Alcohols dehydrate lipid membranes: an infrared study on hydrogen bonding.

The effects of alcohols (methanol, ethanol, and n-butanol) on the hydrogen bonding of dipalmitoylphosphatidylcholine (DPPC) were studied by Fourier-transform infrared spectroscopy (FTIR) in water-in-oil (carbon tetrachloride) reversed micelles. The bound O-H stretching mode of water, bonded to DPPC, appeared as a broad band at around 3400 cm-1. The O-H bending mode of this complex appeared as a weak broad band at 1644 cm-1. No free O-H signal was observed. When alcohols were added, a part of DPPC-bound water was replaced by the alcohols. The released 'free' water appeared at 3680 cm-1. This free O-H stretching band represents water-alcohol complex. A new broad band of O-H stretching appeared at 3235 cm-1, which represents the alcohol molecules bound to the phosphate moiety of DPPC. When the alcohol concentration was increased, the intensities of the free O-H stretching and bending bands increased. The P = O- antisymmetric stretching band at 1238 cm-1 became broader and shifted to lower frequencies. This means that alcohols interacted with the phosphate moiety and replaced the bound water. In the deconvoluted spectra of the C = O stretching mode, the ratio between the free sn-2 and the hydrogen-bonded sn-2 bands increased; a part of the bound water at the sn-2 carbon in the glycerol skeleton is also released and the free sn-2 signal increased. From the change in the intensity of the P = O- stretching band, the partition coefficients of alcohols between the phosphate region of DPPC and water were estimated: methanol 7.8, ethanol 16.7 at 22.0 degrees C in mole fraction bases. In molality, these values translates into methanol 0.21 and ethanol 0.45. These results indicate that short-chain alcohols interact with lipid membranes at the phosphate moiety at the hydrophilic head, weaken the membrane-water interaction, and destabilize membranes.     

The dimerization of protochlorophyll pigments in non-polar solvents

The infrared, visible and nuclear magnetic resonance spectra of protochlorophyll a and vinylprotochlorophyll a in dry non-polar solvents (carbon tetrachloride, chloroform, cyclohexane) are presented and interpreted in terms of dimer interaction. The infrared spectra in the 1600-1800 cm-1 region clearly show the existence of a coordination interaction between the C-9 ketone oxygen function of one molecule and the central magnesium atom of another molecule. Infrared spectra in the OH stretching region (3200-3800 cm-1) provide a valuable test of the water content in the samples. The analysis of the absorption and circular dichroism spectra of protochlorophyll a and vinylprotochlorophyll a in carbon tetrachloride demonstrates the existence of a monomer-dimer equilibrium in the concentration range from 10(-6) to 5.10(-4) M. The dimerization constants are (6 +/-2).10(5)1.M-1 for protochlorophyll a and (4.5 +/-21.10(5) 1.M-1 for vinylprotochlorophyll a at 20 degrees C. The deconvolution of visible spectra in the red region has been performed in order to obtain quantitative information on the dimer structure. Two models involving a parallel or a perpendicular arrangement of the associated molecules are considered. From 1H NMR spectra, it appears that the region of overlap occurs near ring V, in agreement with the interpretation of the infrared spectra.     

Peptide-induced membrane elastic deformations decelerate gramicidin dimer-monomer equilibration

Gramicidin A (gA) is a hydrophobic pentadecapeptide readily incorporating into a planar bilayer lipid membrane (BLM), thereby inducing a large macroscopic current across the BLM. This current results from ion-channel formation due to head-to-head transbilayer dimerization of gA monomers with rapidly established monomer-dimer equilibrium. Any disturbance of the equilibrium, e.g., by sensitized photoinactivation of a portion of gA monomers, causes relaxation toward a new equilibrium state. According to previous studies, the characteristic relaxation time of the gA-mediated electric current decreases as the current increases upon elevating the gA concentration in the membrane. Here, we report data on the current relaxation kinetics for gA analogs with N-terminal valine replaced by glycine or tyrosine. Surprisingly, the relaxation time increased rather than decreased upon elevation of the total membrane conductance induced by these gA analogs, thus contradicting the classical kinetic scheme. We developed a general theoretical model that accounts for lateral interaction of monomers and dimers mediated by membrane elastic deformations. The modified kinetic scheme of the gramicidin dimerization predicts the reverse dependence of the relaxation time on membrane conductance for gA analogs, with a decreased dimerization constant that is in a good agreement with our experimental data. The equilibration process may be also modulated by incorporation of other peptides (“impurities”) into the lipid membrane.     

