Crystal structure of cholesteryl decanoate.

Cholesteryl decanoate (C37H64O2) is monoclinic, space group P2I, with cell dimensions a = 12.931 (6), b = 9.066 (2), c = 30.22 (1) A, beta = 91.14 (4) degrees, and Z = 4. The atomic coordinates from cholesteryl laurate were used in an initial trial structure which was refined by block diagonal least-squares methods with 1846 observed X-ray reflections (R = 0.129). Molecules A and B have almost fully extended conformations, except at the ester bonds and towards the end of the decanoate B chain. The molecules are arranged in antiparallel array forming monolayers of thickness d001 = 30.22 A, with the molecular long axis making an angle of about 67 degrees with the layer interface. The crystal structure is very similar to that of cholesteryl nonanoate and cholesteryl laurate.     

The binary phase diagram of lecithin and cholesteryl linolenate

The condensed binary phase diagram of cholesteryl linolenate-egg yolk lecithin has been determined by polarizing light microscopy, differential scanning calorimetry and X-ray diffraction. On increasing the temperature lecithin forms rectangular, cubic and hexagonal liquid-crystalline structures into which varying amounts of cholesteryl linolenate are incorporated. As more cholesteryl linolenate is incorporated, the transition temperatures between different phases are lowered. The rectangular and cubic structures incorporate only small amounts of cholesteryl linolenate; the molar ratios, lecithin to cholesteryl linolenate, being 11:1 and 16:1, respectively. However, the hexagonal phase, in which the phosphorylcholine groups of the lecithin molecules form the core of the rod-like assembly of molecules, incorporates up to approximately 25% cholesteryl linolenate by weight, corresponding to a molar ratio 3:1. At higher concentrations, cholesteryl linolenate forms an excess phase and may be present as crystals, smectic or cholesteric liquid crystals, or as liquid oil, depending on the temperature. At higher temperatures, a large zone of a single isotropic liquid phase exists in which large amounts of lecithin are solubilized by the cholesterol ester. Up to 40% cholesteryl linolenate by weight, the transition temperatures between different phases are influenced by approximately 1% water (by weight) associated with egg lecithin.It is probable that the incorporated apolar cholesterol ester molecules are associated primarily with the apolar hydrocarbon chain region of the different lecithin structures. The resultant decrease in the observed transition temperatures would suggest an overall chain-disordering role for the incorporated cholesteryl linolenate molecules. The influence of cholesteryl linolenate on the thermodynamic stability of the different lecithin structures, together with the models suggested for the molecular orientations of cholesterol esters in the different liquid crystalline structures, may be relevant to the role of these lipids in more complex biological systems, particularly serum lipoproteins.     

The ternary phase diagram of lecithin, cholesteryl linolenate and water: phase behavior and structure

The ternary phase diagram of cholesteryl linolenate-egg lecithin-water has been determined by polarizing light microscopy, calorimetry and X-ray diffraction at 23 °C. Hydrated lecithin forms a lamellar liquid-crystalline structure into which small amounts of cholesteryl linolenate are incorporated. The maximum incorporation of cholesterol ester into this lamellar structure varies with the degree of hydration. Increasing the water concentration from 10 to 15% (w/w) increased the limiting molar ratio of cholesteryl linolenate to lecithin in the lamellar phase from 1:50 to 1:22. At intermediate concentrations (15 to 30% water) the cholesteryl linolenate:lecithin ratio remains constant at 1:22. When water is increased to 42.5%, the maximum water content in the lamellar phase, the molar ratio decreased to 1:32. At low water concentrations the cholesterol ester appears to be entirely in the apolar region of the lecithin bilayer, while at higher water concentrations the ester groups of cholesteryl linolenate may be located at the lipid-water interface. At high water concentrations the ester appears to disorder the alkyl chains of the lecithin, giving rise to a thinner lipid layer and an increased surface area per lipid molecule when compared to the lecithin-water system in the absence of cholesteryl linolenate.The lamellar phase is the only phase (except at water concentrations less than 5%) in which all three components mutually interact. All mixtures of the three components having compositions outside the one-phase (lamellar) zone produce additional phases of cholesteryl linolenate or water, or both. Between 23 °C and 60 °C only minor changes in the phase diagram are observed.     

