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D M Small

Publications and source records attributed to D M Small.

At least 73 records · Page 4Linked to original sources

Interaction of ApoA-1 and ApoE-3 with triglyceride-phospholipid emulsions containing increasing cholesterol concentrations. Model of triglyceride-rich nascent and remnant lipoproteins.

The cholesterol content of triglyceride-rich lipoproteins increases during their catabolism in circulation. We therefore studied the binding of the exchangeable apoprotein apoA-1 and apoE-3 to triolein-rich emulsions with increasing cholesterol content. Five emulsion systems containing 83.1-88.8% (w/w) triolein, 9.3-10.1% egg yolk phosphatidylcholine, and 1.1-7.3% cholesterol were isolated from sonicated lipid mixtures by flotation. Negative stain EM of emulsions containing 1.1 and 7.3% cholesterol showed polydisperse populations of large spherical particles with diameters of 106 +/- 39 and 108 +/- 57 nm. These values are similar to particle diameters calculated from the lipid composition data. No lamellar structures were observed by EM, even after addition of apoA-1 at a molar ratio to lecithin of 10(-2). Apolipoproteins apoA-1 and apoE-3 bound to the particles in a saturable manner without altering particle morphology. We found a dissociation constant Kd = 7.4 x 10(-7) M and a binding capacity N = 3.9 x 10(-3) proteins/lecithin for apoA-1 with particles containing 1.1% cholesterol; the Kd and N values for apoE-3 were very similar. When the emulsion particles were saturated with cholesterol at 7.3%, the protein binding capacity N sharply decreased to 0.6 x 10(-3) (apoA-1) and 0.7 x 10(-3) proteins/lecithin (apoE-3), but the Kd values were virtually unchanged. No change in N occurred when the particle cholesterol content was increased from 1.1 to 3.7%, which spans the normal physiological range. These results suggest that increases in lipoprotein cholesterol content above 3.7% may be responsible for impaired apoprotein redistribution and altered metabolism of remnants such as beta-VLDL.

Apolipoprotein A-I↗

Physico-chemical properties of cholesterol-fed rabbit beta-VLDL are not affected by different dietary oils.

Various oils have been used as vehicles for cholesterol in diets used to produce atherosclerosis in rabbits. Because such oils may affect the physico-chemical properties of the beta-VLDL produced in response to cholesterol feeding, we have studied the physico-chemical characteristics of beta-VLDL isolated from cholesterol-fed rabbits using several different oils as vehicles (corn, safflower, cod liver, and peanut oils). All animals developed severe hypercholesterolemia by 2 weeks. During the second and third weeks on diet the apo beta-containing lipoproteins began to develop thermal transitions due to order-disorder cholesterol ester transitions in the lipoproteins. By 4 weeks the apo beta-containing lipoproteins (overwhelmingly beta-VLDL) had transitions which were quite similar (transition temperatures 41.0-42.5 degrees C). No statistical differences were noted between the transition temperatures or enthalpies of any of the dietary groups. Thus, the physico-chemical properties of the beta-VLDL of rabbits fed cholesterol appear to be quite similar, despite the vehicles used to carry the cholesterol in the diet. Thus other mechanisms must be looked for to explain the different atherogenicity of different oils used as cholesterol carrying vehicles.

Animals↗

The partitioning of fatty acid and cholesterol between core and surfaces of phosphatidylcholine-triolein emulsions at pH 7.4.

