Solid-liquid phase behavior of binary fatty acid mixtures. 2. Mixtures of oleic acid with lauric acid, myristic acid, and palmitic acid

Solid-liquid phase behavior was investigated for binary fatty acid mixtures composed of oleic acid (OA; cis-9-octadecenoic acid) and saturated fatty acids, lauric acid (LA; dodecanoic acid), myristic acid (MA; tetradecanoic acid), and palmitic acid (PA; hexadecanoic acid), by means of differential scanning calorimetry (DSC) and Fourier transform infrared spectroscopy (FT-IR). When the mixture was heated immediately after the solidification from the melt, the heat effect due to the gamma-to-alpha transformation of OA varied depending on the composition of the mixture. However, the mixture subjected to an annealing at the temperature slightly below the melting temperature provided the transformation at constant temperature which corresponds to the gamma-to-alpha transformation temperature of pure OA. This suggests that a solid phase formed by cooling of the melt of the mixture is not in an equilibrium state, but it relaxes to a stable solid during the annealing process. The T-X phase diagrams of these mixtures constructed from the DSC measurements demonstrate that the two fatty acid species are completely immiscible in a solid phase regardless of the type of polymorphs of OA, alpha- or gamma-form. According to a thermodynamic analysis of liquidus line basing on the regular solution model for the melt, the non-ideality of mixing tends to increase with the decrease in the acyl chain length of the saturated fatty acid, although the mixing is rather close to ideal.     

Solid-liquid phase behavior of binary fatty acid mixtures 3. Mixtures of oleic acid with capric acid (decanoic acid) and caprylic acid (octanoic acid)

Solid-liquid phase behavior of binary mixtures of oleic acid (OA)/capric acid (C10A) and OA/caprylic acid (C8A) were investigated by means of differential scanning calorimetry (DSC), Fourier transform infrared spectroscopy (FT-IR), and X-ray diffraction. The phase diagram of OA/C10A mixture constructed from the DSC results suggested that a molecular compound with the composition of OA:C10A = 3:2 is formed in a solid phase, and OA and the molecular compound are miscible, while C10A and the molecular compound are completely immiscible. The formation of the molecular compound was supported by the IR spectroscopic observation, and a possible model of the structure was proposed on the basis of X-ray diffraction spectrum in small angle region. This compound formation is characteristic of the OA/C10A mixture, and may be attributed to the similarity of the acyl chain length of C10A to the lengths of Delta- and omega-chains of OA (i.e., the chain segments divided by cis-double bond). The mixture of OA and C8A, whose chain length is close to but shorter than the two chain segments of OA, provided a eutectic-type phase diagram showing a partial mixing of the two components in OA-rich region. Thermodynamic analysis of the liquidus line in the phase diagram exhibits a systematic trend for the non-ideality parameter of mixing with the variation of the chain length difference between OA and saturated fatty acid species.     

Dynamical dimer structure and liquid structure of fatty acids in their binary liquid mixture: decanoic/octadecanoic acid and decanoic/dodecanoic acid systems

Dimer structure and liquid structure of fatty acids in their binary mixtures such as decanoic acid (DA)/octadecanoic acid (SA) and DA/dodecanoic acid (LA) were studied through the measurements of self-diffusion coefficient (D), differential scanning calorimetry (DSC), density and viscosity. The obtained phase diagrams showed that DA and SA form a eutectic in the solid state but partly a solid solution in the SA-rich region; DA and LA form an incongruent-melting compound which forms a eutectic with DA. In the liquid mixture of DA and SA, the D of DA is larger than that of SA over the entire range of compositions and tends to approach the D of SA with increasing SA-mole fraction; the D of DA in the DA/LA system is also larger than that of LA especially in the LA-poor region and steeply approaches that of LA with increasing LA-mole fraction. These D values and phase diagrams were compared with those for the binary mixtures of n-alkanes (C14/C20, C19/C20 and C20/C24); it is concluded that the two kinds of fatty acids always form their individual homodimers in their liquid mixtures regardless of their compositions and temperatures.     

