Hydrogen bonding monitored by deuterium isotope effects on carbonyl 13C chemical shift in BPTI: intra-residue hydrogen bonds in antiparallel beta-sheet.

Deuterium isotope effects on carbonyl 13C magnetic shielding were measured for the backbone carbonyl groups in BPTI (basic pancreatic trypsin inhibitor), and interpreted as a measure of hydrogen bond energies. The effects originate from peptide amide proton deuterium substitution and were observed on carbonyl carbons separated by two or three covalent bonds from the amide H/D. Two-bond isotope effects depend on the energy of the hydrogen bond donated by NH/D. Calibration of the effect with model compound data leads to hydrogen bond enthalpies less than 4.7 kcal/mol. Isotope effects over three bonds from the amide H/D to the carbonyl carbon of the same amino acid residue are observed for seven carbonyl resonances in BPTI. The three-bond isotope effects are highly related to the various backbone conformations. The largest effects are observed for residues with an approximate syn- periplanar conformation of the H-N-C alpha-C = O atoms, as realized for many residues in the BPTI antiparallel beta-sheet. The residues that show measurable three-bond effects have unusually short distances between H and O. The size of this effect decreases rapidly with increased O..H distance in the open five-membered ring. This observation suggests appreciable interactions in these rings.     

Pressure response of protein backbone structure. Pressure-induced amide 15N chemical shifts in BPTI.

The effect of pressure on amide 15N chemical shifts was studied in uniformly 15N-labeled basic pancreatic trypsin inhibitor (BPTI) in 90%1H2O/10%2H2O, pH 4.6, by 1H-15N heteronuclear correlation spectroscopy between 1 and 2,000 bar. Most 15N signals were low field shifted linearly and reversibly with pressure (0.468 +/- 0.285 ppm/2 kbar), indicating that the entire polypeptide backbone structure is sensitive to pressure. A significant variation of shifts among different amide groups (0-1.5 ppm/2 kbar) indicates a heterogeneous response throughout within the three-dimensional structure of the protein. A tendency toward low field shifts is correlated with a decrease in hydrogen bond distance on the order of 0.03 A/2 kbar for the bond between the amide nitrogen atom and the oxygen atom of either carbonyl or water. The variation of 15N shifts is considered to reflect site-specific changes in phi, psi angles. For beta-sheet residues, a decrease in psi angles by 1-2 degrees/2 kbar is estimated. On average, shifts are larger for helical and loop regions (0.553 +/- 0.343 and 0.519 +/- 0.261 ppm/2 kbar, respectively) than for beta-sheet (0.295 +/- 0.195 ppm/2 kbar), suggesting that the pressure-induced structural changes (local compressibilities) are larger in helical and loop regions than in beta-sheet. Because compressibility is correlated with volume fluctuation, the result is taken to indicate that the volume fluctuation is larger in helical and loop regions than in beta-sheet. An important aspect of the volume fluctuation inferred from pressure shifts is that they include motions in slower time ranges (less than milliseconds) in which many biological processes may take place.     

Conformation of di-n-propylglycine residues (Dpg) in peptides: crystal structures of a type I' beta-turn forming tetrapeptide and an alpha-helical tetradecapeptide.

The crystal structures of two oligopeptides containing di-n-propylglycine (Dpg) residues, Boc-Gly-Dpg-Gly-Leu-OMe (1) and Boc-Val-Ala-Leu-Dpg-Val-Ala-Leu-Val-Ala-Leu-Dpg-Val-Ala-Leu-OMe (2) are presented. Peptide 1 adopts a type I'beta-turn conformation with Dpg(2)-Gly(3) at the corner positions. The 14-residue peptide 2 crystallizes with two molecules in the asymmetric unit, both of which adopt alpha-helical conformations stabilized by 11 successive 5 --> 1 hydrogen bonds. In addition, a single 4 --> 1 hydrogen bond is also observed at the N-terminus. All five Dpg residues adopt backbone torsion angles (phi, psi) in the helical region of conformational space. Evaluation of the available structural data on Dpg peptides confirm the correlation between backbone bond angle N-C(alpha)-C' (tau) and the observed backbone phi,psi values. For tau > 106 degrees, helices are observed, while fully extended structures are characterized by tau < 106 degrees. The mean tau values for extended and folded conformations for the Dpg residue are 103.6 degrees +/- 1.7 degrees and 109.9 degrees +/- 2.6 degrees, respectively.     

