Fourier transform infrared evidence for a predominantly alpha-helical structure of the membrane bound channel forming COOH-terminal peptide of colicin E1.

The structure of the membrane bound state of the 178-residue thermolytic COOH-terminal channel forming peptide of colicin E1 was studied by polarized Fourier transform infrared (FTIR) spectroscopy. This fragment was reconstituted into DMPC liposomes at varying peptide/lipid ratios ranging from 1/25-1/500. The amide I band frequency of the protein indicated a dominant alpha-helical secondary structure with limited beta- and random structures. The amide I and II frequencies are at 1,656 and 1,546 cm-1, close to the frequency of the amide I and II bands of rhodopsin, bacteriorhodopsin and other alpha-helical proteins. Polarized FTIR of oriented membranes revealed that the alpha-helices have an average orientation less than the magic angle, 54.6 degrees, relative to the membrane normal. Almost all of the peptide groups in the membrane-bound channel protein undergo rapid hydrogen/deuterium (H/D) exchange. These results are contrasted to the alpha-helical membrane proteins, bacteriorhodopsin, and rhodopsin.     

Re-examination of rhodopsin structure by hydrogen exchange

The hydrogen exchange behavior of rhodopsin was re-examined by studies of the protein in the disc membrane and after solubilization in octyl glucoside. The methods used measure either the peptide hydrogens alone (hydrogen-deuterium exchange by infrared spectroscopy) or all slowly exchanging hydrogens (hydrogen-tritium exchange by hel filtration). Under mild exchange conditions, disc membranes and solubilized lipid-free proteins show very similar exchange behavior, indicating the absence of slowly exchanging lipid protons. At high temperature, exchange of an additional large group of very slow peptide NH can be detected. The total number of slow hydrogens significantly exceeds the amide content, and apparently includes slowly exchanging protons from perhaps 40% of the protein's non-amide side chains. This is thought to require the involvement of many polar side chains in internal H-bonding. The exchange rates of the non-amide side chains sites have not been determined. However, to the extent that these contribute to the fast time region of the measured kinetic H-exchange curve, previously identified with exposed, non-H-bonded peptides, the estimate of freely exposed rhodopsin peptides must be reduced. The fraction of free peptides could range from a remarkably high value of 70% down to about 45%.     

Photoactivation of rhodopsin causes an increased hydrogen-deuterium exchange of buried peptide groups.

A key step in visual transduction is the light-induced conformational changes of rhodopsin that lead to binding and activation of the G-protein transducin. In order to explore the nature of these conformational changes, time-resolved Fourier transform infrared spectroscopy was used to measure the kinetics of hydrogen/deuterium exchange in rhodopsin upon photoexcitation. The extent of hydrogen/deuterium exchange of backbone peptide groups can be monitored by measuring the integrated intensity of the amide II and amide II' bands. When rhodopsin films are exposed to D2O in the dark for long periods, the amide II band retains at least 60% of its integrated intensity, reflecting a core of backbone peptide groups that are resistant to H/D exchange. Upon photoactivation, rhodopsin in the presence of D2O exhibits a new phase of H/D exchange which at 10 degrees C consists of fast (time constant approximately 30 min) and slow (approximately 11 h) components. These results indicate that photoactivation causes buried portions of the rhodopsin backbone structure to become more accessible.     

Structural basis of human erythrocyte glucose transporter function in reconstituted system. Hydrogen exchange

Hydrogen exchange kinetic behavior of human erythrocyte glucose transporter protein in vesicles was studied in the absence and in the presence of D-glucose or a well known inhibitor, cytochalasin B. This is to detect a proposed channel of water penetrating into the protein through which the sugar molecule passes and to monitor any conformational changes induced by the substrate or inhibitor. Analyses of the kinetic data revealed several classes of hydrogens which exchange with readily distinguishable rates. Of 660 hydrogens detected per transporter, approximately 30% exchanged with rates generally characterized as those of free amide hydrogens indicating they are interfaced to solvent water. Since the transporter is known to be embedded deep in the hydrophobic area of the membrane with minimum exposure to the outside of the membrane lipid bilayer, a significant portion of these free amide hydrogens must be at the purported channel rather than outside of the membrane. D-Glucose and cytochalasin B affected the exchange kinetics of these presumably channel-associated free amide hydrogens rather differently. D-Glucose reduced the apparent rate constants, but not the total number. Cytochalasin B on the other hand reduced the total number to one-half without significantly changing the apparent rate constants. The remaining 70% of the labeled hydrogens exchanged with much slower rates which vary 10-10,000-fold, indicating that they are internally structured peptide amide and side chain hydrogens. Both D-glucose and cytochalasin B further reduced the rates of these hydrogens, indicating a global stabilization of the protein structure.     

