Mode of assembly of amphipathic helical segments in model high-density lipoproteins

The structure of discoidal apo A-I-phospholipid complexes, representing the metabolic precursors of mature high-density lipoprotein particles, was studied by a combination of both a theoretical and an experimental approach. The secondary structure of the complex was determined by circular dichroic measurements, while the relative orientation of the apo A-I helical segments and of the phospholipid acyl chains was determined by ATR infrared measurements. Fluorescence energy transfer between the tryptophan residues of apo A-I and fluorescent phospholipid probes yielded an estimation of the relative topography of the lipid and apolipoprotein components in discoidal and spherical particles. The theoretical approach consisted of the identification of the helical segments in various apo A-I species. These segments were then oriented at a lipid/water interface by minimization of their hydrophobic and hydrophilic transfer energies. The calculation of the hydrophobicity profiles along the axis of the helices leads to the identification of specific interactions between pairs of helices. The helices were further assembled together with the phospholipids by computer modelling, enabling an estimation of the dimensions of the complex. The combination of the experimental and theoretical results yielded a model for discoidal apolipoprotein-phospholipid complexes, in which the amphipathic helical segments are oriented along the edges of the discs. Such a model can be extended to the conversion of these complexes into mature spherical HDL, through the formation of a cholesteryl ester core.     

Arrangement of apolipoprotein A-I in reconstituted high-density lipoprotein disks: an alternative model based on fluorescence resonance energy transfer experiments

The folding and organization of apolipoprotein A-I (apoA-I) in discoidal, high-density lipoprotein (HDL) complexes with phospholipids are not yet completely resolved. For about 20 years, it was generally accepted that the amphipathic helices of apoA-I lie parallel to the acyl chains of the phospholipids ("picket fence" model). However, based on the X-ray crystal structure of a large, lipid-free fragment of apoA-I, a "belt model" was recently proposed. In this model, the helices of two antiparallel apoA-I molecules are extended in a circular arrangement and lie perpendicular to the phospholipid acyl chains. To obtain conclusive information on the spatial organization of apoA-I in discoidal HDL, we engineered three separate cysteine mutants of apoA-I (D9C, A124C, A232C) for specific labeling with the fluorescence probes ALEXA-488 or ALEXA-546 (fluorescein and rhodamine derivatives). The labeled apoA-I was reconstituted into well-defined HDL complexes containing two molecules of protein and dipalmitoylphosphatidylcholine, and the complexes were used in three quantitative fluorescence resonance energy transfer (FRET) experiments to determine the distances between two specific sites in an HDL particle. Comparison of the distances measured by FRET (4.7-7.8 nm) with those predicted from the existing models indicated that neither the picket fence nor the belt model can account for the experimental results; rather, a hairpin folding of each apoA-I monomer with most helices perpendicular to the phospholipid acyl chains and a random head-to-tail and head-to-head arrangement of the two apoA-I molecules in the HDL particles are strongly suggested by the distance and lifetime data.     

The orientation of helix 4 in apolipoprotein A-I-containing reconstituted high density lipoproteins

The three-dimensional structure of the high density lipoprotein (HDL) component apolipoprotein (apo) A-I and the molecular basis for its protection against coronary artery disease are unknown. In terms of discoidal HDL particles, there has been a debate as to the orientation of the apoA-I alpha-helices around the disc edge. The "picket fence" model states that the alpha-helical repeats, separated by turns, are arranged parallel to the phospholipid acyl chains of the enclosed lipid bilayer. On the other hand, the "belt" model states that the helical segments run perpendicular to the acyl chains. To distinguish between these models, we used nitroxide spin labels present at various depths in the bilayer of reconstituted HDL (rHDL) to measure the position of Trp residues in single Trp mutants of human proapoA-I. Two mutants were studied; the first contained a Trp at position 108, which was located near the center of helix 4. The second contained a Trp at position 115, two turns along the same helix. The picket fence model predicts that these Trp residues should be at different depths in the bilayer, whereas the belt model predicts that they should be at similar depths. Different sized rHDL particles were produced that contained 2, 3, and >4 molecules of proapoA-I per complex. In each case, parallax analysis indicated that Trp-108 and Trp-115 were present at similar depths of about 6 A from the center of the bilayer, consistent with helix 4 being oriented perpendicular to the acyl chains (in agreement with the belt model). Similar experiments showed that control transmembrane peptides were oriented parallel to the acyl chains in vesicles, demonstrating that the method was capable of distinguishing between the two models. This study provides one of the first experimental measurements of the location of an apoA-I helix with respect to the bilayer edge.     

