Interaction of apoprotein from porcine high-density lipoprotein with dimyristoyl lecithin. 1. The structure of the complexes.

The morphology and structural organisation of the complexes formed from the apoprotein of porcine high-density lipoprotein and dimyristoyl phosphatidylcholine (lecithin) have been studied using the technique of small-angle X-ray scattering. Scattering measurements made in solvents of varying electron density were interpreted in terms of a scattering-equivalent model for the structure of the complex. This model is described by an oblate ellipsoidal morphology with dimensions at 20 degrees C: major axis 11.0 nm, minor axis 5.5 nm. Within this overall shape the lipid hydrocarbon chains are organised in an apolar core whilst the lipid polar head groups and protein are located in a outer shell 0.85 nm in thickness. The oblate morphology demonstrates that the structure of the complex is directed by the fundamental bilayer organisation of the lecithin. The dimension of the minor axis (5.5 nm) indicates that phospholipid hydrocarbon chains are orientated perpendicular to the interface.     

A comparison of the interfacial interactions of the apoprotein from high density lipoprotein and beta-casein with phospholipids.

The conformations adopted by beta-casein and the total apoprotein from serum high density lipoprotein when spread at the air-water interface are compared; the monolayer data are consistent with the apoprotein being alpha-helical and the beta-casein being disordered with segments distributed in loops and trains. The penetration of these hydrophobic proteins into phosphatidylcholine monolayers in different physical states was investigated. More protein can penetrate into monolayers when they are in the liquid-expanded state; for penetration at constant total surface area the lateral compressibility of the lipid is an important factor. The charge and conformation of the polar group of the phospholipid does not have a major influence on the interaction. The mixed films of lipid and protein have a mosaic structure; probably the beta-casein is in a compressed state whereas the apoprotein is extended as alpha-helices in the plane of the interface. The chain-length depedences of the interaction of the apoprotein with phosphatidylcholine monolayers and bilayers are different; when the apoprotein binds to bilayers of shorter-chain phosphatidylcholines it alters the shape of the lipid-water interface whereas with monolayers the interface remains planar throughout.     

A comparison of the interfacial interactions of the apoprotein from high density lipoprotein and β-casein with phospholipids

The conformations adopted by β-casein and the total apoprotein from serum high density lipoprotein when spread at the air-water interface are compared; the monolayer data are consistent with the apoprotein being α-helical and the β-casein being disordered with segments distributed in loops and trains. The penetration of these hydrophobic proteins into phosphatidylcholine monolayers in different physical states was investigated. More protein can penetrate into monolayers when they are in the liquid-expanded state; for penetration at constant total surface area the lateral compressibility of the lipid is an important factor. The charge and conformation of the polar group of the phospholipid does not have a major influence on the interaction. The mixed films of lipid and protein have a mosaic structure; probably the β-casein is in a compressed state whereas the apoprotein is extended as α-helices in the plane of the interface. The chain-length dependences of the interaction of the apoprotein with phosphatidylcholine monolayers and bilayers are different; when the apoprotein binds to bilayers of shorter-chain phosphatidylcholines it alters the shape of the lipid-water interface whereas with monolayers the interface remains planar throughout.     

Identification of nascent high density lipoproteins containing arginine-rich protein in human plasma.

A high density lipoprotein fraction accumulates in the plasma of patients with alcoholic hepatitis when a severe lecithin:cholesterol acyltransferase (EC 2.3.1.43) deficiency is present. The major apoprotein present in this fraction is arginine-rich protein, the fraction is a preferred substrate for lecithin:cholesterol acyltransferase, and by electron microscopy appears as stacked bilayer discs. It is proposed that the lipoprotein represents the accumulation of nascent high density lipoprotein and is the principal pathway through which arginine-rich protein is secreted by the liver in man. The results also suggest that apoprotein AI is acquired by normal high density lipoprotein during the course of lipoprotein metabolism.     