Infrared spectroscopic study of photoreceptor membrane and purple membrane. Protein secondary structure and hydrogen deuterium exchange

Infrared spectroscopy in the interval from 1800 to 1300 cm-1 has been used to investigate the secondary structure and the hydrogen/deuterium exchange behavior of bacteriorhodopsin and bovine rhodopsin in their respective native membranes. The amide I' and amide II' regions from spectra of membrane suspensions in D2O were decomposed into constituent bands by use of a curve-fitting procedure. The amide I' bands could be fit with a minimum of three theoretical components having peak positions at 1664, 1638, and 1625 cm-1 for bacteriorhodopsin and 1657, 1639, and 1625 cm-1 for rhodopsin. For both of these membrane proteins, the amide I' spectrum suggests that alpha-helix is the predominant form of peptide chain secondary structure, but that a substantial amount of beta-sheet conformation is present as well. The shape of the amide I' band was pH-sensitive for photoreceptor membranes, but not for purple membrane, indicating that membrane-bound rhodopsin undergoes a conformation change at acidic pH. Peptide hydrogen exchange of bacteriorhodopsin and rhodopsin was monitored by observing the change in the ratio of integrated absorbance (Aamide II'/Aamide I') during the interval from 1.5 to 25 h after membranes were introduced into buffered D2O. The fraction of peptide groups in a very slowly exchanging secondary structure was estimated to be 0.71 for bacteriorhodopsin at pD 7. The corresponding fraction in vertebrate rhodopsin was estimated to be less than or equal to 0.60. These findings are discussed in relationship to previous studies of hydrogen exchange behavior and to structural models for both proteins.     

Structure and orientation of a G protein fragment in the receptor bound state from residual dipolar couplings

Residual dipolar couplings for a ligand that is in fast exchange between a free state and a state where it is bound to a macroscopically ordered membrane protein carry precise information on the structure and orientation of the bound ligand. The couplings originate in the bound state but can be detected on the free ligand using standard high resolution NMR. This approach is used to study an analog of the C-terminal undecapeptide of the alpha-subunit of the heterotrimeric G protein transducin when bound to photo-activated rhodopsin. Rhodopsin is the major constituent of disk-shaped membrane vesicles from rod outer segments of bovine retinas, which align spontaneously in the NMR magnet. Photo-activation of rhodopsin triggers transient binding of the peptide, resulting in measurable dipolar contributions to 1J(NH) and 1J(CH) splittings. These dipolar couplings report on the time-averaged orientation of bond vectors in the bound peptide relative to the magnetic field, i.e. relative to the membrane normal. Approximate distance restraints of the bound conformation were derived from transferred NOEs, as measured from the difference of NOESY spectra recorded prior to and after photo-activation. The N-terminal eight residues of the bound undecapeptide adopt a near-ideal alpha-helical conformation. The helix is terminated by an alpha(L) type C-cap, with Gly9 at the C' position in the center of the reverse turn. The angle between the helix axis and the membrane normal is 40 degrees (+/-4) degrees. Peptide protons that make close contact with the receptor are identified by analysis of the NOESY cross-relaxation pattern and include the hydrophobic C terminus of the peptide.     

Cyclic GMP and photoreceptor function.

