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.     

Discrete subspecies of human low density lipoproteins are heterogeneous in their interaction with the cellular LDL receptor.

The low density lipoproteins (LDL) of human plasma consist of a series of discrete particle subspecies of distinct physicochemical, immunological, and hydrodynamic properties. Such structural differences are intimately linked to the metabolic heterogeneity of circulating LDL in vivo. The current studies were designed to evaluate and compare the interaction of discrete LDL subspecies from normolipidemic subjects with the LDL receptor. Plasma LDL of d 1.019-1.063 g/ml from healthy males were fractionated into 15 subspecies of defined physicochemical characteristics by isopycnic density gradient ultracentrifugation as described earlier (Chapman et al., J. Lipid Res. 1988. 29: 442-458). The major LDL subspecies, LDL-5 to LDL-10, exhibited an overall range in density from 1.0244 to 1.0435 g/ml; individual subspecies increased in density by increments of 0.027 (LDL-5), 0.026 (LDL-6), 0.030 (LDL-7), 0.031 (LDL-8), 0.035 (LDL-9), and 0.042 g/ml (LDL-10), respectively. Taken together, these subspecies accounted for approximately 70% of the total mass of LDL of d 1.019-1.063 g/ml; their cholesterol: protein ratios decreased from 1.70 to 1.12 and particle size from 275 to 260 A with increase in density. ApoB-100 was the unique protein component in subspecies 5-8, with trace amounts (less than 0.2% of apoLDL) of both apoA-I and apoE in subspecies 9 and 10. The interaction of individual LDL subspecies with the LDL receptor on cultured human U-937 monocyte-like cells was compared by determining receptor binding affinities at 4 degrees C. Scatchard analysis of specific binding curves demonstrated a single class of binding site for each subspecies. The lowest dissociation constants were displayed by LDL subspecies 6 (Kd 5.71 nM), 7 (Kd 5.24 nM) and 8 (Kd 4.67 nM), while subspecies 5, 9, and 10 displayed significantly higher Kd values (8.35, 7.20, and 6.87 nM, respectively). Competitive displacement studies at 4 degrees C, in which unlabeled subspecies from the same gradient series competed for binding with 125I-labeled LDL subspecies, confirmed the relative binding affinities of these subspecies. As the hydrophobic lipid core of LDL undergoes a thermotropic transition at approximately 37 degrees C, which may in turn influence the surface structure of the particle, internalization and degradation studies were performed at 37 degrees C. No effect of temperature was detectable; again, LDL subspecies at each extreme of the density distribution (LDL-5 and LDL-10) displayed significantly lower binding affinities for the LDL receptor than that from the peak region (LDL-7).(ABSTRACT TRUNCATED AT 400 WORDS)     

Crystallization and preliminary X-ray diffraction data of two different human low-density lipoprotein (LDL) subfractions

Human LDL subfractions LDL-2 (d = 1.031–1.034 g/ml) and LDL-5 (d = 1.040–1.044 g/ml) were crystallized in two different crystal forms by using polyethylene glycol as a precipitant. Both fractions were from one donor. Crystals of LDL-5 were yellow, hexagonal, and showed no dichroism. Crystals of LDL-2 were of the same color, had a rodlike shape with notches at both ends, and were highly dichroitic. LDL-2 crystals diffracted to a resolution of 29 Å by using synchrotron radiation. Indexing in P1 resulted in preliminary parameters for the reduced cell of a = 171 Å, b = 438 Å, c = 519 Å, α = 102°, β = 99°, γ = 91. These dimensions are consistent with the size of LDL particles. Using Fourier transform infrared spectroscopy (FTIR) and agarose gel electrophoresis, we could further confirm that the crystals consist of LDL. The FTIR spectrum showed bands characteristic for lipids and protein. Dissolved crystals exhibited a mobility similar to native LDL in agarose gels and could be stained with anti-human apolipoprotein B (apoB). Proteins 28:293–297, 1997. © 1997 Wiley-Liss Inc.     

