Sequential resonance assignments in protein 1H nuclear magnetic resonance spectra. Basic pancreatic trypsin inhibitor

The assignment of the ¹H nuclear magnetic resonance spectrum of the basic pancreatic trypsin inhibitor with the use of two-dimensional ¹H nuclear magnetic resonance techniques at 500 MHz is described. The assignments are based entirely on the known amino acid sequence and the nuclear magnetic resonance data. Individual resonance assignments were obtained for all backbone and C^β protons, with the exception of those of Arg1, Pro2, Pro13 and the amide proton of Gly37. The side-chain resonance assignments are complete, with the exception of Pro2 and Pro13, the N^δ protons of Asn44 and the peripheral protons of the lysine residues and all but two of the arginine residues.     

Correlation between the amide proton exchange rates and the denaturation temperatures in globular proteins related to the basic pancreatic trypsin inhibitor.

Nuclear magnetic resonance was used to measure the hydrogen-deuterium exchange rates for individual interior amide protons in a group of small globular proteins related to the basic pancreatic trypsin inhibitor (BPTI). These proteins include two homologous proteins and seven chemical modifications of BPTI. It was previously shown that the spatial structure of BPTI is preserved in all these related proteins. The exchange rates for corresponding amide protons in the different proteins were found to vary by a factor of as much as 5 X 104. The proton exchange is correlated with the thermal stability of the proteins, i.e. the lower the denaturation temperature, the faster the NH exchange. Further evidence that the exchange of interior amide protons is promoted by global fluctuations of the protein structures comes from the observation that the order of the relative exchange rates for the individual protons is the same in all the different species. This is the third in a series of three papers on nuclear magnetic resonance studies of labile protons in BPTI-related proteins. A detailed interpretation of the data will be given in a forthcoming paper.     

Sequential resonance assignments in protein 1H nuclear magnetic resonance spectra: Glucagon bound to perdeuterated dodecylphosphocholine micelles

The assignment of the ¹H nuclear magnetic resonance spectrum of glucagon bound to perdeuterated dodecylphosphocholine micelles with the use of two-dimensional ¹H nuclear magnetic resonance techniques at 360 MHz is described. Sequential resonance assignments were obtained for all backbone and C^β protons except the N-terminal amino group and the amide proton of Ser2. The assignments of the non-labile amino acid side-chain protons are complete except for the γ-methylene protons of Gln20 and Gln24. These assignments provide a basis for the determination of the three-dimensional structure of lipid-bound glucagon.     

NMR spectroscopy of hydroxyl protons in aqueous solutions of peptides and proteins

Summary Hydroxyl groups of serine and threonine, and to some extent also tyrosine are usually located on or near the surface of proteins. NMR observations of the hydroxyl protons is therefore of interest to support investigations of the protein surface in solution, and knowledge of the hydroxyl NMR lines is indispensable as a reference for studies of protein hydration in solution. In this paper, solvent suppression schemes recently developed for observation of hydration water resonances were used to observe hydroxyl protons of serine, threonine and tyrosine in aqueous solutions of small model peptides and the protein basic pancreatic trypsin inhibitor (BPTI). The chemical shifts of the hydroxyl protons of serine and threonine were found to be between 5.4 and 6.2 ppm, with random-coil shifts at 4°C of 5.92 ppm and 5.88 ppm, respectively, and those of tyrosine between 9.6 and 10.1 ppm, with a random-coil shift of 9.78 ppm. Since these spectral regions are virtually free of other polypeptide¹H NMR signals, cross peaks with the hydroxyl protons are usually well separated even in homonuclear two-dimensional¹H NMR spectra. To illustrate the practical use of hydroxyl proton NMR in polypeptides, the conformations of the side-chain hydroxyl groups in BPTI were characterized by measurements of nuclear Overhauser effects and scalar coupling constants involving the hydroxyl protons. In addition, hydroxyl proton exchange rates were measured as a function of pH, where simple first-order rate processes were observed for both acid- and base-catalysed exchange of all but one of the hydroxyl-bearing residues in BPTI. For the conformations of the individual Ser, Thr and Tyr side chains characterized in the solution structure with the use of hydroxyl proton NMR, both exact coincidence and significant differences relative to the corresponding BPTI crystal structure data were observed.[/p]     

Amide-proton exchange studies by two-dimensional correlated 1H NMR in two chemically modified analogs of the basic pancreatic trypsin inhibitor

