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We performed differential scanning calorimetric (DSC) and Fourier transform infrared (FTIR) spectroscopic studies of the effects of cholesterol (Chol), thiocholesterol (tChol) and cholesterol sulfate (CholS) on the thermotropic phase behavior and organization of dipalmitoylphosphatidylcholine (DPPC) bilayer membranes. Our DSC results indicate that Chol and tChol incorporation produce small temperature increases in the main phase transition broad component while CholS markedly decreases it, but Chol decreases cooperativity and enthalpy more strongly than CholS and especially tChol. Hence, Chol and tChol thermally stabilize fluid DPPC bilayer sterol-rich domains while CholS markedly destabilizes them, and CholS and particularly tChol are less miscible in such domains. Our FTIR spectroscopic results indicate that Chol incorporation increases the rotational conformational order of fluid DPPC bilayers to a slightly and somewhat greater degree than tChol and CholS, respectively, consistent with our DSC findings. Also, Chol and CholS produce comparable degrees of H-bonding (hydration) of the DPPC ester carbonyls in fluid bilayers, whereas tChol increases H-bonding. At low temperatures, Chol is fully soluble in gel-state DPPC bilayers, whereas tChol and CholS are not. Thus tChol and CholS incorporation can produce considerably different effects on DPPC bilayers. In particular, the tChol thiol group markedly reduces its lateral miscibility and increases DPPC carbonyl H-bonding without significantly affecting the other characteristic effects of Chol itself, while the CholS sulfate group significantly reduces its ability to thermally stabilize and order fluid DPPC membranes. This latter result suggests that the molecular basis for the purported ability of CholS to "stabilize" various biological membranes should be re-examined.

We performed differential scanning calorimetric (DSC) and Fourier transform infrared (FTIR) spectroscopic studies of the effects of cholesterol (CHOL), 7-dehydrocholeterol (7DHC) and desmosterol (DES) on the thermotropic phase behavior and organization of dipalmitoylphosphatidylcholine (DPPC) bilayer membranes. 7DHC and DES are the immediate biosynthetic precursors of CHOL in the Kandutch-Russell and Bloch pathways and 7DHC and DES differ in structure from CHOL only by the presence of an additional double bond at C7 of ring B or C24 of the alkyl side chain, respectively. Our DSC results indicate that the incorporation of all three sterols produces comparable decreases in the temperature of the pretransition of DPPC, but CHOL decreases its cooperativity and enthalpy more strongly than 7DHC and especially DES. These findings indicate that all three sterols decrease the thermal stability of gel phase DPPC bilayers but that 7DHC and especially DES are less miscible in them. However, the incorporation of CHOL and DES produce comparable increases in the temperature of the broad component of the main phase transition of DPPC while 7DHC decreases it, but again CHOL produces greater decreases in its cooperativity and enthalpy then 7DHC and especially DES. These results indicate that CHOL and DES stabilize the sterol-rich domains of fluid DPPC bilayers, but that 7DHC and especially DES are less miscible in them. Our FTIR spectroscopic results indicate that CHOL increases the rotational conformational order of fluid DPPC bilayers to a somewhat and markedly greater degree than DES and 7DHC, respectively, consistent with our DSC findings. Our spectroscopic results also indicate that although all three sterols produce comparable degrees of H-bonding (hydration) of the DPPC ester carbonyl groups in fluid bilayers, CHOL is again found to be fully soluble in gel state DPPC bilayers at low temperatures, whereas 7DHC and especially DES are not. In general, we find that 7DHC and DES incorporation produce considerably different effects on DPPC bilayer membranes. In particular, the presence of an additional double bond at C7 or C24 produces a marked reduction in the ability of 7DHC to order fluid DPPC bilayers and in the miscibility of DES in such bilayers, respectively. These different effects may be the biophysical basis for the reduction of these double bonds in the last steps of CHOL biosynthesis, and for the deleterious biological effects of the accumulation of these sterols in vivo.

We present the results of a comparative differential calorimetric and Fourier transform infrared spectroscopic study of the effect of cholesterol and five analogues on the thermotropic phase behaviour and organization of dipalmitoylphosphatidylcholine bilayer membranes. These sterols/steroids differ in both the nature and stereochemistry of the polar head group at C3 (βOH, αOH or C O) and in the position(s) of the double bond(s). In the Δ5 sterols/steroid series, the concentration of these compounds required to abolish the DPPC pretransition, inversely related to their relative ability to disorder gel state DPPC bilayers, decreases markedly in the order βOH > αOH > C O. However, in the Δ4,6 series, these concentrations are similar, regardless of polar head group chemical structure. Similarly, the residual enthalpy of the DPPC main phase transition at 50 mol% sterol/steroid, which is inversely related to the miscibility of these compounds in the DPPC bilayer, also increases in the order βOH > αOH > C O, but this effect is attenuated in the Δ4,6 series. In the two pairs of sterol epimers, the Δ4,6 compounds exhibit a greater decrease in the temperature and enthalpy of both the pretransition and the main phase transition, whereas the opposite result is observed in the ketosteroid pair. Similarly, the ability of these compounds to order the DPPC hydrocarbon chains decreases in the order βOH > αOH > C O in both series of compounds, but in the two pairs of sterol epimers, hydrocarbon chain ordering is greater for the Δ5 than the Δ4,6 sterols, whereas the opposite is the case for the steroid pair. Thus, the characteristic effects of sterols/steroids on fluid lipid bilayers are optimal when an OH group rather than C O group is present at C3, and when this OH group is in the equatorial orientation. We suggest that the presence of keto–enol tautomerism in the conjugated Δ4,6 ketosteroid may provide additional H-bonding opportunities to adjacent DPPC molecules in the bilayer, which results in more cholesterol-like effects.

GS10 [cyclo-(VKLdYPVKLdYP)] is a synthetic analog of the naturally occurring antimicrobial peptide gramicidin (GS) in which the two positively charged ornithine (Orn) residues are replaced by two positively charged lysine (Lys) residues and the two less polar aromatic phenylalanine (Phe) residues are replaced by the more polar tyrosine (Tyr) residues. In this study, we examine the effects of these seemingly conservative modifications to the parent GS molecule on the physical properties of the peptide, and on its interactions with lipid bilayer model and biological membranes, by a variety of biophysical techniques. We show that although GS10 retains the largely β-sheet conformation characteristic of GS, it is less structured in both water and membrane-mimetic solvents. GS10 is also more water soluble and less hydrophobic than GS, as predicted, and also exhibits a reduced tendency for self-association in aqueous solution. Surprisingly, GS10 associates more strongly with zwitterionic and anionic phospholipid bilayer model membranes than does GS, despite its greater water solubility, and the presence of anionic phospholipids and cholesterol (Chol) modestly reduces the association of both GS10 and GS to these model membranes. The strong partitioning of both peptides into lipid bilayers is driven by a large favorable entropy change opposed by a much smaller unfavorable enthalpy change. However, GS10 is also less potent than GS at inducing inverted cubic phases in phospholipid bilayer model membranes and at inhibiting the growth of the cell wall-less bacterium Acholeplasma laidlawii B. These results are discussed in terms of the comparative antibiotic and hemolytic activities of these peptides.

We present the results of a comparative differential calorimetric and Fourier transform infrared spectroscopic study of the effect of cholesterol and five of its analogues on the thermotropic phase behaviour and organization of dipalmitoylphosphatidylcholine bilayer membranes. These sterols/steroids differ in both the nature and stereochemistry of the polar head group at C3 (βOH, αOH or C O) and in the position of the double bond (C4–C5 in ring A or C5–C6 in ring B). In the three Δ5 sterols/steroid series, the concentration of these compounds required to abolish the DPPC pretransition, inversely related to their relative ability to disorder gel state DPPC bilayers, decreases in the order βOH > αOH > C O and these differences in concentration are significant. However, in the Δ4 series, these concentrations are more similar, regardless of polar head group nature or stereochemistry. Similarly, the residual enthalpy of the main phase transition of DPPC at 50 mol.% sterol/steroid, which is inversely related to the miscibility of these compounds in the DPPC bilayer, also increases in the order βOH > αOH > C O, but this effect is attenuated in the Δ4 as opposed to the Δ5 series. Both of these results indicate that the presence of a double bond at C4–C5 in ring A, as compared to a C5–C6 double bond in ring B, reduces the effect of variations in the structure of the polar group at C3 on the properties of the host DPPC bilayer. The movement of the double bond from C5 to C4 in the two sterol pairs results in a greater decrease in the temperature and enthalpy of both the pretransition and the main phase transition, whereas the opposite result is observed in the ketosteroid pair. Similarly, the ability of these compounds to order the DPPC hydrocarbon chains decreases in the order βOH > αOH > C O in both series of compounds, but in the two sterol pairs, hydrocarbon chain ordering is greater for the Δ5 than the Δ4 sterols, whereas the opposite is the case for the steroid pair. All of these results indicate that the typical effects of sterols/steroids in increasing the packing density and thermal stability of fluid lipid bilayers are optimal when an OH group rather than C O group is present at C3, and that this OH group is more effective in the equatorial rather than the axial orientation. We can explain all of our sterol results by noting that the shift of the double bond from Δ5 to Δ4 introduces of a bend in ring A, which in turn destroys the coplanarity of the steroid fused ring system and reduces the goodness of sterol packing in the host DPPC bilayer. However, this conformational change should also occur in the ketosteroid pair, yet our experimental results indicate that the presence of the Δ4 double bond is less disruptive than a double bond at Δ5. We suggest that the presence of keto-enol tautomerism in the conjugated Δ4 ketosteroid, but not in the nonconjugated Δ5 compound, may provide additional H-bonding opportunities to adjacent DPPC molecules in the bilayer, which can overcome the unfavourable conformational change in ring A induced by the Δ4 double bond.

Studying the nature of interactions between the sterol ring system and neigbouring phospholipid molecules is important for our understanding of the properties of sterols in biological molecules and the role of such interactions in many disease processes. In this project, the thermotropic phase behaviour of binary dipalmitoylphosphatidylcholine (DPPC)/sterol mixtures with different sterol ring configurations (C5,6 double bond, 5α-H and 5β-H orientation and either 3α-OH, 3β-OH, 3-ketone functional groups) was investigated using differential scanning calorimetry (DSC) and was compared to earlier studies of cholesterol/ and epicholesterol/DPPC mixtures. Given the differences in the thermodynamic parameters obtained from these mixtures and their associated changes in bilayer stability and miscibility, it is clear that changing the sterol chemical configuration has a significant effect on bilayer properties. Any sterol molecule whose ring structure deviates from that of cholesterol is unlikely to be fully miscible in mammalian membranes.