Molecular modeling of the amphipathic helices of the plasma apolipoproteins.

In this paper we propose a classification of the amphipathic helical repeats occurring in the plasma apolipoprotein sequences. It is based upon the calculation of the molecular hydrophobicity potential around the helical segments. The repeats were identified using a new autocorrelation matrix, based upon similarities of hydrophobic and hydrophilic properties of the amino acid residues within the apolipoprotein sequences. The helices were constructed by molecular modeling, the molecular hydrophobicity potential was calculated, and isopotential contour lines drawn around the helices yielded a three-dimensional visualization of the hydrophobicity potential. Two classes of apolipoproteins could be differentiated by comparing the hydrophobic angles obtained by projection of the isopotential contour lines on a plane perpendicular to the long axis of the helix. The isopotential contour lines around apo AI, AIV, and E are more hydrophilic than hydrophobic, whereas they are of similar intensity for apo AII, CI, and CIII. In both cases discoidal lipid-protein complexes are generated, with the amphipathic helices around the edge of the lipid core. The long axis of the helices is oriented parallel to the phospholipid acyl chains and the hydrophilic side of the helix toward the aqueous phase. As a result of the differences in hydrophobicity potential, the contact between the hydrophobic side of the helices and the phospholipid acyl chains is larger for apo AII, CI, and CIII than for the other apolipoproteins. This might account for the greater stability of the discoidal complexes generated between phospholipids and these apoproteins.     

Conformation and lipid binding of a C-terminal (198-243) peptide of human apolipoprotein A-I

Human apolipoprotein A-I (apoA-I) is the principle apolipoprotein of high-density lipoproteins that are critically involved in reverse cholesterol transport. The intrinsically flexibility of apoA-I has hindered studies of the structural and functional details of the protein. Our strategy is to study peptide models representing different regions of apoA-I. Our previous report on [1-44]apoA-I demonstrated that this N-terminal region is unstructured and folds into approximately 60% alpha-helix with a moderate lipid binding affinity. We now present details of the conformation and lipid interaction of a C-terminal 46-residue peptide, [198-243]apoA-I, encompassing putative helix repeats 10 and 9 and the second half of repeat 8 from the C-terminus of apoA-I. Far-ultraviolet circular dichroism spectra show that [198-243]apoA-I is also unfolded in aqueous solution. However, self-association induces approximately 50% alpha-helix in the peptide. The self-associated peptide exists mainly as a tetramer, as determined by native electrophoresis, cross-linking with glutaraldehyde, and unfolding data from circular dichroism (CD) and differential scanning calorimetry (DSC). In the presence of a number of lipid-mimicking detergents, above their CMC, approximately 60% alpha-helix was induced in the peptide. In contrast, SDS, an anionic lipid-mimicking detergent, induced helical folding in the peptide at a concentration of approximately 0.003% (approximately 100 microM), approximately 70-fold below its typical CMC (0.17-0.23% or 6-8 mM). Both monomeric and tetrameric peptide can solubilize dimyristoylphosphatidylcholine (DMPC) liposomes and fold into approximately 60% alpha-helix. Fractionation by density gradient ultracentrifugation and visualization by negative staining electromicroscopy demonstrated that the peptide binds to DMPC with a high affinity to form at least two sizes of relatively homogeneous discoidal HDL-like particles depending on the initial lipid:peptide ratio. The characteristics (lipid:peptide weight ratio, diameter, and density) of both complexes are similar to those of plasma A-I/DMPC complexes formed under similar conditions: small discoidal complexes (approximately 3:1 weight ratio, approximately 110 A, and approximately 1.10 g/cm3) formed at an initial 1:1 weight ratio and larger discoidal complexes (approximately 4.6:1 weight ratio, approximately 165 A, and approximately 1.085 g/cm3) formed at initial 4:1 weight ratio. The cross-linking data for the peptide on the complexes of two sizes is consistent with the calculated peptide numbers per particle. Compared to the approximately 100 A disk-like complex formed by the N-terminal peptide in which helical structure was insufficient to cover the disk edge by a single belt, the compositions of these two types of complexes formed by the C-terminal peptide are more consistent with a "double belt" model, similar to that proposed for full-length apoA-I. Thus, our data provide direct evidence that this C-terminal region of apoA-I is responsible for the self-association of apoA-I, and this C-terminal peptide model can mimic the interaction with the phospholipid of plasma apoA-I to form two sizes of homogeneous discoidal complexes and thus may be responsible for apoA-I function in the formation and maintenance of HDL subspecies in plasma.     

