Molecular dynamics of lipids in human plasma high density lipoproteins. A high field 13C NMR study

Drug delivery through the skin: molecular simulations of barrier lipids to design more effective noninvasive dermal and transdermal delivery systems for small molecules, biologics, and cosmetics

The delivery of drugs through the skin provides a convenient route of administration that is often preferable to injection because it is noninvasive and can typically be self-administered. These two factors alone result in a significant reduction of medical complications and improvement in patient compliance. Unfortunately, a significant obstacle to dermal and transdermal drug delivery alike is the resilient barrier that the epidermal layers of the skin, primarily the stratum corneum, presents for the diffusion of exogenous chemical agents. Further advancement of transdermal drug delivery requires the development of novel delivery systems that are suitable for modern, macromolecular protein and nucleotide therapeutic agents. Significant effort has already been devoted to obtain a functional understanding of the physical barrier properties imparted by the epidermis, specifically the membrane structures of the stratum corneum. However, structural observations of membrane systems are often hindered by low resolutions, making it difficult to resolve the molecular mechanisms related to interactions between lipids found within the stratum corneum. Several models describing the molecular diffusion of drug molecules through the stratum corneum have now been postulated, where chemical permeation enhancers are thought to disrupt the underlying lipid structure, resulting in enhanced permeability. Recent investigations using biphasic vesicles also suggested a possibility for novel mechanisms involving the formation of complex polymorphic lipid phases. In this review, we discuss the advantages and limitations of permeation-enhancing strategies and how computational simulations, at the atomic scale, coupled with physical observations can provide insight into the mechanisms of diffusion through the stratum corneum.

Changes in chemical composition and physico-chemical properties of chick low- and high-density lipoproteins induced by supplementation of coconut oil to the diet

Supplementation of coconut oil to the diet for 1-2 weeks produced a significant hypercholesterolemia in 14-day-old chicks. Changes in plasma fatty acid composition correlated positively with those of diets. In this study, we have shown a different response of low- and high-density lipoprotein (LDL and HDL) fractions to dietary saturated fat (coconut oil) rich in lauric and myristic acids. Although all the components of these particles seemed to increase, the percentages of increases found in total (TC), free (FC) and esterified cholesterol (EC) were higher in LDL than in HDL. TC/phospholipid (PL) ratio, considered as an inverse index of membrane fluidity, also increased with the dietary regimen in LDL, while no significant differences were found in HDL. These results suggest that supplementation of coconut oil to the diet decreased the fluidity of LDL. The EC/triglycerides (TG) ratio was also significantly increased in LDL, corroborating the main atherogenic function of this lipoprotein fraction in response to lauric and myristic acids. We have also estimated the lipidic order parameter, S, from the steady-state fluorescence anisotropy of 1,6-diphenyl-1,3,5-hexatriene (DPH)-labelled low- and high-density lipoproteins. In LDL, temperature dependence of S shows two different behaviour zones at about 20 degrees C. In HDL, the plot of S values versus T is linear. DPH anisotropy and S increased in both LDL and HDL from treated chicks. This increase becomes more evident as temperature rises and also with dietary treatment.

Fluidity changes and chemical composition of lipoproteins in type IIa hyperlipoproteinemia