Fatty acids are important intermediate molecules in lipid metabolism. During lipolysis of intracellular lipid droplets or plasma triacylglycerol-rich lipoproteins, fatty acids are generated and may transiently accumulate. We therefore studied the distribution of both fatty acid and free cholesterol between the core and surface of phosphatidylcholine-triolein emulsions at pH 7.4. Nine emulsion systems containing 0.8 to 6.6% cholesterol and 0.16 to 1.02% oleic acid were formed, and core and surface phases were isolated. Phospholipid distributes only to the surface phase. The distribution coefficient of cholesterol surface to core was 23.9 +/- 3.6 S.D., i.e., there was approx. 24-times more cholesterol per unit mass in the surface than in the core phase. This distribution was unchanged by the presence of different quantities of fatty acid in the emulsion particles. The apparent distribution coefficient of fatty acid in surface to core was about 10 at low cholesterol contents and fell to about 7 at high cholesterol contents. However, when the apparent distribution coefficient of fatty acid was related only to the phospholipid component of the surface, the apparent distribution coefficient was constant at about 12.3 +/- 1.1 S.D. Since the fatty acid in the surface phase is about half ionized the true distribution coefficient of unionized fatty acids is about 6.2. The results indicate that fatty acids partition into the phospholipid domains of the surface and not into cholesterol domains and the distribution of fatty acids into surface phospholipid domain is not affected by cholesterol content.

Algorithms↗

The effect of triacyl-sn-glycerol structure on the metabolism of chylomicrons and triacylglycerol-rich emulsions in the rat.

A systematic study was undertaken to observe the effects of dietary (dioleoyl) triacyl-sn-glycerol structure on chylomicron composition and metabolism. First studied was a series of 1,2-dioleoyl-3-(saturated)acyl-sn-glycerols, where the fatty acid esterified at the 3-position was varied from 14 to 24 carbons. Next a series of 1,3-dioleoyl-2-acyl glycerols was studied, with various fatty acids esterified at the glycerol 2-position. These stereospecific triacyl-sn-glycerols were fed to donor rats and lymph chylomicrons were isolated, analyzed, and reinjected into recipient rats to study their disappearance from plasma and delivery to tissues. As shown by their compositions, chylomicrons obtained after feeding triacylglycerols containing all sn-3 fatty acid of chain length greater than 20 carbons were under-represented, possibly due to poorer digestion by lipases, or poorer absorption by the intestine. The 18-carbon saturated chain fatty acid (stearic acid) was equally well represented in chylomicrons whether in the 2- or 3-position of the fed triacylglycerol. The presence of increased amounts of long-chain saturated fatty acids in donor chylomicron triacylglycerols affected the metabolism of chylomicrons injected into the bloodstream of recipient rats. In particular the rate of removal of labeled cholesteryl esters, tracing removal of the partially degraded chylomicron remnants was slowed by the saturated chains, with palmitic acid and the 20-carbon fatty acid, arachidic acid, showing the most severe effects. There were clear differences in the removal from plasma of injected lymph chylomicrons derived from fed triacylglycerols containing stearic acid in either the 2- or 3-position, with evidence for remnants from the symmetrical triacylglycerols being less rapidly removed from the circulating blood. This effect was investigated further by injected model emulsions of chylomicrons, where the 2-position was substituted with saturated or transunsaturated acyl chains. Quantitation of removal from the blood stream of these model lipoproteins confirmed that a saturated or transunsaturated long chain fatty acid at the 2-position of the emulsion triacylglycerols slowed remnant removal from the blood. In some cases, with both lymph chylomicron and with emulsions, the lipolytic step mediated by lipoprotein lipase was also slowed.

Animals↗

Ionization and phase behavior of fatty acids in water: application of the Gibbs phase rule.

