The effect of cholesterol and gramicidin A′ on the carbonyl groups of dimyristoylphosphatidylcholine dispersions

Proton-enhanced carbon-13 magnetic resonance measurements have been made of the natural abundance carbon-13 carbons in hydrated L_α phase dispersions of 1,2-dimyristoyl-sn-glycero-3-phosphocholine (DMPC) codispersed with cholesterol or with the polypeptide gramicidin A′. The carbonyl group spectrum consists of a superposition of two peaks derived from the two carbonyl sites within the lipid. In the L_α phase of DMPC both carbonyl sites contribute axially symmetric spectra, one with a chemical shift anisotropy of –29 ppm and the other with a chemical shift anisotropy of less than –5 ppm. The chemical shift anisotropy of the broader carbonyl resonance was found to increase with increasing cholesterol content. However, in DMPC dispersions with gramicidin A′, the chemical shift anisotropy of the broader carbonyl signal initially increased slightly from that of pure DMPC and then decreased with increasing concentrations of gramicidin A′. The width of the narrower spectral component was essentially unaltered by cholesterol or gramicidin A′. The presence of a narrow component at all concentrations of cholesterol or gramicidin A′ suggests that it is unlikely that any significant conformational changes have occurred at the carbonyl level of the bilayer. We propose that the major effect of cholesterol or gramicidin A′ is to alter the molecular order parameter, S_mol, which reflects the range of angles through which the local molecular long axis of the phospholipid is tumbling.     

Determination of the structure of a membrane-incorporated ion channel. Solid-state nuclear magnetic resonance studies of gramicidin A.

Solid-state nuclear magnetic resonance (NMR) measurements on 13C-labeled analogues of the ion channel-forming peptide, gramicidin A, have been used to directly determine the structure of this peptide in lipid membranes. Seven gramicidin analogues, each labeled in a single carbonyl group of gly2, L-ala3, D-leu4, L-val7, D-leu10, D-leu12, or D-leu14 were synthesized by the solid-phase method. These gramicidin analogues were incorporated into aligned multilayers of dimyristoylphosphatidylcholine, or diether lipid bearing 14- or 16-carbon chains, at a 1:15 peptide:lipid mole ratio. Proton-enhanced, 13C, solid-state spectra were obtained at several temperatures and over a range of sample orientations with respect to the spectrometer magnetic field to permit accurate measurement of the chemical shift anisotropies. The observed anisotropies indicate that all of the labeled carbonyl bonds are oriented almost parallel to the molecular long axis and perpendicular to the lipid bilayer plane. These orientations are consistent with gramicidin forming a beta 6.3 single-strand helix that is oriented parallel to the methylene chains of the lipid molecules. Comparison of the linewidths from labeled residues that are in the innermost turn of the helix (gly2, ala3, and D-leu4), in the center of the molecule (val7), and in the turn nearest the lipid bilayer surface (D-leu10, D-leu12, and D-leu14) suggests that although the peptide behaves largely as a rigid barrel, segments of the peptide close to the membrane surface possess greater motional freedom.(ABSTRACT TRUNCATED AT 250 WORDS)     

Solid-state nuclear magnetic resonance evidence for an extended beta strand conformation of the membrane-bound HIV-1 fusion peptide.

Solid-state nuclear magnetic resonance (NMR) spectroscopy was applied to the membrane-bound form of a synthetic peptide representing the 23-residue N-terminal fusion peptide domain of the HIV-1 gp41 envelope glycoprotein. 1D solid-state NMR line width measurements of singly 13C carbonyl labeled peptides showed that a significant population of the membrane-bound peptide is well-structured in its N-terminal and central regions while the C-terminus has more disorder. There was some dependence of line width on lipid composition, with narrower line widths and hence greater structural order observed for a lipid composition comparable to that found in the virus and its target T cells. In the more ordered N-terminal and central regions of the peptide, the 13C carbonyl chemical shifts are consistent with a nonhelical membrane-bound conformation. Additional evidence for a beta strand membrane-bound conformation was provided by analysis of 2D rotor-synchronized magic angle spinning NMR spectra of doubly 13C carbonyl labeled peptides. Lipid mixing and aqueous contents leakage assays were applied to demonstrate the fusogenicity of the peptide under conditions comparable to those used for the solid-state NMR sample preparation.     