Crystal structure and microstructure of cholesteryl oleyl carbonate

The crystal structure as well as the microstructure, i.e., size and strain, of crystallites of cholesteryl oleyl carbonate was determined from X-ray powder diffraction data. The X-ray line broadening was analyzed through the refinement of TCH-pseudo-Voigt function parameters (isotropic effects) and the refinement of multipolar functions, i.e., symmetrized cubic harmonics (anisotropic effects). The crystal structure turns out to be primitive monoclinic, space group Pc, type I monolayer having two molecules per unit cell with parameters: a = 18.921 ± 0.006 Å, b = 12.952 ± 0.003 Å, c = 9.276 ± 0.002 Å and β = 91.32 ± 0.03°. The average size of a well ground specimen of crystallites was 60 nm. The average micro-strain, e.g., 45 × 10⁻⁴ has been tentatively attributed to fatty chain conformational disorder. The unit cell parameters, including the lamellar thickness, of COC crystal is very closely similar to those of another, structurally similar cholesterol ester, e.g., cholesteryl oleate (CO) crystal, space group P2₁, type II monolayer. Type I monolayer structure has been established for COC on the basis of the intensity calculations of the XRD profiles of both CO and COC. The dipolar and structural disorder in a 4:1 molar, binary mixture of CO and COC can be accommodated in an induced smectic phase with a lamellar thickness, which is nearly equal to that of pure CO or pure COC.     

Molecular motions and thermotropic phase behavior of cholesteryl esters with triolein

The phase behavior of cholesteryl esters with triglyceride has been characterized by differential scanning calorimetry (DSC), light microscopy, and polarizing light microscopy (PLM). Temperature-dependent molecular motions determined by 13C NMR spectroscopy were correlated with thermotropic phase behavior. Two systems, cholesteryl oleate (CO) and a 3/1 w/w mixture of cholesteryl linoleate (CL) and CO, were examined in the presence of small amounts of triolein (TO). Both systems exhibited metastable cholesteric and smectic (or only smectic) phases. Increasing amounts of TO progressively lowered the liquid-crystalline phase transition temperatures and eventually abolished the cholesteric phase, but at differing amounts of TO for the two systems (between 4% and 5% with CL/CO and between 7% and 10% with CO). DSC and PLM showed a progressive broadening of the phase transitions as well as an overlapping of the temperature ranges of the cholesteric and smectic phases. At greater than or equal to 4% TO, a separate isotropic liquid phase coexisted with liquid-crystalline phases. 13C NMR spectroscopy was used to monitor the molecular motions of the cholesteryl ester steroid ring and acyl chain in liquid and liquid-crystalline phases. In the liquid phase, no significant changes in fatty acyl motions, as reflected in spin-lattice relaxation time (T1) and nuclear Overhauser enhancement (NOE) values, were found on addition of TO. The line width (v 1/2) of the steroid ring resonances increased markedly near (1-5 degrees C above) the isotropic liquid----liquid-crystal phase transition temperature (TLC). However, the C3/C6 v 1/2 ratio at 1 degree C above TLC was greater for mixtures exhibiting an isotropic----cholesteric transition than for mixtures exhibiting an isotropic----smectic transition. Rotational correlation times calculated for motions about the long molecular axis and the nonunique axis showed (i) that the ring motions became more anisotropic as TLC was approached and (ii) that the motions were more anisotropic at TLC + 1 degree C for systems exhibiting a cholesteric phase than for systems exhibiting only a smectic phase. 13C line widths in spectra of the cholesteryl ester liquid-crystalline phases suggested that TO perturbed the cholesteryl ester intermolecular interactions and increased the rates of cholesteryl ester molecular motions relative to neat esters.     

Temperature-dependent molecular motions and phase behavior of cholesteryl ester analogues

The phase behavior and temperature-dependent molecular motions of three cholesteryl ethers (caproyl, myristyl, oleyl) and a cholesteryl carbonate (oleyl) were characterized. The properties of each ether were qualitatively similar to, but quantitatively different from, those of the corresponding cholesteryl ester. For example, cholesteryl oleyl ether exhibited the same phase transitions as cholesteryl oleate, but at much lower temperatures (e.g., the ether isotropic liquid to cholesteric transition is at 29 degrees C). 13C NMR spectra of ethers in the isotropic liquid and liquid crystalline phases were similar to those of the ester analogue. However, near the liquid to liquid crystalline transition, the steroid ring C3 and C6 linewidths, the C3/C6 linewidth ratio, and the steroid ring rotational correlation times tau rx and tau rz calculated from the linewidths were larger for the ether than the ester analogue. The oleyl carbonate had qualitatively different properties from its analogues (e.g., stable vs. metastable cholesteric and smectic phases). Quantitative results (e.g., relatively long tau rx and tau rz in the isotropic liquid phase) for the carbonate were also distinct from those of both the ester and ether analogues. A comparison of analogues in which the polar linkage is the only structural variable yielded insights into the intermolecular interactions which influence phase behavior.     

