Pulsed FT-NMR double resonance studies of yeast tRNAPhe: specific nuclear Overhauser effects and reinterpretation of low temperature relaxation data.

Cross-relaxation effects are demonstrated between the imino protons and other protons in yeast tRNAPhe and H2O. A detailed examination has been made of the observed relaxation rate of the proton resonance at 11.8 ppm from DSS as a function of the D2O content in the solvent. This result, as well as the size and number of observed nuclear Overhauser effects, suggests that dipolar magnetization transfer between solvent H2O, amino, imino, and other tRNA protons may dominate the relaxation processes of the imino protons at low temperature. At higher temperatures the observed relaxation rate is dominated by chemical exchange. The selective nuclear Overhauser effects are shown to be an important aid in resonance assignments. By these means we were able to identify tow protons from the wobble base pair GU4 at 11.8 ppm and 10.4 ppm.     

An NMR study of the exchange rates for protons involved in the secondary and tertiary structure of yeast tRNA Phe.

Solvent exchange rates of all the protons of yeast tRNAphe resonating in the lowfield NMR region (-11 to-15 ppm from DSS) have been measured by saturation-recovery long-pulse Fourier transform NMR. All these protons in yeast tRNAphe are in the fast exchange limit with H2O relative to their intrinsic longitudinal relaxation processes. Most rates show very little temperature dependence; however, tertiary base pair protons are preferentially destabilized in the absence of Mg++ at higher temperatures. The measured exchange rates are between 2 and 125 sec-1 for a temperature range from 10 degrees C to 45 degrees C and MgCl2 concentrations between 0 and 15 mM.     

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.     

Proton exchange and base-pair kinetics of poly(rA).poly(rU) and poly(rI).poly(rC)

Proton exchange of poly(rA).poly(rU) and poly(rI).poly(rC) has been studied by nuclear magnetic resonance line broadening and saturation transfer from H2O. Five exchangeable peaks are observed. They are assigned to the imino, amino and 2'-OH ribose protons. The aromatic spectrum is also assigned. Contrary to previous observations, we find that the exchange of the imino proton is strongly buffer sensitive. This property is used to derive the base-pair lifetime, which is in the range of milliseconds at 27 degrees C, 100 times smaller than published values. The enthalpy for the base-opening reaction (-86 kJ/mol) and the insensitivity of the reaction to magnesium suggest that the open state involves a small number of base-pairs. The similarities in the exchange from the two duplexes indicate that the same open state is responsible for exchange of purine and pyrimidine imino protons. For the lifetime of the open state and for the base-pair dissociation constant, we obtain only lower limits. At 27 degrees C they are three microseconds and 10(-3), respectively. The analysis that yields the much larger values published previously is based on the assumption that amino protons exchange only from open base-pairs. But theory and preliminary experiments indicate that it may occur from the closed duplex. The exchange of amino protons is slower than that of the imino protons. Exchange of the 2'-OH protons from the duplexes is much slower than from single-stranded poly(rU), and it is accelerated by magnesium. This could indicate hydrogen-bonding to backbone phosphate. Discrepancies between our results and those of previous studies are discussed.     

Proton exchange and base pair opening in a DNA triple helix

Nuclear magnetic resonance spectroscopy has been used to characterize opening reactions and stabilities of individual base pairs in two related DNA structures. The first is the triplex structure formed by the DNA 31-mer 5'-AGAGAGAACCCCTTCTCTCTTTTTCTCTCTT-3'. The structure belongs to the YRY (or parallel) family of triple helices. The second structure is the hairpin double helix formed by the DNA 20-mer 5'-AGAGAGAACCCCTTCTCTCT-3' and corresponds to the duplex part of the YRY triplex. The rates of exchange of imino protons with solvent in the two structures have been measured by magnetization transfer from water and by real-time exchange at 10 degrees C in 100 mM NaCl and 5 mM MgCl2 at pH 5.5 and in the presence of two exchange catalysts. The results indicate that the exchange of imino protons in protonated cytosines is most likely limited by the opening of Hoogsteen C+G base pairs. The base pair opening parameters estimated from imino proton exchange rates suggest that the stability of individual Hoogsteen base pairs in the DNA triplex is comparable to that of Watson-Crick base pairs in double-helical DNA. In the triplex structure, the exchange rates of imino protons in Watson-Crick base pairs are up to 5000-fold lower than those in double-helical DNA. This result suggests that formation of the triplex structure enhances the stability of Watson-Crick base pairs by up to 5 kcal/mol. This stabilization depends on the specific location of each triad in the triplex structure.     