A single photon can be detected by a rod photoreceptor cell. The absorption of light by rhodopsin triggers a cascade of reactions that amplifies the photon signal and results in ion channel closure with hyperpolarization of the rod photoreceptor cell. Light-induced conformational changes in rhodopsin facilitate the binding of a guanosine nucleotide-binding protein, transducin, which then undergoes a GTP-GDP exchange reaction and dissociation of the transducin complex. A subunit of transducin then activates a phosphodiesterase complex that hydrolyzes cyclic GMP. In darkness, cyclic GMP binds to cation channels of the photoreceptor plasma membrane, maintaining them in an open configuration. The light-induced reduction in cyclic GMP concentration dissociates the bound cyclic GMP, resulting in channel closure and hyperpolarization. Down-regulation of the cascade involves other proteins that block the interaction of transducin with rhodopsin and another protein that may interfere with transducin recycling. Cone photoreceptors possess a light-activated cascade that follows the rod format, but it is composed of proteins that are homologous to those of rod photoreceptors. Phototransduction in invertebrate photoreceptors uses rhodopsin to activate a cascade that uses phosphoinositides and calcium ion to regulate membrane polarization.     

Hydrogen exchange/electrospray ionization mass spectrometry studies of structural features of proteins and protein/protein interactions

The rate at which amide hydrogens located at the peptide backbone in protein/protein complexes undergo hydrogen/deuterium exchange is highly dependent on whether the amide groups participate in binding. Here, a new mass spectrometric method is presented in which this effect is utilized for the characterization of protein/ligand binding sites. The information obtained is which region within the protein participates in binding. The method includes hydrogen/deuterium exchange of receptor and ligand protein amide protons, binding, and back exchange. After this procedure those backbone amide groups that participate in protein binding are protected from back exchange and therefore still deuterated. These regions were then identified by peptic proteolysis, fast microbore high-performance liquid chromatography separation, and electrospray ionization mass spectrometry. The approach has been applied to the investigation of structural features of insulin-like growth factor I (IGF-I) and the interaction of insulin-like growth factor I with IGF-I binding protein 1. The data show that the approach can provide information on the location of the hydrophobic core of IGF-1 and on two regions that are mainly involved in binding to IGF-I binding protein 1. The data are consistent with results obtained with other approaches. The amount of sample required for one experiment is in the subnanomolar range.     

A neutron Laue diffraction study of endothiapepsin: implications for the aspartic proteinase mechanism.

Current proposals for the catalytic mechanism of aspartic proteinases are largely based on X-ray structures of bound oligopeptide inhibitors possessing nonhydrolyzable analogues of the scissile peptide bond. However, the positions of protons on the catalytic aspartates and the ligand in these complexes have not been determined with certainty. Thus, our objective was to locate crucial protons at the active site of an inhibitor complex since this will have major implications for a detailed understanding of the mechanism of action. We have demonstrated that high-resolution neutron diffraction data can be collected from crystals of the fungal aspartic proteinase endothiapepsin bound to a transition state analogue (H261). The neutron structure of the complex has been refined at a resolution of 2.1 A to an R-factor of 23.5% and an R(free) of 27.4%. This work represents the largest protein structure studied to date by neutron crystallography at high resolution. The neutron data demonstrate that 49% of the main chain nitrogens have exchanged their hydrogen atoms with D2O in the mother liquor. The majority of residues resisting exchange are buried within core beta-sheet regions of the molecule. The neutron maps confirm that the protein has a number of buried ionized carboxylate groups which are likely to give the molecule a net negative charge even at very low pH, thereby accounting for its low pI. The functional groups at the catalytic center have clearly undergone H-D exchange despite being buried by the inhibitor occupying the active site cleft. Most importantly, the data provide convincing evidence that Asp 215 is protonated and that Asp 32 is the negatively charged residue in the transition state complex. This has an important bearing on mechanistic proposals for this class of proteinase.     