Conformation-Determining role for the N-acetyl group in the O-glycosidic linkage, α-GalNAc-Thr

An ¹H-nmr study of 2-acetamido-2-deoxy-3,4,6-tri-O-acetyl-D-galactopyranose (AcGalNAc) glycosylated Thr-containing tripeptides in Me₂SO-d₆ solution reveals two mutually exclusive intramolecular hydrogen bonds. In Z-Thr(AcGalNAc)-Ala-Ala-OMe, there is an intramolecular hydrogen bond between the Thr amide proton and the sugar N-acetyl carbonyl oxygen. The strength of this hydrogen bond will be dependent on the amino acid residues on the Thr C terminal side to some undetermined distance. In Ac-Thr(AcGalNAc)-Ala-Ala-OMe, a different intramolecular hydrogen bond between the sugar N-acetyl amide proton and the Thr carbonyl oxygen exists. The choice of hydrogen bonds seems dependent on the bulkiness of the residues on the Thr N terminal side. The consequence of such strong hydrogen bonds is a clearly defined orientation of the sugar moiety with respect to the peptide backbone. In the former, the plane of the sugar pyranose ring is roughly oriented perpendicularly to the peptide backbone. The latter orientation is where the plane of the sugar ring is roughly in line with the peptide backbone. In both orientations, the sugar moiety can increase the shielding of the neighboring amino acid residues from the solvent. The idea that the amino acid residues near the glycosylated Thr influence orientation of the sugar moiety with respect to the peptide backbone and in turn possibly hinder peptide backbone flexibility has interesting implications in the conformational as well as the biological role of O-glycoproteins.     

The three-dimensional structure of guanine-specific ribonuclease F1 in solution determined by NMR spectroscopy and distance geometry.

Two-dimensional 1H-NMR studies have been performed on ribonuclease F1 (RNase F1), which contains 106 amino acid residues. Sequence-specific resonance assignments were accomplished for the backbone protons of 99 amino acid residues and for most of their side-chain protons. The three-dimensional structures were constructed on the basis of 820 interproton-distance restraints derived from NOE, 64 distance restraints for 32 hydrogen bonds and 33 phi torsion-angle restraints. A total of 40 structures were obtained by distance geometry and simulated-annealing calculations. The average root-mean-square deviation (residues 1-106) between the 40 converged structures and the mean structure obtained by averaging their coordinates was 0.116 +/- 0.018 nm for the backbone atoms and 0.182 +/- 0.015 nm for all atoms including the hydrogen atoms. RNase F1 was determined to be an alpha/beta-type protein. A well-defined structure constitutes the core region, which consists of a small N-terminal beta-sheet (beta 1, beta 2) and a central five-stranded beta-sheet (beta 3-beta 7) packed on a long helix. The structure of RNase F1 has been compared with that of RNase T1, which was determined by X-ray crystallography. Both belong to the same family of microbial ribonucleases. The polypeptide backbone fold of RNase F1 is basically identical to that of RNase T1. The conformation-dependent chemical shifts of the C alpha protons are well conserved between RNase F1 and RNase T1. The residues implicated in catalysis are all located on the central beta-sheet in a geometry similar to that of RNase T1.     

Intramolecular interactions in chemically modified Escherichia coli thioredoxin monitored by hydrogen/deuterium exchange and electrospray ionization mass spectrometry.