Reconstitution of lipoproteins. II. Lipid-protein interaction between dimyristoyl-lecithin and dimyristoyl-lecithin:cholesterol vesicles and purified apolipoprotein C-I and C-III2 studied by isomeric spin-labelled lecithins

The reconstitution of purified apolipoprotein C-I and C-III2 with sn-3-dimyristoyl-lecithin and sn-3-dimyristoyl-lecithin:cholesterol (10:1) vesicles was studied by electron spin resonance spectroscopy using isomeric 5'-, 12'-, and 16'-(N-oxyl-4",4"-dimethyloxazolidine)stearoyl spin-labelled lecithin probes. Results obtained from the temperature-induced changes of lipoprotein recombinants showed the hydrophilic nature of the lipid-protein interactions. The temperature-induced phospholipid phase transition, as measured by 5'-(N-oxyl-4",4"-dimethyloxazolidine)stearoyl spin-labelled lecithin probe in recombinants containing apoprotein C-1 or apoprotein C-iii2, is very broad and has a small cooperative unit indicative of extensive lipid-protein interactions occurring at the head group region of the phospholipid bilayer. When 12"- and 16'-(N-oxyl-4",4"-dimethyloxazolidine)stearoyl spin-labelled lecithins are used as probes in the same system, similar sharper and more cooperative lipid phase changes are detected. These results indicate a surface location for both apoprotein C-I and apoprotein C-III2 with respect to the phospholipid bilayer in lipoprotein recombinants with and without cholesterol.     

Interaction of C-phycocyanin with lipid monolayers under nitrogen and in the presence of air

The surface interaction of C-phycocyanin with lipids was studied using the monolayer technique. The surface activity of the protein was found to be higher at the lipid-water interface than at the nitrogen-water interface, particularly at high surface pressures of the lipid monolayer. The maximum initial surface pressures beyond which phycocyanin could not penetrate the dipalmitoylphosphatidylcholine and monogalactosyldiglycerol monolayers were 27 and 30 mN m-1, respectively. Below these values the protein demonstrated preferential interaction with the monogalactosyldiglycerol monolayer. The surface properties of the unfolded protein at pH 2.5 at the lipid-water interface were compared with those of the protein at pH 7.0. Higher affinity of the three-dimensional structure of the protein to lipid monolayers was observed, in particular by high subphase protein concentration. When the lipid films were subjected to oxidation stress by exposure to air, the surface properties of C-phycocyanin and dipalmitoylphosphatidylcholine were not greatly affected but the surface activity of monogalactosyldiacylglycerol was reduced dramatically by autoxidation. The oxidation of monogalactosyldiacylglycerol could not be prevented by the introduction of C-phycocyanin molecules at the lipid-water interface.     

Interaction between hepatic microsomal membrane lipids and apolipoprotein A-I

Incubation of apoprotein A-I (apo-A-I), the major protein component of human high density lipoprotein, with rat liver microsomal membranes under conditions of elevated pH and ionic strength leads to the production of a soluble protein:lipid complex (A-I/MM complex). The A-I/MM complex, as purified by density gradient centrifugation and agarose column chromatography, possesses a lipid composition similar to the hepatic microsomal membrane and a protein/lipid ratio similar to that of plasma high density lipoproteins, but markedly different from that of recombinant particles prepared with synthetic lipids. The A-I/MM complex constitutes a more physiological recombinant particle than can be formed using synthetic lipids and may be a suitable model for the newly assembled intracellular high density lipoproteins. Incubation of the erythrocyte plasma membranes with apo-A-I under the same conditions as used with microsomal membranes fails to generate any lipid:apoprotein complexes. This membrane specificity for forming soluble lipoprotein complexes suggests that the microsomal membranes possess a unique feature, possibly their lipid composition, which render them particularly suitable to serve as lipid donors to the apoproteins which are undergoing assembly within the endoplasmic reticulum/Golgi organelles.     

