Infrared spectroscopy of human apolipoprotein fragments in SDS/D2O: relative lipid-binding affinities and a novel amide I assignment.

Infrared absorption spectra are reported for six apolipoprotein fragments in SDS/D2O. Five of the peptides correspond to proposed lipid-binding domains of human apolipoproteins [apoC-I(7-24), apoC-I(35-53), apoA-II(18-30)+, apoA-I(166-185), apoE(267-289)], and the sixth is the de novo lipid associating peptide LAP-20. The amide I infrared absorption patterns are generally consistent with predominantly helical structures (as determined previously by NMR spectroscopy and distance geometry calculations) and further suggest that apoA-I(166-185) and apoE(267-289) are bound to SDS relatively weakly in comparison to the other four peptides. The latter conclusion is also supported by the temperature dependence of the infrared spectra, as increasing temperature promotes a distinct increase in random coil structure only for apoA-I(166-185) and apoE(267-289). In addition to features readily ascribed to helices, the infrared spectra of all the peptides show absorptions in the spectral region 1630-1635 cm-1 that is usually associated with beta-structure, a motif that is clearly absent from the NMR-derived structures. Parallel difficulties also arose in the analyses of the circular dichroism spectra. We suggest that both the low-frequency infrared absorptions and the ambiguities in interpreting the CD spectra may be due to unusual structures at the peptide C-termini, involving C=O groups that form hydrogen bonds simultaneously either with two solvent molecules or with donors from the backbone (NH) and the solvent (OH). Analogous absorptions may be a general feature of solvent-exposed helices, which suggests a need for caution in assigning amide I bands below 1640 cm-1.

Conformations of human apolipoprotein E(263-286) and E(267-289) in aqueous solutions of sodium dodecyl sulfate by CD and 1H NMR.

Structures of apoE(263-286) and apoE(267-289) have been determined in aqueous solution containing 90-fold molar excess of perdeuterated sodium dodecyl sulfate by CD and 1H NMR. Conformations were calculated by distance geometry based on 370 and 276 NOE distance restraints, respectively. RMSD for superimposing the region 265-284 from an ensemble of 41 structures for apoE(263-286) is 0.64 +/- 0.17 A for backbone atoms (N, C alpha, C = O) and 1.51 +/- 0.13 A for all atoms. The backbone RMSD for an ensemble of 37 structures for apoE(267-289) is 0.74 +/- 0.21 A for the region 268-275 and 0.34 +/- 0.10 A for the region 276-286. A two-domain structure was found for apoE(267-289) with the C-terminal half adopting a very well defined helix and the N-terminal segment 268-275 a less well defined helix, suggesting that the N-terminus may weakly bind to SDS. For apoE(263-286), an amphipathic helix-bend-helix structural motif was found with all hydrophobic side chains on the concave face. The existence of a bend around residues Q273 to G278 is consistent with their temperature coefficients of amide protons as well as secondary shifts of alpha-protons. Comparison of the structures of the two peptides revealed that the enhanced binding of apoE(263-286) to lipid could be attributed to the formation of a hydrophobic cluster consisting of residues W264, F265, L268, and V269. Aromatic side chains are proposed to be especially important in anchoring apolipoprotein fragments to micelles.

Conformation of human serum apolipoprotein A-I(166-185) in the presence of sodium dodecyl sulfate or dodecylphosphocholine by 1H-NMR and CD. Evidence for specific peptide-SDS interactions.