Site specific amide hydrogen/deuterium content of oxidized and reduced Escherichia colithioredoxin, and alkylated derivatives, Cys-32-ethylglutathionylated and Cys-32-ethylcysteinylated thioredoxins are measured, after exposure for 20 s to D(2)O/phosphate buffer (pH 5.7), by electrospray mass spectrometry. The degree of deuteration of Oxi-TRX and Red-TRX correlated with the rates of H/D exchange measured previously by NMR. The ethylcysteinyl modification was shown to minimally perturb the active site of the reduced protein, but showed more global effects on structures of alpha-helices and beta-strands distant from the site of modification. In contrast, the larger ethylglutathionyl group had little effect on the protein's overall conformation, but significantly affected the structure of loops close to the active site. A molecular model of GS-ethyl-TRX derived from molecular simulation allowed the H/D exchange results to be interpreted in terms of specific interactions between the alkyl chain and the protein surface. The specific conformation of the ethylglutathione modification was predicted to be fixed by salt bridges between the carboxylates of the gamma-Glu and Gly of glutathione and the guanidinium of Arg-73 and epsilon-amino group of Lys-90 of the protein. Specific hydrogen bonding interactions between the glutathione carbonyl oxygens and the amide protons of thioredoxin residues Ile-75 and Ala-93 were predicted. The H/D exchange studies showed low levels of deuterium incorporation at backbone nitrogens of these residues. The data also provided evidence for an unusual amide proton-amide nitrogen hydrogen bond within the ethylglutathionylated chain. These same sets of electrostatic and hydrogen bonding interactions were not predicted or observed for the smaller alkyl modification in Cys-ethyl-TRX.     

Solution structure of a sweet protein single-chain monellin determined by nuclear magnetic resonance and dynamical simulated annealing calculations

Single-chain monellin (SCM), which is an engineered 94-residue polypeptide, has proven to be as sweet as native two-chain monellin. SCM is more stable than the native monellin for both heat and acidic environments. Data from gel filtration HPLC and NMR indicate that the SCM exists as a monomer in aqueous solution. The solution structure of SCM has been determined by nuclear magnetic resonance (NMR) spectroscopy and dynamical simulated annealing calculations. A stable alpha-helix spanning residues Phe11-Ile26 and an antiparallel beta-sheet formed by residues 2-5, 36-38, 41-47, 54-64, 69-75, and 83-88 have been identified. The sheet was well defined by backbone-backbone NOEs, and the corresponding beta-strands were further confirmed by hydrogen bond networks based on amide hydrogen exchange data. Strands beta2 and beta3 are connected by a small bulge comprising residues Ile38-Cys41. A total of 993 distance and 56 dihedral angle restraints were used for simulated annealing calculations. The final simulated annealing structures (k) converged well with a root-mean-square deviation (rmsd) between backbone atoms of 0.49 A for secondary structural regions and 0.70 A for backbone atoms excluding two loop regions. The average restraint energy-minimized (REM) structure exhibited root-mean-square deviations of 1.19 A for backbone atoms and 0.85 A for backbone atoms excluding two loop regions with respect to 20 k structures. The solution structure of SCM revealed that the long alpha-helix was folded into the concave side of a six-stranded antiparallel beta-sheet. The side chains of Tyr63 and Asp66 which are common to all sweet peptides showed an opposite orientation relative to H1 helix, and they were all solvent-exposed. Residues at the proposed dimeric interface in the X-ray structure were observed to be mostly solvent-exposed and demonstrated high degrees of flexibility.     

Hydrogen bonds in rubredoxins from mesophilic and hyperthermophilic organisms

The extent and strength of the hydrogen bond networks in rubredoxins from the hyperthermophile Pyrococcus furiosus (PfRd), and its mesophilic analogue Clostridium pasteurianum (CpRd), are examined and compared using NMR spectroscopy. NMR parameters examined in this study include through-hydrogen bond (h3)J(NC)(') scalar couplings and (1)H, (13)C, and (15)N chemical shifts, as well as covalent (1)J(NH) and (1)J(NC)(') scalar couplings. These parameters have allowed the characterization in solution of 12 hydrogen bonds in each protein. Despite a 83% sequence homology and a low RMSD for the backbone heavy atoms (0.648 A) in the crystalline state, subtle, but definite, changes have been identified in the detailed hydrogen-bonding patterns. CpRd shows an increased number of hydrogen bonds in the triple-stranded beta-sheet and an additional hydrogen bond in the multiple-turn segment including residues 14-32. On the other hand, PfRd exhibits an overall strengthening of N-H...O=C hydrogen bonds in the loops involved at the metal binding site as well as evidence for an additional NH...S(Cys) hydrogen bond involving the alanine residue 44. These data, as well as temperature dependence of the NMR parameters, suggest that the particular NMR hydrogen bond pattern found in the hyperthermophile rubredoxin leads to an increased stabilization at the metal binding pocket. It seems to result from a subtle redistribution of hydrogen-bonding interactions between the triple-stranded beta-sheet and the actual metal binding site.     