Lipid transfer particle-induced transformation of human high density lipoprotein into apolipoprotein A-I-deficient low density particles

Incubation of human high density lipoprotein (HDL) particles (density = 1.063-1.21 g/ml) with catalytic amounts of Manduca sexta lipid transfer particle (LTP) resulted in alteration of the density distribution of HDL protein such that the original HDL particles were transformed into new particles with an equilibrium density = 1.05 g/ml. Concomitantly, substantial amounts of protein were recovered in the bottom fraction of the density gradient. The LTP-induced alteration in HDL protein density distribution was dependent on the LTP concentration and incubation time. Electrophoretic analysis revealed that the lower density fraction contained apolipoprotein A-II (apoA-II) as the major apoprotein component while nearly all of the apoA-I was recovered in the bottom fraction. Lipid analysis of the HDL substrate and product fractions revealed that the apoA-I-rich fraction was nearly devoid of lipid (less than 1%, w/w). The lipid originally associated with HDL was recovered in the low density, apoA-II-rich, lipoprotein fraction, and the ratios of individual lipid classes were the same as in control HDL. Electron microscopy and gel permeation chromatography experiments revealed that the LTP-induced product lipoprotein population comprised particles of larger size (19.7 +/- 1.4-nm diameter) than control HDL (10.6 +/- 1.4-nm diameter). The results suggest that facilitated net lipid transfer between HDL particles altered the distribution of lipid such that apoprotein migration occurred and donor particles disintegrated. Similar results were obtained when human HDL3 or HDL2 density subclasses were employed as substrates for LTP. The lower surface area to core volume ratio of the larger, product lipoprotein particles compared with the substrate HDL requires that there be a decrease in the total exposed lipid/water interface which requires stabilization by apolipoprotein. Selective displacement of apoA-I by apoA-II or apoC, due to their greater surface binding affinity, dictates that apoA-I is preferentially lost from the lipoprotein surface and is therefore recovered as lipid-free apoprotein. Thus, it is conceivable that the structural arrangement of HDL particle lipid and apoprotein components isolated from human plasma may not represent the most thermodynamically stable arrangement of lipid and protein.     

Incorporation of cholesterol into high density lipoprotein recombinants.

Apo-A-1, the principal apoprotein of high density lipoprotein, was incubated with cholesterol containing liposomes of dimyristoyl lecithin, lecithin from high density lipoprotein or sphingomyelin. Conditions were chosen to give 100% conversion of cholesterol-free liposomes into recombinants which were isolated by density gradient ultracentrifugation. For all phospholipids, there was a progressive decrease in incorporation of lipid into recombinants with increasing cholesterol/phospholipid ratio. The cholesterol/phospholipid ratio of recombinants was ～ 45% of unreacted liposomes, for all initial cholesterol/phospholipid ratios. The reduced cholesterol content suggests exclusion of cholesterol from a fraction of recombinant phospholipid, probably a boundary layer in contact with apo A-1.     

Interaction of plasma apolipoproteins with lipid monolayers.

The monolayer technique has been used to study the interaction of lipids with plasma apolipoproteins. Apolipoprotein C-II and C-III from human very low density lipoproteins, apolipoprotein A-I from human high density lipoproteins and arginine-rich protein from swine very low density lipoproteins were studied. The injection of each apoprotein underneath a monolayer of egg phosphatidy[14C]choline at 20 mN/m caused an increase in surface pressure to approximately 30 mN/m. With apolipoprotein C-II and apolipoprotein C-III there was a decrease in surface radioactivity indicating that the apoproteins were removing phospholipid from the interface; the removal of phospholipid was specific for apolipoprotein C-II and apolipoprotein C-III. Although there was a removal of phospholipid from the monolayer, the surface pressure remained constant and was due to the accumulation of apoprotein at the interface. The rate of surface radioactivity decrease was a function of protein concentration, required lipid in a fluid state and, of the lipids tested, was specific for phosphatidylcholine. Cholesterol and phosphatidylinositol were not removed from the interface. The addition of 33 mol% cholesterol to the phosphatidylcholine monolayer did not affect the removal of phospholipids by apolipoprotein C-III. The addition of phospholipid liposomes to the subphase greatly facilitated the apolipoprotein C-II-mediated removal of phospholipid from the interface. Although apolipoprotein A-I and arginine-rich protein gave surface pressure increases, phospholipid was only slightly removed fromthe interface by the addition of liposomes. Based on these findings, we conclude that the apolipoproteins C interact specifically with phosphatidylcholine at the interface. This interaction is important as it relates to the transfer of the apolipoproteins C and phospholipids from very low density lipoproteins to other plasma lipoproteins. The addition of human plasma high density lipoproteins or very low density lipoproteins to the subphase increased the apolipoprotein C-mediated removal of phosphatidyl[14C]choline from the interface 3--4 fold. Low density lipoproteins did not affect the rate of decrease. During lipolysis of very low density lipoproteins to the subphase increased the apolipoprotein C-mediated removal of with the lipid monolayer. Lipolysis experiments were performed in a monolayer trough containing a surface film of egg phosphatidyl[14C]choline and a subphase of very low density lipoproteins and bovine serum albumin. Lipolysis was initiated by the addition of purified milk lipoprotein lipase to the subphase. As a result of lipolysis, there was a decrease in surface radioactivity of phosphatidylcholine. The pre-addition of high density lipoproteins decreased the rate of decrease in surface radioactivity...     