The phase behavior of cholesteryl esters in intracellular inclusions.

Differential scanning calorimetry and polarizing light microscopy have been used to investigate kinetic and thermodynamic properties of the phase behavior of cholesteryl ester contained in Fu5AH rat hepatoma cells and J774 murine macrophages. These cultured cells store cholesteryl esters as cytoplasmic inclusions of approximately 1-micron diameter and thus are models of the foam cells characteristic of atherosclerotic plaque. Simple binary mixtures of cholesteryl palmitate and cholesteryl oleate, the predominant cholesteryl esters in cellular inclusions in both cell types serve as models to explain important aspects of the phase behavior of these inclusions. Although inclusions should exist as stable crystals at 37 degrees C under conditions of thermodynamic equilibrium, microscopic examination of cells indicates that inclusions exist as metastable liquid crystals at 37 degrees C for extended periods of time. Using an analytical model based on nucleation theory, we predict that the cholesteryl ester inclusions should be liquid-crystalline in the cytoplasm of living cells. This may not be true either for lysosomal cholesteryl ester or for extracellular cholesteryl ester present in advanced atherosclerotic plaque where fusion of droplets can enhance the possibility of crystallization. The enhanced metastability of the relatively fluid liquid-crystalline state in cellular inclusions should result in increased activity of the neutral cholesteryl ester hydrolase in living cells.     

Anomeric exchange and the structure of n-alkyl D-glucopyranosides. A study of binary phase behavior

X-Ray diffraction and calorimetric data from the alpha and beta anomers of n-alkyl D-glucopyranosides are analyzed to describe the molecular packing and co-solubility in the crystalline and liquid-crystalline phases. In the smectogenic chain-length series, the beta-glucosides are co-soluble, with almost ideal mixing in the crystalline and meso-phases for chain-length differences of two carbon atoms. The smectic phases of octyl alpha- and beta-glucosides are also co-soluble and a time sequence of phase diagrams (as well as lamellar X-ray data), as the solid obtained from the cooled melt is equilibrated, indicate that a metastable co-crystalline phase may exist until the respective hydrogen-bonding schemes are established. Lamellar spacings from a homologous series of the beta anomers indicate that both the crystal structure and smectic-layer packings involve bilayer stacking of the molecules, a result that is difficult to reconcile with the respective surface-area requirements of the molecular acyl chain and sugar moieties.     

Crystal structure of form II of cholesteryl palmitelaidate at 295 K

Form II for cholesteryl palmitelaidate (trans-9-hexadecenoate) (C43H74O2) is monoclinic P2(1) with a = 12.745(3), b = 9.006(2), c = 18.153(4) A, beta = 96.63 (2) degrees, Z = 2. The X-ray crystal structure of form II has been determined from 2506 reflections of which 2126 gave (F greater than 2 sigma). The data up to sin theta/lambda = 0.44A-1 (Dmin = 1.14 A) were measured with CuK alpha radiation from a sealed tube. These were supplemented up to sin theta/lambda = 0.52 A-1 (Dmin = 0.96 A) by measurements on the same crystal using a rotating anode X-ray source. The electron density was diffuse in the ester chain and the atoms of the cholesteryl tail were found to be disordered. The tail and the chain atoms were refined by restrained least squares methods to give R = 0.087 and Rw = 0.10 for reflections with F greater than 2 sigma. Crystal forms I and II represent two standard structure types already characterized for fatty acid esters of cholesterol. In form II, the ester chain is almost fully extended as is also the case for one of the two independent molecules (A) in form I. In form II, the chains pack loosely together for most of their length. M.s. amplitudes of thermal vibration for the chain C-atoms are almost uniform along the entire chain (approximately 0.25 A2 at 295 K). In form I, the proximal part of the A chain is surrounded by rigid cholesteryl groups. In this region, C-atom m.s. amplitudes are much reduced (approximately 0.10 A2) but they increase to about 0.5 A2 at the distal end of the chain where packing is very loose.     