This review deals with the effect of variations in phospholipid and sterol structure on the nature and magnitude of lipid-sterol interactions in lipid bilayer model membranes. The first portion of the review covers the effect of Chol itself on the thermotropic phase behavior and organization of a variety of different glycero- and sphingolipid membrane lipid classes, varying in the structure and charge of their polar headgroups and in the length and structure of their fatty acyl chains. The second part of this review deals with the effect of variations in sterol structure on the thermotropic phase behavior and organization primarily of the well studied DPPC model membrane system. In the third section, we focus on some of the contributions of sterol functional group chemistry, molecular conformation and dynamics, to sterol-lipid interactions. Using those studies, we re-examine the results of recently published experimental and computer-modeling studies to provide a new more dynamic molecular interpretation of sterol-lipid interactions. We suggest that the established view of the rigid sterol ring system and extended alkyl side-chain obtained from physical studies of cholesterol-phospholipid mixtures may not apply in lipid mixtures differing in their sterol chemical structure.

Non-covalent immobilized artificial membrane reverse-phase high performance liquid chromatography was previously evaluated as a means whereby elution times for antimicrobial peptides from columns mimicking the lipid bilayers of different membrane systems might be used as a fast-screening method to compare relative binding effectiveness. Such a system would aid in the development of antimicrobial peptides that bind preferentially to model pathogenic systems and leave the host’s membranes reasonably unaffected. A non-covalent approach allows for flexibility in membrane composition but was found to be inadequate for analysis of most peptides due to significant lipid loss at high acetonitrile concentrations. A covalent approach where phosphatidylcholine was amide-linked to the silica surface was examined to evaluate its use as a fast-screening method and compare its data to that collected from the non-covalent columns. Initial work with a 1-cm column proved ineffective due to problems with balancing flow rates with retention times, and work was shifted to a longer 10-cm column. Results suggested that peptides bind much more strongly to covalent columns than non-covalent ones, with the binding especially enhanced by the presence of cationic residues. These columns had lipid packing densities much lower than true membranes, indicating that the peptides were partitioning deep into the bonded phase of the columns rather than into the interfacial region of the phosphate head groups, as expected in situations of biologically-relevant lipid packing densities.

Aqueous dispersions of cholesterol-containing phosphatidylethanolamine (PE) bilayers were examined by a combination of high-sensitivity differential scanning calorimetry (DSC), Fourier transform infrared (FTIR) and 31P-nuclear magnetic resonance spectroscopy. Regardless of hydrocarbon chain length, the incorporation of low levels of cholesterol into these bilayers causes progressive reductions in the temperature, enthalpy and overall cooperativity of the lipid hydrocarbon chain-melting phase transition. Moreover, at low cholesterol levels, the heating and cooling thermograms observed for the cholesterol/PE binary mixtures are similar, indicating comparable levels of lateral miscibility of cholesterol with PE bilayers in the gel and liquid-crystalline states. However, at higher levels of cholesterol incorporation, marked differences between the heating and cooling thermograms are noted. Upon heating, complex multicomponent thermograms are observed in PE bilayers containing large amounts of cholesterol, and the temperature and overall enthalpy values increase discontinuously from the pattern of monotonic decrease observed at lower cholesterol levels. Moreover, these discontinuities begin to emerge at progressively lower cholesterol concentrations as PE hydrocarbon chain length increases. Upon cooling, a simpler pattern of thermotropic behavior is observed, and the measured temperature and enthalpy values continue to decrease monotonically with increases in cholesterol content. These results suggest that at higher concentrations cholesterol exhibits a decreased degree of lateral miscibility in the gel or crystalline as compared to the liquid-crystalline states of PE bilayers, particularly in the case of the longer-chain PEs. Our FTIR and 31P-nuclear magnetic resonance spectroscopic studies also show that the thermotropic events observed with mixtures of low cholesterol content are analogous to the gel/liquid-crystalline phase transitions exhibited by the pure PEs. However, lamellar crystalline phases readily form when mixtures of high cholesterol content are cooled to low temperatures. Moreover, these crystalline phases are spectroscopically indistinguishable from those formed by the pure PEs, indicating that cholesterol is excluded from such phases. Upon subsequent heating, the melting of these crystalline phases gives rise to the complex thermograms detected by DSC and to the discontinuities in the phase transition temperature and enthalpy noted above. This pattern of behavior differs markedly from that observed with the corresponding phosphatidylcholines (PCs), where comparable degrees of cholesterol miscibility are observed in the gel and liquid-crystalline states even at high cholesterol concentrations, and where cholesterol inhibits rather than facilitates the formation of lamellar crystalline phases. We also find that the presence of cholesterol does not result in the hydrophobic mismatch-dependent shifts in the phase transition temperature in PE bilayers previously observed in PC bilayers of varying thickness. We attribute these differences in the effects of cholesterol on phospholipid thermotropic phase behavior to stronger electrostatic and hydrogen bonding interactions at the surfaces of PE and compared to PC bilayers.

To investigate the role of peptide–membrane interactions in the biological activity of cyclic cationic peptides, the conformations and interactions of four membrane-active antimicrobial peptides [based on Gramicidin S (GS)] were examined in neutral and negatively charged micelles and phospholipid vesicles, using CD and fluorescence spectroscopy and ultracentrifugation techniques. Moreover, the effects of these peptides on the release of entrapped fluorescent dye from unilamellar vesicles of phosphatidylcholine (PC) and phosphatidylethanolamine/phosphatidylglycerol (PE/PG) were studied. The cyclic peptides include GS10 [Cyclo(VKLdYP)2], GS12 [Cyclo(VKLKdYPKVKLdYP)], GS14 [Cyclo(VKLKVdYPLKVKLdYP)] and [d-Lys]4GS14 [Cyclo(VKLdKVdYPLKVKLdYP)] (underlined residues are d-amino acids), were different in their ring size, structure and amphipathicity, and covered a broad spectrum of hemolytic and antimicrobial activities. Interaction of the peptides with the zwitterionic PC and negatively charged PE/PG vesicles were distinct from each other. The hydrophobic interaction seems to be the dominant factor in the hemolytic activity of the peptides, as well as their interaction with the PC vesicles. A combination of electrostatic and hydrophobic interactions of the peptides induces aggregation and fusion in PE/PG vesicles with different propensities in the order: [d-Lys]4GS14 > GS14 > GS12 > GS10. GS10 and GS14 are apparently located in the deeper levels of the membrane interfaces and closer to the hydrophobic core of the bilayers, whereas GS12 and [d-Lys]4GS14 reside closer to the outer boundary of the interface. Because of differing modes of interaction of the cyclic cationic peptides with lipid bilayers, the mechanism of their biological activity (and its relation to peptide–lipid interaction) proved to be versatile and complex, and dependent on the biophysical properties of both the peptides and membranes.

The interactions of the antimicrobial peptides aurein 1.2, citropin 1.1 and maculatin 1.1 with dimyristoylphosphatidylcholine (DMPC), dimyristoylphosphatidylglycerol (DMPG) and dimyristoylphosphatidylethanolamine (DMPE) were studied by differential scanning calorimetry (DSC) and Fourier-transform infrared (FTIR) spectroscopy. The effects of these peptides on the thermotropic phase behavior of DMPC and DMPG are qualitatively similar and manifested by the suppression of the pretransition, and by peptide concentration-dependent decreases in the temperature, cooperativity and enthalpy of the gel/liquid-crystalline phase transition. However, at all peptide concentrations, anionic DMPG bilayers are more strongly perturbed than zwitterionic DMPC bilayers, consistent with membrane surface charge being an important aspect of the interactions of these peptides with phospholipids. However, at all peptide concentrations, the perturbation of the thermotropic phase behavior of zwitterionic DMPE bilayers is weak and discernable only when samples are exposed to high temperatures. FTIR spectroscopy indicates that these peptides are unstructured in aqueous solution and that they fold into alpha-helices when incorporated into lipid membranes. All three peptides undergo rapid and extensive H-D exchange when incorporated into D(2)O-hydrated phospholipid bilayers, suggesting that they are located in solvent-accessible environments, most probably in the polar/apolar interfacial regions of phospholipid bilayers. The perturbation of model lipid membranes by these peptides decreases in magnitude in the order maculatin 1.1>aurein 1.2>citropin 1.1, whereas the capacity to inhibit Acholeplasma laidlawii B growth decreases in the order maculatin 1.1>aurein 1.2 congruent with citropin 1.1. The higher efficacy of maculatin 1.1 in disrupting model and biological membranes can be rationalized by its larger size and higher net charge. However, despite its smaller size and lower net charge, aurein 1.2 is more disruptive of model lipid membranes than citropin 1.1 and exhibits comparable antimicrobial activity, probably because aurein 1.2 has a higher propensity for partitioning into phospholipid membranes.

We applied precise densimetry and ultrasound velocimetry methods to study the interaction of a synthetic alpha-helical transmembrane peptide, acetyl-K(2)-L(24)-K(2)-amide (L(24)), with model bilayer lipid membranes. The large unilamellar vesicles (LUVs) utilized were composed of a homologous series of n-saturated diacylphosphatidylcholines (PCs). PCs whose hydrocarbon chains contained from 13 to 16 carbon atoms, thus producing phospholipid bilayers of different thicknesses and gel to liquid-crystalline phase transition temperatures. This allowed us to analyze how the difference between the hydrophobic length of the peptide and the hydrophobic thickness of the lipid bilayer influences the thermodynamical and mechanical properties of the membranes. We showed that the incorporation of L(24) decreases the temperature and cooperativity of the main phase transition of all LUVs studied. The presence of L(24) in the bilayer also caused an increase of the specific volume and of the volume compressibility in the gel state bilayers. In the liquid crystalline state, the peptide decreases the specific volume at relatively higher peptide concentration (mole ratio L(24):PC=1:50). The overall volume compressibility of the peptide-containing lipid bilayers in the liquid-crystalline state was in general higher in comparison with pure membranes. There was, however, a tendency for the volume compressibility of these lipid bilayers to decrease with higher peptide content in comparison with bilayers of lower peptide concentration. For one lipid composition, we also compared the thermodynamical and mechanical properties of LUVs and large multilamellar vesicles (MLVs) with and without L(24). As expected, a higher cooperativity of the changes of the thermodynamical and mechanical parameters took place for MLVs in comparison with LUVs. These results are in agreement with previously reported DSC and (2)H NMR spectroscopy study of the interaction of the L(24) and structurally related peptides with phosphatidylcholine bilayers. An apparent discrepancy between (2)H NMR spectroscopy and compressibility data in the liquid crystalline state may be connected with the complex and anisotropic nature of macroscopic mechanical properties of the membranes. The observed changes in membrane mechanical properties induced by the presence of L(24) suggest that around each peptide a distorted region exists that involves at least 2 layers of lipid molecules.