Hydrogen kinetics of peptide amide protons at the bovine pancreatic trypsin inhibitor protein-solvent interface

Hydrogen exchange rate constants of the 25 most rapidly exchanging peptide amide protons in bovine pancreatic trypsin inhibitor have been determined over a range of pH that spans pH min, the pH of minimum rate. Most of these are on the protein surface, exposed to solvent and not hydrogen bonded in the crystal structure. Contrary to commonly held assumptions, the exchange kinetics of surface NH groups are not equivalent to the kinetics of NH groups in peptides in the extended configuration. All surface NH groups exchange more slowly than NH groups in model peptides, with rate constants distributed over a range of more than two orders of magnitude. In addition, their pH min values vary widely. For most of the surface NH groups, pH min is lower than in model compounds and, for several, pH min is less than 1. These results indicate that the local environment of the surface peptide groups when the exchange event occurs is very different from that of extended peptides. Analysis based on consideration of an O-protonation mechanism for acid catalysis and of electrostatic effects on exchange kinetics further indicates (see the accompanying paper) that, in general, exchange of surface NH groups occurs from a conformation of the protein approximated by the crystal structure. The 1H-2H exchange rate constants were measured from 300 MHz nuclear magnetic resonance spectra in which assigned surface N1H resonances are resolved by the use of partially deuterated protein samples. A marked pH dependence of the chemical shifts observed in the pH range 1 to 4.5 for several surface NH groups reflects the titration of nearby carboxyl groups.     

Nuclear magnetic resonance studies of the internal dynamics in Apo, (Cd2+)1 and (Ca2+)2 calbindin D9k. The rates of amide proton exchange with solvent.

The backbone dynamics of the EF-hand Ca(2+)-binding protein, calbindin D9k, has been investigated in the apo, (Cd2+)1 and (Ca2+)2 states by measuring the rate constants for amide proton exchange with solvent. 15N-1H correlation spectroscopy was utilized to follow direct 1H-->2H exchange of the slowly exchanging amide protons and to follow indirect proton exchange via saturation transfer from water to the rapidly exchanging amide protons. Plots of experimental rate constants versus intrinsic rate constants have been analyzed to give qualitative insight into the opening modes of the protein that lead to exchange. These results have been interpreted within the context of a progressive unfolding model, wherein hydrophobic interactions and metal chelation serve to anchor portions of the protein, thereby damping fluctuations and retarding amide proton exchange. The addition of Ca2+ or Cd2+ was found to retard the exchange of many amide protons observed to be in hydrogen-bonding environments in the crystal structure of the (Ca2+)2 state, but not of those amide protons that were not involved in hydrogen bonds. The largest changes in rate constant occur for residues in the ion-binding loops, with substantial effects also found for the adjacent residues in helices I, II and III, but not helix IV. The results are consistent with a reorganization of the hydrogen-bonding networks in the metal ion-binding loops, accompanied by a change in the conformation of helix IV, as metal ions are chelated. Further analysis of the results obtained for the three states of metal occupancy provides insight into the nature of the changes in conformational fluctuations induced by ion binding.     

Proton magnetic resonance study of the influence of heme 2,4 substituents on the exchange rates of labile protons in the heme pocket of myoglobin.

Four exchangeable protons with large hyperfine shifts are assigned in the heme pocket of sperm whale met-cyano myoglobin reconstituted with heme possessing acetyl groups, ethyl groups, bromines, and hydrogens at the 2,4 position, using both relaxation and chemical-shift data. The four protons arise from the ring NH's of the proximal (F8), distal (E7), and FG2 histidines, and the peptide NH of His F8. The similarity of all chemical shifts to those of the native protein as well as the invariance of the relaxation rates of the distal histidyl ring NH dictate essentially the same structure for the heme cavity of both native and reconstituted proteins. The exchange rates with bulk water of the four labile proteins in each modified protein were determined by saturation-transfer and line width methods. All four labile protons were found to have the same exchange rate as in the native protein for acetyl and ethyl 2,4 substituents; the two resolved labile protons in the derivative with 2,4 bromine were also unchanged. The reconstituted protein with hydrogens at the 2,4 position exhibited slower exchange rates for three of the four protons, indicating an increased dynamic stability of the heme pocket in the absence of bulky 2,4 substituents.     

Water and polypeptide conformations in the gramicidin channel. A molecular dynamics study.