Amide temperature coefficients in the protein G B1 domain

Temperature coefficients have been measured for backbone amide ¹H and ¹⁵N nuclei in the B1 domain of protein G (GB1), using temperatures in the range 283–313 K, and pH values from 2.0 to 9.0. Many nuclei display pH-dependent coefficients, which were fitted to one or two pK_a values. ¹H coefficients showed the expected behaviour, in that hydrogen-bonded amides have less negative values, but for those amides involved in strong hydrogen bonds in regular secondary structure there is a negative correlation between strength of hydrogen bond and size of temperature coefficient. The best correlation to temperature coefficient is with secondary shift, indicative of a very approximately uniform thermal expansion. The largest pH-dependent changes in coefficient are for amides in loops adjacent to sidechain hydrogen bonds rather than the amides involved directly in hydrogen bonds, indicating that the biggest determinant of the temperature coefficient is temperature-dependent loss of structure, not hydrogen bonding. Amide ¹⁵N coefficients have no clear relationship with structure.     

Three-dimensional structure of the mini-M conotoxin mr3a

Conotoxin mr3a from the venom of Conus marmoreus, a novel peptide that induces rolling seizures in mice, has the peptide sequence GCCGSFACRFGCVOCCV, where O is trans-4-hydroxyproline, and the chain is cross-linked with disulfide bonds between Cys-2 and Cys-16, Cys-3 and Cys-12, and Cys-8 and Cys-15. The tertiary structure of mr3a was determined by 2D 1H NMR in combination with a standard distance-geometry algorithm. The final set of 22 structures for the peptide had a mean global backbone RMS deviation of 0.53 +/- 0.22 A based on 51 NOE, 6 hydrogen bond, 6 phi dihedral angle, and 3 disulfide bond constraints. Conotoxin mr3a is the first example of the new mini-M branch of conopeptides in the M superfamily. Members of the maxi-M branch, whose structures are known, include the mu- and psi-conotoxins, both of which share a common disulfide bond connectivity. Although mr3a has the same arrangement of Cys residues as the mu- and psi-conotoxins, its disulfide connectivity is different. This gives mr3a a distinctive "triple-turn" backbone.     

Epidermal growth factor from the mouse. Physical evidence for a tiered beta-sheet domain: two-dimensional NMR correlated spectroscopy and nuclear Overhauser experiments on backbone amide protons

When H2O-exchanged, lyophilized mouse epidermal growth factor (mEGF) is dissolved in deuterium oxide at low pH (i.e., below approximately 6.0), 13 well-resolved, amide proton resonances are observed in the downfield region of an NMR spectrum (500 MHz). Under the conditions of these experiments, the lifetimes of these amide protons in exchange for deuterons of the deuterium oxide solvent suggest that these amide protons are hydrogen-bonded, backbone amide protons. Several of these amide proton resonances show splittings (i.e., JNH alpha-CH) of approximately 8-10 Hz, indicating that their associated amide protons are in some type of beta-structure. Selective nuclear Overhauser effect (NOE) experiments performed on all amide proton resonances strongly suggest that all 13 of these backbone amide protons are part of a single-tiered beta-sheet structural domain in mEGF. Correlation of 2D NMR correlated spectroscopy data, identifying scaler coupled protons, with NOE data, identifying protons close to the irradiated amide protons, allows tentative assignment of some resonances in the NOE difference spectra to specific amino acid residues. These data allow a partial structural model of the tiered beta-sheet domain in mEGF to be postulated.     