Gramicidin cation channel: an experimental determination of the right-handed helix sense and verification of beta-type hydrogen bonding

Due to the difficulty of obtaining protein/lipid cocrystals for diffraction studies, structural research on intrinsic membrane proteins and polypeptides has been largely restricted to indirect experimental techniques. Hence, many fundamental questions associated with peptide/lipid systems remain unanswered. In particular, the handedness of the gramicidin A transmembrane ion channel incorporated into lipid bilayers has been an open question for nearly two decades. In this study, solid-state 15N NMR spectroscopy is employed to probe directly the secondary structure of the polypeptide backbone. Recent determinations of the 15N chemical shift anisotropy tensor with respect to the molecular frame enable the quantitative evaluation of the 15N chemical shift resonances obtained from oriented dimyristoylphosphatidylcholine (DMPC) bilayer samples containing specific site 15N labeled gramicidin. This direct structural approach verifies the beta-sheet hydrogen-bonding pattern proposed by Urry [Urry, D. W. (1971) Proc. Natl. Acad. Sci. U.S.A. 68, 672-676] and determines that in our DMPC bilayer preparations the gramicidin channel is right-handed. Additional structural information is provided by the 15N chemical shift data in the form of orientational constraints on the C alpha-C alpha axis orientation of individual peptides relative to the helix axis. The significance of these solid-state NMR results lies in the direct determination of the helix sense and the verification of the beta-type hydrogen bonding, in the development of the solid-state NMR methods for obtaining such information, and in emphasizing the importance of having direct structural data at atomic resolution.     

Solubilization and localization of weakly polar lipids in unsonicated egg phosphatidylcholine: A 13C MAS NMR study

The weakly polar lipids cholesteryl ester, triacylglycerol, and diacylglycerol incorporate to a limited extent into the lamellar structure of small unilamellar vesicles. The localization of the carbonyl group(s) at the aqueous interface was detected by [13C]carbonyl chemical shift changes relative to the neat unhydrated lipid [Hamilton, J.A., & Small, D.M. (1981) Proc. Natl. Acad. Sci. U.S.A. 78, 6878-6882; Hamilton, J.A., & Small, D.M. (1982) J. Biol. Chem. 257, 7318-7321; Hamilton, J.A., Bhamidipati, S.B., Kodali, D.R., & Small, D.M. (1991) J. Biol. Chem. 266, 1177-1186]. This study uses 13C NMR to investigate the interactions of these lipids with unsonicated (multilamellar) phosphatidylcholine, a model system for cellular membranes and surfaces of emulsion particles with low curvature. Magic angle spinning reduced the broad lines of the unsonicated dispersions to narrow lines comparable to those from sonicated dispersions. [13C]Carbonyl chemical shifts revealed incorporation of the three lipids into the lamellar structure of the unsonicated phospholipids and a partial hydration of the carbonyl groups similar to that observed in small vesicles. Other properties of interfacial weakly polar lipids in multilayers were similar to those in small unilamellar bilayers. There is thus a general tendency of weakly polar lipids to incorporate at least to a small extent into the lamellar structure of phospholipids and take on interfacial properties that are distinct from their bulk-phase properties. This pool of surface-located lipid is likely to be directly involved in enzymatic transformations and protein-mediated transport. The 13C magic angle spinning NMR method may be generally useful for determining the orientation of molecules in model membranes.     

