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S M Gruner

Publications and source records attributed to S M Gruner.

At least 37 records · Page 2Linked to original sources
PubMed1996

Small concentrations of alamethicin induce a cubic phase in bulk phosphatidylethanolamine mixtures.

Under normal conditions, excess water dispersions of liquid crystalline 1,2-dielaidoyl-sn-glycero-3- phosphoethanolamine (DEPE) are known to convert from a liquid crystalline lamellar (L alpha) to inverse hexagonal (HII) phase at about 60 degrees Celsius. The nonlamellar phase behavior of lipid systems is also known to depend on the monolayer spontaneous curvature. The single-channel activity of alamethicin in black lipid bilayer membranes has been shown to be dependent upon the lipid composition of the membrane. Since the monolayer spontaneous curvature properties (e.g., the monolayer spontaneous curvature, curvature coefficients and bilayer thickness) vary with lipid composition, the single-channel activity of alamethicin presumably also correlates with the monolayer spontaneous curvature properties. Accordingly, we reasoned that if alamethicin couples to the curvature properties of a lipid film, then the curvature properties must, in turn, be perturbed by the presence of alamethicin and that this perturbation should be observable in the lipid phase behavior. Here X-ray diffraction and NMR are used to show that the presence of as little as 1% alamethicin introduces a large region of cubic phase into the thermal phase diagram. This suggests that perturbation of the nonlamellar phase behavior of a lipid system may be a method to survey different channel-forming molecules for possible behavior that indicates that the ion channel is sensitive to the monolayer spontaneous curvature properties.

Alamethicin↗
PubMed1996

Correlation between lipid plane curvature and lipid chain order.

The 1-palmitoyl-2-oleoyl-phosphatidylethanolamine: 1-palmitoyl-2-oleoyl-phosphatidylcholine (POPE:POPC) system has been investigated by measuring, in the inverted hexagonal (HII) phase, the intercylinder spacings (using x-ray diffraction) and orientational order of the acyl chains (using 2H nuclear magnetic resonance). The presence of 20 wt% dodecane leads to the formation of a HII phase for the composition range from 0 to 39 mol% of POPC in POPE, as ascertained by x-ray diffraction and 2H nuclear magnetic resonance. The addition of the alkane induces a small decrease in chain order, consistent with less stretched chains. An increase in temperature or in POPE proportion leads to a reduction in the intercylinder spacing, primarily due to a decrease in the water core radius. A temperature increase also leads to a reduction in the orientational order of the lipid acyl chains, whereas the POPE proportion has little effect on chain order. A correlation is proposed to relate the radius of curvature of the cylinders in the inverted hexagonal phase to the chain order of the lipids adopting the HII phase. A simple geometrical model is proposed, taking into account the area occupied by the polar headgroup at the interface and the orientational order of the acyl chains reflecting the contribution of the apolar core. From these parameters, intercylinder spacings are calculated that agree well with the values determined experimentally by x-ray diffraction, for the variations of both temperature and POPE:POPC proportion. This model suggests that temperature increases the curvature of lipid layers, mainly by increasing the area subtended by the hydrophobic core through chain conformation disorder, whereas POPC content affects primarily the headgroup interface contribution. The frustration of lipid layer curvature is also shown to be reflected in the acyl chain order measured in the L alpha phase, in the absence of dodecane; for a given temperature, increased order is observed when the curling tendencies of the lipid plane are more pronounced.

Biophysical Phenomena↗
PubMed1995

High-resolution macromolecular structure determination using CCD detectors and synchrotron radiation.