The phase behavior of several medium-chain (10- and 12-carbon) and long-chain (18-carbon) fatty acids in water was examined as a function of the ionization state of the carboxyl group. Equilibrium titration curves were generated above and below fatty acid and acid-soap chain melting temperatures and critical micelle concentrations, and the phases formed were characterized by X-ray diffraction, 13C NMR spectroscopy, and phase-contrast and polarized light microscopy. The resulting titration curves were divided into five regions: (i) at pH values less than 7, a two-phase region containing oil or fatty acid crystals and an aqueous phase; (ii) at pH approximately 7, a three-phase region containing oil, lamellar, and aqueous (or fatty acid crystals, 1:1 acid-soap crystals, and aqueous) phases; (iii) between pH 7 and 9, a two-phase region containing a lamellar fatty acid/soap (or crystalline 1:1 acid-soap) phase in an aqueous phase; (iv) at pH approximately 9, a three-phase region containing lamellar fatty acid-soap (or crystalline 1:1 acid-soap), micellar, and aqueous phases; and (v) at pH values greater than 9, a two-phase region containing micellar and aqueous phases. Interpretation of the results using the Gibbs phase rule indicated that, for oleic acid/potassium oleate, the composition of the lamellar fatty acid/soap phase varied from approximately 1:1 to 1:3 un-ionized to ionized fatty acid species. In addition, constant pH regions observed in titration curves were a result of thermodynamic invariance (zero degrees of freedom) rather than buffering capacity. The results provide insights into the physical states of fatty acids in biological systems.(ABSTRACT TRUNCATED AT 250 WORDS)

Fatty Acids, Nonesterified↗

The ionization and distribution behavior of oleic acid in chylomicrons and chylomicron-like emulsion particles and the influence of serum albumin.

A reproducible, fairly narrow-sized population of rat lymph chylomicrons, approximately 100 nm, was isolated by centrifugation and combined with low levels of [1-13C]oleic acid for NMR studies. The carboxyl chemical shift was monitored as a function of aqueous pH to characterize the ionization behavior of the fatty acid in these particles. The titration curves were very similar to those for oleic acid in equivalent-sized emulsion particles composed of egg phosphatidylcholine and triolein. A simple partition-ionization model was fitted to the data to derive values for apparent ionization constant, expressed as pKapp, of 7.4-7.5 and the "true" surface to core partition coefficient of approximately 7 for oleic acid in chylomicrons. The fatty acid in chylomicrons thus appeared to be largely associated with the surface regions of these particles. Addition of bovine serum albumin to the samples showed that near physiologic pH much of the fatty acid was bound to the albumin at fatty acid to albumin-binding stoichiometries as high as 5.1 and with mass ratios of greater than 2 in favor of the lipid or lipoprotein particles. Lowering the pH of the medium shifted the distribution of fatty acid away from albumin so that at pH 5 with the emulsion, virtually all the fatty acid was associated with the lipid. The behavior observed under physiologic conditions is consistent with the rapid clearance and redistribution of fatty acid generated in these particles by lipolytic processes. However, under conditions of severe acidosis, hyperlipidemia, and hypoalbuminemia a significant portion of fatty acids might be retained in triglyceride-rich lipoproteins and their remnants and affect subsequent metabolism.

Algorithms↗

Secondary and tertiary structure of apolipoproteins.

The advent of these and other high-powered techniques for the detailed study of apoLP organization will allow us to obtain a high resolution picture of apoLP conformation both in solution and on native lipoprotein particles.

Apolipoproteins↗

Mechanisms of reversed cholesterol transport.

Reverse cholesterol transport may be defined as the movement of cholesterol from tissues, organs and cells to the liver (hepatocytes). Once cholesterol enters the hepatocyte it may be catabolized to bile acids, excreted into bile as free cholesterol, secreted back into the plasma compartment in lipoproteins or esterified and stored in the liver. A fraction of the bile acid and cholesterol excreted into bile is lost in the feces and accounts for the major loss of cholesterol and its metabolites from the body. If cholesterol was not added to the body then the mechanisms of reverse transport, bile acid and cholesterol excretion would deplete the body of sterols. Of course the body can absorb dietary cholesterol and synthesize cholesterol to keep overall cholesterol homeostasis. The mechanisms of reverse transport involve 1) the physico-chemical state of cholesterol and potential for movement within peripheral cells, tissues and deposits (e.g., atherosclerotic plaques); 2) the net transfer of free cholesterol from cell, tissues and deposits to acceptors (especially lipoproteins); 3) the physical state of the acceptors (e.g., the core and surface of lipoproteins and their capacity to accept cholesterol; 4) the LCAT reaction; 5) the transfer proteins; 6) the lipase (LPL and HTGL) reactions; and finally 7) the functional state of the LDL and chylomicron remnant receptors in the liver. The net transport of cholesterol from peripheral tissues, deposits and cells to the liver first depends on the rate of influx into the cells plus the rate of de novo cholesterol synthesis being less than the rate of removal. The rates of net removal will depend upon the sum of a variety of complex steps by which cholesterol can move down a gradient to enter acceptors than be transferred to other lipoproteins which are in turn ultimately taken up by the liver. A potentially important fraction of cholesterol leaving cells may be converted into cholesterol ester by LCAT then transferred to larger particles which can then be taken up by receptor medicated endocytosis in the liver. The HDL system must have its phospholipids replenished by both the synthesis of nascent HDL and by the formation of phospholipid-rich surface remnants during lipolysis of nascent triglyceride-rich lipoproteins which enter the HDL fraction. Finally, functionally active and vigorous receptor mechanisms are needed to remove cholesterol-containing particles into the liver.