The backbone amide proton exchange with the solvent was investigated in 2H2O solutions of the basic pancreatic trypsin inhibitor and two chemical modifications thereof, which were obtained by transamination of the N-terminus and by cleavage of the disulfide bond 14-38, respectively. The three proteins have nearly identical conformations, but the stability with respect to thermal denaturation is markedly different. Exchange rates for a large number of individually assigned amide protons located both in central and peripheral parts of the protein structures were measured by two-dimensional correlated spectroscopy (COSY). From analysis of the individual proton exchange rates in the three proteins at different temperatures, an interplay of global and local structure fluctuations was characterized, which promote hydrogen exchange in distinct regions of the molecules. The exchange of particular amide protons may be governed by different motional processes at different temperatures. As a general trend, global fluctuations involving breakage of numerous hydrophilic secondary bonds appear to be dominant at higher temperatures, whereas at lower temperatures the influence of local fluctuations in hydrophobic regions of the protein structures is also clearly noticeable.     

Protein folding kinetics by combined use of rapid mixing techniques and NMR observation of individual amide protons

A method to be used for experimental studies of protein folding introduced by Schmid and Baldwin (J. Mol. Biol. 135: 199-215, 1979), which is based on the competition between amide hydrogen exchange and protein refolding, was extended by using rapid mixing techniques and 1H NMR to provide site-resolved kinetic information on the early phases of protein structure acquisition. In this method, a protonated solution of the unfolded protein is rapidly mixed with a deuterated buffer solution at conditions assuring protein refolding in the mixture. This simultaneously initiates the exchange of unprotected amide protons with solvent deuterium and the refolding of protein segments which can protect amide groups from further exchange. After variable reaction times the amide proton exchange is quenched while folding to the native form continues to completion. By using 1H NMR, the extent of exchange at individual amide sites is then measured in the refolded protein. Competition experiments at variable reaction times or variable pH indicate the time at which each amide group is protected in the refolding process. This technique was applied to the basic pancreatic trypsin inhibitor, for which sequence-specific assignments of the amide proton NMR lines had previously been obtained. For eight individual amide protons located in the beta-sheet and the C-terminal alpha-helix of this protein, apparent refolding rates in the range from 15 s-1 to 60 s-1 were observed. These rates are on the time scale of the fast folding phase observed with optical probes.     

Amide proton exchange in proteins by EX1 kinetics: studies of the basic pancreatic trypsin inhibitor at variable p2H and temperature

With the use of one-dimensional 1H nuclear magnetic resonance, two-dimensional correlated spectroscopy, and two-dimensional nuclear Overhauser enhancement spectroscopy, the exchange mechanisms for numerous individual amide protons in the basic pancreatic trypsin inhibitor (BPTI) were investigated over a wide range of p2H and temperature. Correlated exchange under an EX1 regime was observed only for the most slowly exchanging protons in the central hydrogen bonds of the antiparallel beta-sheet and only over a narrow range of temperature and p2H, i.e., above ca. 55 degrees C and between p2H 7 and 9, where the opening rates of the structure fluctuations which promote the exchange of these protons are of the order 0.1 min-1. At p2H below 7, the exchange of this most stable group of protons is uncorrelated and is governed by an EX2 mechanism. At p2H above 9, the exchange is also uncorrelated and occurs via either EX2 or EX1 processes promoted by strictly local structure fluctuations. For all other backbone amide protons in BPTI, the exchange was found to be uncorrelated and by an EX2 mechanism under all conditions of p2H and temperature where quantitative measurements could be obtained with the methods used, i.e., for kex approximately less than 5 min-1. From these observations with BPTI it can be concluded that the amide proton exchange in globular proteins is quite generally via EX2 processes, with rare exceptions for measurements with extremely stable protons at high temperature and basic p2H. This emphasizes the need for further development of suitable concepts for the structural interpretation of EX2 amide proton exchange [Wagner, G. (1983) Q. Rev. Biophys. 16, 1-57; Wagner, G., Stassinopoulou, C. I., & Wüthrich, K. (1984) Eur. J. Biochem. 145, 431-436] and for more detailed investigations of the intrinsic exchange rates for solvent-exposed amide protons in the "open" states of a protein [Roder, H., Wagner, G., & Wüthrich, K. (1985) Biochemistry (following paper in this issue)].     