The effects of the hydrophobicity and the distribution of hydrophobic residues on the surfaces of some designed alpha-helical transmembrane peptides (acetyl-K2-L(m)-A(n)-K2-amide, where m + n = 24) on their solution behavior and interactions with phospholipids were examined. We find that although these peptides exhibit strong alpha-helix forming propensities in water, membrane-mimetic media, and lipid model membranes, the stability of the helices decreases as the Leu content decreases. Also, their binding to reversed phase high-performance liquid chromatography columns is largely determined by their hydrophobicity and generally decreases with decreases in the Leu/Ala ratio. However, the retention of these peptides by such columns is also affected by the distribution of hydrophobic residues on their helical surfaces, being further enhanced when peptide helical hydrophobic moments are increased by clustering hydrophobic residues on one side of the helix. This clustering of hydrophobic residues also increases peptide propensity for self-aggregation in aqueous media and enhances partitioning of the peptide into lipid bilayer membranes. We also find that the peptides LA3LA2 [acetyl-K2-(LAAALAA)3LAA-K2-amide] and particularly LA6 [acetyl-K2-(LAAAAAA)3LAA-K2-amide] associate less strongly with and perturb the thermotropic phase behavior of phosphatidylcholine bilayers much less than peptides with higher L/A ratios. These results are consistent with free energies calculated for the partitioning of these peptides between water and phospholipid bilayers, which suggest that LA3LA2 has an equal tendency to partition into water and into the hydrophobic core of phospholipid model membranes, whereas LA6 should strongly prefer the aqueous phase. We conclude that for alpha-helical peptides of this type, Leu/Ala ratios of greater than 7/17 are required for stable transmembrane associations with phospholipid bilayers.

We have carried out a comparative differential scanning calorimetric (DSC) study of the effects of cholesterol (C) and the eight most physiologically relevant oxysterols on the thermotropic phase behavior of dipalmitoylphosphatidylcholine (DPPC) bilayer membranes. The structures of these oxysterols differ from that of C by the presence of additional hydroxyl, keto or epoxy groups on the steroid ring system or by the presence of a hydroxyl group in the alkyl side chain. In general, the progressive incorporation of these oxysterols reduces the temperature, cooperativity and enthalpy of the pretransition of DPPC to a greater extent than C, indicating that their presence thermally destabilizes and disorders the gel states of DPPC bilayers to a greater extent than C. Similarly, the incorporation of these oxysterols either increases the temperature of the broad component of the main phase transition to a smaller extent than C or actually decreases it. Again, this indicates that the presence of these compounds is less effective at thermally stabilizing and ordering the sterol-rich domains of DPPC bilayers than is C itself. Moreover, the incorporation of these oxysterols decrease the cooperativity and enthalpy of the main phase transition of DPPC to a smaller extent than C, indicating that they are somewhat less miscible in fluid DPPC bilayers than is C. Particularly notable in this regard is 25-hydroxycholesterol, which exhibits a markedly reduced miscibility in both gel and fluid DPPC bilayers compared to C itself. In general, the effectiveness of these oxysterols in stabilizing and ordering DPPC bilayers decreases as their rate of interbilayer exchange and the polarity of the oxysterol increases. We close by providing a tentative molecular explanation for the results of our DSC studies and of those of previous biophysical studies of the effects of various oxysterol on lipid bilayer model membranes.

We performed comparative DSC and FTIR spectroscopic measurements of the effects of β-sitosterol (Sito) and stigmasterol (Stig) on the thermotropic phase behavior and organization of DPPC bilayers. Sito and Stig are the major sterols in the biological membranes of higher plants, whereas cholesterol (Chol) is the major sterol in mammalian membranes. Sito differs in structure from Chol in having an ethyl group at C24 of the alkyl side-chain, and Stig in having both the C24 ethyl group and trans-double bond at C22. Our DSC studies indicate that the progressive incorporation of Sito and Stig decrease the temperature and cooperativity of the pretransition of DPPC to a slightly lesser and greater extent than Chol, respectively, but the pretransition persists to 10 mol % sterol concentration in all cases. All three sterols produce essentially identical effects on the thermodynamic parameters of the sharp component of the DPPC main phase transition. However, the ability to increase the temperature and decrease the cooperativity and enthalpy of the broad component decreases in the order Chol > Sito > Stig. Nevertheless, at higher Sito/Stig concentrations, there is no evidence of sterol crystallites. Our FTIR spectroscopic studies demonstrate that Sito and especially Stig incorporation produces a smaller ordering of the hydrocarbon chains of fluid DPPC bilayers than does Chol. In general, the presence of a C24 ethyl group in the alkyl side-chain reduces the characteristic effects of Chol on the thermotropic phase behavior and organization of DPPC bilayer membranes, and a trans-double bond at C22 magnifies this effect.

Using differential scanning calorimetry (DSC), X-ray diffraction (XRD) and Fourier transform infrared spectroscopy (FTIR), we determined some thermodynamic and structural parameters for a series of amino acid-linked dialkyl lipids containing a glutamic acid-succinate headgroup and di-alkyl chains: C12, C14, C16 and C18 in CHES buffer, pH 10. Upon heating, DSC shows that the C12, C14 and annealed C16 lipids undergo a single transition which XRD shows is from a lamellar, chain ordered subgel phase to a fluid phase. This single transition splits into two transitions for C18, and FTIR shows that the upper main transition is predominantly the melting of the hydrocarbon chains whereas the lower transition involves changes in the headgroup ordering as well as changes in the lateral packing of the chains. For short incubation times at low temperature, the C16 lipid appears to behave like the C18 lipid, but appropriate annealing at low temperatures indicates that its true equilibrium behavior is like the shorter chain lipids. XRD shows that the C12 lipid readily converts into a highly ordered subgel phase upon cooling and suggests a model with untilted, interdigitated chains and an area of 77.2A(2)/4 chains, with a distorted orthorhombic unit subcell, a=9.0A, b=4.3A and beta=92.7 degrees . As the chain length n increases, subgel formation is slowed, but untilted, interdigitated chains prevail.

The binding of water-soluble peptides or proteins to lipid membranes is an important issue in many biological processes. There are, for instance, several types of amphipathic peptides, including gramicidin S (GS),1 that bind to the bacterial membrane and act as antibiotics (1, 2). These antimicrobial peptides are widely distributed in animals and plants where they act as host defense peptides. Most of these antimicrobial peptides are cationic, thus permitting electrostatic interactions with the bacterial cytoplasmic membrane, which usually contains substantial amounts of negatively charged phospholipids in the outer leaflet of the lipid bilayer, the major target of many of these peptides. GS, a cyclic decameric cationic antimicrobial peptide first isolated from the Gram-positive bacteria Bacillus brevis, is one of a series of antimicrobial peptides produced by this particular organism (3). The GS molecule, of primary structure (cyclo[VOLdFPVOLdFP]), is composed of a double-stranded antiparallel β-sheet connected by a pair of II′ β-turns (3). GS is a powerful antibiotic against a broad range of Gram-negative and Gram-positive bacteria as well as several pathogenic fungi, but it is also highly hemolytic (4–7). As a result, the use of this antimicrobial peptide is restricted to topical applications. However, a dissociation of the antimicrobial and hemolytic activities of GS is possible by simultaneously varying both GS ring size and the enantiomeric configuration of certain amino acid residues (5, 6). This opens the possibility of the use of structural analogues derived from GS as an injectable or oral antibiotics (4, 8). GS14dK4 is a GS analogue that has been identified as a promising candidate because of its comparable antimicrobial activity to that of GS and its substantially lower hemolytic activity, which is about 15–20-fold less than that of GS (6). This analogue consists of two antiparallel β-sheets with aligned sequences of alternating hydrophobic and cationic residues, Val-Lys-Leu-dLys-Val and Val-Lys-Val-Lys-Leu, connected at each end of the ring by the dipeptide sequence dTyr-Pro. Thus, as the structure indicates, it is a diastereo-meric analogue of GS14 in which the L-lysine at position 4 is substituted by its diastereomer, D-lysine. In the parent compound GS14, all four lysine units project to the one hydrophilic face of the ring, while in GS14dK4, the Lys-4 projects partially to the hydrophobic face of the molecule (8). This makes GS14dK4 relatively more water soluble, less amphiphilic, and less susceptible to dimerization than GS14 itself (8). The interaction between GS14dK4 and lipid bilayer model membranes has been studied using FTIR spectroscopy in an effort to understand the basis of its capacity to differentiate between bacterial and mammalian cell membranes (9). The FTIR data show that GS14dK4, like GS, interacts more strongly with anionic lipid bilayers than with zwitterionic, uncharged, or cationic lipid model membranes. The interaction of GS14dK4 with such model membranes is, however, generally weaker than with GS and depends more strongly on the charge of the bilayers. Moreover, GS14dK4, like GS, interacts more strongly with liquid crystalline lipid bilayers than with gel-state lipid bilayers. In addition, GS14dK4 is essentially completely excluded from cholesterol-containing zwitterionic lipid membranes, whereas cholesterol only attenuates the interactions of GS with such lipid bilayers (10). GS14dK4, despite its apparently weaker interactions with phospholipid membranes, is more effective in permeabilizing cholesterol-free lipid membranes than GS (11). These observations suggest that GS14dK4 retains the ability to disrupt bacterial membranes as effectively as GS because of its innately greater ability to disrupt lipid bilayers and its retained selectivity for binding to anionic lipids, but exhibits much weaker hemolytic activity because of its exclusion from cholesterol-containing zwitterionic lipid membranes. Although these semiquantitative studies of the interaction between GS14dK4 and the various model lipid membranes were valuable, there is a clear need for a quantitative determination of the degree of binding of the GS14dK4 to various types of lipid bilayers and for a comprehensive thermodynamic description of the binding process. A quantitative determination of peptide binding to various types of lipid membranes is particularly important as it would allow us determine the amount of the peptide actually present in the membrane as opposed to the amount of added peptide in the aqueous solution. Similarly, a complete thermodynamic description of the binding process would provide key information on the energetics and mechanism of peptide binding to lipid bilayers. We have therefore utilized ITC, a highly sensitive tool for determining the binding of peptide to lipid membranes (12, 13), to examine the binding of GS14dK4 to large unilamellar vesicles (LUVs) composed of various zwitterionic and anionic phospholipids, with or without cholesterol. The degree of binding and the thermodynamic parameters of binding obtained for these different lipid compositions were compared and analyzed to understand the nature of the interactions involved in the binding process.

The effects of the transmembrane alpha-helical peptide Ac-K(2)(LA)(12)K(2)-amide ((LA)(12)) on the phase transition and dynamics of saturated dimyristoylphosphatidylcholine (DMPC) membranes were investigated at different pH using conventional and saturation-recovery EPR observations of phosphatidylcholine spin labels. At a peptide-to-DMPC ratio of 1/10, the main phase-transition temperature of the DMPC bilayer is decreased by 4.0 degrees C when measured at pH 7.0, by 1.6 degrees C when measured at pH 9.5, and not affected when measured at pH 11.5. This reversible pH effect is due to the subsequent neutralization of the positive charges of lysine side chains at both ends of (LA)(12). Apparent pK(a)s of the lysine side chain amino groups of (LA)(12) in DMPC bilayer are 8.6 and approximately 10.9, as compared with the pK(a) value of 10.5 for these groups when lysine is dissolved in water. Saturation-recovery curves as a function of oxygen concentration using phosphatidylcholine spin labels in DMPC bilayer containing (LA)(12) are always mono-exponential when measured at pH 7.0 and 9.5. This observation is consistent with the hypothesis that the lipid exchange rates among the bulk, boundary, and (LA)(12)-rich regions are faster than 0.5 micros, the electron spin-lattice relaxation time in the presence of molecular oxygen, suggesting that stable oligomers of (LA)(12) do not form. Neutralization of one lysine side chain positive charge on each end of the peptide significantly decreases the ordering effect of (LA)(12) on the lipid hydrocarbon chains, while its effect on the reorientational motion of terminal groups of lipid hydrocarbon chains is rather moderate. It does not affect the local diffusion-solubility product of oxygen measured in the DMPC-(LA)(12) membrane interior.

