Sedimentation equilibrium of human low density lipoprotein subfractions

Apolipoprotein B and low-density lipoprotein structure: implications for biosynthesis of triglyceride-rich lipoproteins

ApoB100 is a very large glycoprotein essential for triglyceride transport in vertebrates. It plays functional roles in lipoprotein biosynthesis in liver and intestine, and is the ligand recognized by the LDL receptor during receptor-mediated endocytosis. ApoB100 is encoded by a single gene on chromosome 2, and the message undergoes a unique processing event to form apoB48 message in the human intestine, and, in some species, in liver as well. The primary sequence is relatively unique and appears unrelated to the sequences of other serum apolipoproteins, except for some possible homology with the receptor recognition sequence of apolipoprotein E. From its sequence, structure prediction shows the presence of both sheet and helix scattered along its length, but no transmembrane domains apart from the signal sequence. The multiple carbohydrate attachment sites have been identified, as well as the locations of most of its disulfides. ApoB is the single protein found on LDL. These lipoproteins are emulsion particles, containing a core of nonpolar cholesteryl ester and triglyceride oil, surrounded by an emulsifying agent, a monolayer of phospholipid, cholesterol, and a single molecule of apoB100. An emulsion particle model is developed to predict accurately the physical and compositional properties of an LDL of any given size. A variety of techniques have been employed to map apoB100 on the surface of the LDL, and all yield a model in which apoB surrounds the LDL like a belt. Moreover, it is concluded that apoB100 folds into a long, flexible structure with a cross-section of about 20 x 54 A2 and a length of about 585 A. This structure is embedded in the surface coat of the LDL and makes contact with the core. During lipoprotein biosynthesis in tissue culture, truncated fragments of apoB100 are secreted on lipoproteins. Here, it was found that the lipoprotein core circumference was directly proportional to the apoB fragment size. A cotranslational model has been porposed for the lipoprotein assembly, which includes these structural features, and it is concluded that in permanent hepatocyte cell lines, apoB size determines lipoprotein core circumference.

Heterogeneity of molecular weight and apolipoproteins in low density lipoproteins of healthy human males

The molecular weights of five low density lipoprotein (LDL) subfractions from four normal healthy males were determined by analytic ultracentrifuge sedimentation equilibria. Protein content of each subfraction was determined by elemental CHN analysis, and weights of apoprotein peptides were calculated. Molecular weights in subfractions of increasing density were 2.92 +/- 0.26, 2.94 +/- 0.12, 2.68 +/- 0.09, 2.68 +/- 0.28 and 2.23 +/- 0.22 million Da, and protein weight percentages were 21.05, 21.04, 22.05, 23.10 and 29.10, in subfractions 1, 2, 3, 4 and 5, respectively. Total mean apoprotein weights for respective subfractions were 614 +/- 53, 621 +/- 45, 588 +/- 9, 637 +/- 83 and 645 +/- 62 KDa. In addition to a single apoprotein B-100 (apo B-100) peptide with a mean carbohydrate content of 7.1% and a molecular weight of 550 KDa per LDL particle, there may be one or more apoprotein E peptides of 34 KDa and/or apoprotein C-III of 9 KDa. In addition, subfractions 4 and 5 may contain 3-7% apolipoprotein (a). There is considerable heterogeneity among LDL subfractions as well as within the same fraction from different individuals. This heterogeneity may relate to differences in origin, metabolism and/or atherogenicity as a result of their content of apoproteins other than apo B-100.