The chemical composition and the physical properties of lipoproteins (VLDL, LDL and HDL) were studied in two groups of patients: 14 healthy normolipidemic subjects and 15 type IIa familial hypercholesterolemic patients. The steady-state fluorescence anisotropy rs was estimated in lipoproteins by the fluorescence depolarization of two fluorescent probes: the DPH (1,6-diphenyl-1,3,5-hexatriene) and the TMA-DPH (1,4-trimethylammonium phenyl-6-1,3,5-hexatriene). A structured order parameter S was calculated from the DPH fluorescence anisotropy. The flow activation energies were calculated for LDL and HDL from both groups from the Arrhenius plots (log r DPH versus 1/T). By using TNBS (trinitrobenzene sulfonic acid) as a distance control quencher, the two probes were located in the outer shell of LDL. In HDL, TMA-DPH remained at the surface of the particles, while DPH was more deeply embedded in the lipid core. There was no difference in the physico-chemical properties of VLDL between the two groups studied. DPH fluorescence anisotropies were significantly increased in LDL and HDL from the hypercholesterolemic group compared to the control particles (P less than 0.05 and P less than 0.01, respectively). In LDL this modification of the fluorescence anisotropy can be related to a change in the lipid composition of particles. LDL from hypercholesterolemic patients contained significantly less triacylglycerol (P less than 0.01) and more cholesteryl ester (N.S.). Their cholesteryl ester to triacylglycerol ratio was significantly higher. In HDL, there was no difference in chemical composition between the two groups. The increase in DPH fluorescence anisotropy can be related to the presence of smaller particles in HDL from HC group. No difference was noted in the TMA-DPH fluorescence anisotropy at 37 degrees C in the LDL from the two groups. In contrast, TMA-DPH fluorescence anisotropy in HDL from hypercholesterolemic group was significantly higher than in control HDL. The flow activation energy of DPH was also significantly higher in both LDL and HDL from the hypercholesterolemic group than in control group particles. In both LDL and HDL from the control group, DPH fluorescence anisotropy was negatively correlated with TG/protein and TG/PL ratios and positively correlated with the CE/TG ratio. No correlation was observed between lipid composition and DPH fluorescence anisotropy values in hypercholesterolemic particles. The modification in fluidity parameters, especially the increase in the flow activation energies in LDL and HDL from hypercholesterolemic patients, could lead to a restriction of cholesterol movements in these particles. From a physiological point of view, this could represent a loss of functional capacity.

High-resolution 1H NMR spectral signature from human atheroma

Coronary artery disease due to atherosclerosis takes the lives of approximately 550,000 Americans each year--an enormous toll. Put in economic terms, the cost to the United States alone has been estimated to exceed 60 billion dollars annually. We have found that well-resolved proton (1H) NMR spectra can be obtained from human atheroma (fatty plaque), despite its macroscopic solid appearance. The fraction of the total spectral intensity corresponding to the sharp 1H NMR signals is temperature dependent and approaches unity at body temperature (37 degrees C). Studies of the total lipids extracted from atheroma and cholesteryl esters were conducted to identify the chemical and physical origin of the spectral signature. The samples were characterized through assignment of their chemical shifts and by measurement of their T1 and T2 relaxation times as a function of magnetic field strength. The results suggest that the relatively sharp 1H NMR signals from human atheroma (excluding water) are due to a mixture of cholesteryl esters, whose liquid-crystalline to isotropic fluid phase transition is near body temperature. Preliminary applications to NMR imaging of human atheroma are reported, which demonstrate early fatty plaque formation within the wall of the aorta. These findings offer a basis for noninvasive imaging by NMR to monitor early and potentially reversible stages of human atherogenesis.

Dietary linoleate increases fluidity and influences chemical composition of plasma low density lipoprotein in adult men

Dietary linoleate was effective to increase LDL fluidity in adult men but did not significantly influence VLDL or HDL fluidities. Lipoproteins were isolated ultracentrifugally from plasma of sixteen healthy, free living male volunteers consuming controlled diets formulated from typical U.S.A. foods to have 35 energy % fat with 10 g (diet L) or 30 g (diet H) linoleate per day, 30-50 g saturated fatty acids/day and the balance mainly monounsaturated fatty acids. Calculated cholesterol intakes were 500 mg/day at each calorie level. Changes in LDL fluidity were detected as differences in diphenylhexatriene (DPH) fluorescence polarization upon crossover between the two controlled diets. Thermotropic measurement of DPH fluorescence anisotropy and compositional analyses indicated that LDL and HDL fluidities were dependent upon phospholipid and triacylglycerol concentrations, respectively, and were modulated by the presence of cholesteryl esters. Fatty acid analyses of the major lipid classes of the isolated lipoproteins indicated that changes, upon diet crossover, in DPH fluorescence anisotropy, were a linear function of the incremental change in LDL phospholipid linoleate. The fluorescent probe described an environment corresponding to the fatty acyl moieties of the phospholipids on the LDL periphery, which composition is apparently under dietary control. It is suggested that the diet induced fluidity changes may affect the conformation of the apoprotein moiety on the LDL surface and thus the potential for LDL interaction with cellular LDL receptors.