Induction of morphological changes in model lipid membranes and the mechanism of membrane disruption by a large scorpion-derived pore-forming peptide

The membrane disruption mechanism of pandinin 1 (pin1), an antimicrobial peptide isolated from the venom of the African scorpion, was studied using 31P, 13C, 1H solid-state and multidimensional solution-state NMR spectroscopy. A high-resolution NMR solution structure of pin1 showed that the two distinct alpha-helical regions move around the central hinge region, which contains Pro19. 31P NMR spectra of lipid membrane in the presence of pin1, at various temperatures, showed that pin1 induces various lipid phase behaviors depending on the acyl chain length and charge of phospholipids. Notably, it was found that pin1 induced formation of the cubic phase in shorter lipid membranes above Tm. Further, the 13C NMR spectra of pin1 labeled at Leu28 under magic angle spinning (MAS) indicated that the motion of pin1 bound to the lipid bilayer was very slow, with a correlation time of the order of 10(-3) s. 31P NMR spectra of dispersions of four saturated phosphatidyl-cholines in the presence of three types of pin1 derivatives, [W4A, W6A, W15A]-pin1, pin1(1-18), and pin1(20-44), at various temperatures demonstrated that all three pin1 derivatives have a reduced ability to trigger the cubic phase. 13C chemical shift values for pin1(1-18) labeled at Val3, Ala10, or Ala11 under static or slow MAS conditions indicate that pin1(1-18) rapidly rotates around the average helical axis, and the helical rods are inclined at approximately 30 degrees to the lipid long axis. 13C chemical shift values for pin1(20-44) labeled at Gly25, Leu28, or Ala31 under static conditions indicate that pin1(20-44) may be isotropically tumbling. 1H MAS chemical shift measurements suggest that pin1 is located at the membrane-water interface approximately parallel to the bilayer surface. Solid-state NMR results correlated well with the observed biological activity of pin1 in red blood cells and bacteria.     

The binding site of sodium in the gramicidin A channel: comparison of molecular dynamics with solid-state NMR data.

The location of the main binding site for sodium in the gramicidin A (GA) channel was investigated with molecular dynamics simulations, using an atomic model of the channel embedded in a fully hydrated dimyristoyl phosphatidycholine (DMPC) bilayer. Twenty-four separate simulations in which a sodium was restrained at different locations along the channel axis were generated. The results are compared with carbonyl 13C chemical shift anisotropy solid-state NMR experimental data previously obtained with oriented GA:DMPC samples. Predictions are made for other solid-state NMR properties that could be observed experimentally. The combined information from experiment and simulation strongly suggests that the main binding sites for sodium are near the channel's mouth, approximately 9.2 A from the center of the dimer channel. The 13C chemical shift anisotropy of Leu10 is the most affected by the presence of a sodium ion in the binding site. In the binding site, the sodium ion is lying off-axis, making contact with two carbonyl oxygens and two single-file water molecules. The main channel ligand is provided by the carbonyl group of the Leu10-Trp11 peptide linkage, which exhibits the largest deviation from the ion-free channel structure. Transient contacts with the carbonyl group of Val8 and Trp15 are also present. The influence of the tryptophan side chains on the channel conductance is examined based on the current information about the binding site.     

Low-temperature solid-state 13C NMR studies of the retinal chromophore in rhodopsin

Magic angle sample spinning (MASS) 13C NMR spectra have been obtained of bovine rhodopsin regenerated with retinal prosthetic groups isotopically enriched with 13C at C-5 and C-14. In order to observe the 13C retinal chromophore resonances, it was necessary to employ low temperatures (-15-----35 degrees C) to restrict rotational diffusion of the protein. The isotropic chemical shift and principal values of the chemical shift tensor of the 13C-5 label indicate that the retinal chromophore is in the twisted 6-s-cis conformation in rhodopsin, in contrast to the planar 6-s-trans conformation found in bacteriorhodopsin. The 13C-14 isotropic shift and shift tensor principal values show that the Schiff base C = N bond is anti. Furthermore, the 13C-14 chemical shift (121.2 ppm) is within the range of values (120-123 ppm) exhibited by protonated (C = N anti) Schiff base model compounds, indicating that the C = N linkage is protonated. Our results are discussed with regard to the mechanism of wavelength regulation in rhodopsin.     