The pH dependence of hydrogen exchange in proteins

The static accessibility modified discrete charge model for electrostatic interactions in proteins is extended to the prediction of the pH dependence of hydrogen exchange reactions. The exchange rate profiles of buried amide protons are shown to follow the calculated pH dependence of the electrostatic component of protein stability. Rate profiles are calculated for individual buried amide protons in ribonuclease S and bovine pancreatic trypsin inhibitor. The electrostatic free energy of stabilization of the protein and the energy required to bring the catalytic ion to an exchange site are expressed as an apparent, pH-dependent contribution to the activation energy. Changes in the electrostatic stabilization of the proteins affect the calculated exchange rate for buried amide protons by more than 1000, while local field effects raise or lower the predicted exchange rates by less than 100. The pH dependence of exchangeable protons at the protein surface, such as the C-2 imidazole protons, is shown to follow the estimated energy required to introduce the catalytic ion at the exchange site. These calculations are discussed in terms of current models for proton exchange which incorporate the dynamic nature of the structure to explain exchange data from the interior of a protein.     

Sequence-dependent recognition of DNA duplexes: netropsin complexation to the TATA site of the d(G-G-T-A-T-A-C-C) duplex in aqueous solution

We have recorded one-dimensional exchangeable proton and two-dimensional nonexchangeable proton nmr spectra on the complex of netropsin with the self-complementary d(G-G-T-A-T-A-C-C) duplex in aqueous solution between 25° and 35°C. The antibiotic amide, pyrrole, and methylene protons, and the nucleic acid base and sugar H1′, H2′, H2″, and H3′ protons, have been assigned from an analysis of the two-dimensional nuclear Overhauser effect (NOESY) spectra of the complex. We observe intermolecular NOEs between the antibiotic concave face amide, pyrrole, and CH₂ resonances, and the adenosine H2 and sugar H1′ protons of base-pairs T3·A6 and A4·T5 in the central TATA core of the d(G₁-G₂-T₃-A₄-T₅-A₆-C₇-C₈) duplex. We present a molecular model outlining these seven antibiotic-DNA contacts for the complex in solution. The observed line-broadening of several base and sugar protons at the TATA minor groove netropsin binding site in the complex at 35°C are interpreted in terms of intermediate exchange between two orientations of bound netropsin on the duplex.     

On the pH dependence of amide proton exchange rates in proteins.

We have analyzed the pH dependencies of published amide proton exchange rates (kex) in three proteins: bovine pancreatic trypsin inhibitor (BPTI), bull seminal plasma proteinase inhibitor IIA (BUSI IIA), and calbindin D9K. The base-catalyzed exchange rate constants (kOH) of solvent exposed amides in BPTI are lower for residues with low peptide carbonyl exposure, showing that the environment around the carbonyl oxygen influences kOH. We also examined the possible importance of an exchange mechanism that involves formations of imidic acid intermediates along chains of hydrogen-bonded peptides in the three proteins. By invoking this "relayed imidic acid exchange mechanism," which should be essentially acid-catalyzed, we can explain the surprisingly high pHmin (the pH value at which kex reaches a minimum) found for the non-hydrogen-bonded amide protons in the beta-sheet in BPTI. The successive increase of pHmin along a chain of hydrogen-bonded peptides from the free amide to the free carbonyl, observed in BPTI, can be explained as an increasing contribution of the proposed mechanism in this direction of the chain. For BUSI IIA (pH 4-5) and calbindin D9K (pH 6-7) the majority of amide protons with negative pH dependence of kex are located in chains of hydrogen-bonded peptides; this situation is shown to be consistent with the proposed mechanism.     

Sequence-specific 1H and 15N resonance assignments and secondary structure of GDP-bound human c-Ha-Ras protein in solution

Summary All the backbone ¹H and ¹⁵N magnetic resonances (except for Pro residues) of the GDP-bound form of a truncated human c-Ha-ras proto-oncogene product (171 amino acid residues, the Ras protein) were assigned by ¹⁵N-edited two-dimensional NMR experiments on selectively ¹⁵N-labeled Ras proteins in combination with three-dimensional NMR experiments on the uniformly ¹⁵N-labeled protein. The sequence-specific assignments were made on the basis of the nuclear Overhauser effect (NOE) connectivities of amide protons with preceding amide and/or Cprotons. In addition to sequential NOEs, vicinal spin coupling constants for amide protons and C protons and deuterium exchange rates of amide protons were used to characterize the secondary structure of the GDP-bound Ras protein; six strands and five helices were identified and the topology of these elements was determined. The secondary structure of the Ras protein in solution was mainly consistent with that in crystal as determined by X-ray analyses. The deuterium exchange rates of amide protons were examined to elucidate the dynamic properties of the secondary structure elements of the Ras protein in solution. In solution, the -sheet structure in the Ras protein is rigid, while the second helix (A66-R73) is much more flexible, and the first and fifth helices (S17-124 and V152-L171) are more rigid than other helices. Secondary structure elements at or near the ends of the effector-region loop were found to be much more flexible in solution than in the crystalline state.     