The segment, YSDELRQRLAARLEALKENG, corresponding to residues 166 to 185 of human serum apolipoprotein A-I, was studied by circular dichroism and NMR spectroscopy in sodium dodecyl sulfate and dodecylphosphocholine micelles. 2-Dimensional NOESY, TOCSY and DQF-COSY spectra of apoA-I(166-185) in perdeuterated sodium dodecyl sulfate (SDS-d25) and dodecylphosphocholine (DPC-d38) micelles were collected at a peptide/SDS (DPC) ratio of 1:40. Similar CD spectra and NOE connectivity patterns were observed for apoA-I(166-185) in SDS and DPC, indicating a similar helical conformation in both. Conformations of apoA-I(166-185) in DPC-d38 micelles, and in SDS-d25 micelles at two pH values, 6.6 and 3.7, were determined using distance geometry calculations. Backbone superposition (N,C alpha,C = O) for an ensemble of twenty-nine structures in DPC at pH 6.0 gave a RMSD of 0.45 +/- 0.09 A for the region D168 to K182, while for all atoms it was 1.60 +/- 0.17 A. In SDS, the ensemble of nineteen structures each at pH 6.6 and 3.7 gave RMSDs of 0.28 +/- 0.07 A and 0.35 +/- 0.10 A, respectively, for the region D168 to K182. RMSD for superposition of all atoms was 1.36 +/- 0.10 A and 1.38 +/- 0.21 A at the respective pH values. In all cases a highly defined class A amphipathic helical structure was found for the region R171 to K182. Since the same structure occurs in micelles with either negatively charged or zwitterionic head groups it strongly suggests a dominant role for hydrophobic interactions in stabilizing the complex. The Y166 aromatic ring is bent back upon the helix axis at the lower pH. NMR determination of pKa values for D168, E169, E179 and E183 in the presence of SDS or DPC indicated a micro-pH at the micellar surface approximately one pH unit higher than the normal residue pKa. SDS interactions with the peptide were examined by collecting 1H NOESY spectra in the presence of protiated SDS. Residues R171, R173, R177, as well as the aromatic ring of Y166, were shown by intermolecular NOE measurements to interact with SDS, hence a key interaction in stabilizing the complex appears to be between interfacial basic side-chains and SDS alkyl chains.

Structural studies of a peptide activator of human lecithin-cholesterol acyltransferase.

The synthetic lipid-associating peptide, LAP-20 (VSSLLSSLKEYWSSLKESFS), activates lecithin-cholesterol acyltransferase (LCAT) despite its lack of sequence homology to apolipoprotein A-I, the primary in vivo activator of LCAT. Using SDS and dodecylphosphocholine (DPC) to model the lipoprotein environment, the structural features responsible for LAP-20's ability to activate LCAT were studied by optical and two-dimensional 1H NMR spectroscopy. A large blue shift in the intrinsic fluorescence of LAP-20 with the addition of detergent suggested that the peptide formed a complex with the micelles. Analysis of the CD data shows that LAP-20 lacks well defined structure in aqueous solution but adopts helical, ordered conformations upon the addition of SDS or DPC. The helical nature of the peptides in the presence of both lipids was confirmed by upfield H alpha NMR secondary shifts relative to random coil values. Average structures for both peptides in aqueous solutions containing SDS and DPC were generated using distance geometry methods from 329 (SDS) and 309 (DPC) nuclear Overhauser effect-based distance restraints. The backbone (N, Calpha, C=O) RMSD from the average structure of an ensemble of 17 out of 20 calculated structures was 0.41 +/- 0.15 Angstrom for LAP-20 in SDS and 0.41 +/- 0.12 A for an ensemble of 20 out of 20 calculated structures for LAP-20 in DPC. In the presence of SDS, the distance geometry and simulated annealing calculations show that LAP-20 adopts a well defined class A amphipathic helix with distinct hydrophobic and hydrophilic faces. A similar structure was obtained for LAP-20 in the presence of DPC, suggesting that both detergents may be used interchangeably to model the lipoprotein environment. Conformational features of the calculated structures for LAP-20 are discussed relative to models for apolipoprotein A-I activation of LCAT.

An alternate apoprotein conformation in high density apolipoprotein discoidal complexes. A Fourier transform infra-red study.

Discoidal complexes have been prepared from 1,2-dimyristoyl-sn-glycero-3-phosphocholine (DMPC) and the apoproteins of HDL3 (apo HDL3) or purified apo A-I. Gel electrophoresis established that apo HDL3 contained 74% apo A-I. Deconvolution and curve-fitting of the infra-red amide I band of the apoprotein in the lipid-protein complex revealed a secondary structure containing approximately 40% alpha-helix and 50% beta-structure. This contrasted with the results from circular dichroism studies (Surewicz et al. (1986) J. Biol. Chem., 261, 16191) of apo A-I/DMPC complexes which predicted 68% alpha-helix and 7% beta-structure. The discrepancy between the two methods and limitations of the two techniques for lipoproteins is discussed.

Structure and motion of phospholipids in human plasma lipoproteins. A 31P NMR study.