Physicochemical studies of two major subpopulations of low density lipoproteins by differential scanning calorimetry and n.m.r. spectroscopy

Two subpopulations, layer 2 (density 1.025-1.029 g/ml) and layer 3 (density 1.032-1.043 g/ml) of low density lipoproteins (LDL) were isolated from fresh human plasma of normal lipidaemic subjects by density gradient ultracentrifugation. Chemical analyses demonstrated the ratios of triglyceride/cholesterol ester decreased with increasing densities of subfractions. These subfractions together with triglyceride-rich lipoproteins (layer 1, density less than 1.019 g/ml) were subjected to physicochemical studies by differential scanning calorimetry (d.s.c.) and nuclear magnetic resonance (n.m.r.) spectroscopy. The average transition temperature (Tt) of layer 2 was 34.20 +/- 0.83 degrees C and that of layer 3 was 37.25 +/- 0.35 degrees C. In addition, many of the layer 3, but not layer 2 and layer 1, samples showed structural alteration and gave rise to an average Tt of 39.18 +/- 1.24 degrees C. The structural alteration could be detected with polarizing light microscopy showing birefringent spherulites at body temperature. The peak Tt values obtained by d.s.c. were in good agreement with those by n.m.r. spectroscopy. These results demonstrate the physicochemical heterogeneity within the LDL density region and suggest that layer 3 subpopulation is much more labile than the others.

Determination of size and molecular weight distributions of lipoproteins using automatic image analysis and density gradient ultracentrifugation

A Leitz-Tas automatic image analysis system has been used to investigate the size distributions of human lipoprotein particles isolated by density gradient ultracentrifugation. Computerized image analysis enabled us to obtain more precise determinations of modal diameter and overall range in diameter for each lipoprotein subspecies than those determined by classical methods. In addition, lipoprotein molecular weight distributions were calculated from measurements of flotation density and particle size distributions. This method offers certain advantages over other procedures used to characterize mean molecular weight with regard to the ability to define lipoprotein polydispersity. The method and its limitations are discussed and illustrated with results obtained with human lipoproteins.

Partial specific volume and preferential hydration of low density lipoprotein subfractions

We have determined the partial specific volume (v-) for five low density lipoprotein (LDL) subfractions (n = 5-7) and evaluated preferential hydration (n = 2) for LDL subfraction 3 in normolipoproteinemic subjects in order to characterize these highly atherogenic components of the human plasma lipoprotein spectra. Values for v- at 1 g were determined by sixth place density measurements of the solvent and lipoprotein solutions and carbon, hydrogen and nitrogen (CHN) absolute mass of the lipoprotein concentrations. Mean values for v- were 0.9757 +/- 0.0019, 0.9701 +/- 0.0007, 0.9674 +/- 0.0016, 0.9616 +/- 0.0016 and 0.9550 +/- 0.0025 ml/g for subfractions 1, 2, 3, 4 and 5, respectively. However, molecular densities (sigma) obtained from rho (rho) = 1/v- for respective LDL subfractions were 1.0249, 1.0308, 1.0337, 1.0399 and 1.0471 g/ml, respectively. The preferential hydration of lipoprotein subfraction 3 (n = 2) in NaCl/H2O solutions was 2.9-4.8 wt percent, whereas values were much lower (0.3-0.6 wt percent) in NaCl/NaBr/H2O solvent system. Unhydrated densities for LDL subfraction 3 (n = 2) at 1 g (sixth-place density meter) were 1.0287 and 1.0269 g/ml, whereas at 200,000 X g (used in D2O flotation eta F degrees vs rho determinations) both values were 1.0308 g/ml, indicating that these similar LDL fractions have 23 and 53% higher compressibility than the solvent at 200,000 X g force. It was observed that the linearity of eta F degrees vs rho may not be valid for solvents NaCl/NaBr/H2O of density as high as 1.4744 g/ml. Thus, flotation velocity data using extreme salt concentrations (1.4744 g/ml and higher) may be viewed with caution.