Apoproteins of the lipoproteins in a nonrecirculating perfusate of rat liver.

The apoproteins of serum lipoproteins and of lipoproteins present in a nonrecirculating perfusate of rat liver were compared by immunochemical, gel electrophoretic, and solubility techniques. Serum and perfusate very low density lipoprotein apoprotein composition were not different. No evidence for the presence of a lipoprotein resembling serum low density lipoprotein was obtained. However, the apoprotein composition of circulatory high density lipoprotein was quantitatively different from the secretory product in the density 1.06-1.21 range. As measured by stained sodium dodecyl sulfate gel electrophoretic patterns, the arginine-rich protein was the major secretory apoprotein while the A-I protein was the major apoprotein in circulating high density lipoprotein. A very similar pattern was seen in perfusates of orotic acid-fatty livers. It was concluded that although the liver secrets lipoproteins in the high density class, circulatory high density lipoprotein is largely a product of catabolic processes.     

Concentration effects of volatile anesthetics on the properties of model membranes: a coarse-grain approach

To gain insights into the molecular level mechanism of drug action at the membrane site, we have carried out extensive molecular dynamics simulations of a model membrane in the presence of a volatile anesthetic using a coarse-grain model. Six different anesthetic (halothane)/lipid (dimyristoylphosphatidylcholine) ratios have been investigated, going beyond the low doses typical of medical applications. The volatile anesthetics were introduced into a preassembled fully hydrated 512-molecule lipid bilayer and each of the molecular dynamics simulations were carried out at ambient conditions, using the NPT ensemble. The area per lipid increases monotonically with the halothane concentration and the lamellar spacing decreases, whereas the lipid bilayer thickness shows no appreciable differences and only a slight increase upon addition of halothane. The density profiles of the anesthetic molecules display a bimodal distribution along the membrane normal with maxima located close to the lipid-water interface region. We have studied how halothane molecules fluctuate between the two maxima of the bimodal distribution and we observed a different mechanism at low and high anesthetic concentrations. Through the investigation of the reorientational motions of the lipid tails, we found that the anesthetic molecules increase the segmental order of the lipids close to the membrane surface.     

Studies on the composition of pig serum lipoproteins. Isolation and characterization of different apoproteins.

1. Different lipoprotein density fractions from pig serum were isolated by phosphotungstate precipitation followed by purification in the preparative ultra-centrifuge. 2. The protein part of very low density lipoproteins was composed of approximately 52 percent lipoprotein B apoprotein and the rest of lipoprotein C II apoprotein and other as yet unidentified peptides. 3. The protein moiety of low density lipoproteins consisted primarily of lipoprotein B apoprotein (over 95 percent); the amino acid compositions of lipoprotein B apoprotein of very low and low density lipoproteins were practically identical. 4. The predominant polypeptide of pig serum high density lipoproteins exhibited an amino acid composition and a molecular weight very similar to human liprotein A I apoprotein. In contrast to human lipoprotein A I apoprotein, the apoprotein from pigs was found to release leucine first followed by alanine, threonine, and lysine upon incubation with carboxypeptidase A. 5. In pig serum the major lipoprotein C apoprotein was found to be a polypeptide similar in amino acid composition to lipoprotein C II apoprotein from human serum. The molecular weight of this polypeptide is approximately 8000. Incubation experiments with carboxypeptidase A indicate serine to be the most likely C-terminal amino acid.     