Biological Transport↗

Effect of free cholesterol on incorporation of triolein in phospholipid bilayers.

Triacylglycerols are the major substrates for lipolytic enzymes that act at the surface of emulsion-like particles such as triglyceride-rich lipoproteins, chylomicrons, and intracellular lipid droplets. This study examines the effect of cholesterol on the solubility of a triacylglycerol, triolein, in phospholipid surfaces. Solubilities of [carbonyl-13C]triolein in phospholipid bilayer vesicles containing between 0 and 50 mol % free cholesterol, prepared by cosonication, were measured by 13C NMR. The carbonyl resonances from bilayer-incorporated triglyceride were shifted downfield in the 13C NMR spectra from those corresponding to excess, nonincorporated material. This enabled solubilities to be determined directly from carbonyl peak intensities at most cholesterol concentrations. The bilayer solubility of triolein was inversely proportional to the cholesterol/phospholipid mole ratio. In pure phospholipid vesicles the triolein solubility was 2.2 mol %. The triglyceride incorporation decreased to 1.1 mol % at a cholesterol/phospholipid mole ratio of 0.5, and at a mole ratio of 1.0 for the bilayer lipids, the triolein solubility was reduced to just 0.15 mol %. The effects of free cholesterol were more pronounced and progressive than observed previously on the bilayer solubility of cholesteryl oleate (Spooner, P. J. R., Hamilton, J. A., Gantz, D. L., & Small, D. M. (1986) Biochim. Biophys. Acta 860, 345-353]. As with cholesteryl oleate, we suggest that cholesterol also displaces solubilized triglyceride to deeper regions of the bilayer.

Carbon Isotopes↗

Carbon 13 NMR studies of saturated fatty acids bound to bovine serum albumin. I. The filling of individual fatty acid binding sites.

13C NMR chemical shift and intensity results for a series of carboxyl 13C-enriched saturated fatty acids (8-18 carbons) bound to bovine serum albumin (BSA) are presented as a function of increasing fatty acid (FA)/BSA mole ratio. Spectra for long-chain (greater than or equal to 12 carbons) FA X BSA complexes exhibited up to five FA carboxyl resonances, designated a, b, b', c, and d. Only three resonances (peaks b, b', and d) were observed below 3:1 FA X BSA mole ratio, and at greater than or equal to 3:1 mole ratio, two additional resonances were observed (peaks c and a). In a spectrum of 5:1 stearic acid X BSA complexes, peaks b, b', and d each represented approximately one-fifth, and peak c approximately two-fifths, of the total FA carboxyl intensity. Plots of total carboxyl/carbonyl intensity ratio as a function of FA X BSA mole ratio were linear up to 7-9 mole ratio. Deviation from linearity at mole ratios greater than or equal to 7 was accompanied by the detection of crystalline unbound FA (as 1:1 acid/soap) by X-ray diffraction. In contrast to long-chain FA X BSA complexes, 13C NMR spectra of octanoic acid X BSA complexes yielded only one FA carboxyl resonance (peak c) at FA X BSA mole ratios between 1 and 20. We conclude: peaks b, b', and d represent FA bound to three individual high affinity (primary) long-chain FA binding sites on BSA; peak c represents FA bound to several secondary long-chain (or primary short-chain) FA binding sites on BSA; peak a represents long-chain FA bound to an additional lower affinity binding site. We present a model that correlates the observed 13C NMR resonances with individual binding site locations predicted by a recent three-dimensional model of BSA.