Guinea pig low density lipoproteins: structural and metabolic heterogeneity

The structural and metabolic heterogeneity of low density lipoproteins (LDL, d 1.024-1.100 g/ml) has been investigated in the guinea pig. Two LDL subfractions, of d 1.024-1.050 and 1.050-1.100 g/ml, respectively, were isolated by sequential ultracentrifugation; while both were enriched in cholesteryl ester and apoB-100, the former was heterogeneous displaying three particle size species of diameters 26.9, 25.6, and 24.7 nm, whereas the denser subfraction was relatively homogeneous containing a single, smaller species (diam. 23.6 nm). The fractional catabolic rates (FCR) of the two LDL subfractions were alike (approximately 0.090 pools/hr) in the guinea pig in vivo. After modification of each subfraction by reductive methylation, the FCRs were reduced similarly and indicated that 70-80% of degradation occurred via the cellular LDL receptor pathway. However, the intravascular metabolism of these LDL subfractions, determined from the radioactive content of density gradient fractions as a function of time after injection of radiolabeled native or chemically modified LDL, tended to be distinct. Thus, while radiolabeled apoB-100 in the lighter subfraction maintained the initial density profile up to 48 hr, the radioactive profile of its methylated counterpart changed, the proportion of radioactivity in the lighter gradient fractions (d 1.027-1.032 g/ml) increasing while that in the denser (d 1.037-1.042 g/ml) fractions diminished. A more marked transformation occurred in LDL of d 1.050-1.100 g/ml, in which the radioactive profile shifted towards lighter particles of the d 1.024-1.050 g/ml species; this shift was partially dependent on the LDL receptor, since it was more pronounced in the methylated subfraction. Furthermore, a net increase in the radioactive content of gradient subfractions 7 to 9 (d 1.032-1.042 g/ml) was found 10 hr after injection of methylated LDL of d 1.050-1.100 g/ml, at which time the bulk of LDL radioactivity had been removed from plasma. Several mechanisms, acting alone or in combination, may account for these findings; among them, some degree of transformation of dense to lighter LDL species appears a prerequisite. In conclusion, our data attest to the structural heterogeneity of circulating LDL in the guinea pig, and suggest that the intravascular processing and metabolism of LDL particle subspecies is directly related to their structure and physicochemical properties.     

Further resolution of the low density lipoprotein spectrum in normal human plasma: physicochemical characteristics of discrete subspecies separated by density gradient ultracentrifugation

The molecular basis of the heterogeneity of plasma low density lipoproteins (LDL, d 1.024-1.050 g/ml) was evaluated in 40 normolipidemic male subjects following fractionation by isopycnic density gradient ultracentrifugation into eight major subspecies. The mass profile of our subjects' LDL uniformly displayed single symmetric or asymmetric peaks as a function of density; the peak occurred most frequently (20 subjects) in subfraction 7 (d 1.0297-1.0327 g/ml). Several physicochemical properties (hydrodynamic behavior, electrophoretic mobility, chemical composition, size and particle heterogeneity, and apolipoprotein heterogeneity) of the LDL subfractions were examined. Hydrodynamic analyses revealed unimodal distributions and distinct peak Sf degree rates in individual subfractions. Such behavior correlated well with particle size and heterogeneity data, in which LDL subspecies were typically resolved as unique narrow bands by gradient gel electrophoresis. Subspecies with average densities of 1.024 to 1.0409 g/ml ranged from 229 to 214 A in particle diameter. LDL protein content increased in parallel with density while the proportion of triglyceride diminished; cholesteryl esters predominated, accounting for approximately 40% or more by weight. Distinct differences in net electric charge were demonstrated by electrophoresis in agarose gel, the subspecies with average density of 1.0314 g/ml displaying the lowest net negative charge. ApoB-100 was the major apoprotein in all subspecies, and constituted the unique protein component over the density interval 1.0271-1.0393 g/ml. ApoE and apo[a] were detected at densities less than 1.0271 and greater than 1.0393 g/ml. While apoE was evenly distributed within these two regions, representing up to 2% of apoLDL, the distribution of apo[a] was skewed towards the denser region, in which it amounted to 3-7% of apoLDL. ApoC-III was detectable as a trace component at densities greater than 1.0358 g/ml. Calculation of the number of molecules of each chemical component per LDL subspecies showed the presence of one copy of apoB-100 per particle, in association with decreasing amounts of cholesteryl ester, free cholesterol, and phospholipid. These data indicate that a similar overall molecular organization and structure is maintained in a unimodal distribution of LDL particle subspecies over the density range approximately 1.02 to 1.05 g/ml. In sum, our data may be interpreted to suggest that microheterogeneity in the physicochemical properties of human LDL subspecies reflects dissimilarities in their origins, intravascular metabolism, tissular fate, and possibly in their atherogenicity.     