Comparison of lipid/gramicidin dispersions and cocrystals by Raman scattering

Gramicidin crystals, dimyristoylphosphatidylcholine (DMPC)/gramicidin dispersions, and DMPC/gramicidin cocrystals were examined by Raman scattering to determine lipid/gramicidin stoichiometries and lipid organization. Calibrations of the choline (716-cm-1) and tryptophan (756-cm-1) peaks indicate that the cocrystals contain two lipids for each gramicidin monomer, a result confirmed by chemical analyses of washed crystals. In dispersions with high lipid/gramicidin ratios (e.g., 25:1), the lipid is ordered but becomes increasingly disordered as the gramicidin content is increased. Paradoxically, the DMPC/gramicidin cocrystals have highly ordered lipids that possibly contain no gauche bonds at all, despite their low lipid/gramicidin ratio. In addition, the polypeptide amide I peak position near 1670 cm-1 is found to be independent of the lipid/gramicidin ratio in the complexes and may indicate a beta-helix-type secondary structure at all ratios. However, the amide I peak broadens significantly at low lipid/gramicidin ratios and broadens still further in the cocrystals, suggesting that protein-protein interactions may induce band-broadening distortions of the polypeptide structure.     

The solution conformations of gramicidin A and its analogs

The conformational states in dioxane and ethanol of gramicidin A and of analogs varying in chain length and amino acid sequence have been studied. Infrared, CD, and polarization of fluorescence spectra of the peptides were measured, from which dimerization constants were determined and spectral characteristics of the monomeric and dimeric states obtained. Resonance splitting of the amide I ir band has been calculated for all gramicidin A models proposed earlier. Detailed comparison of the experimental and computed spectra showed that the four dimeric gramicidin species present in solution are predominantly antiparallel double ?ππ_ld helices in equilibrium with smaller amounts of head-to-head associated π_LD helices. The gramicidin A monomer was found to be a π_LD^4.4 helix in dioxane. For each conformational form the number of residues per turn and the helical sense were determined. The relationship between the amino acid sequence and the structure and stability of the dimer in the series of gramicidin A and its analogs is discussed. The above findings are rationalized in terms of the membrane channel properties of gramicidin A, in particular the conformational rearrangements occurring during the passage of metal ions through the channel and also the differences in conformation of the antibiotic in nonpolar solutions and in the membrane.     

Effects of crystallization on the heme-carbon monoxide moiety of bovine heart cytochrome c oxidase carbonyl.

Cytochrome c oxidase isolated from bovine heart was crystallized in the fully reduced carbon monoxide (CO)-bound form. To evaluate the structure of the O2 reaction site in crystals and in solution, the bound C-O stretch infrared band in protein crystals was compared with the band for protein solution. In solution, the C-O stretch band could be deconvoluted into two extremely narrow bands, one at 1963.6 cm-1 with delta v1/2 = 3.4 cm-1 of 60% Gaussian/40% Lorentzian character represented 86% of the total band area and the other at 1960.3 cm-1 with delta v1/2 = 3.0 cm-1 of 47% Gaussian/53% Lorentzian character represented 14% of the total band area. The crystals exhibited two deconvoluted C-O infrared bands having very similar band parameters with those in solution. These findings support the presence of two structurally similar conformers in both crystals and solution. Thus crystallization of this enzyme does not affect the structure at the CO-binding site to as great extent as has been noted for myoglobin and hemoglobin carbonyls, indicating that the active (CO- or O2-binding) site of cytochrome c oxidase must be conformationally very stable and highly ordered compared to other hemoproteins such as hemoglobin.     

Location of ion-binding sites in the gramicidin channel by X-ray diffraction.