Apolipoprotein A-I adopts a belt-like orientation in reconstituted high density lipoproteins

Apolipoprotein A-I (apoA-I) is the major protein associated with high density lipoprotein (HDL), and its plasma levels have been correlated with protection against atherosclerosis. Unfortunately, the structural basis of this phenomenon is not fully understood. Over 25 years of study have produced two general models of apoA-I structure in discoidal HDL complexes. The "belt" model states that the amphipathic helices of apoA-I are aligned perpendicular to the acyl chains of the lipid bilayer, whereas the "picket fence" model argues that the helices are aligned parallel with the acyl chains. To distinguish between the two models, various single tryptophan mutants of apoA-I were analyzed in reconstituted, discoidal HDL particles composed of phospholipids containing nitroxide spin labels at various positions along the acyl chain. We have previously used this technique to show that the orientation of helix 4 of apoA-I is most consistent with the belt model. In this study, we performed additional control experiments on helix 4, and we extended the results by performing the same analysis on the remaining 22-mer helices (helices 1, 2, 5, 6, 7, 8, and 10) of human apoA-I. For each helix, two different mutants were produced that each contained a probe Trp occurring two helical turns apart. In the belt model, the two Trp residues in each helix should exhibit maximal quenching at the same nitroxide group position on the lipid acyl chains. For the picket fence model, maximal quenching should occur at two different levels in the bilayer. The results show that the majority of the helices are in an orientation that is consistent with a belt model, because most Trp residues localized to a position about 5 A from the center of the bilayer. This study corroborates a belt hypothesis for the majority of the helices of apoA-I in phospholipid discs.     

Conformation and lipid binding of the N-terminal (1-44) domain of human apolipoprotein A-I

Because of its role in reverse cholesterol transport, human apolipoprotein A-I is the most widely studied exchangeable apolipoprotein. Residues 1-43 of human apoA-I, encoded by exon 3 of the gene, are highly conserved and less well understood than residues 44-243, encoded by exon 4. In contrast to residues 44-243, residues 1-43 do not contain the 22 amino acid tandem repeats thought to form lipid binding amphipathic helices. To understand the structural and functional roles of the N-terminal region, we studied a synthetic peptide representing the first 44 residues of human apoA-I ([1-44]apoA-I). Far-ultraviolet circular dichroism spectra showed that [1-44]apoA-I is unfolded in aqueous solution. However, in the presence of n-octyl beta-d-glucopyranoside, a nonionic lipid mimicking detergent, above its critical micelle concentration ( approximately 0.7% at 25 degrees C), sodium dodecyl sulfate, an ionic detergent, above its CMC ( approximately 0.2%), trimethylamine N-oxide, a folding inducing organic osmolyte, or trifluoroethanol, an alpha-helix inducer, alpha-helical structure was formed in [1-44]apoA-I up to approximately 45%. Characterization by density gradient ultracentrifugation and visualization by negative staining electron microscopy demonstrated that [1-44]apoA-I interacts with dimyristoylphosphatidylcholine (DMPC) over a wide range of lipid:peptide ratios from 1:1 to 12:1 (w/w). At 1:1 DMPC:[1-44]apoA-I (w/w) ratio, discoidal complexes with composition approximately 4:1 (w/w) and approximately 100 A diameter were formed in equilibrium with free peptide. At higher ratios, discoidal complexes were shown to exist together with a heterogeneous population of lipid vesicles with peptide bound also in equilibrium with free peptide. When bound to DMPC, [1-44]apoA-I has approximately 60% helical structure, independent of whether it forms discoidal or vesicular complexes. This helical content is consistent with that of the predicted G helix (residues 8-33). Our data provide the first strong and direct evidence that the N-terminal region of apoA-I binds lipid and can form discoidal structures and a heterogeneous population of vesicles. In doing so, approximately 60% of this region folds into alpha-helix from random coil. The composition of the 100 A discoidal complex is approximately 5 [1-44]apoA-I and approximately 150 DMPC molecules per disk. The helix length of 5 [1-44]apoA-I molecules in lipid-bound form is just long enough to wrap around the DMPC bilayer disk once.     