Co-solubility of saturated cholesteryl esters: a comparison of calculated and experimental binary phase diagrams

Based on ideal solution theory, phase diagrams are calculated for binary compositions of cholesteryl esters and compared to experimental data from pairwise combinations in a saturated acyl chain series from caprylate to arachidate, which encompasses three crystal packing motifs in the solid state. Within a crystal structure class, nearly ideal co-solubility is found for binary solids, where the acyl chain lengths of the pure components differ by one methylene group. Beyond this chain length difference, nonideal solutions occur until fractionation occurs at e.g., six methylene unit increments between the components. The observed liquidus lines of the eutectic are near the theoretical curves when the combinations of two compounds packing in the same crystal structure fractionate. Fractionation also is found when liquids composed of two esters which favor different crystal structures are solidified from the melt, no matter what the chain length difference is; the liquidus curves for re-heated solids, however, are not necessarily predicted by the Schr?der equation. In general, co-miscibility can be found in mesophases formed from compounds with two different crystal structures.     

Lipid structure and the behavior of cholesteryl esters in monolayer and bulk phases.

The behavior of cholesteryl esters at the air-buffer interface was studied as a function of molecular area and the presence of noncholesterol-containing lipids (colipids). The data obtained indicate that cholesteryl esters with other than long, saturated acyl groups can be present in surface phases up to packing densities approximately those in natural membranes. Their apparent molecular areas in such phases, which are largely determined by colipid structure, suggest their orientation with the ester function toward the interface. The extent of miscibility in the surface phase is also a strong function of colipid structure. Reversibility of the monolayer to bulk phase transition is determined exclusively by the acyl structure of the cholesteryl ester. Of the esters examined, only those with cis unsaturation collapsed reversibly. Our data predict that cholesteryl esters should be present in small, but finite amounts on the surface of arterial lipid deposits and that a prerequisite for the removal of such deposits is that the bulk lipid phase be in a liquid or liquid crystalline state.     

Crystal structure of cholesteryl ester transfer protein reveals a long tunnel and four bound lipid molecules

Cholesteryl ester transfer protein (CETP) shuttles various lipids between lipoproteins, resulting in the net transfer of cholesteryl esters from atheroprotective, high-density lipoproteins (HDL) to atherogenic, lower-density species. Inhibition of CETP raises HDL cholesterol and may potentially be used to treat cardiovascular disease. Here we describe the structure of CETP at 2.2-A resolution, revealing a 60-A-long tunnel filled with two hydrophobic cholesteryl esters and plugged by an amphiphilic phosphatidylcholine at each end. The two tunnel openings are large enough to allow lipid access, which is aided by a flexible helix and possibly also by a mobile flap. The curvature of the concave surface of CETP matches the radius of curvature of HDL particles, and potential conformational changes may occur to accommodate larger lipoprotein particles. Point mutations blocking the middle of the tunnel abolish lipid-transfer activities, suggesting that neutral lipids pass through this continuous tunnel.     

Crystal structure of the stationary phase survival protein SurE with metal ion and AMP

The stationary phase survival protein SurE is a metal ion-dependent phosphatase distributed among eubacteria, archaea, and eukaryotes. In Escherichia coli, SurE has activities as nucleotidase and exopolyphosphatase, and is thought to be involved in stress response. However, its physiological role and reaction mechanism are unclear. We report here the crystal structures of the tetramer of SurE from Thermus thermophilus HB8 (TtSurE) both alone and crystallized with Mn(2+) and substrate AMP. In the presence of Mn(2+) and AMP, differences between the protomers were observed in the active site and in the loop located near the active site; AMP-bound active sites with the loops in a novel open conformation were found in the two protomers, and AMP-free active sites with the loops in a conventional closed conformation were found in the other two protomers. The two loops in the open conformation are entwined with each other, and this entwining is suggested to be required for enzymatic activity by site-directed mutagenesis. TtSurE exists as an equilibrium mixture of dimer and tetramer in solution. The loop-entwined structure indicates that SurE acts as a tetramer. The structural features and the absence of negative cooperativity imply the half-of-the-sites reactivity mechanism resulting from a pre-existing tendency toward structural asymmetry.     