Binding Sites↗

Carbon 13 NMR studies of saturated fatty acids bound to bovine serum albumin. II. Electrostatic interactions in individual fatty acid binding sites.

13C NMR chemical shift results as a function of pH for a series of carboxyl 13C-enriched saturated fatty acids (8-18 carbons) bound to bovine serum albumin (BSA) are presented. For octanoic acid bound to BSA (6:1, mol/mol), the chemical shift of the only FA carboxyl resonance (designated as peak c), plotted as a function of pH, exhibited a complete sigmoidal titration curve that deviated in shape from a corresponding theoretical Henderson-Hasselbach curve. However, FA carboxyl chemical shift plotted as a function of added HCl yielded a linear titration curve analogous to those obtained for protein-free monomeric fatty acid (FA) in water. The apparent pK of BSA-bound octanoic acid was 4.3 +/- 0.2. However, the intrinsic pK (corrected for electrostatic effects resulting from the net positive charge on BSA) was approximately 4.8, a value identical to that obtained for monomeric octanoic acid in water in the absence of protein. For long-chain FA (greater than or equal to 12 carbons) bound to BSA (6:1, mol/mol), chemical shift titration curves for peak c were similar to those obtained for octanoic acid/BSA. However, the four additional FA carboxyl resonances observed (designated as peaks a, b, b', and d) exhibited no change in chemical shift between pH 8 and 3. For C14.0 X BSA complexes (3:1 and 6:1, mol/mol) peaks b' and a exhibited chemical shift changes between pH 8.8 and 11.5 concomitant with chemical shift changes in the epsilon-carbon (lysine) resonance. In contrast, peaks c and d exhibited no change and peak b only a slight change in chemical shift over the same pH range. We conclude: the carboxyl groups of bound FA represented by peaks a, b, b', and d were involved in ion pair electrostatic interactions with positively charged amino acyl residues on BSA; the carboxyl groups of bound FA represented by peak c were not involved in electrostatic interactions with BSA; the similarity of the titration curves of peak c for BSA-bound octanoic acid and long-chain FA suggested that short-chain and long-chain FA represented by peak c were bound to the same binding site(s) on BSA; bound FA represented by peaks b' and a (but not d or b) were directly adjacent to BSA lysine residues. We present a model which correlates NMR peaks b, b', and d with the putative locations of three individual high-affinity binding sites in a three-dimensional model of BSA.

Binding Sites↗

Transbilayer movement of bile acids in model membranes.

The ability of bile acids to traverse membranes has important implications for their reabsorption from the gut, recirculation to and uptake into the liver, and resecretion into bile. The rate constant for transbilayer movement, or "flip-flop", of three common, unconjugated bile acids was determined by 13C nuclear magnetic resonance spectroscopy. At high pH, the sodium salts of the bile acids did not appreciably traverse the bilayer; however, upon protonation a rapid equilibration between the inner and outer monolayers occurred. The rate of flip-flop of each bile acid at 37 degrees C was found to be dependent on both number and location of hydroxyl groups but not on concentration in the bilayer over the range studied (2-4 wt%) nor on the presence of a different bile acid in the same bilayer.

Bile Acids and Salts↗

Synthetic high density lipoprotein particles. Application to studies of the apoprotein specificity for selective uptake of cholesterol esters.