BACKGROUND: Synchrotron radiation sources have made impressive contributions to macromolecular crystallography. The delay in development of appropriate X-ray detectors has, however, been a significant limitation to their efficient use. New technologies, based on charge-coupled devices (CCDs), provide capabilities for faster, more accurate, automated data collection. RESULTS: A CCD-based X-ray detector has been developed for use in macromolecular crystallography and has been in operation for about one and a half years at the Cornell High Energy Synchrotron Source. It has been used for a variety of crystallographic projects, including a number of high-resolution structural studies. The statistical quality of the data, the detector's ease and efficiency of use, and the growing number of structural results illustrate the practical utility of this new detector system. CONCLUSIONS: The new detector has enhanced capabilities for measuring diffraction patterns from crystals of macromolecules, especially at high resolution, when the X-ray intensities are weak. The survey of results described here ranges from virus crystallography to weakly diffracting small-molecule structure determination and demonstrates the potential of CCD detectors when combined with synchrotron radiation sources.

Amino Acid Sequence↗
PubMed1995

Lipid extracts from membranes of Acholeplasma laidlawii A grown with different fatty acids have a nearly constant spontaneous curvature.

X-ray diffraction methods were used to explore the variation in the spontaneous curvature of lipid extracts from Acholeplasma laidlawii strain A-EF22 grown with different mixtures of palmitic acid and oleic acid. It was shown that the cells respond to the different growing conditions by altering the polar head group compositions in order to keep the phase transition between lamellar and nonlamellar structures within a narrow temperature range. This has been interpreted to mean that the membrane lipids are adjusted toward an optimal packing (Lindblom et al. (1986) Biochemistry 25, 7502). Here it is shown that for these extracts, the membrane curvature is kept within a narrow range (58-73 A), compared to the range in curvatures exhibited by pure lipids extracts from the membrane (17-123 A). These observations support the hypothesis (Gruner (1989) J. Phys. Chem. 93, 7562) that the spontaneous curvature is a functionally important membrane parameter which is regulated by the organism and is likely to be one of the constraints controlling the lipid composition of the bilayer.

Acholeplasma laidlawii↗
PubMed1994

Freezing and melting water in lamellar structures.

The manner in which ice forms in lamellar suspensions of dielaidoylphosphatidylethanolamine, dielaidoylphosphatidylcholine, and dioleoylphosphatidylcholine in water depends strongly on the water fraction. For weight fractions between 15 and 9%, the freezing and melting temperatures are significantly depressed below 0 degree C. The ice exhibits a continuous melting transition spanning as much as 20 degrees C. When the water weight fraction is below 9%, ice never forms at temperatures as low as -40 degrees C. We show that when water contained in a lamellar lipid suspension freezes, the ice is not found between the bilayers; it exists as pools of crystalline ice in equilibrium with the bound water associated with the polar lipid headgroups. We have used this effect, together with the known chemical potential of ice, to measure hydration forces between lipid bilayers. We find exponentially decaying hydration repulsion when the bilayers are less than about 7 A apart. For larger separations, we find significant deviations from single exponential decay.

Freezing↗
PubMed1994

Enigmatic thermotropic phase behavior of highly asymmetric mixed-chain phosphatidylcholines that form mixed-interdigitated gel phases.