Interaction of alpha-melanocyte stimulating hormone with binary phospholipid membranes: structural changes and relevance of phase behavior

The interaction of alpha-melanocyte stimulating hormone (alpha-MSH) with negatively charged binary membrane systems composed of either 1,2-dimyristoyl-sn-glycero-3-phosphocholine/1,2-dimyristoyl-sn-glycero-3-[phospho-rac-(1-glycerol)], (DMPC/DMPG) or DMPC/1,2-dimyristoyl-sn-glycero-3-phosphate (DMPC/DMPA), both at a 3:1 ratio, was studied using complementary techniques (differential scanning calorimetry, infrared and ultraviolet absorption spectroscopy, and steady-state and time-resolved fluorescence). The peptide structure in buffer, at medium to high concentrations, is a mixture of aggregated beta-strands and random coil, and upon increasing the temperature the random coil configuration becomes predominant. At low concentrations (micromolar) there are essentially no aggregates. When in interaction with the lipidic systems this transition is prevented and the peptide is stabilized in a specific conformation different from the one in solution. The incorporation of alpha-MSH into phosphatidic acid-containing systems produced a significant alteration of the calorimetric data. Lateral heterogeneity can be induced by the peptide in the DMPA-containing mixture, at variance with the one of DMPG. In addition, the lipid/water partition coefficient for the peptide in the presence of DMPC/DMPA is greater in the gel phase as compared to the fluid phase. From the high values of limiting anisotropies it can be concluded that the peptide presents a very reduced rotational dynamics when in interaction with the lipids, pointing out to a strong interaction. Overall, these results show that the structure and stability of alpha-MSH in a negatively charged membrane environment are substantially different from those of the peptide in solution, being stabilized in a specific conformation that could be important to eliciting its biological activity.     

The crystal structure of cholesteryl octanoate

Crystals of cholesteryl octanoate (C₃₅H₆₀O₂) are monoclinic, space group P2₁, with $\text{a = 12.80(3), b = 9.20(2), c = 14.12(3)}\text{A}\text{?}$, β = 93.81(3)° and 2 molecules per unit cell. The structure has been determined by Patterson rotation and translation methods from the X-ray intensities (Mo-Kα radiation) of 1320 reflections ($\text{sin}\text{θ/λ < 0.59}\text{A}\text{?}{}^{\mathrm{?1}}$) measured with a diffractometer. Refinement by block diagonal least squares and Fourier methods gave R = 0.096. The molecules are arranged in monolayers with their long axes antiparallel and severely tilted (28°). There is a close packing of cholesteryls within the monolayers, but the octanoate chains which form the layer interface regions are conformationally and thermally disordered. The crystal structure is quite different from that of cholesteryl nonanoate, as expected from the discontinuity in thermodynamic properties and phase behaviour which occurs at this point in the homologous series.     

The binary phase behavior of 1,3-dilauroyl-2-stearoyl-sn-glycerol and 1,2-dilauroyl-3-stearoyl-sn-glycerol

The binary phase behavior of purified 1,3-dilauroyl-2-stearoyl-sn-glycerol (LSL) and 1,2-dilauroyl-3-stearoyl-sn-glycerol (LLS) was investigated at a slow (0.1 °C/min) and a relatively fast (3.0 °C/min) cooling rate in terms of melting and crystallization, polymorphism, solid fat content (SFC), hardness and microstructure. Much of the behavior of the system is explained by its polymorphism and the influence of thermal processing. The α-form and the β′-form of a double chain length structure were detected in the mixtures cooled at 3.0 °C/min, whereas only the β′-form was detected in those cooled at 0.1 °C/min. X-ray diffraction data as well as thermodynamic data propose that the most stable phases are promoted by the symmetrical LSL. The measured trends in structural characteristics, thermal properties, SFC, relative hardness and microstructure delimit three groups of mixtures which imply a competition between the stabilizing effect of LSL and disordering introduced by kinetic effects: (a) LLS-rich mixtures with LSL molar fractions (X_LSL) less than 0.3, (b) mixtures with X_LSL clustered around 0.5 and (c) LSL-rich mixtures with X_LSL ≥ 0.7. The balance between ordering and kinetic effects determines the polymorphism of the mixtures, which in turn determines the behavior of the LSL/LLS system. The kinetic phase diagram of the LSL/LLS binary system constructed using heating differential scanning calorimetry thermograms displayed a singularity at the 0.5_LSL molar fraction which delimits two distinct behaviors: eutectic behavior in one region and monotectic behavior in the other. The molecular interactions, as depicted by a non-ideality parameter of mixing obtained from a thermodynamic model based on the Hildebrand equation, suggests an almost ideal mixing behavior and a moderate tendency to the formation of unlike-pairs in the liquid state.     