A differential scanning calorimetry study of the interaction of free fatty acids with phospholipid membranes

Mixtures of stearic, arachic, oleic and linoleic acids with dimyristoylphosphatidylcholine (DMPC) and distearylphosphatidylcholine (DSPC) have been studied by means of differential scanning calorimetry (DSC). The mixtures of stearic (SA) and arachic acids (AA) with DMPC and DSPC show phase diagrams of the peritectic type, with a region of solid phase immiscibility from 0 to 28.5 mol% of fatty acid. A pure component, with a stoichiometry fatty acid/phospholipid (2:1) seems to be formed except for the system AA/DSPC. The mixtures of oleic (OA) and linoleic acids (LA) show complex phase diagrams. In the case of OA, different regions where a phase separation exists can be observed and for the mixture of OA with DMPC, a pure component seems to be formed with a stoichiometry OA/DMPC (1:2). LA shows different behaviour in the mixtures with DMPC and with DSPC. For the mixture, LA/DMPC, a fluid phase immiscibility region is observed over the same range of concentration as for the mixture with OA, however, the mixture with DSPC shows a solid phase immiscibility for the samples containing 45 mol% or more of LA. The interaction of the different free fatty acids with equimolar mixtures of DMPC and DSPC, showing monotectic behaviour, has also been analyzed. From our results it can be clearly concluded that saturated fatty acids partition preferentially into solid-like domains, while cis-unsaturated fatty acids partition preferentially into fluid-like domains.     

Interaction among molecules in mixtures of ceramide/stearic acid,ceramide/cholesterol and ceramide/stearic acid/cholesterol

To elucidate the interaction among the molecules which constitute intercellular lipids of stratum corneum, the phase diagrams in the binary mixtures of N-octadecanoyl-phytosphingosine (CER)/stearic acid (SA) and CER/cholesterol (CHOL) were studied by differential scanning calorimetry and by small- and wide-angle X-ray diffraction. These phase diagrams are mostly expressed by a eutectic type one. However, from their detailed analyses, it was revealed that in the phase diagram of CER/SA a new solid structure is formed just above the eutectic temperature. The lamellar spacing of the new structure is nearly equal to the length given by the sum of the two molecules of CER and/or SA, that is, in the lipid bilayer the hydrocarbon chains of CER and SA lie almost perpendicular to the lipid bilayer surface and the two kinds of molecules distribute homogeneously. On the other hand, in the binary mixture of CER/CHOL, CHOL molecules are apt to be isolated from the mixture. In a ternary mixture composed of equimolar lipids of CER, CHOL and SA, it was found that a pseudo-hexagonal structure takes place even in the solid state. This fact indicates that the three components are miscible and the hydrocarbon chains lie perpendicular to the lipid bilayer surface. We can draw the conclusion that the multi-component mixtures containing ceramide are apt to form the lamellar structure where even in the solid state the hydrocarbon chains lie perpendicular to the lipid bilayer surface and the components with hydrocarbon chains distribute homogeneously.     

Phase behaviour of stearic acid-stearonitrile mixtures. A thermodynamic study in bulk and at the air-water interface

The solid-liquid phase behaviour of stearic acid (SA) and stearonitrile (SN) in binary mixtures was investigated by differential scanning calorimetry (DSC), and the formation of SA-SN mixed monolayers at the air-water interface was followed by surface pressure-area (pi-A) measurements and by Brewster angle microscope (BAM) observation. The solid-liquid phase diagram is a eutectic type phase diagram, with the eutectic composition 0.90相似文献   

Crystallization and phase behavior of 1,3-propanediol esters II. 1,3-propanediol distearate/1,3-propanediol dipalmitate (SS/PP) and 1,3-propanediol distearate/1,3-propanediol dimyristate (SS/MM) binary systems

Polymorphic influences on the phase behavior of two types of binary mixtures of saturated monoacid 1,3-propanediol esters (PADEs), dipalmitate/distearate (PP/SS) and dimyristate/distearate (MM/SS) were examined by X-ray diffraction (XRD), differential scanning calorimetry (DSC), and by solid fat content (SFC), hardness and microscopy measurements. Three stacking modes have been found in the PP/SS binary system. Mixed SS-PP bilayers were detected in all mixtures, SS-SS bilayers in x(PP)=0.0-0.4 mixtures and PP-PP bilayers in x(PP)=0.6-0.1 mixtures. Two different but close beta polymorphs and one beta' polymorph were detected for this system. beta' was only detected in x(PP)=0.5-0.9 mixtures for the mixed bilayers. For the MM/SS binary system, only MM-MM and SS-SS bilayers were detected and both solid phases crystallized in two different beta forms. XRD data evidenced clearly that the MM and SS components were completely immiscible in the solid state. The phase diagrams constructed using DSC data, exhibited a typical eutectic-type phase boundary. The presence of eutectics, the shape of the solidus lines as well as the analysis of the individual enthalpies of melting indicated typical phase separation for both systems. A thermodynamic study based on the Hildebrand equation and using the Bragg-Williams approximation for non-ideality of mixing confirmed the phase separation in the solid phase and suggested that the PP and SS were miscible in the liquid phase and that SS formed an ideal mixing with MM. Avrami analysis of SFC vs. time curves indicated heterogeneous nucleation and spherulitic crystal development from sporadic nuclei, and suggested that the nucleation rate was higher for the mixture at the eutectic composition. The relative hardness was correlated with the enthalpies, the final SFC and the microscopy measurements.     