Twelve saturated mixed-chain phosphatidylcholines have been identified for which the thermotropic phase behavior observed upon cooling from the L alpha phase is dependent upon the thermal history of the sample in the gel phase. If fully hydrated samples of these lipids are cooled and soon thereafter examined by differential scanning calorimetry, one observes a single highly cooperative endotherm (the chain-melting phase transition) upon heating, and on subsequent cooling, a single exotherm that may occur at temperatures as much as 4-6 degrees C below that of the single endotherm observed upon heating. In contrast, if the samples are incubated in the gel state at low temperatures for prolonged periods of time, one observes a single heating endotherm as before, but two sharp exotherms upon cooling. The latter transitions occur at temperatures close to that of the single endotherm observed upon heating and the single cooling exotherm observed prior to incubation in the gel state. The combined enthalpy of the two cooling exotherms is the same as that of the single heating endotherm or the single cooling exotherm initially observed. Infrared spectroscopic and X-ray diffraction studies indicate that the structural conversions characteristic of liquid-crystalline/gel phase transitions occur at both of those cooling exotherms. Of the 12 lipids that exhibit this unusual behavior, nine fulfill the previously defined structural requirements for the formation of the so-called mixed-interdigitated gel phase, and there is evidence in the literature that one of the three remaining lipids also forms such a structure. Infrared spectroscopic studies of the other two lipids indicate that their gel phases exhibit spectroscopic features that closely resemble those of lipids that meet the previously defined structural criteria for the formation of mixed-interdigitated gel phases and that differ markedly from those of both saturated symmetric-chain and saturated mixed-chain phosphatidylcholines that do not normally form mixed-interdigitated gel phases. Also, electron density reconstructions based on small-angle X-ray diffraction studies of the gel phases of those two lipids indicate that the thickness of their gel phase bilayers is consistent with their forming mixed-interdigitated gel phases. Thus the unusual thermotropic phase behavior described here may be a general characteristic of phosphatidylcholines that form mixed-interdigitated gel phases. This unusual behavior is not associated with any major change in any of several physical properties of these lipid bilayers but may arise from an alteration of the size and/or structure of microdomains present in the liquid-crystalline phase.

Gels↗
PubMed1994

Differential scanning calorimetry and X-ray diffraction studies of the thermotropic phase behavior of the diastereomeric di-tetradecyl-beta-D-galactosyl glycerols and their mixture.

We have investigated the thermotropic phase behavior of aqueous dispersions of the 1,2- and 2,3-di-O-tetradecyl-1(3)-O-(beta-D-galactopyranosyl)-sn- glycerols and their diastereomeric mixture using differential scanning calorimetry and low-angle and wide-angle x-ray diffraction. Upon heating, unannealed aqueous dispersions of these compounds all exhibit a lower temperature, moderately energetic phase transition at approximately 52 degrees C and a higher temperature, weakly energetic phase transition at approximately 63 degrees C, both of which are reversible on cooling. X-ray diffraction measurements identify these events as the L beta (or L' beta)/L alpha and L alpha/HII phase transitions, respectively. The structures of the L beta, L alpha, and HII phases of these lipids, as determined by x-ray diffraction measurements, are identical within the error bars for all of these lipids. On annealing below the L beta/L alpha phase transition temperature, the L beta phase converts to an Lc phase at a rate which is strongly dependent on the chirality of the glycerol backbone (1,2-sn > 1,2-rac > 2,3-sn). The temperature of the phase transition from the Lc phase seen on reheating is also dependent on the glycerol chirality. In addition, the nature of the Lc phase changes on subsequent heating in the 1,2-sn and 1,2-rac lipids, but we have not been able to detect this Lc1/Lc2 phase transition by calorimetry. However, wide-angle x-ray diffraction measurements indicate that these Lc phases differ mostly in their hydrocarbon chain packing modes. The Lc2 phase does not appear to be present in the 2,3-sn compound, suggesting that its formation is not favored in this diastereomeric isomer. These observations are discussed in relation to the effect of glycerol chirality on the molecular packing of these glycolipids, particularly on hydrogen bonding and hydration in the interfacial region of the bilayer.

Biophysical Phenomena↗
PubMed1994

Studies of the thermotropic phase behavior of phosphatidylcholines containing 2-alkyl substituted fatty acyl chains: a new class of phosphatidylcholines forming inverted nonlamellar phases.