Structure-activity relationships were examined in seven gramicidin S analogs in which the ring-expanded analog GS14 [cyclo-(VKLKVdYPLKVKLdYP)] is modified by enantiomeric inversions of its lysine residues. The conformation, amphiphilicity, and self-association propensity of these peptides were investigated by circular dichroism spectroscopy and reversed phase high performance liquid chromatography. (31)P nuclear magnetic resonance spectroscopic and dye leakage experiments were performed to evaluate the capacity of these peptides to induce inverse nonlamellar phases in, and to permeabilize phospholipid bilayers; their growth inhibitory activity against the cell wall-less mollicute Acholeplasma laidlawii B was also examined. The amount and stability of beta-sheet structure, effective hydrophobicity, propensity for self-association in water, ability to disrupt the organization of phospholipid bilayers, and ability to inhibit A. laidlawii B growth are strongly correlated with the facial amphiphilicity of these GS14 analogs. Also, the magnitude of the parameters segregate these peptides into three groups, consisting of GS14, the four single inversion analogs, and the two multiple inversion analogs. The capacity of these peptides to differentiate between bacterial and animal cell membranes exhibits a biphasic relationship with peptide amphiphilicity, suggesting that there may only be a narrow range of peptide amphiphilicity within which it is possible to achieve the dual therapeutic requirements of high antibiotic effectiveness and low hemolytic activity. These results were rationalized by considering how the physiochemical properties of these GS14 analogs are likely to be reflected in their partitioning into lipid bilayer membranes.

We studied the interaction of the alpha-helical peptide acetyl-Lys(2)-Leu(24)-Lys(2)-amide (L(24)) with tethered bilayer lipid membranes (tBLM) and lipid monolayers formed at an air-water interface. The interaction of L(24) with tBLM resulted in adsorption of the peptide to the surface of the bilayer, characterized by a binding constant K(c)=2.4+/-0.6 microM(-1). The peptide L(24) an induced decrease of the elasticity modulus of the tBLM in a direction perpendicular to the membrane surface, E(radial). The decrease of E(radial) with increasing peptide concentration can be connected with a disordering effect of the peptide to the tBLM structure. The pure peptide formed a stable monolayer at the air/water interface. The pressure-area isotherms were characterized by a transition of the peptide monolayer, which probably corresponds of the partial intercalation of the alpha-helixes at higher surface pressure. Interaction of the peptide molecules with lipid monolayers resulted in an increase of the mean molecular area of phospholipids both in the gel and liquid crystalline states. With increasing peptide concentration, the temperature of the phase transition of the monolayer shifted toward lower temperatures. The analysis showed that the peptide-lipid monolayer is not an ideally miscible system and that the peptide molecules form aggregates in the monolayer.

Recent advances in the area of glycobiology have been paralleled by progress in our understanding of the physical properties of glycoglycerolipids (GGLs). These advances have been accelerated by interest in the new found roles of these simple glycolipids in nature, by advances in synthetic procedures, and by an interest in the technological application of a group of amphiphiles with unique physical and chemical properties. Here, we consider the phase properties of some GGL/water systems containing either a single hexopyranoside or pentopyranoside headgroup. Recent calorimetric and X-ray diffraction measurements of some GGL diastereomers suggest that both headgroup and interfacial hydration play a major role in determining both lyotropism and mesomorphic phase properties as the chemical structure of the lipid headgroup, interface and hydrocarbon chains are systematically altered. For GGLs of a given chain length, interactions between the headgroup/interface and water determine whether or not a highly ordered, lamellar crystalline phase is formed, the number of such phases and their rate of formation and, in some cases, the nature of the molecular packing of those phases. In the liquid crystalline phases, the hydrocarbon chains determine the area per molecule in the lamellar liquid crystalline phase, but it is the cross-sectional area of the hydrated headgroup and the penetration of water into the interface which determines the nature of the non-lamellar phases, probably through small changes in interfacial geometry as the lateral stresses in the headgroup region increase.

The existence of relatively large and long-lived detergent-insoluble, sphingolipid- and cholesterol-enriched, liquid-ordered lipid raft domains in the plasma membranes of eukaryotic cells has become widely accepted. However, we believe that the evidence for their existence is not compelling despite extensive work on both lipid bilayer model and biological membranes. We review here the results of recent studies, which in our view call into question the existence of lipid rafts in membranes, at least in the form commonly depicted.

High-sensitivity differential scanning calorimetry (DSC) and Fourier transform infrared (FTIR) spectroscopy were used to study the interaction of an alpha-helical transmembrane peptide, acetyl-Lys2-Leu24-Lys2-amide (L24), and odd-chain members of the homologous series of n-saturated diacylphosphatidylcholines. An analogue of L24, in which the lysine residues were all replaced by 2,3-diaminopropionic acid, and another, in which a leucine residue at each end of the polyLeu sequence was replaced by a tryptophan, were also studied. At low peptide concentrations, the DSC thermograms exhibited by these lipid/peptide mixtures are resolvable into two components. One of these components is fairly narrow, highly cooperative, and exhibits properties which are similar to but not identical with those of the pure lipid. In addition, the transition temperature and cooperativity of this component, and its fractional contribution to the total enthalpy change, decrease with an increase in peptide concentration, more or less independently of phospholipid acyl chain length. The other component is very broad and predominates at high peptide concentrations. These two components have been assigned to the chain-melting phase transitions of populations of peptide-poor and peptide-enriched lipid domains, respectively. Moreover, when the mean hydrophobic thickness of the PC bilayer is less than the peptide hydrophobic length, the peptide-associated lipid melts at higher temperatures than does the bulk lipid and vice versa. In addition, the chain-melting enthalpy of the broad endotherm does not decrease to zero even at high peptide concentrations, suggesting that these peptides reduce somewhat but do not abolish the cooperative gel/liquid-crystalline phase transition of the lipids with which it is in contact. Our DSC results indicate that the width of the broad phase transition observed at high peptide concentration is inversely but discontinuously related to hydrocarbon chain length. Our FTIR spectroscopic data indicate that these peptides form a very stable alpha-helix under all of our experimental conditions but that small distortions of their alpha-helical conformation are induced in response to mismatch between peptide hydrophobic length and gel-state bilayer hydrophobic thickness. We also present evidence that these distortions are localized to the N- and C-terminal regions of these peptides. Interestingly, replacing the terminal Lys residues of L24 by 2,3-diaminopropionic acid residues actually attenuates the hydrophobic mismatch effects of the peptide on the thermotropic phase behavior of the host PC bilayer, in contrast to the predictions of the snorkel hypothesis. We rationalize this attenuated hydrophobic mismatch effect by postulating that the 2,3-diaminopropionic acid residues are too short to engage in significant electrostatic and hydrogen-bonding interactions with the polar headgroups of the host phospholipid bilayer, even in the absence of any hydrophobic mismatch between incorporated peptide and the bilayer. Similarly, the reduced hydrophobic mismatch effect also observed when the two terminal Leu residues of L24 are replaced by Trp residues is rationalized by considering the lower energetic cost of exposing the Trp as opposed to the Leu residues to the aqueous phase in thin PC bilayers and the higher cost of inserting the Trp as opposed to the Leu residues into the hydrophobic cores of thick PC bilayers.

IR reflection−absorption spectroscopy (IRRAS) is used to determine the orientation of carbonyl groups in behenic acid methyl ester (BME) and in sn2-13C 1,2 distearoylphosphatidylcholine (sn2-13C-DSPC) in aqueous monolayer films. The CO stretching contour of BME consists of three overlapped peaks arising from unhydrated, monohydrated, and doubly hydrated forms at 1737, 1721, and 1702 cm-1, respectively. Dichroic ratios constructed from the p- and s-polarized IRRAS intensities of the resolved components of the contour were simulated with the optical theory of V. L. Kuzmin.1,2 On the basis of valence bond and molecular modeling considerations, the carbonyl group is essentially perpendicular to the chain axes. The transition moment is determined by IRRAS to indeed lie along the CO bond for the unhydrated groups (thus providing good support for the theory) but changes direction for hydrated groups. A satisfactory fit between simulation and experiment could not be obtained by assuming a uniaxial distribution of...

Phospholipids, sphingolipids, and sterols are the major lipid components of the plasma membranes of eukaryotic cells. Because these three lipid classes occur naturally as enantiomerically pure compounds, enantiospecific lipid-lipid and lipid-sterol interactions could in principle occur in the lipid bilayers of eukaryotic plasma membranes. Although previous biophysical studies of phospholipid and phospholipid-sterol model membrane systems have consistently failed to observe such enantiomerically selective interactions, a recent monolayer study of the interactions of natural and enantiomeric cholesterol with egg sphingomyelin has apparently revealed the existence of enantiospecific sterol-sphingolipid interactions. To determine whether enantiospecific sterol-sphingolipid interactions also occur in more biologically relevant lipid-bilayer systems, differential scanning calorimetric, x-ray diffraction, and neutral buoyant-density measurements were utilized to study the effects of natural and enantiomeric cholesterol on the thermotropic phase behavior and structure of egg sphingomyelin bilayers. The calorimetry experiments show that the natural and enantiomeric cholesterol have essentially identical effects on the temperature, enthalpy, and cooperativity of the gel/liquid-crystalline phase transition of egg sphingomyelin bilayers within the limits of experimental error. As well, the x-ray diffraction and neutral buoyancy experiments indicate that bilayers formed from mixtures of natural or enantiomeric cholesterol and egg sphingomyelin have, within experimental uncertainty, the same structure and mass density. We thus conclude that significant enantioselective cholesterol-sphingolipid interactions do not occur in this lipid-bilayer model membrane system.

Cyclo[VKLdKVdYPLKVKLdYP] (GS14dK(4)), a synthetic tetradecameric ring-size analogue of the naturally occurring antimicrobial peptide gramicidin S (GS), retains the strong antimicrobial activity of GS but is 15-20 times less hemolytic. To characterize its interaction with lipid membranes and to understand the molecular basis of its capacity to lyse bacterial cells, in preference to erythrocytes, we have investigated the interactions of GS14dK(4) with detergent micelles and with lipid bilayer model membranes by Fourier transform infrared spectroscopy and compared our results with those of a similar study of GS [Lewis, R. N. A. H., et al. (1999) Biochemistry 38, 15193-15203]. In both aqueous and organic solvent solutions, GS14dK(4) adopts a beta-sheet conformation that is somewhat distorted and more sensitive to the polarity of its environment than GS. Like GS, GS14dK(4) is completely or partially excluded from gel-state lipid bilayers but interacts strongly with liquid-crystalline lipid bilayers and detergent micelle, and interacts more strongly with more fluid liquid-crystalline lipid systems. However, its interactions are more strongly influenced by membrane lipid order and fluidity, and unlike GS, it is essentially excluded from cholesterol-containing phospholipid bilayers. Also, GS14dK(4) is excluded from cationic lipid bilayers, but partitions more strongly and/or penetrates more deeply into anionic lipid bilayers than into those composed of either zwitterionic or nonionic lipids. Anionic lipids also facilitate GS14dK(4) interactions with multicomponent lipid bilayers which are predominantly zwitterionic or nonionic. Although GS14dK(4) generally penetrates and/or partitions into zwitterionic or uncharged lipid bilayers less strongly than does GS, its greater size and altered distribution of positive charges make it intrinsically more perturbing with regard to membrane organization once associated with lipid bilayers. This fact, combined with its relatively strong interactions with anionic phospholipids, may explain why GS14dK(4) retains relatively high antimicrobial activity. However, its low hemolytic activity is probably largely attributable to its low propensity to penetrate and/or partition into cholesterol-containing zwitterionic lipid membranes.