Receptor-mediated binding and degradation of subfractions of human plasma low-density lipoprotein by cultured fibroblasts

The receptor-mediated metabolism of human plasma low-density lipoprotein (LDL) subfractions was studied. LDL was isolated from healthy donors and further fractionated by density gradient ultracentrifugation into three subfractions: (I) d = 1.031-1.037, (II) d = 1.037-1.041 and (III) d = 1.041-1.047 g/ml, comprising 24 +/- 7%, 46 +/- 8% and 30 +/- 9% of the total LDL protein, respectively. As assessed by electron microscopy and gradient gel electrophoresis, the LDL particle size decreased and the relative protein content increased from fraction I towards fraction III. Fraction II had the highest (Kd 2.6 micrograms/ml) and fraction I the lowest (Kd 5.8 micrograms/ml) binding affinity to LDL receptors of human fibroblasts at 4 degrees C. The rate of receptor-mediated degradation of fraction II was also higher than that of the other two fractions at 37 degrees C. These results suggest that LDL subfractions have different rates of receptor-mediated catabolism depending on particle size or composition, and therefore their metabolic fate and atherogenic properties may also differ.     

Density distribution and physicochemical properties of plasma lipoproteins and apolipoproteins in the goose, Anser anser, a potential model of liver steatosis

The fractionation and physicochemical characterization of the complex molecular components composing the plasma lipoprotein spectrum in the goose, a potential model of liver steatosis, are described. Twenty lipoprotein subfractions (d less than 1.222 g/ml) were separated by isopycnic density gradient ultracentrifugation, and characterized according to their chemical composition, particle size and particle heterogeneity, electrophoretic mobility, and apolipoprotein content. Analytical ultracentrifugal analyses showed high density lipoproteins (HDL) to predominate (approximately 450 mg/dl plasma), the peak of its distribution occurring at d approximately 1.090 g/ml (F1.21 approximately 2.5). The HDL class displayed marked density heterogeneity, HDL1-like particles being detected up to a lower density limit of approximately 1.020 g/ml, particle size decreasing progressively from 17-19 nm at d 1.024-1.028 g/ml to 10.5-12 nm (d 1.055-1.065 g/ml), and then remaining constant (approximately 9 nm) at densities greater than 1.065 g/ml. HDL subfractions displayed multiple size species; five subspecies were present over the range d 1.103-1.183 g/ml with diameters of 10.5, 9.9, 9.0, 8.2, and 7.5 nm, four in the range d 1.090-1.103 g/ml (diameters 10.5, 9.9, 9.0, and 8.2 nm) and three over the range d 1.076-1.090 g/ml (diameters 10.5, 9.9, and 9.0 nm). ApoA-I (Mr 25,000-27,000) was the major apolipoprotein in all goose HDL subfractions, while the minor components (apparent Mr 100,000, 91,000, 64,000, 58,000, approximately 42,000, 18,000 and apoC-like proteins) showed marked quantitative and qualitative variation across this density range (i.e., 1.055-1.165 g/ml). The d 1.063 g/ml boundary for separation of goose low density lipoproteins (LDL) from HDL was inappropriate, since HDL-like particles were present in the density interval 1.024-1.063 g/ml, while particles enriched in apoB (Mr approximately 540,000) and resembling LDL in size (approximately 20.5 nm) were detected up to a density of approximately 1.076 g/ml. Goose LDL itself was a major component of the profile (90-172 mg/dl) with a single peak of high flotation rate (Sf approximately 10.5). The physicochemical properties and apolipoprotein content of intermediate density lipoproteins (IDL) and LDL varied but little over the range d 1.013-1.040 g/ml, presenting as two particle species (diameters 20.5 and 21 nm) of essentially constant chemical composition; LDL (d 1.019-1.040 g/ml) were separated from HDL1 by gel filtration chromatography and appeared to contain primarily apoB with lesser amounts of apoA-I.(ABSTRACT TRUNCATED AT 400 WORDS)     

Structure of the dimyristoylphosphatidylcholine vesicle and the complex formed by its interaction with apolipoprotein C-III: X-ray small-angle scattering studies.

