In this study, we compared the kinetics of cholesterol efflux from cells with 2-hydroxypropyl--cyclodextrins and with discoidal high density lipoprotein (HDL) particles to probe the mechanisms governing the remarkably rapid rates of cyclodextrin-mediated efflux. The rate of cholesterol efflux was enhanced by shaking cells growing in a monolayer and further enhanced by placing cells in suspension to achieve maximal efflux rates. The extent of efflux was dependent on cyclodextrin concentration, and maximal efflux was observed at concentrations >50 mM. For several cell types, biexponential kinetics of cellular cholesterol efflux were observed, indicating the existence of two kinetic pools of cholesterol: a fast pool (half-time (t1 ⁄2 ) ϳ19 -23 s) and a slow pool with t1 ⁄2 of 15-30 min. Two distinct kinetic pools of cholesterol were also observed with model membranes (large unilamellar cholesterol-containing vesicles), implying that the cellular pools are in the plasma membrane. Cellular cholesterol content was altered by incubating cells with solutions of cyclodextrins complexed with increasing levels of cholesterol. The number of kinetic pools was unaffected by raising the cellular cholesterol content, but the size of the fast pool increased. After depleting cells of the fast pool of cholesterol, this pool was completely restored after a 40-min recovery period. The temperature dependence of cyclodextrinmediated cholesterol efflux from cells and model membranes was compared; the activation energies were 7 kcal/mol and 2 kcal/mol, respectively. The equivalent activation energy observed with apo-HDL-phospholipid acceptor particles was 20 kcal/mol. It seems that cyclodextrin molecules are substantially more efficient than phospholipid acceptors, because cholesterol molecules desorbing from a membrane surface can diffuse directly into the hydrophobic core of a cyclodextrin molecule without having to desorb completely into the aqueous phase before being sequestered by the acceptor.The first step in reverse cholesterol transport is the efflux of cellular cholesterol molecules to extracellular acceptors (1-3). This initial step is thought to be mediated by high density lipoproteins (HDL) 1 or by specific subpopulations of HDL (1-3). It is generally accepted that cholesterol efflux occurs by an aqueous diffusion mechanism whereby the cholesterol molecules desorb from the plasma membrane into the aqueous phase, diffuse, and are solubilized by an acceptor particle (2, 4).-Cyclodextrins are cyclic heptasaccharides consisting of (1-4)-glucopyranose units (5). These water-soluble compounds contain a hydrophobic core capable of solubilizing nonpolar substances (5, 6). Thus, cyclodextrins have been used as vehicles to deliver hydrophobic drugs (5, 6). The -cyclodextrins (7 glucose units), when compared with ␣ (6 glucose units) and ␥ (8 glucose units) cyclodextrins, have the highest affinity for encapsulating sterols, in particular cholesterol (7). Chemical modifications of the hydroxyl groups of cyclodextrins often enhance b...
Despite extensive studies and characterizations of the high density lipoprotein-cholesteryl ester (HDL-CE)-selective uptake pathway, the mechanisms by which the hydrophobic CE molecules are transferred from the HDL particle to the plasma membrane have remained elusive, until the discovery that scavenger receptor BI (SR-BI) plays an important role. To elucidate the molecular mechanism, we examined the quantitative relationships between the binding of HDL and the selective uptake of its CE in the murine adrenal Y1-BS1 cell line. A comparison of concentration dependences shows that half-maximal high affinity cell association of HDL occurs at 8.7 ؎ 4.7 g/ml and the K m of HDL-CE-selective uptake is 4.5 ؎ 1.5 g/ml. These values are similar, and there is a very high correlation between these two processes (r 2 ؍ 0.98), suggesting that they are linked. An examination of lipid uptake from reconstituted HDL particles of defined composition and size shows that there is a non-stoichiometric uptake of HDL lipid components, with CE being preferred over the major HDL phospholipids, phosphatidylcholine and sphingomyelin. Comparison of the rates of selective uptake of different classes of phospholipid in this system gives the ranking: phosphatidylserine > phosphatidylcholine Ϸ phosphatidylinositol > sphingomyelin. The rate of CE-selective uptake from donor particles is proportional to the amount of CE initially present in the particles, suggesting a mechanism in which CE moves down its concentration gradient from HDL particles docked on SR-BI into the cell plasma membrane. The activation energy for CE uptake from either HDL 3 or reconstituted HDL is about 9 kcal/mol, indicating that HDL-CE uptake occurs via a non-aqueous pathway. HDL binding to SR-BI allows access of CE molecules to a "channel" formed by the receptor from which water is excluded and along which HDL-CE molecules move down their concentration gradient into the cell plasma membrane.