The thermal unfolding of xylanase A from Streptomyces lividans, and of its isolated substrate binding and catalytic domains, was stud- ied by differential scanning calorimetry and Fou- rier transform infrared and circular dichroism spec- troscopy. Our calorimetric studies show that the thermal denaturation of the intact enzyme is a complex process consisting of two endothermic events centered near 57 and 64°C and an exothermic event centered near 75°C, all of which overlap slightly on the temperature scale. A comparison of the data obtained with the intact enzyme and iso- lated substrate binding and catalytic domains indi- cate that the lower- and higher-temperature endo- thermic events are attributable to the thermal unfolding of the xylan binding and catalytic do- mains, respectively, whereas the higher-tempera- ture exothermic event arises from the aggregation and precipitation of the denatured catalytic do- main. Moreover, the thermal unfolding of the two domains of the native enzyme are thermodynami- cally independent and differentially sensitive to pH. The unfolding of the substrate binding domain is a reversible two-state process and, under appropriate conditions, the refolding of this domain to its native conformation can occur. In contrast, the unfolding of the catalytic domain is a more complex process in which two subdomains unfold independently over a similar temperature range. Also, the unfolding of the catalytic domain leads to aggregation and pre- cipitation, which effectively precludes the refolding of the protein to its native conformation. These observations are compatible with the results of our spectroscopic studies, which show that the catalytic and substrate binding domains of the enzyme are structurally dissimilar and that their native confor- mations are unaffected by their association in the intact enzyme. Thus, the calorimetric and spectro- scopic data demonstrate that the S. lividans xyla- nase A consists of structurally dissimilar catalytic and substrate binding domains that, although co- valently linked, undergo essentially independent thermal denaturation. These observations provide valuable new insights into the structure and ther- mal stability of this enzyme and should assist our efforts at engineering xylanases that are more ther- mally robust and otherwise better suited for indus- trial applications. Proteins 2003;50:341-354.

We have examined the effects of three ring-size analogs of the cyclic beta-sheet antimicrobial peptide gramicidin S (GS) on the thermotropic phase behavior and permeability of phospholipid model membranes and on the growth of the cell wall-less Gram-positive bacteria Acholeplasma laidlawii B. These three analogs have ring sizes of 10 (GS10), 12 (GS12) or 14 (GS14) amino acids, respectively. Our high-sensitivity differential scanning calorimetric studies indicate that all three of these GS analogs perturb the gel/liquid-crystalline phase transition of zwitterionic phosphatidylcholine (PtdCho) vesicles to a greater extent than of zwitterionic phosphatidylethanolamine (PtdEtn) or of anionic phosphatidylglycerol (PtdGro) vesicles, in contrast to GS itself, which interacts more strongly with PtdGro than with PtdCho and PtdEtn bilayers. However, the relative potency of the perturbation of phospholipid phase behavior varies markedly between the three peptides, generally decreasing in the order GS14 > GS10 > GS12. Similarly, these three GS ring-size analogs also differ considerably in their ability to cause fluorescence dye leakage from phospholipid vesicles, with the potency of permeabilization also generally decreasing in the order GS14 > GS10 > GS12. Finally, these GS ring-size analogs also differentially inhibit the growth of A. laidlawii with growth inhibition also decreasing in the order GS14 > GS10 > GS12. These results indicate that the relative potencies of GS and its ring-size analogs in perturbing the organization and increasing the permeability of phospholipid bilayer model membranes, and of inhibiting the growth of A. laidlawii B cells, are at least qualitatively correlated, and provide further support for the hypothesis that the primary target of these antimicrobial peptides is the lipid bilayer of the bacterial membrane. The very high antimicrobial activity of GS14 against the cell wall-less bacteria A. laidlawii as compared to various conventional bacteria confirms our earlier suggestion that the avid binding of this peptide to the bacterial cell wall is primarily responsible for its reduced antimicrobial activity against such organisms. The relative magnitude of the effects of GS itself, and of the three ring-size GS analogs, on phospholipid bilayer organization and cell growth correlate relatively well with the effective hydrophobicities and amphiphilicities of these peptides but less well with their relative charge density, intrinsic hydrophobicities or conformational flexibilities. Nevertheless, all of these parameters, as well as others, may influence the antimicrobial potency and hemolytic activity of GS analogs.

The large intrinsic membrane dipole potential, phi(d), is important for protein insertion and functioning as well as for ion transport across natural and model membranes. However, the origin of phi(d) is controversial. From experiments carried out with lipid monolayers, a significant dependence on the fatty acid chain length is suggested, whereas in experiments with lipid bilayers, the contribution of additional -CH(2)-groups seems negligibly small compared with that of the phospholipid carbonyl groups and lipid-bound water molecules. To compare the impact of the -CH(2)-groups of dipalmitoylphosphatidylcholine (DPPC) near and far from the glycerol backbone, we have varied the structure of DPPC by incorporation of sulfur atoms in place of methylene groups in different positions of the fatty acid chain. The phi(d) of symmetric lipid bilayers containing one heteroatom was obtained from the charge relaxation of oppositely charged hydrophobic ions. We have found that the substitution for a S-atom of a -CH(2)-group decreases phi(d). The effect (deltaphi(d) = -22.6 mV) is most pronounced for S-atoms near the lipid head group while a S-atom substitution in the C(13)- or C(14)-position of the hydrocarbon chain does not effect the bilayer dipole potential. Most probably deltaphi(d) does not originate from an altered dipole potential of the acyl chain containing an heteroatom but is mediated by the disruption of chain packing, leading to a decreased density of lipid dipoles in the membrane.

Acholeplasma laidlawii B cells made fatty acid auxotrophic by growth in the presence of the biotin-binding agent avidin grow increasingly poorly at 37 degrees C when supplemented with single exogenous linear saturated fatty acids of decreasing hydrocarbon chain length. Interestingly, this progressive decrease in growth yields with decreasing hydrocarbon chain length is not observed when cells are cultured in the presence of other classes of exogenous fatty acids. Moreover, normal growth is observed is other types of fatty acids with equivalent or shorter hydrocarbon chain lengths, indicating that poor growth in the presence of short-chain linear saturated fatty acids cannot be due to a decrease in membrane lipid bilayer thickness per se. To understand the molecular basis of such growth inhibition, we determined the growth yields, membrane lipid fatty acid and polar headgroups compositions, and phase state and fluidity of the membrane lipids in cells progressively biosynthetically enriched in tridecanoic acid (13:0) or dodecanoic acid (12:0). The growth of fatty acid auxotrophic A. laidlawii B cells grown in the presence of binary combinations of an exogenous fatty acid which supports normal growth on its own and 13:0 or 12:0 revealed that growth inhibition is not observed until 13:0 and 12:0 biosynthetic incorporation levels reach about 90 and 60 mol %, respectively, after which growth is markedly inhibited. Differential scanning calorimetric analyses of membranes from cells maximally enriched in 13:0 indicate that the lipid gel/liquid-crystalline phase transition temperature is unexpectedly high but that at the growth temperature of 37 degrees C, the membrane lipid bilayer is almost exclusively in the liquid-crystalline state but is certainly not excessively fluid. However, high levels of 13:0 incorporation produce a greatly elevated level of the high melting, reversed nonlamellar phase-preferring lipid component monoglucosyl diacylglycerol, and greatly reduced levels of all other membrane lipid components. This marked elevation of monoglucosyl diacylglycerol levels can be rationalized as a regulatory response which maintains the lamellar/nonlamellar phase-forming propensity of the total membrane lipid mixture relatively constant in the face of the biosynthetic incorporation of increasing quantities of short-chain saturated fatty acids, which favor the lamellar phase. However, this lipid biosynthetic response produces a marked decline in the levels of anionic phospholipid and phosphoglycolipid which are probably required to maintain the minimal negative surface charge density of the lipid bilayer, which we suggest is responsible for the observed growth inhibition. This work shows that the lipid biosynthetic regulatory mechanisms present in this organism may sometimes operate at cross purposes such that it is not possible to simultaneously optimize all of the biologically relevant physical properties of the membrane lipid bilayer.

The synthetic peptide acetyl-K(2)-G-L(24)-K(2)-A-amide (P(24)) and its analogs have been successfully utilized as models of the hydrophobic transmembrane alpha-helical segments of integral membrane proteins. The central polyleucine region of these peptides was designed to form a maximally stable, very hydrophobic alpha-helix which will partition strongly into the hydrophobic environment of the lipid bilayer core, while the dilysine caps were designed to anchor the ends of these peptides to the polar surface of the lipid bilayer and to inhibit the lateral aggregation of these peptides. Moreover, the normally positively charged N-terminus and the negatively charged C-terminus have both been blocked in order to provide a symmetrical tetracationic peptide, which will more faithfully mimic the transbilayer region of natural membrane proteins and preclude favorable electrostatic interactions. In fact, P(24) adopts a very stable alpha-helical conformation and transbilayer orientation in lipid model membranes. The results of our recent studies of the interaction of this family of alpha-helical transmembrane peptides with phospholipid bilayers are summarized here.

We present the results of a comparative differential calorimetric and Fourier transform infrared spectroscopic study of the effect of cholesterol and five analogs on the thermotropic phase behavior and organization of dipalmitoylphosphatidylcholine bilayer membranes. These sterols/steroids differ in both the nature and stereochemistry of the polar head group at C3 (β-OH, α-OH or C=O) and in the presence or absence of a double bond in ring B. In both the Δ(5) and saturated sterols/steroid series, the concentration of these compounds required to abolish the DPPC pretransition, inversely related to their relative ability to disorder gel state DPPC bilayers, decreases in the order β-OHα-OHC=O. However, in the saturated series, these concentrations are much more similar, regardless of polar head group chemical structure. Similarly, the residual enthalpy of the DPPC main phase transition at 50 mol% sterol/steroid, inversely related to the miscibility of these compounds in fluid DPPC bilayers, also increases in the order β-OHα-OHC=O, but this effect is again attenuated in the saturated series. Moreover, replacement of the double bond at C5 with a saturated linkage also reduces sterol/steroid solubility in all cases. Interestingly, the C5 double bond has no effect on DPPC hydrocarbon chain ordering in the βOH sterol pair, considerably increases ordering in the αOH pair, and considerably reduces ordering in the C=O pair. Moreover, the ability of these compounds to order the DPPC hydrocarbon chains decreases in the order β-OHα-OHC=O in the Δ(5) series of compounds, but in the order β-OHC=Oα-OH in the saturated series. Our results indicate that the effects of the presence or absence of a double bond at C5 of ring B on the thermotropic phase behavior and organization of DPPC bilayers are influenced by the nature and stereochemistry of the polar group present at C3 and vice versa. Nevertheless, the characteristic effects of sterols/steroids on fluid lipid bilayers are optimal when an OH group rather than C=O group is present at C3, and when this OH group is in the equatorial (β) orientation. Moreover, the presence of a single double bond specifically at C5 is required to maximize sterol solubility in fluid DPPC bilayers, which is probably its primary function in natural sterols.