We report the first X-ray diffraction on gramicidin in its membrane-active form by using uniformly aligned multilayer samples of membranes containing gramicidin and ions (T1+, K+, Ba2+, Mg2+ or without ions). From the difference electron density profiles, we found a pair of symmetrically located ion-binding sites for T1- at 9.6 (+/- 0.3) A and for Ba2+ at 13.0 (+/- 0.2) A from the midpoint of the gramicidin channel. The location of Ba(2+)-binding sites is near the ends of the channel, consistent with the experimental observation that divalent cations do not permeate but block the channel. The location of T1(+)-binding sites is somewhat of a surprise. It was generally thought that monovalent cations bind to the first turn of the helix from the mouth of the channel. (It is now generally accepted that the gramicidin channel is a cylindrical pore formed by two monomers, each a single-stranded beta 6.3 helix and hydrogen-bonded head-to-head at their N termini.) But our experiment shows that the T1(+)-binding site is either near the bottom of or below the first helix turn.     

Tryptophan perturbation in the L intermediate of bacteriorhodopsin: fourier transform infrared analysis with indole-15N shift.

In the photoreaction of bacteriorhodopsin, the L intermediate shows an intense band at 3486 cm-1 which is unaffected by 2H2O (Maeda, A., Sasaki, J., Shichida, Y., & Yoshizawa, T. (1992) Biochemistry 31, 462-467]. This band is shifted to 3477 cm-1 by [indole-15N]tryptophan substitution and therefore is assigned to the N-H stretching vibration of the indole of tryptophan. Free indole in carbon tetrachloride shows its N-H stretching vibration at 3491 cm-1 [Fuson, N., Josien, M.-L., Powell, R. L., & Utterback, E. (1952) J. Chem. Phys. 20, 145-152]. Thus, it is suggested that at least one tryptophan residue in the L intermediate is not hydrogen bonded.     

Head-to-head dimerization of parallel beta helices in a synthetic model of the linear gramicidins

In chloroform solution, the D ,L -alternating stereo-co-oligopeptide HCO-L -Phe-(D -Phe-L -Phe)₃-OMe (I) forms three major species, two of which are dimeric and one tetrameric. One of the two dimeric species gives a specific set of ¹H-nmr signals at 25°C; the other, together with the tetrameric species, gives another set of resonance signals. In a carbon tetrachloride or cyclohexane solution at 25°C, I forms virtually only the tetrameric species. From the nmr data, it can be shown that the dimeric and tetrameric species, that are in rapid equilibrium with each other in chloroform solutions, are a right-handed ↑↑β^5.6 helical dimer and the head-to-head (formyl-ends-to-formyl-ends) dimerization product of this dimer. It is suggested that the linear gramicidins may also form head-to-head dimers of parallel β helices, as observed for the model oligopeptide I.     

Fourier transform infrared study of proteins with parallel beta-chains

Deconvolved and second derivative Fourier transform infrared spectra of the proteins flavodoxin and triosephosphate isomerase have been obtained in the 1600 to 1700 cm-1 (amide I) region. To our knowledge these results provide the first experimental infrared data on proteins with parallel beta-chains. Characteristic absorption bands for the parallel beta-segments are observed at 1626-1639 cm-1 (strong) and close to 1675 cm-1 (weak). Previous theoretical studies based on hypothetical models with large, regular beta-sheets had suggested bands close to 1650 and 1666 cm-1. Our new assignments were confirmed by band area measurements, which yield conformational information in good agreement with results from X-ray diffraction data. The spectra were compared with corresponding spectra of concanavalin A and carboxypeptidase A. The first contains only antiparallel beta-segments, the second "mixed" beta-segments, with some strands lying antiparallel and others parallel. None of the observed amide I band frequencies assigned to parallel beta-chains occurs in the 1650 cm-1 region associated with helical segments.     

Gramicidin channels in phospholipid bilayers with unsaturated acyl chains.