The structure and motion of phospholipids in human plasma lipoproteins have been studied by using 31P NMR. Lateral diffusion coefficients, DT, obtained from the viscosity dependence of the 31P NMR line widths, were obtained for very low density lipoprotein (VLDL), low-density lipoprotein (LDL), high-density lipoproteins (HDL2, HDL3), and egg PC/TO microemulsions at 25 degrees C, for VLDL at 40 degrees C, and for LDL at 45 degrees C. At 25 degrees C, the rate of lateral diffusion in LDL (DT = 1.4 x 10(-9) cm2/s) is an order of magnitude slower than in the HDLs (DT = 2 x 10(-8) cm2/s). At 45 degrees C, DT for LDL increases to 1.1 x 10(-8) cm2/s. In contrast, DT for VLDL increases only slightly going from 25 to 40 degrees C. The large increase in diffusion rate observed in LDL occurs over the same temperature range as the smectic to disordered phase transition of the core cholesteryl esters, and provides evidence for direct interactions between the monolayer and core. In order to prove the orientation and/or order of the phospholipid head-group, estimates of the residual chemical shift anistropy, delta sigma, have been obtained for all the lipoproteins and the microemulsions from the viscosity and field dependence of the 31P NMR line widths. For VLDL and LDL, the anisotropy is 47-50 ppm at 25 degrees C, in agreement with data from phospholipid bilayers. For the HDLs, however, significantly larger values of 69-75 ppm (HDL2) and greater than 120 ppm (HDL3) were obtained.(ABSTRACT TRUNCATED AT 250 WORDS)

Dynamic structure of the lower density lipoproteins. I. Incorporation of high levels of labelled lipids into very low and low density lipoproteins.

Selectively labelled lipids have been incorporated into the surface monolayer of human serum low density lipoprotein (LDL) and very low density lipoprotein (VLDL). From 3 to 17 mol% of phosphatidylcholine, selectively deuterated at various positions along the sn-2-acyl chain, was transferred from unilamellar vesicles to VLDL using a partially purified phosphatidylcholine transfer protein. Selectively deuterated palmitic acids were incorporated into LDL (6-20 mol%) and into VLDL (7-10 mol%). Electron microscopy, light scattering, and 31P nuclear magnetic resonance indicated that particle size remained unchanged. Gel exclusion chromatography and chemical analysis showed no difference in hydrodynamic properties and only slight alteration to particle component ratios. Biological activity of labelled VLDL was measured from the rate of cholesterol esterification by cultured J774A.1 cells. Effect of labelling LDL was evaluated by monitoring LDL uptake and degradation by cultured human skin fibroblasts. In all cases the lipoproteins containing labels were indistinguishable from their native counterparts.

Dynamic structure of the lower density lipoproteins. II. Deuterium NMR studies of the monolayer of very low and low density lipoproteins.

The order of phosphatidylcholine (PC) acyl chains in the surface monolayer of very low density lipoproteins (VLDL) and low density lipoproteins (LDL) has been determined from 2H nuclear magnetic resonance order parameters, SCD, using selectively deuterated PC or palmitic acids. From the computer simulated line shapes, we find two distinct phospholipid domains within the amphiphilic monolayer of both VLDL and LDL. In the more ordered domain of LDL, SCD was approximately 0.3 for the "plateau" chain region. The SCD values of VLDL particles are similar to those of LDL for the 5,6- and 11,12-positions, hence we suggest the organization of the more ordered region of VLDL and LDL are similar. The domain of low order in LDL comprises less than 10% of the phospholipid molecules (we do not distinguish between PC and sphingomyelin), having approximately the same order (SCD less than 0.1) as egg PC - sphingomyelin unilamellar vesicles. In VLDL, the domain of low order comprises between approximately 10 and approximately 20% of the phospholipid molecules and the entire acyl chain is in an essentially isotropic environment (SCD less than 0.02). We prepared VLDL-sized microemulsions composed of egg PC, deuterated PC, and triolein to test whether the apoproteins were responsible for creating the two differently organized domains in VLDL and LDL. Surprisingly, these protein-free particles also showed two domains of different order at two temperatures. The high order region, however, is less ordered than in VLDL and LDL. We explain two surface domains of PC in terms of lipid organization and the unique interactions of lipids in the various lipoprotein particles.

Lipid-lipid interactions in reconstituted high-density lipoproteins by deuterium nuclear magnetic resonance.