We present a comparative differential scanning calorimetric study of the effects of the animal sterol cholesterol (Chol) and the plant sterols campesterol (Camp) and brassicasterol (Bras) on the thermotropic phase behavior of dipalmitoylphosphatidylcholine (DPPC) bilayers. Camp and Bras differ from Chol in having a C24 methyl group and, additionally for Bras, a C22 trans-double bond. Camp and especially Bras decrease the temperature, cooperativity and enthalpy of the DPPC pretransition more than Chol, although these effects are attenuated at higher sterol levels. This indicates that they destabilize gel-state DPPC bilayers to a greater extent, but are less soluble, than Chol. Not surprisingly, all three sterols have similar effects on the sterol-poor sharp component of the DPPC main phase transition. However, Camp and especially Bras less effectively increase the temperature and decrease the cooperativity and enthalpy of the broad component of the main transition than Chol. This indicates that at higher sterol concentrations, Camp and Bras are less miscible and less effective than Chol at ordering the hydrocarbon chains of the sterol-enriched fluid DPPC bilayers. Overall, these alkyl side chain modifications generally reduce the ability of Chol to produce its characteristic effects on DPPC bilayer physical properties. These differences are likely due to the less extended and more bent conformations of the alkyl side chains of Camp and Bras, producing sterols with a greater effective cross-sectional area and reduced length than Chol. Hence, the structure of Chol is likely optimized for maximum solubility in, as opposed to maximum ordering of, phospholipid bilayers.

X-ray diffraction is used to solve the low-resolution structures of fully hydrated aqueous dispersions of seven different diacyl phosphatidylethanolamines (PEs) whose hydrocarbon chains have the same effective chain length but whose structures vary widely. Both the lower-temperature, liquid-crystalline lamellar (L) and the higher-temperature, inverted hexagonal (HII) phase structures are solved, and the resultant internal dimensions (d-spacing, water layer thickness, average lipid length, and headgroup area at the lipid-water interface) of each phase are determined as a function of temperature. The magnitude of the L and HII phase d-spacings on either side of the L/HII phase transition temperature (Th) depends significantly on the structure of the PE hydrocarbon chains. The L phase d-spacings range from 51.2 to 56.4 A, whereas those of the HII phase range from 74.9 to 82.7 A. These new results differ from our earlier measurements of these PEs (Lewis et al., Biochemistry, 28:541-548, 1989), which found near constant d-spacings of 52.5 and 77.0 -78.0 A for the L and HII phases, respectively. In both phases, the d-spacings decrease with increasing temperature independent of chain structure, but, in both phases, the rate of decrease in the L phase is smaller than that in the HII phase. A detailed molecular description of the L/HII phase transition in these PEs is also presented. A complete understanding of the physical properties of specific membrane lipids requires a determination of the phase structures that are formed by these lipids under de- fined conditions. Because the lipid phases of biological interest are fully hydrated liquid- crystal mesophases, such a structural measurement involves a determination of the electron density distribution of the lipid/water system from a small number of powder-pattern-averaged orders of x-ray diffraction. In this article, we describe such a structure determination method that is then applied to aqueous dis- persions of various phosphatidylethanolamines (PEs). In an accompanying article to be published elsewhere (D. A. Mannock, R. N. A. H. Lewis, R. N. McElhaney, P. E. Harper, and S. M. Gruner, submitted for publication), these results will be used in a comparative study of PEs and diacyl--D-glucosyl-glycerols containing fatty acyl chains of various lengths and structures. To illuminate the physical principles at work in these systems, it is important to study systems with a variety of chemical structures to differentiate between general physi- cal behavior and physical behavior that varies with the lipid chemical structure. In this paper, we determine the struc- tural parameters of seven PEs with hydrocarbon chains having different chemical structures, but the same effective chain length (ECL). The ECL of a hydrocarbon chain is defined by the total number of carbons in the "main chain." For linear saturated and unsaturated fatty acyl groups, the ECL equals the total number of carbon atoms present, whereas for the branched fatty acyl chains, the ECLs equal the total number of carbon atoms minus those present in the branch(es). For -cyclo- hexyl fatty acyl groups, where three carbon atoms of the terminal six-membered ring actually form part of the main chain, the ECL is equal to the total number of carbon atoms present minus three. Although the unit cell basis vector lengths (d-spacings) of both the lamellar liquid-crystalline (L) and inverted hex- agonal phases (HII) are readily measured, additional infor- mation about the specific chemical structures of these lipids may be used to compute the electron density reconstructions to determine such quantities as average lipid length (l) and water layer thickness (w and r). We first detail the theory and practice of this method of performing the reconstruc- tions and then apply the method to various PEs. The results presented here also serve to correct earlier measurements (Lewis et al., 1989), in which some of the structural dimen- sions versus temperature were incorrect by as much as 10% due to a faulty temperature calibration arising from a volt- age bias in the temperature controller.

As a step towards understanding the mechanism of the biological activity of cyclic antimicrobial peptides, the biophysical properties and conformations of four membrane-active cyclic peptide antibiotics, based on gramicidin S (GS), were examined in aqueous environments. These cyclic peptides, GS10 [cyclo(VKLdYP)2], GS12 [cyclo(VKLKdYPKVKLdYP)], GS14 [cyclo(VKLKVdYPLKVKLdYP)] and [d-Lys]4GS14 [cyclo(VKLdKVdYPLKVKLdYP)] (d-amino acid residues are denoted by d and are underlined) had different ring sizes of 10, 12 and 14 residues, were different in structure and amphipathicity, and covered a broad spectrum of hemolytic and antimicrobial activities. GS10, GS12 and [d-Lys]4GS14 were shown to be monomeric in buffer systems with ionic strength biological environments. GS14 was also monomeric at low concentrations, but aggregated at concentrations > 50 microm. The affinity of peptides for self-assembly and interaction with hydrophobic surfaces was related to their free energy of intermolecular interaction. The effects of variations in salt and organic solvent (trifluoroethanol) concentration and temperature on peptide conformation were also examined. Similar to GS, GS10 proved to have a stable and rather rigid conformation in different environments and over a broad range of temperatures, whereas GS12, GS14 and [d-Lys]4GS14 had more flexible conformations. Despite its conformational similarity to GS10, GS14 had unique physicochemical properties due to its tendency to aggregate at relatively low concentrations. The biophysical data explain the direct relation between structure, amphipathicity and hydrophobicity of the cyclic peptides and their hemolytic activity. However, this relation with the antimicrobial activity of the peptides is of a more complex nature due to the diversity in membrane structures of microorganisms.

The conformation and amide proton exchangeability of the peptide acetyl-K(2)-A(24)-K(2)-amide (A(24)) and its interaction with phosphatidylcholine bilayers were examined by a variety of physical techniques. When dissolved in or cast from methanol as a dried film, A(24) is predominantly alpha-helical. In aqueous media, however, A(24) exists primarily as a mixture of helical (though not necessarily alpha-helical) and random coiled structures, both of which allow rapid H-D exchange of all amide protons. When incorporated into phospholipids in the absence of water, A(24) also exists primarily as a transmembrane alpha-helix. However, upon hydration of that system, rapid exchange of all amide protons also occurs along with a marked change in the amide I absorption band of the peptide. Also, when dispersed with phosphatidylcholine in aqueous media, the conformation and thermal stability of A(24) are not significantly altered by the presence of the phospholipid or by its gel/liquid-crystalline phase transition. Differential scanning calorimetric and electron spin resonance spectroscopic studies indicate that A(24) has relatively minor effects on the thermodynamic properties of the lipid hydrocarbon chain-melting phase transition, that it does not abolish the lipid pretransition, and that its presence has no significant effect on the orientational order or rates of motion of the phospholipid hydrocarbon chains. We therefore conclude that A(24) has sufficient alpha-helical propensity, but insufficient hydrophobicity, to maintain a stable transmembrane association with phospholipid bilayers in the presence of water. Instead, it exists primarily as a dynamic mixture of helices and other conformers and resides mostly in the aqueous phase where it interacts weakly with the bilayer surface or with the polar/apolar interfacial region of phosphatidylcholine bilayers. Thus, polyalanine-based peptides are not good models for the transmembrane alpha-helical segments of natural membrane proteins.

We have synthesized a homologous series of saturated 1,2-di-O-n-acyl-3-O-(beta-D-galactopyranosyl)-sn-glycerols with odd- and even-numbered hydrocarbon chains ranging in length from 10 to 20 carbon atoms, and have investigated their physical properties using differential scanning calorimetry (DSC), X-ray diffraction (XRD) and Fourier-transform infrared (FTIR) spectroscopy. The DSC results show a complex pattern of phase behaviour, which in a typical preheated sample consists of a lower temperature, moderately energetic lamellar gel/lamellar liquid-crystalline (L(beta)/L(alpha)) phase transition and a higher temperature, weakly energetic lamellar/nonlamellar phase transition. On annealing at a suitable temperature below the L(beta)/L(alpha) phase transition, the L(beta) phase converts to a lamellar crystalline (L(c1)) phase which may undergo a highly energetic L(c1)/L(alpha) or L(c1)/inverted hexagonal (H(II)) phase transition at very high temperatures on subsequent heating or convert to a second L(c2) phase in certain long chain compounds on storage at or below 4 degrees C. The transition temperatures and phase assignments for these galactolipids are supported by our XRD and FTIR spectroscopic measurements. The phase transition temperatures of all of these events are higher than those of the comparable phase transitions exhibited by the corresponding diacyl alpha- and beta-D-glucosyl glycerols. In contrast, the L(beta)/L(alpha) and lamellar/nonlamellar phase transition temperatures of the beta-D-galactosyl glycerols are lower than those of the corresponding diacyl phosphatidylethanolamines (PEs) and these glycolipids form inverted cubic phases at temperatures between the lamellar and H(II) phase regions. Our FTIR measurements indicate that in the L(beta) phase, the hydrocarbon chains form a hexagonally packed structure in which the headgroup and interfacial region are undergoing rapid motion, whereas the L(c) phase consists of a more highly ordered, hydrogen-bonded phase, in which the chains are packed in an orthorhombic subcell similar to that reported for the diacyl-beta-D-glucosyl-sn-glycerols. A comparison of the DSC data presented here with our earlier studies of other diacyl glycolipids shows that the rate of conversion from the L(beta) to the L(c) phase in the beta-D-galactosyl glycerols is slightly faster than that seen in the alpha-D-glucosyl glycerols and much faster than that seen in the corresponding beta-D-glucosyl glycerols. The similarities between the FTIR spectra and the first-order spacings for the lamellar phases in both the beta-D-glucosyl and galactosyl glycerols suggest that the headgroup orientations may be similar in both beta-anomers in all of their lamellar phases. Thus, the differences in their L(beta)/L(c) conversion kinetics and the lamellar/nonlamellar phase properties of these lipids probably arise from subtly different hydration and H-bonding interactions in the headgroup and interfacial regions of these phases. In the latter case, such differences would be expected to alter the ability of the polar headgroup to counterbalance the volume of the hydrocarbon chains. This perspective is discussed in the context of the mechanism for the L(alpha)/H(II) phase transition which we recently proposed, based on our X-ray diffraction measurements of a series of PEs.