Phase behaviour of stearic acid-stearonitrile mixtures: A thermodynamic study in bulk and at the air-water interface

The solid-liquid phase behaviour of stearic acid (SA) and stearonitrile (SN) in binary mixtures was investigated by differential scanning calorimetry (DSC), and the formation of SA-SN mixed monolayers at the air-water interface was followed by surface pressure-area (π-A) measurements and by Brewster angle microscope (BAM) observation. The solid-liquid phase diagram is a eutectic type phase diagram, with the eutectic composition 0.90 < X_SN < 0.95 and T^eut = 40.9 °C. The DSC results also suggest that the two components are immiscible in the solid phase but form a liquid mixture with positive deviations to the ideal behaviour. At the air-water interface, the two components form liquid condensed monolayers in the entire range of compositions, at low surface pressures, while solid mixed monolayers only form at high surface pressures for X_SN < 0.8. Thermodynamic analysis indicates that SA and SN are miscible in the liquid condensed phase, with negative deviations from the ideal behaviour. The variation of the collapse surface pressure of mixed monolayers also indicates miscibility at the air-water interface.     

Dynamical dimer structure and liquid structure of fatty acids in their binary liquid mixture: dodecanoic and 3-phenylpropionic acids system

Dimer structure and liquid structure of fatty acids in the binary liquid mixture of dodecanoic (LA) and 3-phenylpropionic acids (PPA) were studied through the measurements of DSC, self-diffusion coefficient (D), density, viscosity, 13C NMR spin-lattice relaxation time, small-angle X-ray scattering (SAXS), and small-angle neutron scattering (SANS). The phase diagram of LA/PPA mixture exhibited a typical eutectic pattern, which means that LA and PPA are completely immiscible in solid phase. In the liquid phase of the LA/PPA mixture, D of LA always differed from that of PPA irrespective of their compositions. This exhibited that, in the liquid phase of the binary mixture of fatty acids giving a complete eutectic in the solid phase, the fatty acid dimers are composed of the same fatty acid species irrespective of their compositions. The liquid structure of the LA/PPA mixture was clarified through the SAXS and also the SANS measurements.     

The solid–liquid phase diagrams of binary mixtures of consecutive, even saturated fatty acids

For the first time, the solid–liquid phase diagrams of five binary mixtures of saturated fatty acids are here presented. These mixtures are formed of caprylic acid (C_8:0) + capric acid (C_10:0), capric acid (C_10:0) + lauric acid (C_12:0), lauric acid (C_12:0) + myristic acid (C_14:0), myristic acid (C_14:0) + palmitic acid (C_16:0) and palmitic acid (C_16:0) + stearic acid (C_18:0). The information used in these phase diagrams was obtained by differential scanning calorimetry (DSC), X-ray diffraction (XRD), FT–Raman spectrometry and polarized light microscopy, aiming at a complete understanding of the phase diagrams of the fatty acid mixtures. All of the phase diagrams reported here presented the same global behavior and it was shown that this was far more complex than previously imagined. They presented not only peritectic and eutectic reactions, but also metatectic reactions, due to solid–solid phase transitions common in fatty acids and regions of solid solution not previously reported. This work contributes to the elucidation of the phase behavior of these important biochemical molecules, with implications in various industrial applications.     

Unit cell volume and liquid-phase immiscibility in oleate-stearate lipid mixtures

The structural basis of immiscibility of stearic acid (SA) in two unsaturated lipids at room temperature was examined. A 5% SA mixture in octadec-9-enoic acid (OA) is cloudy; a 5% SA solution in the methyl ester of OA (MeOA) is fully miscible. At 10% SA in MeOA, a clear and immiscible phase formed. The composition of this immiscible phase however was not 10% SA, but 25% SA. Adding additional SA altered the amount of the second phase, not its stoichiometry. Molecular mechanics explains the molecular basis for the ratio of saturated and unsaturated lipids in the different phases. Packing order of lipids within a unit volume explains the discrete lipid composition ratio forming each of the observed miscible and immiscible phases. The smallest unit cell volume that explains the observed stoichiometry is a cube (not a sphere).     