LCAT activation properties of apo A-I CNBr fragments and conversion of discoidal complexes into spherical particles.

We studied the substrate properties of the phospholipid-cholesterol-apolipoprotein complexes generated with apo A-I, apo A-I-CNBr fragments, apo A-II and apo A-IV for cholesterol esterification by the enzyme lecithin-cholesterol acyltransferase (LCAT). The kinetic parameters determined with the different complexes as substrates, showed that the complexes containing apo A-I and apo A-IV were about 40-times more efficient than those generated with the apo A-I fragments. In this system, the substrates containing apo A-II had the lowest efficiency. In spite of the differences in the kinetic parameters observed with the various apolipoprotein-lipid complexes, the cholesterol inserted in the complexes was esterified for more than 90% after 24 h in all systems studied. Based upon the results of the kinetic experiments, we followed the transformation of the discoidal complexes into spherical particles, due to the formation of a cholesteryl esters core, in the presence of low-density lipoproteins as an external source of cholesterol. We observed the formation of spherical particles by electron microscopy, after incubation of the discoidal complexes with LCAT for 24 h. The average percentage of cholesteryl esters in the converted particles was around 60% of the total cholesterol, varying between 40% for the apo A-I-CNBr-1-DPPC-cholesterol complex and up to 86% for the apo A-I-DPPC-cholesterol complex. The secondary structure of protein in the complexes was not significantly modified. However, the phospholipid phase transition disappeared, together with the parallel orientation of the phospholipid acyl chains with the helical segments of the apolipoproteins, as the phospholipids are organized in a monolayer at the surface of the spheres.     

Apolipoprotein A-I structure and lipid properties in homogeneous, reconstituted spherical and discoidal high density lipoproteins

We prepared a spherical reconstituted high density lipoprotein (rHDL) particle in pure form and compared it with its homogeneous discoidal rHDL precursors, in terms of the structure and stability of the apolipoprotein A-I (apoA-I) component, the dynamics of the surface lipids, and the relative reactivity with lecithin-cholesterol acyltransferase. The apoA-I-structure was examined in the rHDL particles by circular dichroism and fluorescence spectroscopic methods, and the binding of monoclonal antibodies specific for apoA-I epitopes. The stability of apoA-I on the rHDL particles was assessed by the effects of guanidine hydrochloride on the wavelength of maximum intrinsic fluorescence of the apolipoprotein. Lipid dynamics in the acyl chain region and the polarity of the lipid-water interface were investigated by means of fluorescence probes. The conformation of apoA-I in the spherical 93-A rHDL particles was found to be very similar to that in the 96-A rHDL discs but distinct from the apoA-I structure in the 78-A rHDL discs. The stability of apoA-I to denaturation by guanidine hydrochloride was highest in the 93-A rHDL spheres. The experiments on the lipids indicate somewhat more ordered and motionally restricted acyl chains in the spheres, relative to the discs, but a similar surface polarity. These results suggest that the folding and organization of apoA-I on the three particles include protein domains consisting of interacting alpha-helical segments in the carboxyl-terminal region and a globular domain in the amino-terminal region of each apoA-I molecule. The reactivity with lecithin-cholesterol acyltransferase was highest for the 96-A rHDL disc, and 16- and 34-fold lower for the 78-A rHDL disc and the 93-A rHDL sphere, respectively, possibly as a result of differences in apoA-I structure and product inhibition in these particles.     