Single bilayer vesicles of dimyristoylphosphatidylcholine have been investigated by small-angle X-ray scattering at 28 degrees C. The results indicate that these vesicles are hollow spherical shell structures with an outer radius of approximately 12 nm and a molecular weight of (3.2 +/- 0.5) X 10(6). The shell was found to be 4.4 +/- 0.2 nm thick with a cross-sectional electron-density profile characteristic for a single phospholipid bilayer. Upon interaction of these vesicles with apolipoprotein C-III from human very low density lipoproteins at a protein/lipid ratio greater than 0.08 (g/g), a complex containing 0.25 g of protein/g of lipid, with molecular weight of (3.9 +/- 0.4) X 10(5), is formed. The shape analysis indicates a highly asymmetric particle with an internal partition of low and high electron density resembling that produced by a bilayer structure. Model calculations and curve-fitting procedures show good agreement between the experimental scattering curve and that computed for an oblate ellipsoidal structure with dimensions of 17 X 17 X 5 nm and a 1 nm thick shell of high electron density surrounding the core of low electron density.     

Enhancing the contrast of ApoB to locate the surface components in the 3D density map of human LDL

A 26 Å resolution map of the structure of human low-density lipoprotein (LDL) was obtained from electron cryomicroscopy and single-particle image reconstruction. The structure showed a discoidal-shaped LDL particle with high-density regions mainly distributed at the edge of the particle and low-density regions at the flat surface that covers the core region. To determine the chemical components that correspond to these density regions and to delineate the distribution of protein and phospholipid located at the particle surface at the resolution of the map, we used Mono-Sulfo-NHS-Undecagold labeling to increase preferentially the contrast of the apolipoprotein B component on the LDL particle. In the three-dimensional map from the image reconstruction of the undecagold-labeled LDL particles, the high-density region from the undecagold label was distributed mainly at the edge of the particle, and lower density regions were found at the flat surfaces that cover the neutral lipid core. This suggests that apolipoprotein B mainly encircles LDL at the edge of the particle and the phospholipid monolayers are located at the flat surfaces, which are parallel to the cholesterol ester layers in the core and may interact with the core lipid layers through the acyl chains.     

Plasma lipoproteins and apolipoproteins in the preruminant calf, Bos spp: density distribution, physicochemical properties, and the in vivo evaluation of the contribution of the liver to lipoprotein homeostasis

The in vivo role of the liver in lipoprotein homeostasis in the preruminant calf, a functional monogastric, has been evaluated. To this end, the hydrodynamic and physicochemical properties, density distribution, apolipoprotein content, and flow rates of the various lipoprotein particle species were determined in the hepatic afferent (portal vein and hepatic artery) and efferent (hepatic vein) vessels in fasting, 3-week-old male preruminant calves. Plasma lipoprotein profiles were established by physicochemical analyses of a series of subfractions isolated by isopycnic density gradient ultracentrifugation. Triglyceride-rich very low density lipoproteins (VLDL) (d less than 1.018 g/ml) were minor plasma constituents (approximately 1% or less of total d less than 1.180 g/ml lipoproteins). The major apolipoproteins of VLDL were apoB-like species, while the complement of minor components included bovine apoA-I and apoC-like peptides. Particles with diameters (193-207 A) typical of low density lipoproteins (LDL) were present over the density interval 1.026-1.076 g/ml; however, only LDL of d 1.026-1.046 g/ml were present as a unique and homogeneous size subspecies, containing the two apoB-like species as major protein components in addition to elevated cholesteryl ester contents. LDL represented approximately 10% of total d less than 1.180 g/ml lipoproteins in fasting plasma from all three hepatic vessels. Overlap in the density distribution of particles with the diameters of LDL and of high density lipoproteins (HDL) occurred in the density range from 1.046 to 1.076 g/ml; these HDL particles were 130-150 A in diameter. HDL were the major plasma particles (approximately 90% of total d less than 1.180 g/ml substances) and presented as two distinct populations which we have termed light (HDLL) and heavy (HDLH) HDL. Light HDL (d 1.060-1.091 g/ml) ranged in size from 120 to 140 A, and were distinguished by their high cholesteryl ester (29-33%) and low triglyceride (1-3%) contents; apoA-I was the principal apolipoprotein. Small amounts of apolipoproteins with Mr less than 60,000, including apoC-like peptides, were also present. Heavy HDL (d 1.091-1.180 g/ml) accounted for almost half (47%) of total calf HDL, and like HDLL, were also enriched in cholesteryl ester and apoA-I; they ranged in size from 93 to 120 A. The protein moiety of HDLH was distinct in its possession of an apoA-IV-like protein (Mr 42,000). Blood flow rates were determined by electromagnetic flowmetry, thereby permitting determination of net lipoprotein balance across the liver. VLDL were efficiently removed during passage through the liver (net uptake 1.06 mg/min per kg body weight).(ABSTRACT TRUNCATED AT 400 WORDS)     

