also provide insight into the function of apoE in the pathophysiology of specific neurological diseases such as Alzheimer's disease.     

Changes in the secondary structure of apolipoprotein B-100 after Cu2+-catalysed oxidation of human low-density lipoproteins monitored by Fourier transform infrared spectroscopy

Fourier transform infrared (FTIR) spectra have been obtained of human low-density lipoproteins (LDL) in H2O and 2H2O buffers. The absorption bands are assigned to vibrations of the lipid and apolipoprotein B-100 components. The analysis of second-derivative spectra allowed an assignment of individual protein bands to alpha-helical, random, coil or beta-structure and beta-turn conformations. Changes in the FTIR spectra after Cu2+-catalysed oxidation of the LDL particles indicate that the structure of apolipoprotein B-100 becomes less ordered, with some alterations of alpha-helical and beta-turn conformation. The main beta-structure absorption at 1620 cm-1 is unaffected by oxidation. Taking into account the resistance to oxidation and the slow H-2H exchange it is suggested that the beta-structure is hidden from external factors whereas other structures are mostly present on the surface of the LDL particle. Oxidation affects mainly the surface region of apolipoprotein B-100 and leads to a structural rearrangement which consequently changes the receptor specificity of the LDL.     

Predicting the structure of apolipoprotein A-I in reconstituted high-density lipoprotein disks.

In reconstituted high-density lipoproteins, apolipoprotein A-I and phosphatidylcholines combine to form disks in which the amphipathic alpha-helices of apolipoprotein A-1 bind to the edge of a lipid bilayer core, shielding the hydrophic lipid tails from the aqueous environment. We have employed experimental data, sequence analysis, and molecular modeling to construct an atomic model of such a reconstituted high-density lipoprotein disk consisting of two apolipoprotein A-I proteins and 160 palmitoyloleoylphosphatidylcholine lipids. The initial globular domain (1-47) of apolipoprotein A-I was excluded from the model, which was hydrated with an 8-A shell of water molecules. Molecular dynamics and simulated annealing were used to test the stability of the model. Both head-to-tail and head-to-head forms of a reconstituted high-density lipoprotein were simulated. In our simulations the protein contained and adhered to the lipid bilayer while providing good coverage of the lipid tails.     

Alterations in plasma lipoproteins and apolipoproteins associated with estrogen-induced hyperlipidemia in the laying hen

The laying hen represents a physiological model in which the mechanisms of action of estrogens on lipid transport can be evaluated. The plasma lipoproteins in the laying hen were subfractionated into discrete particle species by isopycnic density gradient ultracentrifugation and the physicochemical properties and apolipoprotein contents of individual subfractions evaluated. The qualitative and quantitative aspects of this estrogen-specific profile were then compared to those of the immature chicken. As observed earlier, estrogens induced dramatic elevation in very-low-density lipoproteins (VLDL) (up to 900 mg/dl). Indeed, triglyceride-rich lipoproteins with densities up to 1.035 g/ml, i.e. VLDL and their remnants, behaved as a continuum which displayed little variation in size (20.5-21 nm), electrophoretic mobility (beta-like) and apolipoprotein content; apo B-100 (540 kDa) predominated while apo A-I (27 kDa), apo VLDL-II (19 kDa) and an apo-C-like protein (13 kDa) were present as minor components. The typical high-density lipoproteins (HDL) in the immature chicken were replaced by a lipoprotein population whose physicochemical properties were quite distinct. Thus these particles were distributed as a single, asymmetric peak over the density range 1.030-1.158 g/ml, a wide interval which overlapped that of apo-B-rich particles at its lower limit. The rho 1.030-1.158 g/ml lipoproteins were present at concentrations (approximately equal to 200 mg/dl) some twofold to threefold lower than those of HDL in immature birds. Furthermore, they displayed physical and chemical properties in common with both low-density lipoproteins (LDL) and HDL and were LDL-like in exhibiting beta mobility but HDL-like in size (9-15 nm diameter). Their protein moiety was also HDL-like in its predominant content of apo A-I; small amounts of apo VLDL-II and the apo-C-like protein were also detected. Substantial amounts of lipid were found at rho greater than 1.195 g/ml: such substances are absent in the immature chicken and may reflect the presence of vitellogenins. The hyperestrogenic state in the laying hen is therefore associated with major modifications in lipoprotein and apolipoprotein profile. Such modifications may be of relevance to clinical disorders involving estrogen-induced hyperlipidemia.     

Structure of human low-density lipoprotein subfractions determined by X-ray small-angle scattering

The structure of low-density lipoprotein (LDL) particles from three different density ranges (LDL-1: d = 1.006−1.031 g/ml; LDL-3: d = 1.034−1.037 g/ml; LDL-6: d = 1.044−1.063 g/ml) was determined by X-ray small-angle scattering. By using a theoretical particle model, which accounted for the polydispersity of the samples, we were able to obtain fits of the scattering intensity that were inside the noise interval of the measured intensity. The assumption of deviations from radial symmetry is not supported by our data. This implies a spread-out conformation of the apolipoprotein B (apoB) molecule, which appears to be localized in the outer surface shell. A globular structure is not consistent with our data. Furthermore, different models exist concerning the structure of the cholesterol ester core below the phase transition temperature. The electron density data suggest an arrangmeent in which the steroid moieties are localized at average radii of 3.2 and 6.4 nm. Model calculations show that packing problems can only be avoided if approximately half of the acyl chains of each shell are pointing towards the center of the particle, the other half towards the surface. This arrangement of the acyl chains has never been proposed before. The LDL particles of different density classes differ mainly with respect to the size of the core but also with respect to the width of the surface shells. Model calculations show that the size of different LDL particles can be accurately predicted from the compositional data.     

The effect of histidine modification on copper-dependent lipid peroxidation in human low-density lipoprotein

Summary

Lipid peroxidation and subsequent oxidative modification of low-density lipoprotein (LDL) have been implicated as causal events in atherosclerosis. Cu²⁺ may play an important role in LDL oxidation by binding to histidine residues of apolipoprotein B-100 (apo B) and initiating and propagating lipid peroxidation. To investigate the role of histidine residues, we used diethylpyrocarbonate (DEPC), a lipid-soluble histidine-specific modifying reagent. When LDL (0.1 mg protein/ml, or 0.2 µM) was incubated with DEPC (1 mM), at least 76 ± 7% of the histidine residues in apo B were modified. Treatment of LDL with DEPC led to an increase in the rate of Cu²⁺-induced initiation of lipid peroxidation (R_i), but a significant decrease in the rate of propagation. These changes resulted in an overall increased resistance of LDL to oxidation, with a significantly increased lag phase preceding the propagation phase of lipid peroxidation. In contrast to DEPC, ascorbate completely prevented the initiation of LDL oxidation (R_i = 0). Our data indicate that there are two types of copper/histidine binding sites on apo B: those facing the lipid core of the LDL particle, which mediate the propagation of lipid peroxidation and are modified by DEPC; and those found on the surface of the LDL particle exposed to the aqueous environment, which are responsible for mediating the initiation of lipid peroxidation and are modifiable by ascorbate in the presence of Cu²⁺.