In organic solvents gramicidin A (gA) occurs as a mixture of slowly interconverting double-stranded dimers. Membrane-spanning gA channels, in contrast, are almost exclusively single-stranded beta(6,3)-helical dimers. Based on spectroscopic evidence, it has previously been concluded that the conformational preference of gA in phospholipid bilayers varies as a function of the degree of unsaturation of the acyl chains. Double-stranded pi pi(5,6)-helical dimers predominate (over single-stranded beta(6,3)-helical dimers) in lipid bilayer membranes with polyunsaturated acyl chains. We therefore examined the characteristics of channels formed by gA in 1-palmitoyl-2-oleoylphosphatidylcholine/n-decane, 1,2-dioleoylphosphatidylcholine/n-decane, and 1,2-dilinoleoylphosphatidylcholine/n-decane bilayers. We did not observe long-lived channels that could be conducting double-stranded pi pi(5,6)-helical dimers in any of these different membrane environments. We conclude that the single-stranded beta(6,3)-helical dimer is the only conducting species in these bilayers. Somewhat surprisingly, the average channel duration and channel-forming potency of gA are increased in dilinoleoylphosphatidylcholine/n-decane bilayers compared to 1-palmitoyl-2-oleoylphosphatidylcholine/n-decane and dioleoylphosphatidylcholine/n-decane bilayers. To test for specific interactions between the aromatic side chains of gA and the acyl chains of the bilayer, we examined the properties of channels formed by gramicidin analogues in which the four tryptophan residues were replaced with naphthylalanine (gN), tyrosine (gT), and phenylalanine (gM). The results show that all of these analogue channels experience the same relative stabilization when going from dioleoylphosphatidylcholine to dilinoleoylphosphatidylcholine bilayers.     

Raman spectra of heme a, cytochrome oxidase-ligand complexes, and alkaline denatured oxidase.

We report 441.6 nm excitation resonance Raman spectra of oxidized and reduced monomeric heme a-imidazole, cytochrome oxidase-exogenous ligand complexes in various redox states, and alkaline denatured oxidase. These data show that, in reduced oxidase, the cytochrome a3 Raman spectrum has bands at 215, 364, 1230, and 1670 cm-1 not observed in the cytochrome a spectrum. The appearance of these bands in the reduced cytochrome a3 spectrum is due to interactions between the heme a of cytochrome a3 and its protein environment and not to intrinsic properties of heme a. These interactions are pH sensitive and strongly influence the vibrational spectra of both heme a groups. We assign the 1670-cm-1 band to the heme a formyl substituent and propose that the intensity of the 1670 cm-1 is high for reduced cytochrome a3 because the C==O lies in the porphyrin plane and is very weak for oxidized and reduced cytochrome a, oxidized cytochrome a3, and oxidized and reduced heme a-imidazole because the C==O lies out of the plane. We suggest that movement of the C==O in and out of the plane explains the ligand induced spectral shift in the optical absorption spectrum of reduced cytochrome a3. Finally, we confirm the observation of Adar & Yonetani (private communication) that, under laser illumination, resting oxidase is photoreactive.     

Effect of the G.T mismatch on backbone and sugar conformations of Z-DNA and B-DNA: analysis by Raman spectroscopy of crystal and solution structures of d(CGCGTG) and d(CGCGCG)

The Z-DNA crystal structures of d(CGCGTG) and d(CGCGCG) are compared by laser Raman spectroscopy. Raman bands originating from vibrations of the phosphodiester groups and sensitive to the DNA backbone conformation are similar for the two structures, indicating no significant perturbation to the Z-DNA backbone as a result of the incorporation of G.T mismatches. Both Z structures also exhibit Raman markers at 625 and 670 cm-1, assigned respectively to C3'-endo/syn-dG (internal) and C2'-endo/syn-dG conformers (3' terminus). Additional Raman intensity near 620 and 670 cm-1 in the spectrum of the d(CGCGTG) crystal is assigned to C4'-exo/syn-dG conformers at the mismatch sites (penultimate from the 5' terminus). A Raman band at 1680 cm-1, detected only in the d(CGCGTG) crystal, is assigned to the hydrogen-bonded dT residues and is proposed as a definitive marker of the Z-DNA wobble G.T pair. For aqueous solutions, the Raman spectra of d(CGCGTG) and d(CGCGCG) are those of B-DNA, but with significant differences between them. For example, the usual B-form marker band at 832 cm-1 in the spectrum of d(CGCGTG) is about 40% less intense than the corresponding band in the spectrum of d(CGCGCG), and the former structure exhibits a companion band at 864 cm-1 not observed for d(CGCGCG). The simplest interpretation of these results is that the conventional B-form OPO geometry occurs for only 6 of the 10 OPO groups of d(CGCGTG). The remaining four OPO groups, believed to be those at or near the mismatch site, are in an "unusual B" conformation which generates the 864 cm-1 band.(ABSTRACT TRUNCATED AT 250 WORDS)     