We have studied the effects of the incorporation of the alpha-helical transmembrane peptides Ac-K(2)-L(24)-K(2)-amide (L(24)) and Ac-K(2)-(L-A)(12)-K(2)-amide ((LA)(12)) on the thermotropic phase behavior of 1,2-dipalmitoyl-d(62)-sn-glycero-3-phosphocholine (DPPC-d(62)) and 1-palmitoyl-d(31)-2-oleoyl-sn-glycero-3-phosphocholine (POPC-d(31)) lipid bilayer model membranes by differential scanning calorimetry (DSC) and the conformational and orientational order of the phospholipid chains by Fourier transform infrared (FTIR) spectroscopy and (2)H nuclear magnetic resonance ((2)H-NMR) spectroscopy, respectively. Our DSC and FTIR spectroscopic studies indicate that the peptides L(24) and (LA)(12) both decrease the temperature and enthalpy of the gel/liquid-crystalline phase transition of DPPC-d(62) bilayers, with (LA)(12) having the greater effect in this regard. An examination of the frequencies of the CH(2) and CD(2) symmetric stretching bands of the infrared spectra of liquid-crystalline states of the peptide-free and peptide-containing DPPC-d(62) and POPC-d(31) samples, and a comparison with the orientational order as measured by (2)H-NMR spectroscopy as well as with the chain order as measured by electron spin resonance spectroscopy, lead us to conclude that the CH(2) (or CD(2)) stretching frequencies of lipid hydrocarbon chains are not a reliable measure of chain conformational order in lipid bilayers containing significant amounts of peptides or other lipophilic inclusions. In contrast, the results of our (2)H-NMR spectroscopic studies present a consistent picture in which both L(24) and (LA)(12) increased in a similar way the time-averaged orientational order of the lipid chains of their liquid-crystalline lipid bilayer hosts. The comparison of the effects L(24) and (LA)(12) on phosphatidylcholine bilayers indicates that the gel-to-liquid-crystalline phase transition appears to be more sensitive to small changes in transmembrane peptide surface topology than hydrocarbon carbon chain orientational order in the liquid-crystalline state.

We have investigated the effect of the presence of 25 mol percent cholesterol on the interactions of the antimicrobial peptide gramicidin S (GS) with phosphatidylcholine and phosphatidylethanolamine model membrane systems using a variety of methods. Our circular dichroism spectroscopic measurements indicate that the incorporation of cholesterol into egg phosphatidylcholine vesicles has no significant effect on the conformation of the GS molecule but that this peptide resides in a range of intermediate polarity as compared to aqueous solution or an organic solvent. Our Fourier transform infrared spectroscopic measurements confirm these findings and demonstrate that in both cholesterol-containing and cholesterol-free dimyristoylphosphatidylcholine liquid-crystalline bilayers, GS is located in a region of intermediate polarity at the polar–nonpolar interfacial region of the lipid bilayer. However, GS appears to be located in a more polar environment nearer the bilayer surface when cholesterol is present. Our 31P-nuclear magnetic resonance studies demonstrate that the presence of cholesterol markedly reduces the tendency of GS to induce the formation of inverted nonlamellar phases in model membranes composed of an unsaturated phosphatidylethanolamine. Finally, fluorescence dye leakage experiments indicate that cholesterol inhibits the GS-induced permeabilization of phosphatidylcholine vesicles. Thus in all respects the presence of cholesterol attenuates but does not abolish the interactions of GS with, and the characteristic effects of GS on, phospholipid bilayers. These findings may explain why it is more potent at disrupting cholesterol-free bacterial than cholesterol-containing eukaryotic membranes while nevertheless disrupting the integrity of the latter at higher peptide concentrations. This additional example of the lipid specificity of GS may aid in the rational design of GS analogs with increased antibacterial but reduced hemolytic activities.

We have investigated the effects of the model alpha-helical transmembrane peptide Ac-K(2)L(24)K(2)-amide (L(24)) on the thermotropic phase behavior of aqueous dispersions of 1,2-dielaidoylphosphatidylethanolamine (DEPE) to understand better the interactions between lipid bilayers and the membrane-spanning segments of integral membrane proteins. We studied in particular the effect of L(24) and three derivatives thereof on the liquid-crystalline lamellar (L(alpha))-reversed hexagonal (H(II)) phase transition of DEPE model membranes by differential scanning calorimetry and (31)P nuclear magnetic resonance spectroscopy. We found that the incorporation of L(24) progressively decreases the temperature, enthalpy, and cooperativity of the L(alpha)-H(II) phase transition, as well as induces the formation of an inverted cubic phase, indicating that this transmembrane peptide promotes the formation of inverted nonlamellar phases, despite the fact that the hydrophobic length of this peptide exceeds the hydrophobic thickness of the host lipid bilayer. These characteristic effects are not altered by truncation of the side chains of the terminal lysine residues or by replacing each of the leucine residues at the end of the polyleucine core of L(24) with a tryptophan residue. Thus, the characteristic effects of these transmembrane peptides on DEPE thermotropic phase behavior are independent of their detailed chemical structure. Importantly, significantly shortening the polyleucine core of L(24) results in a smaller decrease in the L(alpha)-H(II) phase transition temperature of the DEPE matrix into which it is incorporated, and reducing the thickness of the host phosphatidylethanolamine bilayer results in a larger reduction in the L(alpha)-H(II) phase transition temperature. These results are not those predicted by hydrophobic mismatch considerations or reported in previous studies of other transmembrane alpha-helical peptides containing a core of an alternating sequence of leucine and alanine residues. We thus conclude that the hydrophobicity and conformational flexibility of transmembrane peptides can affect their propensity to induce the formation of inverted nonlamellar phases by mechanisms not primarily dependent on lipid-peptide hydrophobic mismatch.

This is the second of two papers dealing with the structure of lipid-water phases based on Infinite Periodic Minimal Surfaces (IPMS). The first paper describes mathematical modeling of such phases. In this paper, a new reconstruction method, called the methyl trough search, is described and used to solve the structures based on powder pattern X-ray diffraction data. Structures are derived for both a single chain lipid-water system (mono-olein) and a diacyl phospholipid-water system (2-2 methyl butyl 16:0 phosphatidylcholine). The methyl trough search uses the low electron density of the lipid methyl tails to determine the correct phasing for the electron density reconstruction. The data are consistent with a structure based on the IPMS D surface. The results are compared to other methods used to solve the mono-olein structure; the structure of the diacyl lipid has never before been solved. We discuss the subtleties involved in reconstruction of D surface based phases and the substantial artifacts that arise in low-resolution reconstructions of hydrocarbon lipids lacking heavy-atom sites.

The influence of the lipidic phase structures on their susceptibility to solubilization by the nonionic detergent C12E8 has been explored. To this aim, a phase diagram for dimyristoylphosphatidylch...

Gramicidin S (GS) is a cyclic decapeptide of primary structure [cyclo-(Val-Orn-Leu- d -Phe-Pro)2] secreted by Bacillus brevis. It is a powerful antimicrobial agent with potent cidal action on a wide variety of Gram-negative and Gram-positive bacteria as well as on several pathogenic fungi. Unfortunately, however, GS is rather non-specific in its actions and also exhibits a high hemolytic activity, limiting its use as an antibiotic to topical applications. In a wide variety of environments, the GS molecule exists as a very stable amphiphilic antiparallel β-sheet structure with a polar and a non-polar surface. Moreover, the large number of structure–activity studies of GS analogs which have been carried out indicate that this ‘sidedness’ structure is required for its antimicrobial action. In this review, we summarize both published and unpublished biophysical studies of the interactions of GS with lipid bilayer model and with biological membranes. In general, these studies show that GS partitions strongly into liquid–crystalline lipid bilayers in both model and biological membranes, and seems to be located primarily in the glycerol backbone region below the polar headgroups and above the hydrocarbon chains. The presence of GS appears to perturb lipid packing in liquid–crystalline bilayers and GS can induce the formation of inverted cubic phases at lower temperatures in lipids capable of forming such phases at higher temperature in the absence of peptide. The presence of GS at lower concentrations also increases the permeability of model and biological membranes and at higher concentrations causes membrane destabilization. There is good evidence from studies of the interaction of GS with bacterial cells that the destruction of the integrity of the lipid bilayer of the inner membrane is the primary mode of the antimicrobial action of this peptide. The considerable lipid specificity of GS for binding to and destabilization of lipid bilayer model membranes indicates that the design of GS analogs with an improved antimicrobial potency and a markedly decreased toxicity for eukaryotic cell plasma membranes should be possible.

We investigated the effects of various concentrations of staphylococcal delta-lysin on the thermotropic phase behavior of large multilamellar dimyristoylphosphatidylcholine (DMPC) vesicles by differential scanning calorimetry (DSC), 31P nuclear magnetic resonance (NMR) and Fourier transform infrared (FTIR) spectroscopy, and X-ray diffraction. The DSC studies revealed that at all concentrations, the addition of delta-lysin progressively decreases the enthalpy of the pretransition of DMPC bilayers without significantly affecting its temperature or cooperativity. Similarly, the addition of smaller quantities of peptide has little effect on the temperature of the main phase transition of DMPC bilayers but does reduce the cooperativity and enthalpy of this transition somewhat. However, at higher peptide concentrations, a second phase transition with a slightly increased temperature and a markedly reduced cooperativity and enthalpy is also induced, and this latter phase transition resolves itself into two components at the highest peptide concentrations that are tested. Moreover, our 31P NMR spectroscopic studies reveal that at relatively low delta-lysin concentrations, essentially all of the phospholipid molecules produce spectra characteristic of the lamellar phase, whereas at the higher peptide concentrations, an increasing proportion exhibit an isotropic signal. Also, at the highest delta-lysin concentrations that are studied, the isotropic component of the 31P NMR spectrum also resolves itself into two components. At the highest peptide concentration that was tested, we are also able to effect a macroscopic separation of our sample into two fractions by centrifugation, a pellet containing relatively smaller amounts of delta-lysin and a supernatant containing larger amounts of peptide relative to the amount of lipid present. We are also able to show that the more cooperative phase transition detected calorimetrically, and the lamellar phase 31P NMR signal, arise from the pelleted material, while the less cooperative phase transition and the isotropic 31P NMR signal arise from the supernatant. In addition, we demonstrate by X-ray diffraction that the pelleted material corresponds to delta-lysin-containing large multilamellar vesicles and the supernatant to a mixture of delta-lysin-containing small unilamellar vesicles and discoidal particles. We also show by FTIR spectroscopy that delta-lysin exists predominantly in the alpha-helical conformation in aqueous solution or when interacting with DMPC, and that a large fraction of the peptide bonds undergo H-D exchange in D(2)O. However, upon interaction with DMPC, the fraction of exchangeable amide protons decreases. We also demonstrate by this technique that both of the phase transitions detected by DSC correspond to phospholipid hydrocarbon chain-melting phase transitions. Finally, we show by several techniques that the absolute concentrations of delta-lysin and the thermal history, as well as the lipid:peptide ratio, can affect the thermotropic phase behavior and morphology of peptide-lipid aggregates.