The binary phase behavior of 1,3-dicaproyl-2-stearoyl-sn-glycerol and 1,2-dicaproyl-3-stearoyl-sn-glycerol

The phase behavior of a binary system constituted of purified 1,3-dicaproyl-2-stearoyl-sn-glycerol (CSC) and 1,2-dicaproyl-3-stearoyl-sn-glycerol (CCS) was investigated at a very slow (0.1 °C/min) and a relatively fast (3.0 °C/min) cooling rate using differential scanning calorimetry (DSC), low resolution NMR, X-ray diffraction (XRD), and polarized light microscopy (PLM). Related forms of the β′ polymorph were detected for all mixtures as well as a β form for CSC-rich mixtures. A double chain length (DCL) stacking of the non-mixed CCS-CCS and CSC-CSC phases and a triple chain length (TCL) stacking of mixed CCS-CSC structure were detected for the different β′ forms. The kinetic phase diagram demonstrated an apparent eutectic at the 0.5_CSC composition when cooled at 0.1 °C/min and at the 0.25_CSC composition when cooled at 3.0 °C/min. The application of a thermodynamic model based on the Hildebrand equation suggests that compounds CSC and CCS are not fully miscible. In addition, the miscibility changes according to the structure of the growing solid phase which is dependent on CSC molar ratio as well as on the kinetics. It was also shown that the miscibility is concentration dependent and that the solid phase, which is growing at conditions well away from equilibrium, is determined kinetically. The molecular interactions were found to be strong and to favor the formation of CSC-CCS pairs in the liquid state. CSC and CCS were also shown to be immiscible in the solid state. Depressions in solid fat content (SFC) were observed for both rates. Relatively complex networks made of needle-like, spherulitic and granular crystals were observed in the CSC/CCS system. A pure CSC phase was found to be instrumental in promoting a higher SFC, and more stable polymorphic forms. The microstructure was shown to be strongly dependent on the cooling rate and was linked to the different polymorphic forms observed by DSC and XRD. Correlations between SFC and the eutectic behavior have been observed for the 3.0 °C/min cooling rate, but not directly in the case of the 0.1 °C/min cooling rate, where slower kinetics which favors the metastable to stable phase conversion processes prevented the same shifts in behavior.     

The binary phase behavior of 1,3-dimyristoyl-2-stearoyl-sn-glycerol and 1,2-dimyristoyl-3-stearoyl-sn-glycerol

The binary phase behavior of pure 1,3-dimyristoyl-2-stearoyl-sn-glycerol (MSM) and 1,2-dimyristoyl-3-stearoyl-sn-glycerol (MMS) was investigated in terms of polymorphism, melting and crystallization behavior, SFC, hardness and microstructure. Samples were crystallized at cooling rates of 3.0 and 0.1 degrees C/min. The asymmetric TAG demonstrated lower melting and crystallization points at both cooling rates. All samples crystallized in the beta' polymorph when cooled at 0.1 degrees C/min and in the alpha polymorph when cooled at 3.0 degrees C/min. The experimentally determined kinetic phase diagram of MSM-MMS was monotectic for both cooling rates. This data was well described by a thermodynamic model using the Bragg-Williams approximation for non-ideality of mixing and suggested that in both the solid and liquid states, like pair interactions (MSM-MSM and MMS-MMS) were favored over MSM-MMS interaction. A strong tendency to phase separation in the solid phase was also observed. For both cooling rates, the fit of the SFC (%)-time curves to a modified form of the Avrami model indicated that crystallization occurred in two distinct kinetic steps. Depressions seen in SFC did not correspond to depressions in hardness or melting temperatures.     

Eutectic interactions in binary systems containing cholesterol, cholesteryl esters and triacylglycerols

Binary phase behavior of saturated cholesterol esters with trilaurin or cholesterol, and cholesterol with trilaurin, is studied. The existence of specific molecular interactions is detected by comparing the liquidus curve of the eutectic with ideal theory of freezing point depression and correcting the theoretical curve with the Bragg-Williams model when necessary. X-ray data indicate that all eutectic solids are nearly totally fractionated. The phase diagrams are sometimes well-explained by ideal solution theory indicating that polar interactions (e.g., the hydrogen bonding of cholesterol) are much less important than van der Waals interactions between neighboring molecules. However, the hydrogen bonding networks of cholesterol can lead to nonideal solution behavior with other lipids, a phenomenon consistent with previous observations on simpler molecular binaries. An observed nonideal solution behavior of triacylglycerol with cholesterol esters, on the other hand, is unexpected since significant polar interactions are expected to be 'buried' in the predominant nonpolar volume of the molecules involved.