Lipid-free structure and stability of apolipoprotein A-I: probing the central region by mutation

To probe the structure and stability of the central region of lipid-free apolipoprotein (apo) A-I (residues 123-165), we studied the effects of four mutations made in this region on the conformation, stability, dimyristoylphosphatidylcholine (DMPC) binding kinetics, and size of discoidal reconstituted high-density lipoprotein (rHDL) particles. The apoA-I deletion delta(144-165) leads to a red shift in the wavelength of maximum fluorescence and a reduction in the alpha-helical content, the stability, the initial rate of association with DMPC liposomes, and the size of the discoidal particles. The data are consistent with the helical structure of residues 144-165, and the deletion appears to perturb the tertiary organization of the N-terminal half of apoA-I. In contrast, the deletion of the adjacent region, delta(136-143), leads to stabilization without altering the number of residues in the helical conformation or the initial rate of association with DMPC liposomes. The quadruple substitution E125K/E128K/K133E/E139K leads to approximately 17 additional residues in the helical conformation and an increase in the stability, the initial rate of association with DMPC liposomes, and the size of the rHDL particles. The findings are consistent with the disordered structure of the segment of residues 123-142, which becomes helical as a result of the quadruple mutation or upon lipid binding. The naturally occurring mutation L141R (also associated with coronary heart disease) that is located in this segment does not change the protein conformation but leads to a reduced stability and a decreased rate of association with DMPC liposomes that may relate to the observed altered functions of this mutant.     

Interaction of human plasma high-density lipoprotein HDL2b with discoidal complexes of dimyristoylphosphatidylcholine and apolipoprotein A-I

The interaction of HDL2b, a major subclass (d = 1.063 - 1.100 g/ml) of human plasma high-density lipoproteins, with discoidal complexes composed of dimyristoylphosphatidylcholine (DMPC) and apolipoprotein A-I (weight ratio, DMPC/apolipoprotein A-I (2.1 - 2.5:1); dimensions, 10.0 x 4.4 nm) was investigated. Incubation at 37 degrees C for 4.5 h of HDL2b with discoidal complexes resulted in a transfer of DMPC from the discoidal complexes to the HDL2b, a release of lipid-free apolipoprotein A-I from the discoidal complexes during such transfer, and a dissociation of some apolipoprotein A-I from the HDL2b surface. The number of discoidal complexes degraded during interaction with HDL2b depended on the initial molar ratio of HDL2b to discoidal complexes. Approximately one molecule of HDL2b was required for the degradation of one discoidal complex particle, and the degradation process appeared limited by the capacity of the HDL2b for uptake of DMPC. Degradation of discoidal complexes was also observed when human plasma LDL (d = 1.006-1.063 g/ml) was substituted for HDL2b in the interaction mixture.     

Identification and structural ramifications of a hinge domain in apolipoprotein A-I discoidal high-density lipoproteins of different size

Apolipoprotein (apo) A-I is the major protein constituent of human high-density lipoprotein (HDL) and is likely responsible for many of its anti-atherogenic properties. Since distinct HDL size subspecies may play different roles in interactions critical for these properties, a key question concerns how apoA-I can adjust its conformation in response to changes in HDL particle size. A prominent hypothesis states that apoA-I contains a flexible "hinge domain" that can associate/dissociate from the lipoprotein as its diameter fluctuates. Although flexible domains clearly exist within HDL-bound apoA-I, this hypothesis has not been directly tested by assessing the ability of such domains to modulate their contacts with the lipid surface. In this work, discoidal HDL particles of different size were reconstituted with a series of human apoA-I mutants containing a single reporter tryptophan residue within each of its 22 amino acid amphipathic helical repeats. The particles also contained nitroxide spin labels, potent quenchers of tryptophan fluorescence, attached to the phospholipid acyl chains. We then measured the relative exposure of each tryptophan probe with increasing quencher concentrations. We found that, although there were modest structural changes across much of apoA-I, only helices 5, 6, and 7 exhibited significant differences in terms of exposure to lipid between large (96 A) and small (78 A) HDL particles. From these results, we present a model for a putative hinge domain in the context of recent "belt" and "hairpin" models of apoA-I structure in discoidal HDL particles.     