Several subspecies of human high density lipoprotein (HDL) have been shown to exist, and particle size is one parameter that can be used to distinguish them. Recently, a small HDL subspecies has been described that may be a particularly efficient acceptor of peripheral cell unesterified (free) cholesterol (FC). To address the effects of particle size on the ability of HDL to remove FC from cells, homogeneous, well defined HDL particles were reconstituted (rHDL) that varied in particle diameter within the size range of human HDL particles (7-13 nm). The abilities of each of these particles to remove cellular FC from mouse L-cells and rat Fu5AH hepatoma cells were compared on the basis of their phospholipid (PL) content as well as on a per particle basis. The effect of particle size was also examined using small unilamellar vesicles (SUV) of 25 nm in diameter and large unilamellar vesicles (LUVs) of 70-180 nm in diameter. The SUV were prepared by sonication, and the LUVs were prepared by extrusion techniques. The FC efflux efficiency of these particles (in order of decreasing efficiency) was: rHDL > SUV > LUV when compared on the basis of acceptor PL content across a range of concentrations (i.e. at a given PL concentration for these three acceptor classes, smaller particles were more efficient). The FC efflux differences between the rHDL and the vesicles were not due to the absence of apolipoprotein in the vesicles. No difference was detected among the rHDL of varying size, nor was a difference detected among the LUVs of varying size when compared on the basis of PL content. When the FC efflux data for rHDL and LUVs were normalized on the basis of the number of acceptor particles present at a given PL concentration, a correlation was found between acceptor particle radius and the ability to accept cellular FC with larger particles being the most efficient. However, the dependence of the rate of FC efflux on acceptor particle size was not quantitatively the same within the rHDL and LUV classes of acceptor particles. The dependence of FC efflux on acceptor particle size may reflect differing abilities of the variously sized acceptor particles to access the region very close to the cell plasma membrane where most of the FC removal is expected to occur.
The influence of membrane pH gradients on the transbilayer distribution of some common phospholipids has been investigated. We demonstrate that the transbilayer equilibrium of the acidic phospholipids egg phosphatidylglycerol (EPG) and egg phosphatidic acid (EPA) can be manipulated by membrane proton gradients, whereas phosphatidylethanolamine, a zwitterionic phospholipid, remains equally distributed between the inner and outer monolayers of large unilamellar vesicles (LUVs). Asymmetry of EPG is examined in detail and demonstrated by employing three independent techniques: ion-exchange chromatography, 13C NMR, and periodic acid oxidation of the (exterior) EPG headgroup. In the absence of a transmembrane pH gradient (delta pH) EPG is equally distributed between the outer and inner monolayers of LUVs. When vesicles composed of either egg phosphatidylcholine (EPC) or DOPC together with 5 mol % EPG are prepared with a transmembrane delta pH (inside basic, outside acidic), EPG equilibrates across the bilayer until 80-90% of the EPG is located in the inner monolayer. Reversing the pH gradient (inside acidic, outside basic) results in the opposite asymmetry. The rate at which EPG equilibrates across the membrane is temperature dependent. These observations are consistent with a mechanism in which the protonated (neutral) species of EPG is able to traverse the bilayer. Under these circumstances EPG would be expected to equilibrate across the bilayer in a manner that reflects the transmembrane proton gradient. A similar mechanism has been demonstrated to apply to simple lipids that exhibit weak acid or base characteristics [Hope, M. J., & Cullis, P. R. (1987) J. Biol. Chem 262, 4360-4366]
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