Fluorescence polarization order parameters and phase transitions in lipids and lipoproteins

Fluorescence polarization measurements with 1,6-diphenyl-1,3,5-hexatriene (DPH) were used to monitor phase changes in sonicated dispersions of triacylglycerols, cholesteryl esters and phospholipids. Lipid transitions to a fluid state were detected in a novel way by noting the temperature, t0.08, at which rs, the steady state anisotropy, was equal to 0.08. According to published equations (Van Blitterswijk , W.J., Van Hoeven , R.P. and Van der Meer , B.W. (1981) Biochim. Biophys. Acta 644, 323-332), this value for rs corresponds to a value of zero for S, a structural order parameter. Saturated and trans monounsaturated fatty triacylglycerols and distearoylphosphatidylcholine yielded t0.08 values in close agreement with transition temperatures found by differential scanning calorimetry (DSC), whereas cis unsaturated triacylglycerols displayed residual anisotropy, rs greater than 0.08, at temperatures above the DSC transition. The bent configuration of the cis double-bonded fatty acyl chains probably limits freedom of movement even in the liquid state when three such chains are bound to the glycerol molecule. Cholesteryl esters of 14:0, 18:0 and cis 18:1 fatty acids all showed rs greater than 0.08 above the DSC melting point. The difference in rotational freedom of DPH in triacylglycerol and cholesteryl esters even in the 'liquid' state explains the low t0.08 in the more fluid plasma VLDL and the contrastingly high t0.08 in plasma LDL, and HDL, which contain more cholesteryl ester an less triacylglycerol.

Organization of unesterified cholesterol in high density lipoproteins probed by filipin

The initial rate of filipin association with unesterified cholesterol in high density lipoproteins (HDL) was measured by stopped-flow spectrophotometry to assess the roles played by apolipoproteins and phospholipids in modulating the surface exposure of cholesterol. The initial rate of filipin-unesterified cholesterol association was enhanced upon hydrolysis of the glycerophospholipids of human HDL3 by phospholipase A2. Rate enhancements were also observed following trypsin-catalyzed hydrolysis of apolipoprotein A-I in canine HDL and of apolipoproteins A-I and A-II in human HDL3. However, the initial rate of filipin-unesterified cholesterol association was not altered upon incubation of HDL3 with polymorphonuclear cells, which causes hydrolysis of apolipoprotein A-II but leaves apolipoprotein A-I intact. These results are consistent with the general structural model of HDL in which unesterified cholesterol, apolipoproteins and glycerophospholipids are presumed to be localized at the surface of the HDL particle. From these studies and from results indicating that the initial rate of filipin-unesterified association was enhanced in canine HDL hybrids in which 50% of the apolipoprotein A-I had been replaced by apolipoprotein A-II, we also conclude that apolipoprotein A-I in HDL is in closer proximity to unesterified cholesterol than apolipoprotein A-II. Thus, it appears that rapid kinetic measurements of filipin-cholesterol association may be useful in assessing the organization of unesterified cholesterol in serum lipoproteins.

Cholesterol solubilization by short-chain lecithins: characterization of mixed micelles and cholesterol oxidase activity

The synthetic short-chain lecithins diheptanoylphosphatidylcholine and dioctanoylphosphatidylcholine solubilize cholesterol up to 10 and 18 mol %, respectively. The half-time for diheptanoylphosphatidylcholine solubilization of solid cholesterol is 80 (+/- 30) min. This is much faster than Triton X-100 micelle or egg lecithin vesicle solubilization of solid cholesterol. Both the broadening of lecithin and [4-13C]cholesterol carbon resonances by Mn2+ and the observation of surface dilution kinetics for phospholipase A2 (Naja naja naja) and phospholipase C (Bacillus cereus) hydrolysis of the lecithins indicate that the cholesterol 3 beta-hydroxyl group resides at the particle surface exposed to solvent. Analysis of lecithin 13C chemical shifts suggests that cholesterol causes the short-chain lecithin acyl chains to become slightly more trans, although to a lesser extent than it affects egg lecithin chains in liposomes. Lecithin motion as characterized by 13C T1s and line widths is unaffected by the incorporation of cholesterol. [3,4-13C2]Cholesterol line widths are 5-10-fold narrower in these mixed micelles than in egg lecithin sonicated vesicles, while T1s in the two systems are comparable. These mixed micelles serve as substrates for cholesterol oxidase (Nocardia erythropolis) with a 40-fold rate increase over comparable cholesterol concentrations in egg lecithin vesicles. Part of this rate enhancement can be understood as an increase in interfacial area available to cholesterol oxidase in the micellar systems. These studies suggest that cholesterol oxidase has a weaker affinity for interfaces than other surface active enzymes.