We have utilized Fourier transform infrared spectroscopy to study the interaction of the antimicrobial peptide gramicidin S (GS) with lipid micelles and with lipid monolayer and bilayer membranes as a function of temperature and of the phase state of the lipid. Since the conformation of GS does not change under the experimental conditions employed in this study, we could utilize the dependence of the frequency of the amide I band of the central beta-sheet region of this peptide on the polarity and hydrogen-bonding potential of its environment to probe GS interaction with and location in these lipid model membrane systems. We find that the GS is completely or partially excluded from the gel states of all of the lipid bilayers examined in this study but strongly partitions into lipid micelles, monolayers, or bilayers in the liquid-crystalline state. Moreover, in general, the penetration of GS into zwitterionic and uncharged lipid bilayer coincides closely with the gel to liquid-crystalline phase transition of the lipid. However, GS begins to penetrate into the gel-state bilayers of anionic phospholipids prior to the actual chain-melting phase transition, while in cationic lipid bilayers, GS does not partition strongly into the liquid-crystalline bilayer until temperatures well above the chain-melting phase transition are reached. In the liquid-crystalline state, the polarity of the environment of GS indicates that this peptide is located primarily at the polar/apolar interfacial region of the bilayer near the glycerol backbone region of the lipid molecule. However, the depth of GS penetration into this interfacial region can vary somewhat depending on the structure and charge of the lipid molecule. In general, GS associates most strongly with and penetrates most deeply into more disordered bilayers with a negative surface charge, although the detailed chemical structure of the lipid molecule and physical organization of the lipid aggregate (micelle versus monolayer versus bilayer) also have minor effects on these processes.

We have studied the effects of the antimicrobial peptide gramicidin S (GS) on the thermotropic phase behavior of large multilamellar vesicles of dimyristoylphosphatidylcholine (DMPC), dimyristoylphosphatidylethanolamine (DMPE) and dimyristoyl phosphatidylglycerol (DMPG) by high-sensitivity differential scanning calorimetry. We find that the effect of GS on the lamellar gel to liquid-crystalline phase transition of these phospholipids varies markedly with the structure and charge of their polar headgroups. Specifically, the presence of even large quantities of GS has essentially no effect on the main phase transition of zwitterionic DMPE vesicles, even after repeating cycling through the phase transition, unless these vesicles are exposed to high temperatures, after which a small reduction in the temperature, enthalpy and cooperativity of the gel to liquid-crystalline phase transitions is observed. Similarly, even large amounts of GS produce similar modest decreases in the temperature, enthalpy and cooperativity of the main phase transition of DMPC vesicles, although the pretransition is abolished at low peptide concentrations. However, exposure to high temperatures is not required for these effects of GS on DMPC bilayers to be manifested. In contrast, GS has a much greater effect on the thermotropic phase behavior of anionic DMPG vesicles, substantially reducing the temperature, enthalpy and cooperativity of the main phase transition at higher peptide concentrations, and abolishing the pretransition at lower peptide concentrations as compared to DMPC. Moreover, the relatively larger effects of GS on the thermotropic phase behavior of DMPG vesicles are also manifest without cycling through the phase transition or exposure to high temperatures. Furthermore, the addition of GS to DMPG vesicles protects the phospholipid molecules from the chemical hydrolysis induced by their repeated exposure to high temperatures. These results indicate that GS interacts more strongly with anionic than with zwitterionic phospholipid bilayers, probably because of the more favorable net attractive electrostatic interactions between the positively charged peptide and the negatively charged polar headgroup in such systems. Moreover, at comparable reduced temperatures, GS appears to interact more strongly with zwitterionic DMPC than with zwitterionic DMPE bilayers, probably because of the more fluid character of the former system. In addition, the general effects of GS on the thermotropic phase behavior of zwitterionic and anionic phospholipids suggest that it is located at the polar/apolar interface of liquid-crystalline bilayers, where it interacts primarily with the polar headgroup and glycerol-backbone regions of the phospholipid molecules and only secondarily with the lipid hydrocarbon chains. Finally, the considerable lipid specificity of GS interactions with phospholipid bilayers may prove useful in the design of peptide analogs with stronger interactions with microbial as opposed to eucaryotic membrane lipids.

Fourier transform infrared (FTIR) spectroscopy is a powerful yet relatively inexpensive spectroscopic technique for studying the structure and organization of phospholipid bilayers. This technique yields information about all regions of the phospholipid molecule simultaneously without the necessity of introducing perturbing extrinsic probes. In this review we summarize some recent FTIR spectroscopic studies of the structure and organization of phospholipids in their lamellar liquid-crystalline, gel, and crystalline phases and show that interconversions between these phases can be readily monitored by this technique. We also demonstrate that this technique can yield valuable information about nonlamellar phospholipid phases as well. Finally, we point out that in principle FTIR spectroscopy is capable of yielding fairly high resolution structural and conformational information about phospholipid molecules in multi-molecular aggregates and give several examples of how this potential is beginning to be realized.

The molecular organization and dynamics have been investigated in membranes consisting of 1-palmitoyl-2-oleoyl-l-alpha-phosphatidylcholine (POPC) and various ratios of a transmembrane alpha-helical peptide, Ac-K2L24K2-amide (L24), in order to gain insights into how the transmembrane portions of membrane proteins are mixed with phospholipids and organized in biological membranes. Particular attention was paid to membranes with high peptide concentrations. The molecular organization and dynamics were studied in the ps-to-micros regime using various spin-labeling techniques. Conventional ESR spectra as well as saturation-recovery curves measured in both the presence and the absence of molecular oxygen showed that phosphatidylcholine spin-labels detect the existence of a single homogeneous environment, indicating that both L24 and POPC are likely to be undergoing fast translational diffusion in L24-POPC membranes of up to 9 mol % peptide. Since 16-18 molecules of phosphatidylcholine are required to surround a transmembrane alpha-helical peptide [Morrow, M. R., Huschilt, J. C., and Davis, J. H. (1985) Biochemistry 24, 5396-5406], L24 must form L24-rich regions at a P/L ratio of 1/10 instantaneously. However, these results suggest that the lipid exchange rates among the bulk, boundary, and L24-rich regions are fast, and that the L24-rich regions must be forming and dispersing rapidly in a time scale shorter than 0.1 micros, the conventional ESR spin-label time scale and the electron spin-lattice relaxation time scale in the presence of molecular oxygen. Although this does not exclude the possibility of the formation of small, stable oligomers of L24, it is unlikely because L24 lacks features that would favor their formation. L24 (9 mol %) increases the hydrophobicity of the central part of the POPC membrane from the level of 1-decanol to that of pure hexane and also increases the hydrophobicity near the membrane surface from the level of 2-propanol to that of 1-decanol. The effect of 9 mol % L24 on the order parameter profile is similar to that of decreasing the temperature by approximately 8 degrees C between 10 and 55 degrees C. It is concluded that L24 is highly miscible in POPC membranes even at high concentrations in the membrane.

It is shown by thin-layer and high-performance liquid chromatography that the two membrane lipids monoacyl-diglucosyl-diacyl-glycerol (MADGlcDAG) and monoacyl-bis-glycerophosphoryl-diglucosyl-diacyl-glycerol are synthesized by Acholeplasma laidlawii strain B-PG9 when the cells are grown in two different growth media. The two lipids are also synthesized by A. laidlawii strain A-EF22 and their chemical structures have been determined previously by NMR spectroscopy. Since a reversed hexagonal phase is the only liquid-crystalline phase formed by MADGlcDAG, it is concluded that A. laidlawii strain B-PG9, in resemblance to strain A-EF22, synthesizes three membrane lipids that are able to form reversed nonlamellar phases. A comparison of the membrane lipids from the two strains shows that there is essentially one lipid from each strain that differs. However, both these lipids have common physico-chemical properties, namely the ability to form reversed nonlamellar phases. Finally, it is also shown that novel lipids may be synthesized by A. laidlawii through long-time adaptation to altered growth conditions.

The interactions of the cyclic peptide gramicidin S (GS) with a variety of single-component lipid bilayers, and with membrane polar lipid extracts of Acholeplasma laidlawii B and Escherichia coli, were examined by differential scanning calorimetry (DSC), 31P-nuclear magnetic resonance (NMR) spectroscopy, and X-ray diffraction. The DSC data indicate that the effects of GS on the thermotropic phase behavior of phosphatidylcholine and phosphatidylethanolamine dispersions are compatible with those expected of peptides interacting primarily with the polar headgroup and/or the polar/apolar interfaces of lipid bilayers. These DSC studies also suggest that GS exhibits stronger interactions with the more fluid bilayers. For mixtures of GS with lipids such as phosphatidylcholine, phosphatidylserine, cardiolipin, and sphingomyelin, axially symmetric 31P-NMR powder patterns are observed throughout the entire temperature range examined (0-90 degrees C), and there is little evidence for significant destabilization of the lipid bilayer with respect to nonlamellar phases. With mixtures of GS with either phosphatidylethanolamine, phosphatidylglycerol, or a nonlamellar phase-forming phosphatidylcholine, axially symmetric 31P-NMR powder patterns are also observed at low temperatures. However, at high temperatures, an isotropic component is observed in their 31P-NMR spectra, and the relative intensity of this component increases significantly with temperature and with GS concentration. Once formed at high temperatures, this isotropic component exhibits a marked cooling hysteresis and in most cases disappears only when the sample is recooled to temperatures well below the lipid hydrocarbon chain-melting phase transition temperature. We also show that GS induces the formation of isotropic components in the 31P-NMR spectra of heterogeneous lipid mixtures such as occur in A. laidlawii B and E. coli membranes. These observations suggest that GS induces the formation of cubic or other three dimensionally ordered inverted nonlamellar phases when it interacts with some types of lipid bilayers, a suggestion strongly supported by our X-ray diffraction studies. Our results also suggest that the capacity of GS to induce the formation of such phases increases with the intrinsic nonlamellar phase-preferring tendencies of the lipids with which it interacts probably by producing localized increases in membrane monolayer curvature stress. The latter effect could be part of the mechanism through which this peptide exhibits its antimicrobial and hemolytic activities.