Phase diagram of mixed monolayers of stearic acid and dimyristoylphosphatidylcholine. Effect of the acid ionization

The aim of this work is to study the phase diagram of mixed monolayers composed of dimyristoylphosphatidylcholine (DMPC) and stearic acid (SA) at different ionic strength and bulk pH of the aqueous subphase. In this way, the effect of ionization of SA on the interaction and thus on phase separation with the DMPC matrix can be analyzed. To this purpose, we first determined the ionization state of pure SA monolayers as a function of the bulk subphase pH. The SA monolayers are nearly fully ionized at pH 10 and essentially neutral at pH 4 and the mixture of DMPC and SA was studied at those two pHs. We found that the DMPC-enriched phase admits more SA if the SA monolayer is in a liquid-expanded state, which is highly related to the acid ionization state, and thus to the bulk pH and ionic strength. At pH 4 the molecules hardly mix while at pH 10 the mixed monolayer with DMPC can admit between 30 and 100% of SA (depending on the lateral pressure) before phase separation is established. The addition of calcium ions to the subphase has a condensing effect on SA monolayers at all pHs and the solubility of SA in the DMPC matrix does not depend on the bulk pH in these conditions. The observed phase diagrams are independent on the manner in which the state of the mixed film is reached and may thus be considered states of apparent equilibrium.     

Calorimetric and Fourier transform infrared spectroscopic studies on the interaction of glycophorin with phosphatidylserine/dipalmitoylphosphatidylcholine-d62 mixtures

Glycophorin has been isolated in pure form from human erythrocyte membranes and reconstituted into lipid vesicles composed of binary mixtures of bovine brain phosphatidylserine (PS) and acyl-chain perdeuterated dipalmitoylphosphatidylcholine (DPPC-d62). The effect of protein on lipid melting behavior and order has been monitored with differential scanning calorimetry and Fourier transform infrared spectroscopy (FT-IR). The phase diagram for PS/DPPC-d62 is consistent with that previously reported for PS/DPPC (Stewart et al. (1979) Biochim. Biophys. Acta 556, 1-16) and indicates that acyl chain perdeuteration does not greatly alter the lipid mixing characteristics. The use of deuterated lipid allows the examination of lipid order by FT-IR of each lipid component in the binary mixtures as well as in the ternary (lipid/lipid/protein) systems. Addition of glycophorin to a 30:70 PS/DPPC-d62 binary lipid mixture results in a preferential glycophorin/PS interaction leading to bulk lipid enriched in DPPC-d62. This is revealed in two ways: first, through cooperative calorimetric transitions increased in temperature from the binary lipid system and second, through FT-IR melting curves of the DPPC-d62 component which shows transitions increased in both onset and completion temperatures in the presence of protein. In addition, non-cooperative melting events are observed at temperatures below the onset of phase separation. The FT-IR data are used to assign these non-cooperative events to the melting of the PS component. For the 50:50 lipid mixture with protein, two transitions are observed in the DSC experiments. The IR results indicate that both lipid components are involved with the lower temperature event.     

Unusual partitioning behavior of CaATPase in dipalmitoylphosphatidylethanolamine/dielaidoylphosphatidylcholine++ + mixtures.

CaATPase from rabbit sarcoplasmic reticulum has been isolated, purified, stripped of its native lipids, and reconstituted into binary lipid mixtures of dielaidoylphosphatidylcholine (DEPC) and dipalmitoylphosphatidylethanolamine (DPPE) or acyl-chain perdeuterated DPPE (DPPE-d62). The partitioning properties of the protein were determined from differential scanning calorimetry (DSC) and Fourier transform infrared (FT-IR) spectroscopy. Acyl-chain perdeuteration allows the separate determination of the order and melting characteristics of each lipid species with FT-IR. The binary lipid mixture has been shown to be phase separated in the gel state (Brauner, J. W., and R. Mendelsohn, 1986, Biochim. Biophys. Acta, 861:16-24). The solid phases present at low temperatures correspond to a pure DEPC phase and a mixed phase of DEPC/DPPE-d62. Insertion of protein at 37 degrees C leads to a domain of relatively protein-free DPPE-d62 and a phase containing both lipids plus CaATPase. We suggest that CaATPase selects a fixed composition (60% DEPC, 40% DPPE-d62) for its immediate environment. The composition of the lipid in the immediate vicinity of protein is largely independent of the initial DEPC/DPPE-d62 ratios in the reconstitution protocol. The relevance of these results to observations of discrete domains in native membranes is discussed.     