Characterization of equine plasma lipoproteins after separation by density gradient

1. Plasma lipoproteins from six thoroughbred horses were separated by density gradient ultracentrifugation. For each sample, lipoprotein bands were visualized by means of a prestained plasma control and characterized by electrophoretic, chemical and morphological analysis. 2. Very low density lipoproteins (VLDL) were isolated at d less than 1.018 g/ml. 3. Two clearly resolved bands were detected in the low density lipoprotein fraction (LDL). The density limits were evaluated as follows: LDL1(1.028 less than d less than 1.045 g/ml) and LDL2(1.045 less than d less than 1.070 g/ml). Marked differences were observed in the chemical composition and particle size of LDL1 and LDL2 fractions. 4. High density lipoprotein fraction (HDL) was usually isolated as a single band, distributed over the range 1.075 less than d less than 1.180 g/ml. However, chemical composition and particle size revealed heterogeneity in HDL subfractions. 5. The density limit of LDL and HDL bands varied in each animal, indicating differences in equine lipoprotein distribution.     

The visceral yolk sac--an important site of synthesis and secretion of apolipoprotein B containing lipoproteins in the feto-placental unit of the rat.

Rat fetuses exhibit a high serum LDL concentration at term. Delivery caused a marked decrease of the LDL apolipoprotein (apo) B concentration independent of whether this occurred on days 21, 22 or 23 of gestation. The interruption of the yolk sac circulation by a ligature in situ for 6 h led to the same alterations of the LDL-apo B concentration as Caesarean section. Immunoelectronmicroscopic studies provided evidence that the epithelial cells of the visceral yolk sac exhibited electron dense LDL-sized and apo B containing particles which were localized over the compartments of the Golgi complexes, endoplasmatic reticulum, secretory vesicles and intercellular spaces, but not over the cell nuclei, mitochondria or lysosomes. ApoB containing LDL-sized particles could be obtained by ultracentrifugation from the disrupted material of the microsomal fraction of yolk sac homogenates. Isolated segments of the yolk sac membranes were capable to secrete apoB containing lipoproteins floating in the d less than 1.020 g/ml as well as in the d = 1.020-1.064 g/ml fraction with a 10-fold higher amount of apoB in the higher density class. Incorporation experiments with [35S] methionine gave evidence that these lipoproteins were at least partially provided with newly synthesized apoB predominantly found in the LDL fraction. The size of the negatively stained particles in the d = 1.020-1.064 g/ml fraction secreted from yolk sac segments corresponded to that of LDL from fetal rat serum. In contrast their acylglycerol content was significantly higher, whereas the percentage contribution of total cholesterol and protein was markedly reduced in comparison with serum LDL of the fetus. In summary, biochemical and ultrastructural studies provide clear cut evidence that the rat yolk sac is able to synthesize and to deliver apo B containing lipoproteins in the density ranges of VLDL, IDL and particular of LDL thus contributing to the supply of serum lipoproteins in the rat fetus. By recalculation of recent tracer kinetic data (Plonné et al. (1990) J. Lipid Res. 31, 747) using a mathematical step function model it was possible to assess the contribution of the rat yolk sac to the LDL influx into the fetal serum.     

High-density lipoprotein particle uptake and selective uptake of high-density lipoprotein-associated cholesteryl esters by J774 macrophages