Contributions of residue pairing to beta-sheet formation: conservation and covariation of amino acid residue pairs on antiparallel beta-strands

In an effort to better understand beta-sheet assembly, we have investigated the evolutionary behavior of neighboring residues on adjacent antiparallel beta-strands. Residue pairs were classified according to solvent exposure as well as by whether their backbone NH and C==O groups are hydrogen bonded. The conservation and covariation of 19,241 pairs in 219 sequence alignments was analyzed. Buried pairs were found to be the most conserved, while stronger covariation was detected in the solvent-exposed pairs. However, residues on neighboring strands showed a degree of conservation and covariation similar to that of well-separated residues on the same strand, suggesting that evolutionary pressure to maintain complementarity between pairs on neighboring strands is weak. Moreover, in spite of the preference of certain amino acid pairs to occupy neighboring positions on adjacent strands, such favored pairs are neither more strongly mutually conserved nor covary more strongly than pairs of the same type in non-interacting positions. Although the beta-sheet pairs did not show outstanding evolutionary coupling, in many protein families significant conservation and covariation patterns were detected for some of the residue pairs. Overall, the weak evolutionary conservation and covariation of the beta-sheet pairs indicates that sheet structure is unlikely to be dictated by specific side-chain interactions.     

Molecular dynamics simulations of a beta-hairpin fragment of protein G: balance between side-chain and backbone forces

How is the native structure encoded in the amino acid sequence? For the traditional backbone centric view, the dominant forces are hydrogen bonds (backbone) and phi-psi propensity. The role of hydrophobicity is non-specific. For the side-chain centric view, the dominant force of protein folding is hydrophobicity. In order to understand the balance between backbone and side-chain forces, we have studied the contributions of three components of a beta-hairpin peptide: turn, backbone hydrogen bonding and side-chain interactions, of a 16-residue fragment of protein G. The peptide folds rapidly and cooperatively to a conformation with a defined secondary structure and a packed hydrophobic cluster of aromatic side-chains. Our strategy is to observe the structural stability of the beta-hairpin under systematic perturbations of the turn region, backbone hydrogen bonds and the hydrophobic core formed by the side-chains, respectively. In our molecular dynamics simulations, the peptides are solvated. with explicit water molecules, and an all-atom force field (CFF91) is used. Starting from the original peptide (G41EWTYDDATKTFTVTE56), we carried out the following MD simulations. (1) unfolding at 350 K; (2) forcing the distance between the C(alpha) atoms of ASP47 and LYS50 to be 8 A; (3) deleting two turn residues (Ala48 and Thr49) to form a beta-sheet complex of two short peptides, GEWTYDD and KTFTVTE; (4) four hydrophobic residues (W43, Y45, F52 and T53) are replaced by a glycine residue step-by-step; and (5) most importantly, four amide hydrogen atoms (T44, D46, T53, and T55, which are crucial for backbone hydrogen bonding), are substituted by fluorine atoms. The fluorination not only makes it impossible to form attractive hydrogen bonding between the two beta-hairpin strands, but also introduces a repulsive force between the two strands due to the negative charges on the fluorine and oxygen atoms. Throughout all simulations, we observe that backbone hydrogen bonds are very sensitive to the perturbations and are easily broken. In contrast, the hydrophobic core survives most perturbations. In the decisive test of fluorination, the fluorinated peptide remains folded under our simulation conditions (5 ns, 278 K). Hydrophobic interactions keep the peptide folded, even with a repulsive force between the beta-strands. Thus, our results strongly support a side-chain centric view for protein folding.     

Localization of bound water in the solution structure of the immunoglobulin binding domain of streptococcal protein G. Evidence for solvent-induced helical distortion in solution.

The presence of bound water in the solution structure of the IgG binding domain of streptococcal protein G has been investigated by nuclear magnetic resonance using three-dimensional 1H rotating frame Overhauser 1H-15N multiple quantum coherence spectroscopy. The backbone amide protons of three residues, Ala20, Gln32 and Tyr33, are found to be in close proximity to bound water. Examination of the three-dimensional structure of the IgG binding domain indicates that in the vicinity of these three residues there are no backbone groups that do not already participate in hydrogen bonding and there are no suitably placed side-chain groups available for hydrogen bonding with water. As the lifetime of the bound water detected in this nuclear magnetic resonance experiment is greater than about one nanosecond, it is likely that the two bound water molecules participate in a bifurcating hydrogen bonding network comprising a CO-NH hydrogen bonded pair, such that the water molecule accepts a hydrogen bond from the NH proton and donates one to the carbonyl oxygen with the result that the amide proton is involved in a three center hydrogen bond. On the basis of the structure, one water molecule participates in such an interaction with the Ala20(NH)-Met1(CO) hydrogen bonded pair at the beginning of an anti-parallel beta-sheet, and the other with the Tyr33(NH)-Val29(CO) hydrogen bonded pair in the single alpha-helix. The latter, which is external and solvent accessible, is associated with a distortion in the alpha-helix centered around Tyr33 which consists of a significant increase in the CO(i-4)-N(i) and CO(i-4)-NH(i) distances relative to those in the rest of the helix, as well as a significant departure in the phi, psi angles of Tyr33 relative to regular helical geometry. Such solvent induced distortions in alpha-helices have been previously noticed in crystal structures and were postulated as possible folding intermediates for helical structures. The present observation of this phenomenon in solution indicates, however, that these water molecules are tightly bound and represent an integral part of the protein framework.     