We have synthesized a number of 1,2-diacyl phosphatidylcholines with hydrophobic substituents adjacent to the carbonyl group of the fatty acyl chain and studied their thermotropic phase behavior by differential scanning calorimetry, 31P-nuclear magnetic resonance spectroscopy, and x-ray diffraction. Our results indicate that the hydrocarbon chain-melting phase transition temperatures of these lipids are lower than those of the n-saturated diacylphosphatidylcholines of similar chain length. In the gel phase, the 2-alkyl substituents on the fatty acyl chains seem to inhibit the formation of tightly packed, partially dehydrated, quasi-crystalline bilayers (Lc phases), although possibly promoting the formation of chain-interdigitated bilayers. In the liquid-crystalline state, however, these 2-alkyl substituents destabilize the lamellar phase with respect to one or more inverted nonlamellar structures. In general, increases in the length, bulk, or rigidity of the alkyl substituent result in an increased destabilization of the lamellar gel and liquid-crystalline phases and a greater tendency to form inverted nonlamellar phases, the nature of which depends upon the size of the 2-alkyl substituent. Unlike normal non-lamella-forming lipids such as the phosphatidylethanolamines, increases in the length of the main acyl chain stabilize the lamellar phases and reduce the tendency to form nonlamellar structures. Our results establish that with a judicious choice of a 2-alkyl substituent and hydrocarbon chain length, phosphatidylcholines (and probably most other so-called "bilayer-preferring" lipids) can be induced to form a range of inverted nonlamellar structures at relatively low temperatures. The ability to vary the lamellar/nonlamellar phase preference of such lipids should be useful in studies of bilayer/nonbilayer phase transitions and of the molecular organization of various nonlamellar phases. Moreover, because the nonlamellar phases can easily be induced at physiologically relevant temperatures and hydration levels while avoiding changes in polar headgroup composition, this new class of 2-alkyl-substituted phosphatidylcholines should prove valuable in studies of the physiological role of non-lamella-forming lipids in reconstituted lipid-protein model membranes.

Biophysical Phenomena↗
PubMed1993

Curvature dependent induction of the interdigitated gel phase in DPPC vesicles.

Ethanol causes biphasic melting behavior in saturated lecithins (Rowe (1983) Biochemistry 22, 3299-3305), a consequence of the formation of the stable interdigitated phase (Simon, S.A. and McIntosh, T.J. (1984) Biochim. Biophys. Acta 773, 169-172). The membrane systems studied to date have been large vesicle systems in which the membrane surface can be assumed to be locally planar. An immediate question arises as to whether surfaces of higher curvature interdigitate. To address this question we have prepared DPPC vesicles of varying diameters which we employed to determine the limiting size at which interdigitation occurs using ethanol as the inducer. We find that with decreasing vesicle size the concentration of ethanol necessary for the onset of interdigitation increases. Small isolated vesicles, at inducing concentrations of ethanol, do not stably interdigitate but rupture and coalesce into a viscous gel comprised of interdigitated lipid sheets. As discussed elsewhere (Ahl et al. (1992) Biophys. J. 243a) these sheets can be used as precursors for producing liposomes of large size and high internal volumes useful in drug delivery or modeling applications.

1,2-Dipalmitoylphosphatidylcholine↗
PubMed1993

Probability of alamethicin conductance states varies with nonlamellar tendency of bilayer phospholipids.

With few exceptions, membrane lipids are usually regarded as a kind of filler or passive solvent for membrane proteins. Yet, cells exquisitely control membrane composition. Many phospholipids found in plasma membrane bilayers favor packing into inverted hexagonal bulk phases. It was suggested that the strain of forcing such lipids into a bilayer may affect membrane protein function, such as the operation of transmembrane channels. To investigate this, we have inserted the peptide alamethicin into bilayer membranes composed of lipids of empirically determined inverted hexagonal phase "spontaneous radii" Ro, which will have expectably different degrees of strain when forced into bilayer form. We observe a correlation between measured Ro and the relative probabilities of different conductance states. States of higher conductance are more probable in dioleoylphosphatidylethanolamine, the lipid of highest curvature, 1/Ro, than in dioleoylphosphatidylcholine, the lipid of lowest curvature.

Alamethicin↗
PubMed1992

X-ray diffraction reconstruction of the inverted hexagonal (HII) phase in lipid-water systems.