Recombination of human erythrocyte apoprotein and lipid. I. Interaction of apoprotein and lipid at the air-water interface

The formation and stabilization of a complex between total erythrocyte apoprotein and monolayers of total erythrocyte lipid as measured by changes of surface pressure (Δπ) and rate of change of surface pressure (dπ/dt) was studied as a function of pH, ionic strength, and lipid surface pressure. Penetration of apoprotein into lipid monolayers was favored by conditions in which lipid and apoprotein were oppositely charged. Once the interaction was completed, the resultant surface complex was resistant to large changes in subphase pH and ionic strength as shown by the insensitivity of Δπ to these parameters. The dπ/dt, however, showed strong dependence on pH and ionic strength, but not on lipid surface pressure. A sharp decrease in dπ/dt around pH 3.5–4.5 is associated with the change in apoprotein charge from (+) to (?). Comparison of complex formation between apoprotein and bovine serum albumin, cytochrome c, and human hemoglobin suggests that erythrocyte apoprotein was specialized in its interaction with erythrocyte lipids. The data show that formation of an apoprotein-lipid complex at the air-water interface has both electrostatic and hydrophobic components. This contradicts results from other laboratories studying erythrocyte membrane recombination by bulk methods.     

A possible correlation between lipid hydration and lipid activation of the C55-isoprenoid alcohol phosphokinase apoprotein.

1. A direct method for determining the binding of triated water to lipids is described. The experimental conditions were practically identical to those previously employed (1974) in the determination of the cofactor activities of a series of oleyl-lipids in reactivation of the C55-isoprenoid alcohol phosphokinase apoprotein. 2. Active cofactor lipids (dioleyl lecithin, sodium oleate, 1-monoolein, 1-monomyristin)bound between 2.3 and 5.3 nmol 3H2O per nmol lipid, whereas less than 0.14 nmol 3H2O were bound per nmol of the inactive lipids (1,2- and 1,3-diolein, triolein, oleyl alcohol, methyl oleate, cholesteryl oleate). 3. When exposed to 3H2O vapour, the active lipids adsorbed between 1 and 2 nmol 3H2O per nmol lipid, whereas the inactive lipids adsorbed less than 0.1 nmol 3H2O per nmol lipid. 4. The active lipid cofactor, egg lecithin, bound more than twice as much 3H2O as egg phosphatidylethanolamine which was devoid of cofactor activity in the absence of detergent. 5. Appropriately hydrated lipid polar groups are concluded to be required for an alignment with polar amino acid side chains of the enzyme apoprotein in the formation of a mixed micellar lipoprotein complex. The enzyme reaction might occur at the resulting lipoprotein/water interface.     

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.     

Biosynthesis of high density lipoprotein by chicken liver: nature of nascent intracellular high density lipoprotein

Young chickens were administered L-[(3)H]leucine and after 10 or 30 min the livers were removed and fractioned into rough (RER) and smooth (SER) endoplasmic reticulum fractions and into light, intermediate, and heavy golgo cell fractions. The labeled high density lipoprotein (HDL), contained within these intracellular organelles was isolated either by immunoprecipitation using rabbit antiserum to rooster HDL, or by ultracentrifugal glotation between densities 1.063 and 1.21 g/ml. The radioactive apoproteins of nascent HDL were analyzed by SDS PAGE and detected by fluorography. Analyses of radioactive apoproteins obtained by immunoprecipitation from the contents of the RER, the SER, and the three golgi complex fractions revealed only one apoprotein, A1. The C peptide present in serum HDL was not detected intracellularly. The radioactive apoprotein A1 which is present within the cisternae of the RER and the SER fractions failed to float, whereas apoprotein A1, present within the golgi apparatus, readily floated between densities 1.063 and 1.21 g/ml. The HDL particles, isolated by flotation from the golgi apparatus content, were further characterized by lipid and protein analyses and by electron microscopy. Golgi HDL particles have the same density as serum HDL. On a percentage basis, golgi HDL contains less protein and more phospholipids than does serum HDL. Morphologically, golgi HDL is different in appearance from serum HDL. It is more heterogeneous in size, with most of the particles ranging 8.3-25 nm in diameter. The spherical particles contain small membrane tails. Occasionally, a few disk-shaped bilayer structures are also found within the golgi apparatus. These studies show that the newly synthesized apoprotein A1, present within the RER and the SER cell fractions, is not fully complexed with lipid and that apoprotein A1 does not acquire sufficient lipid to float at the proper HDL density until it enters the golgi apparatus. The difference in chemical composition and the heterogeneous size of golgi HDL may be attributed to the different stages of HDL maturation.     