Electron transfer induces side-chain conformational changes of glutamate-286 from cytochrome bo3

Heme-copper oxidases have two putative proton channels, the so-called K-channel and the membrane-spanning D-channel. The latter contains a number of polar groups with glutamate-286 located in its center, which could-together with bound water-contribute to a transmembrane hydrogen-bonded network. Protonation states of carboxyl groups from cytochrome bo3 of Escherichia coli were studied by redox Fourier transform infrared (FTIR) difference spectroscopy. A net absorbance increase in the carboxyl region was observed upon reduction. The band signature typically found in heme-copper oxidases comprises an absorbance decrease (reduced-minus-oxidized difference spectra) at 1745 cm-1 and increase at 1735 cm-1. No significant changes in the carboxyl region were found in the site-specific mutants D135E and D407N. The difference bands were lacking in redox spectra of mutants at position 286; they could clearly be related to Glu-286. In wild-type oxidase, the pK of Glu-286 appears to be higher than 9.8. Upon solvent isotope exchange from H2O to D2O, the band at 1745 cm-1 shifts more readily than the one at 1735 cm-1, indicating dissimilar accessibility of the carboxyl side chain to the hydrogen-bonded network in both redox states. The data are consistent with a redox-triggered conformational change of Glu-286, which attributes to the carboxyl group an orientation toward the interior of the D-channel for the oxidized form. The change of Glu-286 is retained in cyanide complexes of cytochrome bo3 and of cytochrome c oxidase; therefore it should be related to oxidoreduction of the heme b and/or CuB metal centers.     

Dynamic interactions of CO with a3Fe and CuB in cytochrome c oxidase in beef heart mitochondria studied by Fourier transform infrared spectroscopy at low temperatures

Carbon monoxide bound to cytochrome c oxidase has been observed by Fourier transform infrared spectroscopy between 10 K and 280 K in the dark and during and after continuous photolysis. CO bound to a3Fe absorbs near 1963 cm-1, with minor bands at lower frequencies. Photolysis at low temperatures transfers CO to CuB, with the major component near 2062 cm-1 and a minor one near 2043 cm-1. Vibrational absorptions are assigned by comparison with heme and copper carbonyls, by frequency dependence of all bands on the isotopic mass of CO, and by similar behavior of major and minor components with photolysis and relaxation kinetics as a function of temperature. Reformation of a3FeCO after photolysis is an apparent first order process below 210 K with a distribution of rate constants. The kinetics are well described by a power law. Arrhenius behavior is followed between 140 K and 180 K to yield a peak activation enthalpy of 40.3 kJ/mol and a distribution in g(H) = 2.56 kJ/mol (full width at half-maximum). The major component of a3FeCO shows a very narrow CO absorption band (full width at half-maximum = 2.4 cm-1), while that of CuBCO shows a broader CO absorption (full width at half-maximum = 6 cm-1). These data indicate that in the reduced carbon monoxide complex, a3FeCO is in highly ordered nonpolar surroundings sufficiently separated from CuB that it is not perturbed by motion of the latter, while CuBCO is in less ordered, more flexible surroundings.     

The pH dependence of the resonance raman spectra and structural alterations at heme moieties of various c-type cytochromes.

The pH dependence of resonance Raman spectra were studied for ferrous and ferric cytochromes c, c2, c3, c-551, and c-555. The frequencies of the 1565 cm-1 (ferric) and 1539 cm-1 lines (ferrous) were sensitive to the replacement of the sixth ligand. The titration curve for the 1565 cm-1 line of cytochrome c was parallel with that for the 695 nm band. The pH dependence of the 1539 cm-1 line of ferrous cytochrome c3 suggested the stepwise replacement of the sixth ligand of its four hemes, although such pH dependence was not recognized for the Raman spectra of other ferrous cytochromes investigated. The relative intensities of three Raman lines at 1639, 1587, and 1561 cm-1 of ferric protoporphyrin bis-imidazole complex were changed clearly by the presence of detergents. The relative intensities of the corresponding three Raman lines of cytochromes b5 and c were close to those of the ferric porphyrin complex in the presence and absence of detergents, respectively, suggesting an appreciable difference in their heme environments. Reduced hemin in detergent solution, unexpectedly, gave the Raman spectrum of ferric low spin type.     