The structure of the inverted hexagonal (HII) phase in biological lipid-water systems is studied to examine the physical interactions which drive the polymorphic phase behavior and which are also thought to play a relevant role in biological membrane function. A method is derived which yields the complex phase factors of the HII phase diffraction amplitudes from examination of a single sample. This method is applied to a low-resolution Fourier reconstruction of the HII phase in dioleoylphosphatidylethanolamine (DOPE) + water, specifically to examine deviations from the presumed circular model of the HII phase. It is found that the average radius of the water core, Rw, as determined from a Fourier reconstruction, is in good agreement with previously measured values of Rw obtained from more time-consuming traditional methods [Tate, M. W., & Gruner, S. M. (1989) Biochemistry 28, 4245]. In addition to the average value of Rw, the Fourier reconstruction also can be used to determine the true shape of the water core. It is found that the water core is circular to within 5% of Rw when the unit cell size is less than approximately 75 A. Above 75 A, however, a definite shape deformation becomes apparent, with radial noncircularities of 5-10%, probably in response to the increased entropic cost of packing the hydrocarbon chains into the anisotropic environment of the HII unit cell [Kirk, G. L., Gruner, S. M., & Stein D. E. (1984) Biochemistry 23, 1093]. As a more direct probe of the packing anisotropy, Fourier reconstructions of DOPE + dodecane and DOPE + squalene systems were compared with the reconstruction of DOPE. These oils are known to promote the low temperature occurrence of the HII phase, presumably by a reduction in the hydrocarbon packing stress. In support of this hypothesis, the alkanes were observed to relax the water core to a circular shape for even large lattices. In addition, anisotropy of the electron density near the end of the lipid chains is reduced when alkane is added, implying a more uniform hydrocarbon packing environment, consistent with the results of neutron diffraction upon the addition of deuterated decane [Turner, D. C., Gruner, S. M., & Huang, J. (1992) Biochemistry (following paper in this issue)].

Alkanes↗
PubMed1992

Distribution of decane within the unit cell of the inverted hexagonal (HII) phase of lipid-water-decane systems determined by neutron diffraction.

The addition of a free alkane such as decane to lipid-water systems is known to promote the formation of a low-temperature inverted hexagonal (HII) phase [Kirk, G. L., & Gruner, S. M. (1985) J. Phys. (Paris) 46, 761]. Kirk et al. [Kirk, G. L., Gruner, S. M., & Stein, D. E. (1984) Biochemistry 23, 1093] have discussed the hydrocarbon packing anisotropy in the HII unit cell and have suggested that free alkane will distribute in a way that reduces this packing anisotropy by allowing the lipid chain environment to become more uniform. By combining neutron and X-ray diffraction data to do a Fourier reconstruction of the HII phase of dioleoylphosphatidylethanolamine (DOPE) + water + deuterated decane, it was found that the decane preferentially partitions into the interstitial regions of the HII unit cell where it should be the most effective in alleviating the hydrocarbon chain packing stress, supporting the suggestion of Kirk et al. Using the distribution of decane within the unit cell, we have calculated the lipid length distribution for the situations with and without added alkane. With a suitable molecular model, this lipid length distribution may eventually be used to calculate the free energy change upon the addition of alkane. Such a measurement is important for a more realistic understanding of the interactions which lead to the formation of the HII phase.

Alkanes↗
PubMed1992

Kinetics of the lamellar-inverse hexagonal phase transition determined by time-resolved X-ray diffraction.