Phase behaviour of oleanolic acid,pure and mixed with stearic acid: Interactions and crystallinity

The phase behaviour of pure oleanolic acid (OLA) and in mixtures with stearic acid (SA) was characterized by differential scanning calorimetry (DSC), X-ray powder diffraction (XRD), diffuse reflectance infrared Fourier transform spectroscopy (DRIFTS) and nuclear magnetic resonance (NMR). The crystalline OLA as received (OLA_ar) becomes amorphous after being dissolved in chloroform and vacuum-dried at 50 °C (OLA₅₀). Upon heating, both forms transform to the needle shape crystalline form (OLA₂₂₀). Dimerization through H-bonding between COOH groups was detected both in OLA_ar and OLA₂₂₀. Dimers are stronger in OLA₂₂₀, where H-bonding also involves the alcohol groups and plays a role in the crystalline organization. A eutectic type phase diagram was established for mixtures, with the eutectic composition close to pure SA. Mixtures rich in SA are miscible in the liquid and in the amorphous solid states, where the presence of SA–OLA co-dimers, formed through H-bonding between carboxyl groups, was detected. Miscibility and SA crystallinity decrease drastically with the OLA content.     

Infrared spectroscopy and differential scanning calorimetry studies of binary combinations of cis-6-octadecenoic acid and octadecanoic acid

Fourier transform infrared (FTIR) spectroscopy and differential scanning calorimetry (DSC) studies are reported for combinations of cis-6-octadecenoic acid (also termed petroselinic acid, PSA) and octadecanoic acid (also termed stearic acid, SA) across a wide range of binary mole ratio combinations. The data are then used to plot the phase diagram which is found to be montotectic with the PSA reducing the melting temperature of SA at all compositions. The relevance of these experiments to stratum corneum (SC) biophysical behavior, particularly the influence and potential mechanisms of PSA on dermal permeation, is discussed. The potential role of cis-6-octadecenoic acid as a permeation enhancer is discussed in the context of these studies of its interaction with saturated fatty acids.     

The solid-liquid phase diagrams of binary mixtures of consecutive, even saturated fatty acids: differing by four carbon atoms

The complete solid-liquid phase diagrams for four binary mixtures of saturated fatty acids are presented, for the first time, in this work. These mixtures are formed by caprylic acid (C_8:0) + lauric acid (C_12:0), capric acid (C_10:0) + myristic acid (C_14:0), lauric acid (C_12:0) + palmitic acid (C_16:0) and myristic acid (C_14:0) + stearic acid (C_18:0). The phase diagrams were obtained by differential scanning calorimetry (DSC) and X-ray diffraction (XRD). FT-Raman spectrometry and polarized light microscopy were used to complement the characterization for a complete understanding of the phase diagram. All of the phase diagrams here reported show the same global behavior that is far more complex than previously accepted. They present not only peritectic and eutectic reactions, but also metatectic reactions, due to solid-solid phase transitions common in fatty acids, and regions of solid solution not previously reported. This work contributes to the elucidation of the phase behavior of these important biochemical molecules with implications in various industrial applications.     

On the miscibility of cardiolipin with 1,2-diacyl phosphoglycerides: binary mixtures of dimyristoylphosphatidylethanolamine and tetramyristoylcardiolipin