13C solid-state NMR chemical shift anisotropy analysis of the anomeric carbon in carbohydrates

(13)C NMR solid-state structural analysis of the anomeric center in carbohydrates was performed on six monosaccharides: glucose (Glc), mannose (Man), galactose (Gal), galactosamine hydrochloride (GalN), glucosamine hydrochloride (GlcN), and N-acetyl-glucosamine (GlcNAc). In the 1D (13)C cross-polarization/magic-angle spinning (CP/MAS) spectrum, the anomeric center C-1 of these carbohydrates revealed two well resolved resonances shifted by 3-5ppm, which were readily assigned to the anomeric alpha and beta forms. From this experiment, we also extracted the (13)C chemical shift anisotropy (CSA) tensor elements of the two forms from their spinning sideband intensities, respectively. It was found out that the chemical shift tensor for the alpha anomer was more axially symmetrical than that of the beta form. A strong linear correlation was obtained when the ratio of the axial asymmetry of the (13)C chemical shift tensors of the two anomeric forms was plotted in a semilogarithmic plot against the relative population of the two anomers. Finally, we applied REDOR spectroscopy to discern whether or not there were any differences in the sugar ring conformation between the anomers. Identical two-bond distances of 2.57A (2.48A) were deduced for both the alpha and beta forms in GlcNAc (GlcN), suggesting that the two anomers have essentially identical sugar ring scaffolds in these sugars. In light of these REDOR distance measurements and the strong correlation observed between the ratio of the axial asymmetry parameters of the (13)C chemical shift tensors and the relative population between the two anomeric forms, we concluded that the anomeric effect arises principally from interaction of the electron charge clouds between the C-1-O-5 and the C-1-O-1 bonds in these monosaccharides.     

Conformation and Orientation of Gramicidin a in Oriented Phospholipid Bilayers Measured by Solid State Carbon-13 NMR

Three analogues of the helical ionophore gramicidin A have been synthesized with ¹³C-labeled carbonyls (¹³C=O) incorporated at either Gly², Ala³, or Val⁷. A fourth compound incorporated ¹³C at both the carbonyl and α-carbon of Gly² within the same molecule. These labels were studied using solid-state, proton-enhanced, ¹³C nuclear magnetic resonance (NMR) in hydrated dispersions of dimyristoylphosphatidylcholine (DMPC)-gramicidin A. The dispersions were aligned on glass coverslips whose orientation to the magnetic field could be varied through 180°. The orientation dependence of the NMR spectrum was used to obtain an accurate measurement of the ¹³C chemical shift anisotropy (CSA), and in the case of the fourth compound, the ¹³C—¹³C dipolar coupling constant. From the measured CSA and estimates of the orientation of the ¹³C shielding tensor, we are able to determine the direction of the ¹³C=O bonds and to compare these with the predictions of the various reported models for the configuration of gramicidin A in phospholipid bilayers. Our results are consistent with the left-handed ππ^6.3_LD single-stranded helix (Urry, D. W., J. T. Walker, and T. L. Trapane. 1982. J. Membr. Biol. 69:225-231). The right-handed ππ^6.3_LD single-stranded helix observed for gramicidin A in sodium dodecyl sulfate micelles (Arseniev, A. S., I. L. Barsukov, V. F. Bystrov, A. L. Loize, and Yu A. Ovchinnikov. 1985. FEBS (Fed. Eur. Biochem. Soc.) Lett. 186:168-174) yields a poorer fit to the data. However, the width of the carbonyl resonances suggests a distribution of molecular geometries possibly resulting from a spread in the helix pitch and handedness. Double-stranded helices and β sheet structures are excluded. In dispersions in which the lipid is in the L_α phase, the gramicidin A undergoes rapid reorientation about an axis which is centered on the normal to the plane of the coverslips. When the supporting lipid is in the L_β′ phase the helices are rigid on the timescale of ¹³C-NMR. The configuration of gramicidin A is unaltered by L_α-L_β′ phase transition of the bilayer lipid.     