The kinetics of the lamellar (L alpha)-inverse hexagonal (HII) phase transition in diacylphosphatidylethanolamine (PE)--water systems were probed with time-resolved X-ray diffraction. Transition kinetics in the fast time regime (approximately 100 ms) were studied by initiating large temperature jumps (up to 30 degrees C) with a 50-ms electrical current pulse passed through a lipid-salt water dispersion, resulting in ohmic heating of the sample. Diffraction with a time resolution to 10 ms was acquired at the National Synchrotron Light Source. The time constant for the phase transition for 1,2-dioleoyl-sn-glycero-3-phosphoethanolamine (DOPE) was on the order of 100 ms for the largest temperature jumps recorded. Faster transition behavior was found for a 1,2-dielaidoyl-sn-glycero-3-PE mixture. The HII lattice parameters for both systems were seen to swell from an initial value commensurate with the lamellar lattice to the final equilibrium value. The rate of swelling was seen to be independent of the magnitude of the temperature jump. For small temperature jumps (less than 10 degrees C), the phase transition kinetics slow dramatically, and transition studies can readily be performed on a conventional rotating anode X-ray source. At 4 degrees C, a DOPE sample was observed to slowly convert to the hexagonal phase over the course of a week, with the decay in the lamellar intensity fitting a power law behavior over four decades of time. This power law behavior is shown to have interesting consequences to the determination of the phase transition temperature of lipid-water dispersions by conventional methods such as calorimetry.

Kinetics↗
PubMed1992

Effect of the chirality of the glycerol backbone on the bilayer and nonbilayer phase transitions in the diastereomers of di-dodecyl-beta-D-glucopyranosyl glycerol.

We have studied the physical properties of aqueous dispersions of 1,2-sn- and 2,3-sn-didodecyl-beta-D-glucopyranosyl glycerols, as well as their diastereomeric mixture, using differential scanning calorimetry and low angle x-ray diffraction. Upon heating, both the chiral lipids and the diastereomeric mixture exhibit characteristically energetic L beta/L alpha phase transitions at 31.7-32.8 degrees C and two or three weakly energetic thermal events between 49 degrees C and 89 degrees C. In the diastereomeric mixture and the 1,2-sn glycerol derivative, these higher temperature endotherms correspond to the formation of, and interconversions between, several nonlamellar structures and have been assigned to L alpha/QIIa, QIIa/QIIb, and QIIb/HII phase transitions, respectively. The cubic phases QIIa and QIIb, whose cell lattice parameters are strongly temperature dependent, can be identified as belonging to space groups Ia3d and Pn3m/Pn3, respectively. In the equivalent 2,3-sn glucolipid, the QIIa phase is not observed and only two transitions are seen at 49 degrees C and 77 degrees C, which are identified as L alpha/QIIb and QIIb/HII phase transitions, respectively. These phase transitions temperatures are some 10 degrees C lower than those of the corresponding phase transitions observed in the diastereomeric mixture and the 1,2-sn glycerol derivative. On cooling, all three lipids exhibit a minor higher temperature exothermic event, which can be assigned to a HII/QIIb phase transition. An exothermic L alpha/L beta phase transition is observed at 30-31 degrees C. A shoulder is sometimes discernible on the high temperature side of the L alpha/L beta event, which may originate from a QIIb/L alpha phase transition prior to the freezing of the hydrocarbon chains. None of the lipids show evidence of a QIIa phase on cooling. No additional exothermic transitions are observed on further cooling to -3 degrees C. However, after nucleation at 0 degrees C followed by a short period of annealing at 22 degrees C, the 1,2-sn glucolipid forms an Lc phase that converts to an L alpha phase at 39.5 degrees C on heating. Neither the diastereomeric mixture nor the 2,3-sn glycerol derivative shows such behavior even after extended periods of annealing. Our results suggest that the differences in the phase behavior of these glycolipid isomers may not be attributable to headgroup size per se, but rather to differences in the stereochemistry of the lipid polar/apolar interfacial region, which consequently effects hydrogen-bonding, hydration, and the hydrophilic/hydrophobic balance.

Biophysical Phenomena↗
PubMed1991

Nonbilayer phases of membrane lipids.