The channel properties of possible gramicidin dimers

Extending previous work (Sung & Jordan, 1987 a, Biophys. J. 51, 661-672; 1988, Biophys. J.54, 519-526), we describe channel properties of five possible gramicidin dimers by studying dimerization energies and axial electrical potentials. Unlike the head-to-head dimer (the predominant channel former), both tail-to-tail and head-to-tail dimers with the same beta-helical monomer structure as the head-to-head dimer only form four intermonomer hydrogen bonds and are much less stable. Were channels formed from these dimers to be observed, their electrical potential profiles suggest that they should be cation selective, probably conduct less than the head-to-head dimer, have a central cation binding site, bind cations preferentially if crystallizable, and in the case of the head-to-tail dimer, rectify. Like the antiparallel double stranded helical dimer (a possible minor conducting pathway) the parallel double stranded helical dimer has 28 interstrand hydrogen bonds, but its hydrogen bond network is quite distorted and it is much less stable. If it formed, its electrical potential profile suggests that it would be cation selective, bind anions preferentially if crystallizable, rectify, and at high enough voltages, might exhibit a conductance greater than that of the antiparallel form.     

Influence of acylation on the channel characteristics of gramicidin A.

The influence of acylation on the conductance, average duration, and channel-forming potency of channels formed by gramicidin A analogues was investigated using single-channel and multichannel techniques. Lauroyl-, myristoyl-, palmitoyl-, stearoyl-, and oleoylgramicidin A were prepared by covalent coupling of that fatty acid to the C-terminal ethanolamine group. Acylation of gramicidin A does not affect the single-channel conductance or the minichannel frequency in diphytanoylphosphatidylcholine/n-decane black lipid membranes. However, the average duration of all acylgramicidin channels was increased approximately 5-fold as compared to unmodified gramicidin A, which has a duration of 0.9 s at 200-mV applied potential. Somewhat surprisingly the rate of channel formation of the acylgramicidins is decreased relative to gramicidin A: lauroyl- and stearoylgramicidin are approximately 200 times less effective in channel formation as compared to gramicidin A. We conclude that channels formed by the acylgramicidins and by gramicidin A are structurally and conformationally equivalent.     

A study of the permeation of dihexadecyl phosphate vesicles by various anesthetics

A simple spectroscopic method for the evaluation of the effect that perturbers may have on a membrane model is described. The model was made from dihexadecyl phosphate (DHP) bilayers. The perturbers used were unconventional anesthetics (n-alcohols C1-C8; n-hexane and n-pentane) and conventional anesthetics (chloroform, methoxyflurane, halothane and enflurane). The results show a correlation between vesicle permeation by anesthetics and their clinical potency. Two modes of perturbation by which the anesthetics may induce vesicle permeation are proposed.     

Electric field effects on membranes: gramicidin A as a test ground

Electric fields due to transmembrane potential differences or ionic gradients across the membrane are presumably crucial for many reactions across membranes or close to membranes like signal transduction, control of ion channels or the generation of neural impulses. Molecular dynamics simulations have been used to study the influence of external electric fields on a mixed gramicidin/phospholipid bilayer system. At high field strengths, formation of membrane electropores occurred both close and distal to the gramicidin. Gramicidin was found to stabilize the membrane adjacent to the protein but also at larger distances of up to 2-3 nm. As a result, membrane pore formation was found to be significantly suppressed for the mixed gramicidin/DMPC system. Moderate field strengths only weakly affected the structure and dynamics of the gramicidin. Spontaneous potassium passage events in external electric fields were observed for both the head-to-head helical conformation as well as for the double helical conformation of gramicidin A. The double-helical conformation was found to facilitate ion passage compared to the head-to-head helical dimer.