Vibrio cholerae hemolysin. Implication of amphiphilicity and lipid-induced conformational change for its pore-forming activity.

Vibrio cholerae hemolysin (HlyA), a water-soluble protein with a native monomeric relative molecular mass of 65 000, forms transmembrane pentameric channels in target biomembranes. The HlyA binds to lipid vesicles nonspecifically and without saturation; however, self-assembly is triggered specifically by cholesterol. Here we show that the HlyA partitioned quantitatively to amphiphilic media irrespective of their compositions, indicating that the toxin had an amphiphilic surface. Asialofetuin, a beta1-galactosyl-terminated glycoprotein, which binds specifically to the HlyA in a lectin-glycoprotein type of interaction and inhibits carbohydrate-independent interaction of the toxin with lipid, reduced effective amphiphilicity of the toxin significantly. Resistance of the HlyA to proteases together with the tryptophan fluorescence emission spectrum suggested a compact structure for the toxin. Fluorescence energy transfer from the HlyA to dansyl-phosphatidylethanolamine required the presence of cholesterol in the lipid bilayer and was synchronous with oligomerization. Phospholipid bilayer without cholesterol caused a partial unfolding of the HlyA monomer as indicated by the transfer of tryptophan residues from the nonpolar core of the protein to a more polar region. These observations suggested: (a) partitioning of the HlyA to lipid vesicles is driven by the tendency of the amphiphilic toxin to reduce energetically unfavorable contacts with water and is not affected significantly by the composition of the vesicles; and (b) partial unfolding of the HlyA at the lipid-water interface precedes and promotes cholesterol-induced oligomerization to an insertion-competent configuration.     

Studies of a serum albumin-liposome complex as a model lipoprotein membrane.

Electron microscopy shows that the lipoprotein dispersions formed from the interaction of negatively charged liposomes with bovine serum albumin contain closed, vesicu lar, multilamellar structures. Discontinuous density gradient studies indicate that the lipoprotein suspensions are vesicles in which bovine serum albumin homogenously associates with lipid. Low angle X-ray diffraction results show that all the systems, positively and negatively charged, with and without protein, have the characteristic lamellar structure observed in biological membranes. The lamellar spacing (bilayer plus water layer) of negatively charged liposomes without bovine serum albumin is 55 A. The same lamellar separation in the positively charged system is 108 A. The lamellar spacing corresponding to bilayer, water, and protein for the negatively charged lipoprotein system is 93 A while that for the positively charged lipoprotein system is 91 A. These dimensions suggest that a layer of protein one molecule thick is incorporated between the lamellae bound to the surface of the bilayer. Wide angle X-ray diffraction results indicate no major effect of the protein on the 4.1 A spacing, characteristic of hexagonal packing of the hydrocarbon chains. A classical light scattering technique is used to show that the lipoprotein systems are osmotically active. The solute permeability exhibited by these lipoprotein systems follows the sequence (glucose smaller than arabinose smaller than malonamide smaller than glycerol). K+ diffusion from negatively charged lipoprotein systems is greater than that found for positively charged lipoprotein systems.     

D-galactosamine induced hepatitis in the rabbit: effect on lecithin:cholesterol acyltransferase activity, plasma lipid transfer protein activity and high density lipoproteins

Hepatitis was induced in rabbits by a single intraperitoneal injection of D(+)-galactosamine-HCl (750 mg/kg body wt). Plasma lecithin:cholesterol acyltransferase activity fell to 5% and lipid transfer protein activity to 50% of control values 48 hr after injection. Discoid high density lipoprotein began to appear in plasma of treated rabbits 36 hr after injection, along with populations of high density lipoprotein (HDL) which were both smaller (radius 3.7 nm) and larger (radius 5.9 nm) than the original HDL population (radius 4.8 nm).