Conformation and dynamics of melittin bound to magnetically oriented lipid bilayers by solid-state (31)P and (13)C NMR spectroscopy

The conformation and dynamics of melittin bound to the dimyristoylphosphatidylcholine (DMPC) bilayer and the magnetic orientation in the lipid bilayer systems were investigated by solid-state (31)P and (13)C NMR spectroscopy. Using (31)P NMR, it was found that melittin-lipid bilayers form magnetically oriented elongated vesicles with the long axis parallel to the magnetic field above the liquid crystalline-gel phase transition temperature (T(m) = 24 degrees C). The conformation, orientation, and dynamics of melittin bound to the membrane were further determined by using this magnetically oriented lipid bilayer system. For this purpose, the (13)C NMR spectra of site-specifically (13)C-labeled melittin bound to the membrane in the static, fast magic angle spinning (MAS) and slow MAS conditions were measured. Subsequently, we analyzed the (13)C chemical shift tensors of carbonyl carbons in the peptide backbone under the conditions where they form an alpha-helix and reorient rapidly about the average helical axis. Finally, it was found that melittin adopts a transmembrane alpha-helix whose average axis is parallel to the bilayer normal. The kink angle between the N- and C-terminal helical rods of melittin in the lipid bilayer is approximately 140 degrees or approximately 160 degrees, which is larger than the value of 120 degrees determined by x-ray diffraction studies. Pore formation was clearly observed below the T(m) in the initial stage of lysis by microscope. This is considered to be caused by the association of melittin molecules in the lipid bilayer.     

Structure and protein environment of the retinal chromophore in light- and dark-adapted bacteriorhodopsin studied by solid-state NMR

Our previous solid-state 13C NMR studies on bR have been directed at characterizing the structure and protein environment of the retinal chromophore in bR568 and bR548, the two components of the dark-adapted protein. In this paper, we extend these studies by presenting solid-state NMR spectra of light-adapted bR (bR568) and examining in more detail the chemical shift anisotropy of the retinal resonances near the ionone ring and Schiff base. Magic angle spinning (MAS) 13C NMR spectra were obtained of bR568, regenerated with retinal specifically 13C labeled at positions 12-15, which allowed assignment of the resonances observed in the dark-adapted bR spectrum. Of particular interest are the assignments of the 13C-13 and 13C-15 resonances. The 13C-15 chemical resonance for bR568 (160.0 ppm) is upfield of the 13C-15 resonance for bR548 (163.3 ppm). This difference is attributed to a weaker interaction between the Schiff base and its associated counterion in bR568. The 13C-13 chemical shift for bR568 (164.8 ppm) is close to that of the all-trans-retinal protonated Schiff base (PSB) model compound (approximately 162 ppm), while the 13C-13 resonance for bR548 (168.7 ppm) is approximately 7 ppm downfield of that of the 13-cis PSB model compound. The difference in the 13C-13 chemical shift between bR568 and bR548 is opposite that expected from the corresponding 15N chemical shifts of the Schiff base nitrogen and may be due to conformational distortion of the chromophore in the C13 = C14-C15 bonds.(ABSTRACT TRUNCATED AT 250 WORDS)     

The structural properties of the transmembrane segment of the integral membrane protein phospholamban utilizing (13)C CPMAS, (2)H, and REDOR solid-state NMR spectroscopy