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.     

Kinetic isotope effects reveal the presence of significant secondary structure in the transition state for the folding of the N-terminal domain of L9

Our present understanding of the nature of the transition state for protein folding depends predominantly on studies where individual side-chain contributions are mapped out by mutational analysis (phi value analysis). This approach, although extremely powerful, does not in general provide direct information about the formation of backbone hydrogen bonds. Here, we report the results of amide H/D isotope effect studies that probe the development of hydrogen bonded interactions in the transition state for the folding of a small alpha-beta protein, the N-terminal domain of L9. Replacement of amide protons by deuterons in a solvent of constant isotopic composition destabilized the domain, decreasing both its T(m) and Delta G(0) of unfolding. The folding rate also decreased. The parameter Phi(H/D), defined as the ratio of the effect of isotopic substitution upon the activation free energy to the equilibrium free energy was determined to be 0.6 in a D(2)O background and 0.75 in a H(2)O background, indicating that significant intraprotein hydrogen bond interactions are developed in the transition state for the folding of NTL9. The value is in remarkably good agreement with more traditional measures of the position of the transition state, which report on the relative burial of surface area. The results provide a picture of a compact folding transition state containing significant secondary structure. Indirect analysis argues that the bulk of the kinetic isotope effect arises from the beta-sheet-rich region of the protein, and suggests that the development of intraprotein hydrogen bonds in this region plays a critical role in the folding of NTL9.     

Porcine pancreatic phospholipase A2: sequence-specific 1H and 15N NMR assignments and secondary structure

The solution structure of porcine pancreatic phospholipase A2 (124 residues, 14 kDa) has been studied by two-dimensional homonuclear 1H and two- and three-dimensional heteronuclear 15N-1H nuclear magnetic resonance spectroscopy. Backbone assignments were made for 117 of the 124 amino acids. Short-range nuclear Overhauser effect (NOE) data show three alpha-helices from residues 1-13, 40-58, and 90-109, an antiparallel beta-sheet for residues 74-85, and a small antiparallel beta-sheet between residues 25-26 and 115-116. A 15N-1H heteronuclear multiple-quantum correlation experiment was used to monitor amide proton exchange over a period of 22 h. In total, 61 amide protons showed slow or intermediate exchange, 46 of which are located in the three large helices. Helix 90-109 was found to be considerably more stable than the other helices. For the beta-sheets, four hydrogen bonds could be identified. The secondary structure of porcine PLA in solution, as deduced from NMR, is basically the same as the structure of porcine PLA in the crystalline state. Differences were found in the following regions, however. Residues 1-6 in the first alpha-helix are less structured in solution than in the crystal structure. Whereas in the crystal structure residues 24-29 are involved both in a beta-sheet with residues 115-117 and in a hairpin turn, the expected hydrogen bonds between residues 24-117 and 25-29 do not show slow exchange behavior. This and the absence of several expected NOEs imply that this region has a less well defined structure in solution. Finally, the hydrogen bond between residues 78-81, which is part of a beta-sheet, does not show slow exchange behavior.     