Particles closely resembling rat high density lipoproteins (HDL) in terms of equilibrium density profile and particle size were prepared by sonication of apoA-I with a microemulsion made with egg lecithin and cholesterol oleate. These particles, like authentic HDL, allowed selective uptake of their cholesterol ester moieties by cultured cells without parallel uptake of the particle itself. That uptake was saturable and competed by HDL. In rats, the plasma decay kinetics and sites of uptake of a cholesteryl ether tracer were similar whether that tracer was incorporated into synthetic or authentic HDL. Synthetic particles containing other apoproteins were made by generally the same method, but using in place of apoA-I either a mixture of rat apoCs or apoE that was either competent or reductively methylated to prevent interaction with the B/E receptor. These particles, of lower density and larger Stokes radius than those made with apoA-I, also allowed selective uptake of cholesterol esters, albeit with a lower degree of selectivity than in the case of apoA-I. Thus a specific apoprotein component in the subject lipoprotein particle is not required for selective uptake. However, selective uptake was shown to be a function of particle density or size, and part of the difference in rates of selective uptake from the particles made with various apoproteins was explained by their differences in density or size.

Animals↗

Structure and polymorphism of 18-carbon fatty acyl triacylglycerols: effect of unsaturation and substitution in the 2-position.

The polymorphic behavior of symmetric diacid triacylglycerols (TGs), 1,3-dioleoyl-2-stearoyl (OSO), 2-elaidoyl (OEO), and 2-vaccinoyl (OVO) glycerols were studied by differential scanning colorimetry (DSC) and X-ray diffraction and compared with the corresponding monoacid TGs triolein (OOO), tristearin (SSS), trielaidin (EEE), and trivaccinin (VVV). The monoacid TGs formed a bilayered structure in all the polymorphic forms. On quenching from the melt, the diacid TGs OEO and OVO formed a bilayered (D = 45 A) beta'-phase with the exception of OSO, which formed a hexagonally packed bilayered (D = 52 A) alpha-phase. At -7 degrees C, the alpha-phase of OSO quickly transformed to a bilayered (D = 45 A) beta'-phase. Incubation at the beta'-phase melting temperature transformed OVO, OEO, and OSO into a trilayered (D = 65 A) beta-phase, where the 1,3-dioleoyl chains are segregated from the vaccinoyl, elaidoyl, or stearoyl chains into alternating layers. In summary, when all the acyl chains in a TG are the same (saturated, cis or trans unsaturated), the stable beta-phase packs into a bilayered structure. However, when the 1- and 3-acyl chains are cis unsaturated (bent) and the 2-acyl chain is either saturated or trans-unsaturated (straight), a bilayered beta'-phase can form, but transforms to a stable trilayered beta-phase, where the 2-acyl chains form a layer between two different layers of 1,3-oleoyl chains.

Calorimetry, Differential Scanning↗

The effect of free cholesterol on the solubilization of cholesteryl oleate in phosphatidylcholine bilayers: A 13C-NMR study.

The solubilization of cholesteryl oleate in sonicated phosphatidylcholine vesicles containing between 0 and 50 mol% cholesterol was studied by 13C-NMR using isotopically enriched [carbonyl-13C]cholesteryl oleate. The carbonyl-13C chemical shift from cholesteryl oleate in the phospholipid/cholesterol bilayer was significantly downfield from that for cholesteryl oleate in an oil phase and the peak area, relative to that of the phospholipid carbonyl, was used to determine bilayer solubility of the ester. The solubility (with respect to phospholipid) in the phospholipid bilayer without cholesterol (2.9 mol%) was only moderately reduced (to 2.3 mol%) at cholesterol levels up to 33 mol% but showed a more marked reduction to 1.4 mol% at 40 mol% cholesterol or 1.2 mol% at 50 mol% cholesterol. Since the vesicles containing 50 mol% cholesterol were larger (520 +/- 152 A diameter) than those with no cholesterol (291 +/- 97 A diameter), we measured the solubility of cholesteryl oleate in large vesicles with no cholesterol, prepared by extrusion through polycarbonate membrane filters, and found it similar to that in small, sonicated vesicles with no cholesterol. Therefore, the larger size of vesicles was not the factor responsible for the decreased cholesteryl oleate solubility at high cholesterol contents. A more direct effect of cholesterol is envisioned where the ester becomes displaced to deeper regions of the bilayer.