Interaction of human-plasma low-density lipoproteins with discoidal complexes of apolipoprotein A-I and phosphatidylcholine, and characterization of the interaction products

Interaction of human low-density lipoproteins (LDL) with discoidal complexes comprised of egg yolk phosphatidylcholine and human apolipoprotein A-I (molar ratio, 88:1, respectively) was investigated. The multicomponent gradient gel electrophoretic pattern of LDL is transformed to one that includes a predominant component with an apparent particle diameter larger than that of the initial major LDL but still in the size range of normal LDL. The apparent particle diameter increase (range, 0.2-3.5 nm) is proportional to the increase (range, 6-40%) in LDL phospholipid/protein weight ratio following incubation (37 degrees C; 6 and 24 h); the smaller the initial LDL diameter, the greater the apparent particle diameter increase and percentage of phospholipid uptake. The LDL unesterified cholesterol/protein weight ratio decreases (range, 33-39%), but does not correlate with the increase in apparent particle diameter value. Interaction products are round particles with intact apolipoprotein B and show no evidence of phospholipid degradation. The products appear more dense than expected from the size vs. density relationship observed for nonincubated LDL subspecies. In addition to products in the normal LDL size range, larger components (apparent particle diameter range, 29.0-41.2 nm) also form and may be association complexes of phospholipid-modified LDL. Our results indicate that phospholipid uptake by LDL may contribute to the particle size polydispersity observed in plasma LDL.

Characterization with zonal ultracentrifugation of low-density lipoproteins in type V hyperlipoproteinemia

Low-density lipoproteins (density = 1.019-1.063 g/ml) were isolated in 10 subjects with type V hyperlipoproteinemia by ultracentrifugation in a zonal rotor under rate flotation conditions. Plasma LDL concentrations in these patients were extremely reduced, as well as being heterogeneous, and two different subclasses consisting of LDL2 (density = 1.019-1.045 g/ml) and LDL3 (density = 1.045-1.063 g/ml) were observed. LDL2 and LDL3 have similar electrophoretic mobilities in beta position in agarose gel, and their diameters, calculated from gel filtration studies, were inversely proportional to their densities. LDL2 and LDL3 have a mean hydrated density of 1.034 and 1.054 g/ml, respectively. In comparison with normal LDL2, the LDL2 and LDL3 of hypertriglyceridemic subjects are particularly rich in triacylglycerols and poor in cholesteryl esters and free cholesterol, while they have an increasing amount of proteins. The protein moiety is composed almost exclusively of apolipoprotein B-100 in IDL, LDL2 and LDL3 ; in addition, IDL also contain apolipoprotein C peptides. This characterization of LDL heterogeneity in type V hyperlipoproteinemia should be considered in interpreting kinetic data in human normal and pathological lipid metabolism and in evaluating the atherogenic risk of hypertriglyceridemia.

Human low density lipoprotein structure: correlations with serum lipoprotein concentrations

Human low density lipoproteins (LDL) were isolated and purified from individuals having widely differing serum lipid concentrations. Very low density lipoproteins (VLDL) and high density lipoproteins (HDL) were also isolated and quantitated. HDL2 and HDL3 were separated by flotation velocity in the analytical ultracentrifuge and their relative weight percent determined. The mean density of LDL from 41 individuals was determined by flotation velocity at two different solvent densities. The mean density of LDL was directly proportional to the triglyceride (r = 0.65) and VLDL (r = 0.50) concentrations and inversely proportional to the HDL (r = -0.55) and HDL2 (r = -0.74) concentrations (all significant at P less than 0.001). The mean molecular weight of LDL from 42 individuals was determined by flotation equilibrium centrifugation. The mean molecular weight of LDL was directly proportional to the HDL (r = 0.49) and HDL2 (r = 0.48) concentrations and inversely proportional to the serum triglyceride (r = -0.60) and VLDL (r = -0.48) concentrations (all significant at P less than 0.005 except triglyceride--P less than 0.001). The molecular weight of LDL was inversely proportional to its density, and thus inversely proportional to its protein/lipid ratio which was confirmed by composition measurements. The density and molecular weight of LDL had no relationship to the concentration of LDL (r = 0.04 and 0.03).