High-density lipoprotein (HDL) cholesteryl esters are taken up by fibroblasts via HDL particle uptake and via selective uptake, i.e., cholesteryl ester uptake independent of HDL particle uptake. In the present study we investigated HDL selective uptake and HDL particle uptake by J774 macrophages. HDL3 (d = 1.125-1.21 g/ml) was labeled with intracellularly trapped tracers: 125I-labeled N-methyltyramine-cellobiose-apo A-I (125I-NMTC-apo A-I) to trace apolipoprotein A-I (apo A-I) and [3H]cholesteryl oleyl ether to trace cholesteryl esters. J774 macrophages, incubated at 37 degrees C in medium containing doubly labeled HDL3, took up 125I-NMTC-apo A-I, indicating HDL3 particle uptake (102.7 ng HDL3 protein/mg cell protein per 4 h at 20 micrograms/ml HDL3 protein). Apparent HDL3 uptake according to the uptake of [3H]cholesteryl oleyl ether (470.4 ng HDL3 protein/mg cell protein per 4 h at 20 micrograms/ml HDL3 protein) was in significant excess on 125I-NMTC-apo A-I uptake, i.e., J774 macrophages demonstrated selective uptake of HDL3 cholesteryl esters. To investigate regulation of HDL3 uptake, cell cholesterol was modified by preincubation with low-density lipoprotein (LDL) or acetylated LDL (acetyl-LDL). Afterwards, uptake of doubly labeled HDL3, LDL (apo B,E) receptor activity or cholesterol mass were determined. Preincubation with LDL or acetyl-LDL increased cell cholesterol up to approx. 3.5-fold over basal levels. Increased cell cholesterol had no effect on HDL3 particle uptake. In contrast, LDL- and acetyl-LDL-loading decreased selective uptake (apparent uptake 606 vs. 366 ng HDL3 protein/mg cell protein per 4 h in unloaded versus acetyl-LDL-loaded cells at 20 micrograms HDL3 protein/ml). In parallel with decreased selective uptake, specific 125I-LDL degradation was down-regulated. Using heparin as well as excess unlabeled LDL, it was shown that HDL3 uptake is independent of LDL (apo B,E) receptors. In summary, J774 macrophages take up HDL3 particles. In addition, J774 cells also selectively take up HDL3-associated cholesteryl esters. HDL3 selective uptake, but not HDL3 particle uptake, can be regulated.     

A density gradient study of the lipoprotein and apolipoprotein distribution in the chicken, Gallus domesticus

Plasma lipoproteins from 5-week old male chickens were separated over the density range 1.006-1.172 g/ml into 22 subfractions by isopycnic density gradient ultracentrifugation, in order to establish the distribution of these particles and their constituent apolipoproteins as a function of density. Lipoprotein subfractions were characterized by electrophorectic, chemical and morphological analyses, and their protein moieties were defined according to net charge at alkaline pH, molecular weight and isoelectric point. These analyses have permitted us to reevaluate the density limits of the major chicken lipoprotein classes and to determine their main characteristics, which are as follows: (1) very-low-density lipoproteins (VLDL), isolated at d less than 1.016 g/ml, were present at low concentrations (less than 0.1 mg/ml) in fasted birds; their mean diameter determined by gradient gel electrophoresis and by electron microscopy was 20.5 and 31.4 nm respectively; (2) as the the density increased from VLDL to intermediate density lipoproteins (IDL), d 1.016-l.020 g/ml) and low-density lipoproteins (LDL, d 1.020-1.046 g/ml), the lipoprotein particles contained progressively less triacylglycerol and more protein, and their Stokes diameter decreased to 20.0 nm; (3) apolipoprotein B-100 was the major apolipoprotein in lipoproteins of d less than 1.046 g/ml, with an Mr of 350000; small amounts of apolipoprotein B-100 were detectable in HDL subfractions of d less than 1.076 g/ml; urea-soluble apolipoproteins were present in this density range as minor components of Mr 38000-39000, 27000-28000 (corresponding to apolipoprotein A-1) and Mr 11000-12000; (4) high density lipoprotein (HDL, d 1.052-1.130 g/ml) was isolated as a single band, whose protein content increased progressively with increase in density; the chemical composition of HDL resembled that of human HDL2, with apolipoprotein A-1 (M 27000-28000) as the major protein component, and a protein of Mr 11000-12000 as a minor component; (5) heterogeneity was observed in the particle size and apolipoprotein distribution of HDL subfractions: two lipoprotein bands which additional apolipoproteins of Mr 13000 and 15000 were detected. These studies illustrate the inadequacy in the chicken of the density limits applied to fractionate the lipoprotein spectrum, and particularly the inappropriateness of the 1.063 g/ml density limit as the cutoff for LDL and HDL particle populations in the species.     

Structure of human serum lipoproteins in solution. II. Small-angle x-ray scattering study of HDL and LDL.