Cholesterol↗

Surface properties of 1,2-dipalmitoyl-3-acyl-sn-glycerols.

Stereospecific 1,2-dipalmitoyl-sn-glycerol and a series of 1,2-dipalmitoyl-3-acyl-sn-glycerols (TGs) with 3-acyl chains of two through six and eight carbons in length were synthesized. Pressure-area isotherms at 27 degrees C, surface melting temperatures (Ts), and equilibrium spreading pressures (esp) measured at the bulk melting temperature (Tf) were obtained for each TG and for dipalmitin. Whereas dipalmitin and the 3-acetyl-TG condense directly to an expanded mesomorphous state (30-33 A2/palmitoyl chain at the vapor pressure, pi v), the 3-propionyl- through 3-octanoyl-TGs show an area per molecule (in the liquid at pi v) that increases linearly from 105 to 130 A2/molecule (slope = 5 A2/CH2 group). This slope suggests that the 3-acyl chains are lying flat on the water at the end of the gas-liquid transition. Before solidification at 42-47 A2/molecule, the 3-propionyl- through 3-hexanoyl-TGs show a transition corresponding to the immersion of the 3-acyl chain. The pressure at this transition, pi tr, vs. 3-acyl carbon number is linear and indicates a chain immersion energy of 497 cal mol-1 per CH2. In contrast, the 3-octanoyl chain is not forced into the water but rather is pushed into the monolayer to lie parallel to the palmitoyl chains. As the sn-3 chain is lengthened, Ts decreases from 68 to 25 degrees C, but the 3-octanoyl monolayer does not solidify even at 5 degrees C because the short upright octanoyl chains fluidize the palmitoyl chains. The esp (at Tf) drops from 31.7 mN m-1 for dipalmitin to 20.6 mN m-1 for the 3-acetyl-TG.(ABSTRACT TRUNCATED AT 250 WORDS)

Diglycerides↗

Phase behavior and bilayer properties of fatty acids: hydrated 1:1 acid-soaps.

The physical properties in water of a series of 1:1 acid-soap compounds formed from fatty acids and potassium soaps with saturated (10-18 carbons) and omega-9 monounsaturated (18 carbons) hydrocarbon chains have been studied by using differential scanning calorimetry (DSC), X-ray diffraction, and direct and polarized light microscopy. DSC showed three phase transitions corresponding to the melting of crystalline water, the melting of crystalline lipid hydrocarbon chains, and the decomposition of the 1:1 acid-soap compound into its parent fatty acid and soap. Low- and wide-angle X-ray diffraction patterns revealed spacings that corresponded (with increasing hydration) to acid-soap crystals, hexagonal type II liquid crystals, and lamellar liquid crystals. The lamellar phase swelled from bilayer repeat distances of 68 (at 45% H2O) to 303 A (at 90% H2O). Direct and polarized light micrographs demonstrated the formation of myelin figures as well as birefringent optical textures corresponding to hexagonal and lamellar mesophases. Assuming that 1:1 potassium hydrogen dioleate and water were two components, we constructed a temperature-composition phase diagram. Interpretation of the data using the Gibbs phase rule showed that, at greater than 30% water, hydrocarbon chain melting was accompanied by decomposition of the 1:1 acid-soap compound and the system changed from a two-component to a three-component system. Comparison of hydrated 1:1 fatty acid/soap systems with hydrated soap systems suggests that the reduced degree of charge repulsion between polar groups causes half-ionized fatty acids in excess water to form bilayers rather than micelles.(ABSTRACT TRUNCATED AT 250 WORDS)

Calorimetry, Differential Scanning↗