Hydrogen bonds between short polar side chains and peptide backbone: prevalence in proteins and effects on helix-forming propensities

A survey of 322 proteins showed that the short polar (SP) side chains of four residues, Thr, Ser, Asp, and Asn, have a very strong tendency to form hydrogen bonds with neighboring backbone amides. Specifically, 32% of Thr, 29% of Ser, 26% of Asp, and 19% of Asn engage in such hydrogen bonds. When an SP residue caps the N terminal of a helix, the contribution to helix stability by a hydrogen bond with the amide of the N3 or N2 residue is well established. When an SP residue is in the middle of a helix, the side chain is unlikely to form hydrogen bonds with neighboring backbone amides for steric and geometric reasons. In essence the SP side chain competes with the backbone carbonyl for the same hydrogen-bonding partner (i.e., the backbone amide) and thus SP residues tend to break backbone carbonyl-amide hydrogen bonds. The proposition that this is the origin for the low propensities of SP residues in the middle of alpha helices (relative to those of nonpolar residues) was tested. The combined effects of restricting side-chain rotamer conformations (documented by Creamer and Rose, Proc Acad Sci USA, 1992;89:5937-5941; Proteins, 1994;19:85-97) and excluding side- chain to backbone hydrogen bonds by the helix were quantitatively analyzed. These were found to correlate strongly with four experimentally determined scales of helix-forming propensities. The correlation coefficients ranged from 0.72 to 0.87, which are comparable to those found for nonpolar residues (for which only the loss of side-chain conformational entropy needs to be considered).     

Temperature-dependence of protein hydrogen bond properties as studied by high-resolution NMR

The temperature-dependence of a large number of NMR parameters describing hydrogen bond properties in the protein ubiquitin was followed over a range from 5 to 65 degrees C. The parameters comprise hydrogen bond (H-bond) scalar couplings, h3JNC', chemical shifts, amide proton exchange rates, 15N relaxation parameters as well as covalent 1JNC' and 1JNH couplings. A global weakening of the h3JNC' coupling with increasing temperature is accompanied by a global upfield shift of the amide protons and a decrease of the sequential 1JNC' couplings. If interpreted as a linear increase of the N...O distance, the change in h3JNC' corresponds to an average linear thermal expansion coefficient for the NH-->O hydrogen bonds of 1.7 x 10(-4)/K, which is in good agreement with overall volume expansion coefficients observed for proteins. A residue-specific analysis reveals that not all hydrogen bonds are affected to the same extent by the thermal expansion. The end of beta-sheet beta1/beta5 at hydrogen bond E64-->Q2 appears as the most thermolabile, whereas the adjacent hydrogen bond I3-->L15 connecting beta-strands beta1 and beta2 is even stabilized slightly at higher temperatures. Additional evidence for the stabilization of the beta1/beta2 beta-hairpin at higher temperatures is found in reduced hydrogen exchange rates for strand end residue V17. This reduction corresponds to a stabilizing change in free energy of 9.7 kJ/mol for the beta1/beta2 hairpin. The result can be linked to the finding that the beta1/beta2 hairpin behaves as an autonomously folding unit in the A-state of ubiquitin under changed solvent conditions. For several amide groups the temperature-dependencies of the amide exchange rates and H-bond scalar couplings are uncorrelated. Therefore, amide exchange rates are not a sole function of the hydrogen bond "strength" as given by the electronic overlap of donors and acceptors, but are clearly dependent on other blocking mechanisms.     

N.m.r. study on conformation of Ac-Thr(alpha-GalNAc)-Ala-Ala-OMe as a model for mucin type glycoprotein

This study report on the results of high resolution 1H n.m.r. investigations on Ac-Thr(alpha-GalNAc)-Ala-Ala-OMe 1 as a mucin type model glycopeptide of antifreeze glycoprotein (AFGP) in both dimethyl sulfoxide (DMSO) and H2O. The temperature dependence of amide proton chemical shifts strongly suggested the presence of the intramolecular hydrogen bond between the amide proton of GalNAc and the carbonyl oxygen of the Thr residues. Due to this bond, the orientation of the sugar residue of 1 appears to be fairly restricted relative to its peptide backbone. Despite the lack of the clear evidence for such intramolecular hydrogen bond in H2O, 1H coupling constant data suggested the structural similarity of 1 in DMSO and H2O, indicating the presence of the intramolecular hydrogen bond even in H2O, which may play an important role in determining the orientation of the sugar moiety with respect to the peptide backbone in glycoprotein.