Effect of phosphatidylethanolamine on the properties of phospholipid-apolipoprotein complexes

Plasma high density lipoproteins (HDL) are synthesized in intestinal mucosal cells and hepatocytes and are secreted into the blood. Factors influencing the structure and function of these HDL, such as lipid and protein composition, are poorly understood. It appears, however, that intracellular, discoidal HDL are enriched, relative to plasma HDL, in phosphatidylethanolamine (PE), a phospholipid known to generate unusual, nonbilayer structures of putative physiological significance. Although incubation of dimyristoylphosphatidylcholine (DMPC) with apolipoprotein A-I at the gel-liquid crystalline phase transition temperature results in the spontaneous formation of lipid-protein complexes, the presence of proportionately small amounts of PE prevents the formation of such complexes, suggesting that PE profoundly alters the phase properties of the phospholipid bilayers. However, by using a detergent-mediated method for the formation of PE-rich model nascent HDL from phospholipids and apolipoprotein A-I, lipid-protein complexes containing as much as 75% DLPE could be formed, thus demonstrating that the presence of PE causes a kinetic, rather than a thermodynamic, barrier to spontaneous complex formation. The products contained a DLPE:DMPC molar ratio similar to that of the initial incubation mixture; however, as the mole percentage of DLPE increased, the products became less heterogeneous, the buoyant density of the products increased, and the Stokes diameter of the products decreased. Similar results were obtained when dimyristoylphosphatidylethanolamine (DMPE) and dipalmitoylphosphatidylethanolamine (DPPE) were employed in lieu of DLPE. Electron microscopy of complexes containing DLPE and DMPC at a 1:1 molar ratio showed that these particles possessed a discoidal, bilayer morphology similar to that seen with complexes containing only phosphatidylcholine.(ABSTRACT TRUNCATED AT 250 WORDS)     

Assessment of the validity of the double superhelix model for reconstituted high density lipoproteins: a combined computational-experimental approach

For several decades, the standard model for high density lipoprotein (HDL) particles reconstituted from apolipoprotein A-I (apoA-I) and phospholipid (apoA-I/HDL) has been a discoidal particle ∼100 Å in diameter and the thickness of a phospholipid bilayer. Recently, Wu et al. (Wu, Z., Gogonea, V., Lee, X., Wagner, M. A., Li, X. M., Huang, Y., Undurti, A., May, R. P., Haertlein, M., Moulin, M., Gutsche, I., Zaccai, G., Didonato, J. A., and Hazen, S. L. (2009) J. Biol. Chem. 284, 36605–36619) used small angle neutron scattering to develop a new model they termed double superhelix (DSH) apoA-I that is dramatically different from the standard model. Their model possesses an open helical shape that wraps around a prolate ellipsoidal type I hexagonal lyotropic liquid crystalline phase. Here, we used three independent approaches, molecular dynamics, EM tomography, and fluorescence resonance energy transfer spectroscopy (FRET) to assess the validity of the DSH model. (i) By using molecular dynamics, two different approaches, all-atom simulated annealing and coarse-grained simulation, show that initial ellipsoidal DSH particles rapidly collapse to discoidal bilayer structures. These results suggest that, compatible with current knowledge of lipid phase diagrams, apoA-I cannot stabilize hexagonal I phase particles of phospholipid. (ii) By using EM, two different approaches, negative stain and cryo-EM tomography, show that reconstituted apoA-I/HDL particles are discoidal in shape. (iii) By using FRET, reconstituted apoA-I/HDL particles show a 28–34-Å intermolecular separation between terminal domain residues 40 and 240, a distance that is incompatible with the dimensions of the DSH model. Therefore, we suggest that, although novel, the DSH model is energetically unfavorable and not likely to be correct. Rather, we conclude that all evidence supports the likelihood that reconstituted apoA-I/HDL particles, in general, are discoidal in shape.     

Protein-lipid interactions in reconstituted high density lipoproteins: apolipoprotein and cholesterol influence.

Two fluorescent probes-cis- and trans-parinaric acids were used to study the dimensions, lipid dynamics and apolipoprotein location in the reconstituted discoidal high density lipoproteins (rHDL). The rHDL particles made from apolipoprotein A-I (apoA-I), dipalmitoylphosphatidylcholine (DPPC), with or without cholesterol (Chol) were compared with the analogous particles with two other apolipoproteins-apoE and apoA-II. The data obtained for apoA-I-containing rHDL were as follows: (1) the inclusion of 8 mol.% of cholesterol did not significantly change the particle dimensions (13+/-1 nm) or the mean distance between apoA-I and the disc axis; (2) the phospholipid domains-boundary lipid region in the close vicinity to apoA-I molecule and the remaining part of the bilayer-existed at temperatures both lower and above DPPC transition temperature T(t); (3) at T相似文献   