Lipid-lipid interactions between the core and monolayer have been studied by using reconstituted high-density lipoproteins (rHDLs) composed of apoHDL3 with either dipalmitoylphosphatidylcholine (DPPC) or egg phosphatidylcholine (egg PC) as the monolayer and either cholesteryl oleate (CO) or triolein (TO) as the core. The effect of the monolayer on the core was observed by deuterium nuclear magnetic resonance (2H NMR) studies of rHDLs containing the core component cholesteryl [18, 18, 18-2H3] oleate [( 2H3]CO) or tri[16,16-2H2]oleoylglycerol [( 2H6]TO) surrounded by a monolayer of either DPPC or egg PC as a function of temperature. The reverse effect, that of the core on the monolayer, was examined by both 2H and 31P NMR studies of rHDLs containing [5,5-2H2]PC in the presence of CO or TO as a function of temperature. The 2H NMR line widths of [2H3]CO and [2H6]TO were considerably broader and showed a greater temperature dependence in rHDLs containing DPPC than in those containing egg PC. Similarly, the C-2H order parameters of [2H2]PC were higher and showed a greater temperature dependence in rHDLs containing CO than in those containing TO. In contrast, the 31P NMR line widths were identical for both [2H2]-PC/CO/apoHDL3 and [2H2]PC/TO/apoHDL3 at 25 and 6 degrees C, showing only a slight temperature dependence. Thus, acyl chains of both the monolayer and core components show increased order when in contact with neighboring lipids of higher order. The data demonstrate a direct effect of core cholesteryl esters and triglycerides with the phospholipid monolayer of HDL.

Surface diffusion in human serum lipoproteins.

From the viscosity dependence of the 31P NMR signals, the diffusion coefficients DT of phospholipid molecules in the surface monolayer of HDL, LDL and VLDL have been determined. DT for HDL3 and HDL2 are found to be 2.3 X 10(-8) cm2/s and 1.8 X 10(-8) cm2/s, respectively. These values are similar to values reported for diffusion of phospholipid molecules in phospholipid bilayers above the gel to liquid crystalline phase transition temperature. Viscosity dependence of [16,16,16-2H3]phosphatidylcholine incorporated into HDL2 yielded a value similar to that determined by 31P (DT = 1.9 X 10(-8) cm2/s). Slower diffusion coefficients were measured for LDL2 and VLDL. VLDL had a value DT = 9.1 X 10(-9) cm2/s. The diffusion coefficient for LDL2 was 1.4 X 10(-9) cm2/s. Thus, diffusion of phospholipids in LDL2 is a full order of magnitude slower at 25 degrees C than diffusion of phospholipids in the HDLs.

Orientational order of cholesteryl oleate in low-density lipoprotein observed by 2H-NMR.

Cholesteryl oleate, selectively deuterated at various positions along the acyl chain, has been incorporated into fresh human serum low-density lipoprotein (LDL2). Temperature-dependent 2H-NMR spectra were recorded between 15 and 45 degrees C. For deuterons at C-2' and C-5' of the acyl chain, two 2H-NMR spectral components, a broad and a narrow signal, are observed. This is interpreted as reflecting the coexistence of two cholesteryl ester regions in the LDL2 core which possess different degrees of order. The C-2H bond order parameters, SCD, are approx. 0.12-0.20 for the more ordered region and approx. 0.04-0.06 for the less ordered region. Longitudinal relaxation times, T1, of deuterated cholesteryl oleate are found to increase between C-8' and the terminal -C2H3 group, which is consistent with an increased rate of chain motion toward the free ends of the ester acyl chains.

Carbon-13 nuclear magnetic resonance study of spin labelled cholesteryl ester in model membranes.

Carbon-13 NMR longitudinal relaxation times for unilamellar vesicles of egg phosphatidylcholine (PC) in aqueous dispersion have been measured following the incorporation of spin labelled cholesteryl palmitate. The spin label induced relaxation rates, 1/T1,SL, for fatty acyl chain carbons show that the C5 segment of the cholesteryl ester acyl chain is located near the C1 and C2 segments of the phospholipid acyl chains. A greater spin label induced enhancement of relaxation rate was observed for the inner vesicle layer than for the outer, and is attributed to a higher ester incorporation and/or tighter lipid packing in the inner layer.