Lipoprotein-X: carbon-13 nuclear magnetic resonance studies on native, reconstituted, and model systems

Lipoprotein-X (LP-X), a lipoprotein isolated from human cholestatic plasma by ethanol--acetate precipitation and zonal ultracentrifugation, has been studied by 13C NMR at 67.9 MHz. Spectra of LP-X and its three subfractions are markedly different from those of normal human high-density lipoprotein3 (HDL3) or low-density lipoprotein (LDL). Spectra of LP-X are characterized by the presence of unusually broad resonance lines, especially those attributable to C6 of unesterified cholesterol (160--260 Hz) and to C beta of phospholipid glyceride (240--290 Hz). In contrast, the CH2O, CH2N, and N(CH3)3 choline resonances have line widths comparable to those of normal LDL and HDL3. For the subfraction LP-X1, spin--lattice relaxation times (T1) of the fatty acyl olefin resonances at 129.8 and 128.0 ppm and of the unesterified cholesterol C6 at 120.1 ppm were measured to be 675, 766, and 162 ms, respectively. These times are comparable to those measured for the corresponding resonances in single bilayer vesicles whose lipid composition approximates that of LP-X. The three LP-X subfractions isolated by zonal ultracentrifugation gave spectra which are identical, within experimental error, as judged qualitatively from their appearance and quantitatively from the line widths of selected resonances. In addition, 13C NMR spectra of sonicated total LP-X lipids are similar to spectra of the intact native lipoprotein. This study suggests (a) that motions of lipids in LP-X as probed by 13C NMR are similar to the motions of lipids found in model vesicular systems, (b) that the motions of the cholesterol rings and phospholipid fatty acyl chains are significantly more restricted in LP-X than in HDL3 and LDL, and (c) that the motions of the phosphoryl moieties in all three systems are similar.

Dissociation of apolipoprotein A-I from porcine and bovine high density lipoproteins by guanidine hydrochloride

Dissociation of apolipoprotein A-I from pig and steer high density lipoproteins (HDL) deficient in apoA-II was determined by exposing native HDL fractions to 6 M guanidine hydrochloride (Gdn-HCl) at 37 degrees C for periods from 5 min to 18 h. Bovine high density lipoprotein (HDL-B) was isolated at d 1.063--1.100 g/ml while porcine high density lipoprotein (HDL-P) was isolated at d 1.125--1.21 g/ml. Incubation for 5 min with Gdn-HCl resulted in a 45 and 3% loss of apo-A-I from HDL-P and HDL-B, respectively. Exposure to the denaturant for 3 h resulted in a 75% loss of apoA-I from HDL-P and a 30% loss from HDL-B. Analytic ultracentrifugation, patterns paralleled the degree of apoA-I dissociation from each HDL species. The initial flotation peak for HDL-P shifted from F degrees 1.20 2.68 to F degrees 1.20 10.75 after 3 h exposure while HDL-B showed only a small shift from F degrees 1.20 8.30 to F degrees 1.20 8.96 after 3 h exposure. HDL-P particle diameter increased 25% after 5 min of Gdn-HCl treatment and large, flattened structures predominated after 3 h. There was no changes in the size of HDL-B after 5 min exposure and only 16% increase in particle diameter after 3 h. The difference in behavior of HDL-B and HDL-P to Gdn-HCl exposure is discussed in terms of differences in apolipoprotein A-I amino acid composition, interaction of apolipoprotein A-I with phospholipids and the possible involvement of the cholesteryl ester core.

Structural organization of free and esterified cholesterol in human high density lipoproteins. A 100.6 MHz 13C NMR study

The structural organization of free and esterified cholesterol in human high density lipoproteins has been studied by high-field 1H and 13C NMR. The measurements are consistent with free cholesterol being present in at least two different environments. Part of the free cholesterol is oriented in the outer surface layer of the high density lipoprotein particle in contact with phospholipid or apoprotein, or both. The rest is probably present in the liquid, hydrophobic core of the HDL particle.