Solid-state NMR spectroscopic techniques were used to investigate the secondary structure of the transmembrane peptide phospholamban (TM-PLB), a sarcoplasmic Ca(2+) regulator. (13)C cross-polarization magic angle spinning spectra of (13)C carbonyl-labeled Leu39 of TM-PLB exhibited two peaks in a pure 1-palmitoyl-2-oleoyl-phosphocholine (POPC) bilayer, each due to a different structural conformation of phospholamban as characterized by the corresponding (13)C chemical shift. The addition of a negatively charged phospholipid (1-palmitoyl-2-oleoylphosphatidylglycerol (POPG)) to the POPC bilayer stabilized TM-PLB to an alpha-helical conformation as monitored by an enhancement of the alpha-helical carbonyl (13)C resonance in the corresponding NMR spectrum. (13)C-(15)N REDOR solid-state NMR spectroscopic experiments revealed the distance between the (13)C carbonyl carbon of Leu39 and the (15)N amide nitrogen of Leu42 to be 4.2+/-0.2A indicating an alpha-helical conformation of TM-PLB with a slight deviation from an ideal 3.6 amino acid per turn helix. Finally, the quadrupolar splittings of three (2)H labeled leucines (Leu28, Leu39, and Leu51) incorporated in mechanically aligned DOPE/DOPC bilayers yielded an 11 degrees +/-5 degrees tilt of TM-PLB with respect to the bilayer normal. In addition to elucidating valuable TM-PLB secondary structure information, the solid-state NMR spectroscopic data indicates that the type of phospholipids and the water content play a crucial role in the secondary structure and folding of TM-PLB in a phospholipid bilayer.     

The interfacial conformation and transbilayer movement of diacylglycerols in phospholipid bilayers

The interaction of diacylglycerols, primarily 1,2-dilauroyl-sn-glycerol (1,2-DLG), with egg phosphatidylcholine (PC) bilayers was studied by NMR spectroscopy and other physical techniques. In the low proportions used (less than or equal to 20 mol % with respect to total lipid), 1,2-DLG formed bilayers with PC with no hexagonal phase separation, as assessed by light, polarizing and electron microscopy, and 31P and 13C NMR spectroscopy. The 13C-carbonyl chemical shift of 90% [13C]carbonyl 1,2-DLG was monitored in small unilamellar vesicles as a function of relative DLG content (1.5-20%) and temperature (10-55 degrees C). The chemically inequivalent sn-1 and sn-2 carbonyls gave a single, narrow resonance in vesicles, in contrast to neat 1,2-DLG and 1,2-DLG in organic solvents, whose spectra showed two well-separated carbonyl resonances. The chemical shift of 1,2-DLG in PC shows that the carbonyl groups are proximal to the aqueous interface, necessitating orientation of the DLG molecule along the normal to the bilayer. Both carbonyl groups are H-bonded to H2O, but the secondary ester (sn-2) carbonyl is relatively more hydrated than the primary ester (sn-1) carbonyl. The 13C-carbonyl chemical shift data further suggest that the interfacial conformation resembles that of crystalline and liquid crystalline lamellar 1,2-dilauroyl-sn-glycero-3-phosphatidylethanolamine and certain PCs, in which the glycerol backbone is perpendicular to the bilayer plane. This conformation is different from that of crystalline 1,2-dilauroyl-sn-glycerol, in which the glycerol backbone is parallel to the bilayer plane. Between 1.5 and 8% DLG in vesicles, the chemical shift of the 1,2-DLG carbonyl at a given temperature was constant. However, above 8% DLG the chemical shift at each temperature increased with increasing DLG concentration, suggesting increased hydration at higher DLG content. At low temperatures 13C NMR spectra of vesicles with the highest proportions of 1,2-DLG studied (15 and 20%) showed two DLG carbonyl resonances, which most likely represent 1,2-DLG on outer and inner leaflets of the vesicle bilayer. The two peaks collapsed into a single resonance by 38 degrees C, at which temperature the two environments equilibrate with a rate constant of approximately 60 s-1 (t1/2 approximately 10 ms). Thus, transbilayer movement of DLG is extremely fast compared with phospholipids. In vesicles the 1,3-isomer of DLG exhibited a narrow carbonyl peak slightly downfield from that of 1,2-DLG. Acyl chain migration from 1,2-DLG to 1,3-DLG was monitored directly in the vesicle by time-dependent NMR measurements.     