The thermotropic phase behavior and organization of model membranes composed of binary mixtures of the quadruple-chained, anionic phospholipid tetramyristoylcardiolipin (TMCL) with the double-chained zwitterionic phospholipid dimyristoylphosphatidylethanolamine (DMPE) were examined by a combination of differential scanning calorimetry (DSC) and Fourier-transform infrared (FTIR) spectroscopy. After equilibration at low temperature, DSC thermograms exhibited by binary mixtures of TMCL and DMPE containing < 80 mol DMPE exhibit a fairly energetic lower temperature endotherm and a highly energetic higher temperature endotherm. As the relative amount of TMCL in the mixture decreases, the temperature, enthalpy and cooperativity of the lower temperature endotherm also decreases and is not calorimetrically detectable when the TMCL content falls below 20 mol%. In contrast, the temperature of the higher temperature endotherm increases as the proportion of TMCL decreases, but the enthalpy and cooperativity both decrease and the transition endotherms become multimodal. The FTIR spectroscopic results indicate that the lower temperature endotherm corresponds to a lamellar crystalline (L(c)) to lamellar gel (L(β)) phase transition and that the higher temperature transition involves the conversion of the L(β) phase to the lamellar liquid-crystalline (L(α)) phase. Moreover, the FTIR spectroscopic signatures observed at temperatures below the onset of the L(c)/L(β) phase transitions are consistent with the coexistence of structures akin to a TMCL-like L(c) phase and the L(β) phase, and with the relative amount of the TMCL-like L(c) phase increasing progressively as the TMCL content of the mixture increases. These latter observations suggest that the TMCL and DMPE components of these mixtures are poorly miscible at temperatures below the L(β)/L(α) phase transition temperature. Poor miscibility of these two components is also suggested by the complexity of the DSC thermograms observed at the L(β)/L(α) phase transitions of these mixtures and with the complex relationship between their L(β)/L(α) phase transition temperatures and the composition of the mixture. Overall, our data suggests that TMCL and DMPE may be intrinsically poorly miscible across a broad composition range, notwithstanding the homogeneity of the fatty acid chains of the two components and the modest (~10 °C) difference between their L(β)/L(α) phase transition temperatures.     

Bilayer structures in dioctadecyldimethylammonium bromide/oleic acid dispersions

This paper reports on the properties of bilayers composed of dioctadecyldimethylammonium bromide (DODAB) and oleic acid (OA) at various molar ratios. The mole fraction of OA, X_OA, was varied in the range of 0–1 and the total lipid content was constant and equal to 10 mM. The DODAB/OA dispersions were extruded at a temperature higher than that of the gel–liquid transition of DODAB. The morphology of bilayer structures formed in the dispersions was inspected using a cryogenic transmission electron microscopy (cryo-TEM) and a differential interference contrast microscopy (DIC). The observations revealed that the incorporation of OA into DODAB bilayer results in a decrease of the membrane curvature. Anisotropy measurements using 1,6-diphenylhexatriene (DPH) as a rotator probe demonstrated that the DODAB/OA membrane microviscosity decreased considerably for X_OA > 0.4. The thermal behavior of DODAB/OA membranes has been studied by differential scanning calorimetry (DSC). In the case of the systems in which X_OA < 0.8, the DODAB/OA membranes are in the gel phase at room temperature. Additionally, Langmuir monolayer experiments of the DODAB/OA mixtures showed that due to the electrostatic interactions between the oppositely charged head groups of DODAB and OA they get close to each other, which results in a decrease of the mean area per molecule. The results were next discussed based on the packing parameter concept. The reduction of the mean area per head group (a) in the DODAB/OA systems leads to subsequent increase in the so-called packing parameter (S), which governs the morphology of surfactant aggregates.     

A comparison of differential scanning calorimetric and Fourier transform infrared spectroscopic determination of mixing behavior in binary phospholipid systems

Fourier transform infrared (FT-IR) spectroscopy and differential scanning calorimetry (DSC) have been used to elucidate the phase behavior of two binary lipid mixtures, acyl chain perdeuterated 1,2-dipalmitoylphosphatidylethanolamine (DPPE-d62)/1,2-dielaidoylphosphatidylcholine (DEPC) and acyl chain perdeuterated 1,2-dipalmitoylphosphatidylcholine (DPPC-d62)/1,2-dimyristoylphosphatidylethanolamine (DMPE). The former shows gel state immiscibility over most of the composition range. The FT-IR data indicate that one of the solid phases is essentially pure DEPC, while the other solid phase contains both lipids. The DPPC-d62/DMPE pair are miscible over the entire composition range. The use of deuterated lipids as one component in the mixture permits the melting characteristics of each component to be separately determined in the FT-IR experiment. The FT-IR data are used to assign the endotherms observed in the DSC to particular molecular components. For the DPPE-d62/DEPC system, two endotherms are observed at compositions between 10 and 67 mol% DPPE-d62. The lower transition is assigned to the DEPC component, while the higher event contains contributions to the enthalpy from both lipids in the mixture. The midpoint of the DEPC melting occurs substantially below that for DPPE-d62. For the miscible pair, each of the lipids melt over approximately the same temperature range. The complementary and consistent nature of the information available from FT-IR and from DSC is demonstrated from the current work.