Two human serum lipoprotein particles, HDL₃ and LDL, were studied in solution in solvents of variable density (NaBr in water) by small-angle X-ray scattering using a position-sensitive proportional counter. The data were analysed using the theoretical approach outlined in the accompanying paper (Luzzati et al., 1976). The structures of the particles were found to be independent of the salt concentration of the solution (i.e. the particles are impenetrable to NaBr). Density heterogeneities are negligible and size and shape heterogeneities appear to be small.The particle structures could be quantitatively described in terms of a set of parameters and of a few one-dimensional functions. The parameters are the volume, radius of gyration and surface area of the shape functions; the second moment and square average of the electron density contrast at buoyancy; the electron density level, volume, radius of gyration and surface area of the hydrocarbon and polar regions. The one-dimensional functions are: the distribution of chords, the spherical average of the shape function and of the electron density at buoyancy, and the fraction of each spherical shell occupied by the hydrocarbon and polar regions. These parameters and functions are internally consistent and agree with the chemical data confirming the assumptions made in their derivation.The results are compatible with the shape of the particle being compact and quasi-spherical although with deeply convoluted surfaces. They also indicate that the outer layers of the particles are occupied by the proteins and the polar groups of phospholipids and free cholesterol, and the cores by neutral lipids. The maximum diameters of the particles are 130Å and 280Å for HDL₃ and LDL, respectively, while the hydrocarbon cores have diameters of 80Å and 230Å, respectively. The solvent is considered to penetrate to 25Å from the center of the HDL₃ particle with a minimum solvation at a radius of 45Å. In the case of LDL, the solvent penetrates to 55Å from the center of the particle. The lipids in the cores of the particles, particularly the cholesterol esters, appear to display a micelle-like organization with the steroid nuclei segregated in regions distinct from those occupied by the hydrocarbon chains.Although the data are consistent with several aspects of previously proposed models, they indicate that the structures of the HDL₃ and LDL particles are more complex than previously believed.     

Characterization of a more electronegatively charged LDL subfraction by ion exchange HPLC

Low density lipoproteins (LDL), collected from 32 normal male subjects (aged 30-60), were subfractionated by high resolution ion exchange chromatography (IE-HPLC). By this procedure two LDL subfractions were eluted. The first corresponds to normal LDL (nLDL); while the second one corresponds to a more electronegative subfraction, called LDL-. The mean percentage contribution of LDL- to native plasma LDL was of 3.9% (range 0.5-9.8%). The percentage concentration of LDL- in total native LDL did not correlate with plasma total cholesterol, triglycerides, and LDL cholesterol, whereas a significant negative correlation with high density lipoprotein cholesterol was found (r = -.38; p less than .05). LDL- was negatively correlated with LDL phospholipids (r = -.59; p less than .001), and with the LDL vitamin E content (r = -.63; p less than .001), and positively correlated with LDL proteins (r = -.35; p less than .05) and the content of thiobarbituric acid reactive substances (TBARS) in total LDL (r = .43; p less than .05). The TBARS molar content of LDL- was three times higher than in nLDL, with a mean concentration in LDL- of 7.3 mol/mol lipoprotein. By preparative IE-HPLC significant differences of the LDL- chemical composition were observed. The percentage content of cholesterol esters and of phospholipids was decreased, whereas proteins and free cholesterol were increased. Analysis by sodium dodecyl sulphate polyacrylamide gel electrophoresis revealed that besides apolipoprotein B-100 there was evidence of peptides with a higher molecular weight in LDL-.(ABSTRACT TRUNCATED AT 250 WORDS)     

13C-NMR spectroscopy of human serum high density lipoprotein enriched with labelled phospholipids.

Native human serum high density lipoprotein (HDL) (d = 1.063--1.21g x cm-3) was enriched with phosphatidylcholines labelled with 13C in the polar head group ([N-13CH3]choline) and in the fatty acyl chains ([26-13C]cholesterol) and its linoleic acid ester using the previously described exchange method (Stoffel et al. 1978). The properties of the HDL particles with the exchanged lipid classes were the same as those of the native particles (Mr, CD, fluorescence, lipid and apoprotein stoichiometry, electrophoretic mobility). The T1-times were very similar to those obtained previously with recombined apolipoprotein-[13C]lipid complexes and further support our proposals concerning lipid and apoprotein interactions in the HDL particle.     

Interaction of human low density lipoprotein and apolipoprotein B with ternary lipid microemulsion. Physical and functional properties