Raman spectroscopy of the thermal properties of reassembled high-density lipoprotein: apolipoprotein A-I complexes of dimyristoylphosphatidylcholine

Isolated complexes of apolipoprotein A-I (apoA-I), the major apoprotein of human plasma high-density lipoproteins, and dimyristoylphosphatidylcholine (DMPC) have been prepared and studied by differential scanning calorimetry (DSC) and Raman spectroscopy. DSC studies establish that complexes having lipid to protein ratios of 200, 100, and 50 to 1 each exhibit a broad reversible thermal transition at Tc = 27 degrees C. The enthalpy of lipid melting for each of the three complexes is about 3 kcal/mol of DMPC. Raman spectroscopy indicates that the physical state of lipid molecules in the complexes is different from that in DMPC multilamellar liposomes. Analysis of the C-H stretching region (2800-3000 cm-1) of the complexes and of the pure components in water suggests that below 24 degrees C (Tc for DMPC) there is considerably less lateral order among lipid acyl chains in the complexes than in DMPC liposomes. Above 24 degrees C, these types of interactions appear to contribute equally or slightly less to the complex structure than in pure DMPC. The temperature dependence of peaks in the C-C stretching region (1000-1180 cm-1) reveals a continuous increase in the number of lipid acyl chain C-C gauche isomers over a broad range with increasing temperature. Compared to liposomes, DMPC in the complexes has more acyl chain trans isomers at temperatures above 24 degrees C; at temperatures above ca. 30 degrees C, trans isomer content is about the same for complexes and liposomes. A large change was observed in a protein vibrational band at 1340 cm-1 for pure vs. complexed apoA-I, indicating that protein hydrocarbon side chains are immobilized by lipid binding. The Raman data indicate that the reduction in melting enthalpy for complexes DMPC (approximately 3 kcal/mol) compared to that for free DMPC (approximately 6 kcal/mol) is due to reduced van der Waals interactions in the low-temperature lipid phase.     

The conformation of apolipoprotein A-I in discoidal and spherical recombinant high density lipoprotein particles. 13C NMR studies of lysine ionization behavior.

To elucidate the molecular details of how high density lipoprotein (HDL) microstructure affects the conformation of apolipoprotein (apo) A-I in various classes of HDL particles, apoA-I structure in homogeneous recombinant HDL (rHDL) complexes containing palmitoyl-oleoyl phosphatidylcholine (POPC) and cholesteryl oleate has been investigated by NMR spectroscopy of [13C]lysine-labeled apoA-I. All Lys residues in rHDL apoA-I were labeled with 13C by reductive methylation, and then their ionization behavior was characterized by 13C NMR spectroscopy. Four discoidal particles were prepared to contain from 64 to 256 molecules of POPC and 2 molecules of apoA-I; their major diameters ranged from 9.3 to 12.1 nm. (13CH3)2-Lys resonances from apoA-I in discoidal complexes exhibit six distinct chemical shifts at pH 10. The various Lys have pKa values ranging from 8.3 to 10.5, indicating that they exist in different microenvironments. More than 80% of the Lys residues in small (9.3 nm) discoidal particles titrate at a significantly lower pH than in the large (12.1 nm) discoidal particles. This indicates that apoA-I has a different conformation on the differently size discs. Two spherical particles were prepared with POPC:cholesteryl oleate:apoA-I molar stoichiometries of 56:16:2 and 232:84:4 and diameters of 7.4 and 12.6 nm, respectively. On spherical rHDL, apoA-I (13CH3)2-Lys resonances exhibit five distinct chemical shifts at pH 10. The titration behavior of apoA-I Lys residues is the same in small and large spherical particles, indicating that apoA-I conformation is similar on the two particles. The Lys microenvironments indicate that the conformation of apoA-I in discoidal complexes is dependent on particle size and that these conformations are substantially different from that of apoA-I on spherical complexes. Lys microenvironments in discoidal complexes differ from that of spherical complexes by 4 to 5 ysines which titrate with relatively low pKa values on discs. This reflects apparent differences in conformation in the NH2-terminal one-third of apoA-I on discs and spheres.     