NMR observation of gramicidin A' in phosphatidylcholine vesicles.

Dimyristoyl phosphatidylcholine was prepared with perdeuterated hydrocarbon chains and sonicated into bilayer vesicles together with gramicidin A'. The 1H NMR resonance from the tryptophan residues in the gramicidin has a linewidth of approximately 80 Hz, indicating significant local mobility for these residues. Paramagnetic lanthanides added to the aqueous medium cause a chemical shift of this signal indicating that some of the tryptophans may be located in the interfacial region of the bilayer.     

Solid state NMR studies of hydrogen bonding in a citrate synthase inhibitor complex.

The ionization state and hydrogen bonding environment of the transition state analogue (TSA) inhibitor, carboxymethyldethia coenzyme A (CMX), bound to citrate synthase have been investigated using solid state NMR. This enzyme-inhibitor complex has been studied in connection with the postulated contribution of short hydrogen bonds to binding energies and enzyme catalysis: the X-ray crystal structure of this complex revealed an unusually short hydrogen bond between the carboxylate group of the inhibitor and an aspartic acid side chain [Usher et al. (1994) Biochemistry 33, 7753-7759]. To further investigate the nature of this short hydrogen bond, low spinning speed 13C NMR spectra of the CMX-citrate synthase complex were obtained under a variety of sample conditions. Tensor values describing the chemical shift anisotropy of the carboxyl groups of the inhibitor were obtained by simulating MAS spectra (233 +/- 4, 206 +/- 5, and 105 +/- 2 ppm vs TMS). Comparison of these values with our previously reported database and ab initio calculations of carbon shift tensor values clearly indicates that the carboxyl is deprotonated. New data from model compounds suggest that hydrogen bonds in a syn arrangement with respect to the carboxylate group have a pronounced effect upon the shift tensors for the carboxylate, while anti hydrogen bonds, regardless of their length, apparently do not perturb the shift tensors of the carboxyl group. Thus the tensor values for the enzyme-inhibitor complex could be consistent with either a very long syn hydrogen bond or an anti hydrogen bond; the latter would agree very well with previous crystallographic results. Two-dimensional 1H-13C heteronuclear correlation spectra of the enzyme-inhibitor complex were obtained. Strong cross-peaks were observed from the carboxyl carbon to proton(s) with chemical shift(s) of 22 +/- 5 ppm. Both the proton chemical shift and the intensity of the cross-peak indicate a very short hydrogen bond to the carboxyl group of the inhibitor, the C.H distance based upon the cross-peak intensity being 2.0 +/- 0.4 A. This proton resonance is assigned to Hdelta2 of Asp 375, on the basis of comparison with crystal structures and the fact that this cross-peak was absent in the heteronuclear correlation spectrum of the inhibitor-D375G mutant enzyme complex. In summary, our NMR studies support the suggestion that a very short hydrogen bond is formed between the TSA and the Asp carboxylate.     

Solid-state 13C-NMR studies of the effects of sodium ions on the gramicidin A ion channel.

End-to-end helical dimers of gramicidin A form transmembrane pores in lipid bilayers, through which monovalent ions may pass. The groups within the peptide that interact with these ions have been studied by application of solid-state spectroscopic methods to a series of gramicidin A analogues synthesized with 13C in selected peptide carbonyl groups. The resonances of D-Leu10, D-Leu12 and D-Leu14 analogues were perturbed in the presence of 0.16 M sodium ions, whereas the resonances of the carbonyls of Gly2, Ala3, D-Leu4 and Val7, which are closer to the formylated N-terminal end of the peptide, were unaffected. The observed changes in chemical shift anisotropy are indicative of a change in orientation of the abovementioned leucine carbonyls.     