Based on data from sedimentation velocity experiments, electrophoresis, electron microscopy, cellular uptake studies, scanning molecular sieve chromatography using a quasi-three-dimensional data display and flow performance liquid chromatography (FPLC), models for the interaction of human serum low density lipoprotein (LDL) and of apolipoprotein B (apo B) with a ternary lipid microemulsion (ME) are proposed. The initial step in the interaction of LDL (Stokes radius 110 A) with the ternary microemulsion (Stokes radius 270 A) appears to be attachment of the LDL to emulsion particles. This attachment is followed by a very slow fusion into particles having a radius of approx. 280 A. Sonication of this mixture yields large aggregates. Electron micrographs of deoxycholate-solubilized apo B indicate an arrangement of apo B resembling strings of beads. During incubation, these particles also attach to the ternary microemulsion particles and, upon sonication, spherical particles result which resemble native LDL particles in size. Scanning chromatography corroborates the electron microscopy results. By appropriate choice of display angles in a quasi-three-dimensional display of the scanning data (corrected for gel apparent absorbance) taken at equal time intervals during passage of a sample through the column, changes in molecular radius of less than 10 A can be detected visually. Such a display gives a quantitative estimate of 101 +/- 2 A for these particles (compared to 110 A for native LDL). The LDL-ME particles and apo B-ME particles compete efficiently with native LDL for cellular binding and uptake. Cellular association studies indicate that both LDL- and apo B-ME particles are effective vehicles for lipid delivery into cells.     

Physico-chemical properties of low density lipoproteins isolated in an equilibrium density gradient

The tryptophanyls of total low density lipoproteins (LDL) (1.006-1.063 g/ml) from coronary heart disease (CHD) patients and subjects without CHD signs had different accessibility to fluorescence quenchers (I-and acrylamide). LDL were separated into subfractions in equilibrium density gradient. The coefficient of extinction , quantum yield and other spectral characteristics of LDL intrinsic fluorescence, rotational mobility of maleimide spin labels and fatty acid spin probe were different in LDL subfractions from healthy subjects. LDL subfractions with hydrated density 1.045-1.05 g/ml bound to B,E-receptors of cultured fibroblasts more effectively than did subfractions with density 1.01-1.03 g/ml. Structural differences of apo-B in the particles with different lipid to protein ratio are supposed.     

Characterization of apolipoprotein B-containing lipoproteins separated by preparative free flow isotachophoresis

Preparative free flow isotachophoresis (ITP) was used for the fractionation of apoB-containing lipoproteins (d less than 1.063 g/ml) from fasting and postprandial sera derived from normolipidemic individuals. According to their net electric mobility, four major particle groups (I-IV) have been recognized. The fast-migrating particles in group I, which correspond predominantly to very low density lipoproteins (VLDL), are rich in triglycerides, free cholesterol, phosphatidylcholine, and apoE and C apolipoproteins. This group expresses nonspecific binding to fibroblasts but binds to HepG2 cells with high affinity (KD = 3.6 micrograms/ml, Bmax = 37 ng) to a single class of binding sites. The particles migrating in group II, which are related to intermediate density lipoproteins (IDL), are richer in cholesteryl esters and apoB than those in group I. They interact specifically with a single site on fibroblasts (KD = 7.8 micrograms/ml, Bmax = 54 ng) while on HepG2 cells two binding sites, one with a higher (KD = 3.5 micrograms/ml, Bmax = 22 ng) and one with a lower affinity component (KD = 16.9 micrograms/ml, Bmax = 53 ng), are involved. The particles migrating in groups III and IV correspond to low density lipoproteins (LDL). The protein moiety of both fractions consists almost exclusively of apoB. Group III represents cholesteryl ester-rich LDL particles, while the particles in group IV contain smaller amounts of cholesteryl esters. The lipoproteins of both groups are ligands for apoB,E-receptors. However, the particles in group IV interact with fibroblasts with the highest affinity (KD = 2.3 micrograms/ml, Bmax = 58 ng) and with the biphasic HepG2 cell binding sites with the lowest affinity of all analyzed groups (KD1 = 11.2 micrograms/ml, Bmax1 = 58 ng, KD2 = 68 micrograms/ml, Bmax2 = 170 ng). When apoB-containing lipoproteins were isolated from postprandial sera of the same individuals, significant changes in the lipid composition were observed only in particle groups I and II, where the triglyceride and phospholipid content was enhanced. Group I particles from postprandial serum bind to HepG2 cells with a higher affinity (KD = 2.5 micrograms/ml) than group I particles from fasting serum. Postprandial group II particles bind with the same affinity to the biphasic HepG2 cell receptor as fasting group II particles, while the affinities of postprandial group III (KD1 = 4.1 micrograms/ml, KD1 = 47 micrograms/ml) and group IV particles (KD1 = 3.9 micrograms/ml, KD2 = 38 micrograms/ml) to the high affinity binding site of the biphasic receptor are enhanced.(ABSTRACT TRUNCATED AT 400 WORDS)