The spatial organization of apolipoprotein A-I on the edge of discoidal high density lipoprotein particles: a mass specrometry study

The three-dimensional structure of human apoA-I on nascent, discoidal HDL particles has been debated extensively over the past 25 years. Recent evidence has demonstrated that the alpha-helical domains of apoA-I are arranged in a belt-like orientation with the long axis of the helices perpendicular to the phospholipid acyl chains on the disc edge. However, experimental information on the spatial relationships between apoA-I molecules on the disc is lacking. To address this issue, we have taken advantage of recent advances in mass spectrometry technology combined with cleavable cross-linking chemistry to derive a set of distance constraints suitable for testing apoA-I structural models. We generated highly homogeneous, reconstituted HDL particles containing two molecules of apoA-I. These were treated with a thiol-cleavable cross-linking agent, which covalently joined Lys residues in close proximity within or between molecules of apoA-I in the disc. The cross-linked discs were then exhaustively trypsinized to generate a discrete population of peptides. The resulting peptides were analyzed by liquid chromatography/mass spectrometry before and after cleavage of the cross-links, and resulting peaks were identified based on the theoretical tryptic cleavage of apoA-I. We identified at least 8 intramolecular and 7 intermolecular cross-links in the particle. The distance constraints are used to analyze three current models of apoA-I structure. The results strongly support the presence of the salt-bridge interactions that were predicted to occur in the "double belt" model of apoA-I, but a helical hairpin model containing the same salt-bridge docking interface is also consistent with the data.     

Interaction of the alpha-helices of apolipophorin III with the phospholipid acyl chains in discoidal lipoprotein particles: a fluorescence quenching study.

Quenching of tryptophan fluorescence by nitroxide-labeled phospholipids and nitroxide-labeled fatty acids was used to investigate the lipid-binding domains of apolipophorin III. The location of the Trp residues relative to the lipid bilayer was investigated in discoidal lipoprotein particles made with 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine and five different single-Trp mutants of apoLp-III. A comparison of the quenching efficiencies of phospholipids containing nitroxide groups at the polar head, and at positions 5 and 16 of the sn-2 acyl chain, indicated that the protein is interacting with the acyl chains of the phospholipid along the periphery of the bilayer of the discoidal lipoprotein. N-Bromosuccinimide readily abolished 100% of the fluorescence of all Trp residues in the lipid-bound state. Larger quenching rates were observed for the Trp residues in helices 1, 4, and 5 than for those located in helices 2 and 3, suggesting differences between the interaction of these two groups of helices. However, the extent of Trp fluorescence quenching observed in lipoproteins made with any of the mutants was comparable to that reported for deeply embedded Trp residues, suggesting that all Trp residues interact with the phospholipid acyl chains. This study provides the first experimental evidence of a massive interaction of the alpha-helices of apoLp-III with the phospholipid acyl chains in discoidal lipoproteins. The extent of interaction deduced is consistent with the apolipoprotein adopting a highly extended conformation.     

Conformational reorganization of the four-helix bundle of human apolipoprotein E in binding to phospholipid

Conformational reorganization of the amino-terminal four-helix bundle (22-kDa fragment) of apolipoprotein E (apoE) in binding to the phospholipid dimyristoylphosphatidylcholine (DMPC) to form discoidal particles was investigated by introducing single, double, and triple interhelical disulfide bonds to restrict the opening of the bundle. Interaction of apoE with DMPC was assessed by vesicle disruption, turbidimetric clearing, and gel filtration assays. The results indicate that the formation of apoE.DMPC discoidal particles occurs in a series of steps. A triple disulfide mutant, in which all four helices were tethered, did not form complexes but could release encapsulated 5-(6)-carboxylfluorescein from DMPC vesicles, indicating that the initial interaction does not involve major reorganization of the helical bundle. Initial interaction is followed by the opening of the four-helix bundle to expose the hydrophobic faces of the amphipathic helices. In this step, helices 1 and 2 and helices 3 and 4 preferentially remain paired, since these disulfide-linked mutants bound to DMPC in a manner similar to that of the 22-kDa fragment of apoE4. In contrast, mutants in which helices 2 and 3 and/or helices 1 and 4 paired bound poorly to DMPC. However, all single and double helical pairings resulted in the formation of larger discs than were formed by the 22-kDa fragment, indicating that further reorganization of the helices occurs following the initial opening of the four-helix bundle in which the protein assumes its final lipid-bound conformation. In support of this rearrangement, reducing the disulfide bonds converted the large disulfide mutant discs to normal size.