13C NMR spectroscopy of labeled pyridoxal 5'-phosphate. Model studies, D-serine dehydratase, and L-glutamate decarboxylase.

Pyridoxal 5'-phosphate labeled to the extent of 90% with 13C in the 4' (aldehyde) and 5' (methylene) positions has been synthesized. 13C NMR spectra of this material and of natural abundance pyridoxal 5'-phosphate are reported, as well as 13C NMR spectra of the Schiff base formed by reaction of pyridoxal 5'-phosphate with n-butylamine, the secondary amine formed by reduction of this Schiff base, the thiazolidine formed by reaction of pyridoxal 5'-phosphate with cysteine, the hexahydropyrimidine formed by reaction of pyridoxal 5'-phosphate with 1,3-diaminobutane, and pyridoxamine 5'-phosphate. The range of chemical shifts for carbon 4' in these compounds is more than 100 ppm, and thus this chemical shift is expected to be a sensitive indicator of structure in enzyme-bound pyridoxal 5'-phosphate. The chemical shift of carbon 5', on the other hand, is insensitive to these structure changes. 13C NMR spectra have been obtained at pH 7.8 and 9.4 for D-serine dehydratase (Mr = 46,000) containing natural abundance pyridoxal 5'-phosphate and containing 13C-enriched pyridoxal 5'-phosphate. The enriched material contains two new resonances not present in the natural abundance material, one at 167.7 ppm with a linewidth of approximately 24 Hz, attributed to carbon 4' of the Schiff base in the bound coenzyme, and one at 62.7 Hz with a linewidth of approximately 48 Hz attributed to carbon 5' of the bound Schiff base. A large number of resonances due to individual amino acids are assigned. The NMR spectrum changes only slightly when the pH is raised to 9.4. The widths of the two enriched coenzyme resonances indicate that the coenzyme is rather rigidly bound to the enzyme but probably has limited motional freedom relative to the protein. 13C NMR spectra have been obtained for L-glutamate decarboxylase containing natural abundance pyridoxal 5'-phosphate and 13C-enriched pyridoxal 5'-phosphate. Under conditions where the two enriched 13C resonances are clearly visible in D-serine dehydratase, no resonances are visible in enriched L-glutamate decarboxylase, presumably because the coenzyme is rigidly bound to the protein and the 300,000 molecular weight of this enzyme produces very short relaxation times for the bound coenzyme and thus very broad lines.     

Solid-state 13C NMR detection of a perturbed 6-s-trans chromophore in bacteriorhodopsin

Solid-state 13C magic angle sample spinning NMR spectroscopy has been used to study the ionone ring portion of the chromophore of bacteriorhodopsin. Spectra were obtained from fully hydrated samples regenerated with retinals 13C labeled at positions C-5, C-6, C-7, C-8, and C-18 and from lyophilized samples regenerated with retinals labeled at C-9 and C-13. C-15-labeled samples were studied in both lyophilized and hydrated forms. Three independent NMR parameters (the downfield element of the C-5 chemical shift tensor, the C-8 isotropic chemical shift, and the C-18 longitudinal relaxation time) indicate that the chromophore has a 6-s-trans conformation in the protein, in contrast to the 6-s-cis conformation that is energetically favored for retinoids in solution. We also observe an additional 27 ppm downfield shift in the middle element of the C-5 shift tensor, which provides support for the existence of a negatively charged protein residue near C-5. Evidence for a positive charge near C-7, possibly the counterion for the negative charge, is also discussed. On the basis of these results, we present a new model for the retinal binding site, which has important implications for the mechanism of the "opsin shift" observed in bacteriorhodopsin.