Theoretical studies of ion channels address several important questions. The mechanism of ion transport, the role of water structure, the fluctuations of the protein channel itself, and the influence of structural changes are accessible from these studies. In this paper, we have carried out a 70-ps molecular dynamics simulation on a model structure of gramicidin A with channel waters. The backbone of the protein has been analyzed with respect to the orientation of the carbonyl and the amide groups. The results are in conformity with the experimental NMR data. The structure of water and the hydrogen bonding network are also investigated. It is found that the water molecules inside the channel act as a collective chain; whereas the conformation in which all the waters are oriented with the dipoles pointing along the axis of the channel is a preferred one, others are also accessed during the dynamics simulation. A collective coordinate involving the channel waters and some of the hydrogen bonding peptide partners is required to describe the transition of waters from one configuration to the other.     

GuHCl and NaCl-dependent hydrogen exchange in MerP reveals a well-defined core with an unusual exchange pattern

We have analysed hydrogen exchange at amide groups to characterise the energy landscape of the 72 amino acid residue protein MerP. From the guanidine hydrochloride (GuHCl) dependence of exchange in the pre-transitional region we have determined free energy values of exchange (DeltaG(HX)) and corresponding m-values for individual amide protons. Detailed analysis of the exchange patterns indicates that for one set of amide protons there is a weak dependence on denaturant, indicating that the exchange is dominated by local fluctuations. For another set of amide protons a linear, but much stronger, denaturant dependence is observed. Notably, the plots of free energy of exchange versus [GuHCl] for 16 amide protons show pronounced upward curvature, and a close inspection of the structure shows that these residues form a well-defined core in the protein. The hydrogen exchange that was measured at various concentrations of NaCl shows an apparent selective stabilisation of this core. Detailed analysis of this exchange pattern indicates that it may originate from selective destabilisation of the unfolded state by guanidinium ions and/or selective stabilisation of the core in the native state by chloride ions.     

Hydrogen exchange study of membrane-bound rhodopsin. II. Light-induced protein structure change.

Hydrogen exchange studies of rhodopsin in disc membranes demonstrated that photolysis induces changes in the protein itself. Two different altered forms were detected. A late photointermediate in the bleaching sequence, which can be identified with metarhodopsin II, displays accelerated exchange. Subsequently, at the stage of fully bleached opsin, exchange becomes even slower than in rhodopsin. These changes involve only a small fraction of the protein's internally hydrogen-bonded peptide groups. The unusually large fraction of exposed peptide hydrogens observed previously for rhodopsin is unaltered in the photolyzed forms.     

Microscopic stability of cold shock protein A examined by NMR native state hydrogen exchange as a function of urea and trimethylamine N-oxide

Native state hydrogen exchange of cold shock protein A (CspA) has been characterized as a function of the denaturant urea and of the stabilizing agent trimethylamine N-oxide (TMAO). The structure of CspA has five strands of beta-sheet. Strands beta1-beta4 have strongly protected amide protons that, based on experiments as a function of urea, exchange through a simple all-or-none global unfolding mechanism. By contrast, the protection of amide protons from strand beta5 is too weak to measure in water. Strand beta5 is hydrogen bonded to strands beta3 and beta4, both of which afford strong protection from solvent exchange. Gaussian network model (GNM) simulations, which assume that the degree of protection depends on tertiary contact density in the native structure, accurately predict the strong protection observed in strands beta1-beta4 but fail to account for the weak protection in strand beta5. The most conspicuous feature of strand beta5 is its low sequence hydrophobicity. In the presence of TMAO, there is an increase in the protection of strands beta1-beta4, and protection extends to amide protons in more hydrophilic segments of the protein, including strand beta5 and the loops connecting the beta-strands. TMAO stabilizes proteins by raising the free energy of the denatured state, due to highly unfavorable interactions between TMAO and the exposed peptide backbone. As such, the stabilizing effects of TMAO are expected to be relatively independent of sequence hydrophobicity. The present results suggest that the magnitude of solvent exchange protection depends more on solvent accessibility in the ensemble of exchange susceptible conformations than on the strength of hydrogen-bonding interactions in the native structure.     