Numerous liquid crystalline biomembrane lipids are known to exhibit non-lamellar phases characterized by curvature of their component lipid monolayers. An understanding of the phase stability of these systems begins with analysis of the energy of bending the monolayers, the interactions which lead to the bending energy, and the geometrical constraints which lead to competing energy terms which arise when the monolayers are bent and packed onto lattices with different structures. Diffraction and other techniques suitable for probing lipid phase structure are described. A phenomenological model is reviewed which successfully explains many of the qualitative features of lipid mesomorphic phase behavior. A key result of this model is that lipid bilayer compositions which are close to the non-lamellar phase boundaries of their phase diagrams are characterized by a frustrated elastic stress which may modulate the activity of imbedded membrane proteins and which may provide a rationale for the prevalence of non-lamellar-tending lipid species in biomembrane bilayers. Areas in need of future research are discussed.

Kinetics↗
PubMed1991

Is the mechanism of general anesthesia related to lipid membrane spontaneous curvature?

Lipid bilayers in biomembranes may exist in a state of elastic curvature stress which may couple to the conformation of integral membrane proteins in a logical, and energetically significant, fashion. Many biomembranes contain sufficiently large fractions of nonlamellar-prone lipids to have monolayers under substantial curvature stress. Although very few experiments have been performed that can be used to correlate protein activity with curvature stress, the literature does contain a small number of studies that indicate that some protein function is nonspecifically modulated by the amounts of nonlamellar-prone lipid in the imbedding bilayers. The spontaneous curvature, is altered by the presence of anesthetics in physiologically relevant concentrations. This leads us to suggest that anesthetic action may be coupled to protein function via alteration of the tensions leading to the spontaneous curvature of biomembrane layers. The spontaneous curvature is also sufficiently sensitive to pressure that a mechanism for the pressure reversal of anesthesia follows if the effects of pressure are to counter changes in membrane lateral tension induced by anesthetics. It is emphasized that many more experimental data must be acquired to determine whether the ideas presented in this paper have validity. In particular, there is a need for data on the effects of different anesthetics and pressure on the spontaneous curvature and, more generally, lipid monolayer lateral tensions. Most importantly, experiments must be performed to investigate whether protein function correlates with these quantities.

Anesthesia, General↗
PubMed1990

Thermotropic characterization of the 2-O-acyl,polyprenyl alpha-D-glucopyranoside isolated from palmitate-enriched Acholeplasma laidlawii B membranes.

The thermotropic phase behavior of a monoacylated neutral glucolipid (2-O-acyl,polyprenyl alpha-D-glucopyranoside), isolated from palmitate-enriched Acholeplasma laidlawii B membranes, was studied by differential scanning calorimetry, infrared spectroscopy and X-ray diffraction. When equilibrated at low temperatures, aqueous dispersions of this lipid form an ordered, crystal-like lamellar gel phase which transforms to an inverted hexagonal phase at temperatures near 65 degrees C upon heating. However, upon cooling from high temperatures, the inverted hexagonal phase remains stable down to temperatures near 45 degrees C. Further cooling first results in the formation of a metastable lamellar liquid crystalline phase at temperatures near 35 degrees C and then a metastable gel phase at lower temperatures. The metastable gel phase, if immediately reheated at a fast scan rate, undergoes a gel/liquid-crystalline phase transition at temperatures near 33 degrees C. These results indicate that this monoacylated glucolipid exhibits its gel/liquid-crystalline phase transition and its lamellar/non-lamellar phase transition at considerably lower temperatures than does the monoglycosyldiacylglycerol formed under the same conditions. When cultured in media enriched in 'high-melting' fatty acids, Acholeplasma laidlawii B synthesizes large quantities of the 2-O-acyl,polyprenyl alpha-D-glucopyranoside (up to 60 mol%) mainly at the expense of the monoglucosyldiacylglycerol (the only other nonbilayer-forming liquid normally found in the cell membrane of this organism). We thus suggest that the biosynthesis of this novel glucolipid, in response to the biosynthetic incorporation of high-melting exogenous fatty acids, is an adaptive response designed to maintain a predominantly liquid-crystalline membrane lipid bilayer at the growth temperature, while retaining the high proportion of nonbilayer-forming glucolipid species characteristic of A. laidlawii B cells cultured under these conditions.

Acholeplasma laidlawii↗