Backbone dynamics of a model membrane protein: measurement of individual amide hydrogen-exchange rates in detergent-solubilized M13 coat protein using 13C NMR hydrogen/deuterium isotope shifts

Hydrogen-exchange rates have been measured for individual assigned amide protons in M13 coat protein, a 50-residue integral membrane protein, using a 13C nuclear magnetic resonance (NMR) equilibrium isotope shift technique. The locations of the more rapidly exchanging amides have been determined. In D2O solutions, a peptide carbonyl resonance undergoes a small upfield isotope shift (0.08-0.09 ppm) from its position in H2O solutions; in 1:1 H2O/D2O mixtures, the carbonyl line shape is determined by the exchange rate at the adjacent nitrogen atom. M13 coat protein was labeled biosynthetically with 13C at the peptide carbonyls of alanine, glycine, phenylalanine, proline, and lysine, and the exchange rates of 12 assigned amide protons in the hydrophilic regions were measured as a function of pH by using the isotope shift method. This equilibrium technique is sensitive to the more rapidly exchanging protons which are difficult to measure by classical exchange-out experiments. In proteins, structural factors, notably H bonding, can decrease the exchange rate of an amide proton by many orders of magnitude from that observed in the freely exposed amides of model peptides such as poly(DL-alanine). With corrections for sequence-related inductive effects [Molday, R. S., Englander, S. W., & Kallen, R. G. (1972) Biochemistry 11, 150-158], the retardation of amide exchange in sodium dodecyl sulfate solubilized coat protein has been calculated with respect to poly(DL-alanine). The most rapidly exchanging protons, which are retarded very little or not at all, are shown to occur at the N- and C-termini of the molecule.(ABSTRACT TRUNCATED AT 250 WORDS)     

Hydrogen exchange of individual amide protons in the F helix of cyanometmyoglobin

Hydrogen exchange of the individual amide protons of alanine-90 (F5), glutamine-91 (F6), serine-92 (F7), and histidine-93 (F8) residues in cyanometmyoglobin of sperm whale has been studied by 1H nuclear magnetic resonance spectroscopy at 360 MHz. The amide proton resonance of F5, F6, and F7 have been assigned by use of the selective nuclear Overhauser effect between the consecutive amide protons. At pH 6.8, and in the temperature range of 5-20 degrees C, these protons show a 10(4)-fold retardation compared to the rates in free peptides. Apparent activation enthalpies for hydrogen exchange of F5, F6, and F8 protons are 18.5 +/- 0.4, 9.5 +/- 0.3, and 18.5 +/- 0.3 kcal/mol, respectively. Some implications of these results on the nature of the opening processes involved in hydrogen exchange are considered.     

Measurement of amide proton exchange rates and NOEs with water in 13C/15N-enriched calcineurin B

Summary A rapid and sensitive 2D approach is presented for measuring amide proton exchange rates and the NOE interaction between amide protons and water. The approach is applicable to uniformly ¹³C/¹⁵N-enriched proteins and can measure magnetization exchange rates in the 0.02 to >20s^–1 range. The experiments rely on selective excitation of the water resonance, coupled with purging of underlying H resonances, followed by NOESY-or ROESY-type transfer to amide protons, which are dispersed by the amide ¹⁵N frequencies in an HSQC-type experiment. Two separate but interleaved experiments, with and without selective inversion of the H₂O resonance, yield quantitative results. The method is demonstrated for a sample of the calcium-binding protein calcineurin B. Results indicate rapid amide exchange for the five calcineurin B residues that are analogous to the five rapidly exchanging residues in the central helix of the homologous protein calmodulin.     