A membrane cell for on-line hydrogen/deuterium exchange to study protein folding and protein-protein interactions by mass spectrometry

A membrane cell for hydrogen and deuterium exchange on-line with mass spectrometry has been developed to monitor protein-protein interactions and protein conformations. It consists of two channels separated by a semipermeable membrane, where one channel carries the protein sample and the other deuterium oxide. The membrane allows transfer of deuterium oxide into the sample flow. The labeling time is controlled via the flow rate in the sample channel. This cell was validated against three models commonly used in hydrogen-deuterium exchange mass spectrometry: monitoring of folded and unfolded states in a protein, mapping the protein secondary structure at the peptide level, and detection of protein and antibody interactions. The system avoids the conventionally used sample dilution and handling, allowing for potential automation.     

Rapid amide proton exchange rates in peptides and proteins measured by solvent quenching and two-dimensional NMR.

In an effort to develop a more versatile quenched hydrogen exchange method for studies of peptide conformation and protein-ligand interactions, the mechanism of amide proton exchange for model peptides in DMSO-D2O mixtures was investigated by NMR methods. As in water, H-D exchange rates in the presence of 90% or 95% DMSO exhibit characteristic acid- and base-catalyzed processes and negligible water catalysis. However, the base-catalyzed rate is suppressed by as much as four orders of magnitude in 95% DMSO. As a result, the pH at which the exchange rate goes through a minimum is shifted up by about two pH units and the minimum exchange rate is approximately 100-fold reduced relative to that in D2O. The solvent-dependent decrease in base-catalyzed exchange rates can be attributed primarily to a large increase in pKa values for the NH group, whereas solvent effects on pKW seem less important. Addition of toluene and cyclohexane resulted in improved proton NMR chemical shift dispersion. The dramatic reduction in exchange rates observed in the solvent mixture at optimal pH makes it possible to apply 2D NMR for NH exchange measurements on peptides under conditions where rates are too rapid for direct NMR analysis. To test this solvent-quenching method, melittin was exchanged in D2O (pH 3.2, 12 degrees C), aliquots were quenched by rapid freezing, lyophilized, and dissolved in quenching buffer (70% DMSO, 25% toluene, 4% D2O, 1% cyclohexane, 75 mM dichloroacetic acid) for NMR analysis. Exchange rates for 21 amide protons were measured by recording 2D NMR spectra on a series of samples quenched at different times. The results are consistent with a monomeric unfolded conformation of melittin at acidic pH. The ability to trap labile protons by solvent quenching makes it possible to extend amide protection studies to peptide ligands or labile protons on the surface of a protein involved in macromolecular interactions.     

Interactions of antibody aromatic residues with a peptide of cholera toxin observed by two-dimensional transferred nuclear Overhauser effect difference spectroscopy

The interactions between a peptide of cholera toxin and the aromatic amino acids of the TE33 antipeptide antibody, cross-reactive with the toxin, have been studied by NOESY difference spectroscopy. The 2D difference between the NOESY spectrum of the Fab with a 4-fold excess of the peptide and that of the peptide-saturated Fab reveals cross-peaks growing with excess of the peptide. These cross-peaks are due to magnetization transfer between the Fab and neighboring bound peptide protons, and a further transfer to the free peptide protons by exchange between bound and free peptide (transferred NOE). Additional cross-peaks appearing in the difference spectrum are due to a combination of intramolecular interactions between bound peptide protons and exchange between bound and free peptide. Assignment of cross-peaks is attained by specific deuteration of antibody aromatic amino acids using also the resonance assignment of the free peptide, deduced from the COSY spectrum of the peptide solution. The antibody combining site is found to be highly aromatic. We have identified one or two histidine, two tyrosine, and two tryptophan residues and one phenylalanine residue of the antibody interacting with valine-3, proline-4, glycine-5, glutamine-7, histidine-8, and aspartate-10 of the peptide. The 2D TRNOE difference spectroscopy can be used to study protein-ligand interactions, given that the ligand off rate is fast relative to the spin-lattice relaxation time of the protein and ligand protons (about 1 s). The resolution obtained in the difference spectra implies that the technique is equally applicable for studying proteins having a molecular weight larger than 50,000.(ABSTRACT TRUNCATED AT 250 WORDS)