Protein hydration studied with homonuclear 3D1H NMR experiments

Summary Homonuclear 3D¹H NOESY-TOCSY and 3D¹H ROESY-TOCSY experiments were used to resolve and assign nuclear Overhauser effect (NOE) cross peaks between the water signal and individual polypeptide proton resonances in H₂O solutions of the basic pancreatic trypsin inhibitor. Combined with a novel, robust water-suppression technique, positive and negative intermolecular NOEs were detected at 4°C. The observation of positive NOEs between water protons and protein protons enables more precise estimates of the very short residence times of the water molecules in the hydration sites on the protein surface.     

The conformational characteristics in solution of the synthetic cyclic hexapeptide 5L-ala-D-ala

An attempt to elucidate the solution conformation(s) of the synthetic cyclic hexapeptide 5L -ala·D-ala is described. Nuclear magnetic resonance (nmr) spectra are recorded for the purpose of measuring the vicinal coupling constant between the amide and α-protons in each residue and to observe the deuterium exchange rate and temperature dependence of the chemical shift of each amide proton. Low-energy cyclic conformations, whose individual residues are in conformations consistent with the observed amide to α-proton coupling constant, are searched for in an approximate theoretical treatment. The two lowest energy, all trans peptide bond conformations generated are distinguishable by the presence or absence of a single intramolecular hydrogen bond. The observed temperature independence of the chemical shift of one of the amide protons is consistent with the presence of a single intramolecular hydrogen bond, while the observation of similar deuterium exchange rates for each of the amide protons indicates their comparable availability to solvent. Consequently, it is concluded that 5L -ala·D-ala is in rapid equilibrium between conformations with and without a single internal hydrogen bond and possesses considerable conformational flexibility in solution.     

Sequence and conformational effects on imino proton exchange in A.T- and A.U-containing DNA and RNA duplexes

¹H-nmr relaxation has been used to study the effect of sequence and conformation on imino proton exchange in adenine–thymine (A · T) and adenine–uracil (A · U) containing DNA and RNA duplexes. At low temperature, relaxation is caused by dipolar interactions between the imino and the adenine amino and AH2 protons, and at higher temperature, by exchange with the solvent protons. Although room temperature exchange rates vary between 3 and 12s^?1, the exchange activation energies (E_α) are insensitive to changes in the duplex sequence (alternating vs homopolymer duplexes), the conformation (B-form DNA vs A-form RNA), and the identity of the pyrimidine base (thymine vs uracil). The average value of the activation energy for the five duplexes studied, poly[d(A-T)], poly[d(A) · d(T)], poly[d(A-U)], Poly[d(A) · d(U)], and poly[r(A) · r(U)], was 16.8 ± 1.3 kcal/mol. In addition, we find that the average E_α for the A.T base pairs in a 43-base-pair restriction fragment is 16.4 ± 1.0 kcal/mol. This result is to be contrasted with the observation that the E_α of cytosine-containing duplexes depends on the sequence, conformation, and substituent groups on the purine and pyrimidine bases. Taken together, the data indicate that there is a common low-energy pathway for the escape of the thymine (uracil) imino protons from the double helix. The absolute values of the exchange rates in the simple sequence polymers are typically 3–10 times faster than in DNAs containing both A · T and G · C base pairs.     

Protein proton–proton dynamics from amide proton spin flip rates

Residue-specific amide proton spin-flip rates K were measured for peptide-free and peptide-bound calmodulin. K approximates the sum of NOE build-up rates between the amide proton and all other protons. This work outlines the theory of multi-proton relaxation, cross relaxation and cross correlation, and how to approximate it with a simple model based on a variable number of equidistant protons. This model is used to extract the sums of K-rates from the experimental data. Error in K is estimated using bootstrap methodology. We define a parameter Q as the ratio of experimental K-rates to theoretical K-rates, where the theoretical K-rates are computed from atomic coordinates. Q is 1 in the case of no local motion, but decreases to values as low as 0.5 with increasing domination of sidechain protons of the same residue to the amide proton flips. This establishes Q as a monotonous measure of local dynamics of the proton network surrounding the amide protons. The method is applied to the study of proton dynamics in Ca²⁺-saturated calmodulin, both free in solution and bound to smMLCK peptide. The mean Q is 0.81 ± 0.02 for free calmodulin and 0.88 ± 0.02 for peptide-bound calmodulin. This novel methodology thus reveals the presence of significant interproton disorder in this protein, while the increase in Q indicates rigidification of the proton network upon peptide binding, confirming the known high entropic cost of this process.