Accurate Quantitation of Water-amide Proton Exchange Rates Using the Phase-Modulated CLEAN Chemical EXchange (CLEANEX-PM) Approach with a Fast-HSQC (FHSQC) Detection Scheme

Measurement of exchange rates between water and NH protons by magnetization transfer methods is often complicated by artifacts, such as intramolecular NOEs, and/or TOCSY transfer from C protons coincident with the water frequency, or exchange-relayed NOEs from fast exchanging hydroxyl or amine protons. By applying the Phase-Modulated CLEAN chemical EXchange (CLEANEX-PM) spin-locking sequence, 135°(x) 120°(-x) 110°(x) 110°(-x) 120°(x) 135°(-x) during the mixing period, these artifacts can be eliminated, revealing an unambiguous water-NH exchange spectrum. In this paper, the CLEANEX-PM mixing scheme is combined with Fast-HSQC (FHSQC) detection and used to obtain accurate chemical exchange rates from the initial slope analysis for a sample of 15N labeled staphylococcal nuclease. The results are compared to rates obtained using Water EXchange filter (WEX) II-FHSQC, and spin-echo-filtered WEX II-FHSQC measurements, and clearly identify the spurious NOE contributions in the exchange system.     

Contribution of tryptophan residues to the combining site of a monoclonal anti dinitrophenyl spin-label antibody

Two Fab fragments of the monoclonal anti dinitrophenyl (DNP) spin-label antibody AN02 were prepared by recombination of specifically deuterated heavy and light chains. In the recombinant H(I)L(II) all the tyrosines and phenylalanines were perdeuterated as were the tryptophan residues of the heavy chain. In the recombinant H(II)L(I) all the tyrosines and phenylalanines were perdeuterated as were the tryptophan residues of the light chain. Saturation of three resonances of H(I)L(II), assigned to tryptophan protons of the light chain, resulted in magnetization transfer to the aromatic proton at position 6 of the DNP ring and to the CH2 protons of the glycines linked to the DNP in a diamagnetic hapten (DNP-DG). Saturation of three resonances of H(II)L(I) assigned to tryptophan protons of the heavy chain resulted in magnetization transfer to the CH2 protons of the glycines in DNP-DG. From the dependence of the magnetization transfer on the irradiation time, the cross relaxation rates between the involved protons were estimated. The inferred distances between these protons of the hapten and certain tryptophan protons are 3-4 A. It is concluded that in the combining site of AN02 there is one tryptophan from the light chain and one tryptophan from the heavy chain that are very near the hapten. When all tyrosines and phenylalanines were perdeuterated and all tryptophan aromatic protons were deuterated except for the protons at positions 2 and 5, titration of the Fab fragments with variable amounts of paramagnetic hapten showed that one proton from the light chain tryptophan is near (less than 7 A) the unpaired electron and that three other protons are significantly closer than 15 A.(ABSTRACT TRUNCATED AT 250 WORDS)     

Observation of the phosphatidyl ethanolamine amino proton magnetic resonance in phospholipid vesicles: inside/outside ratios and proton transport.

The amino proton resonance of phosphatidyl ethanolamine in sonicated mixed phospholipid vesicles is observed 3.3 ppm downfield from H₂O. Above pH ～ 5 it is broadened beyond detectability as a result of exchange with H₂O protons. In low salt, resonances of amino protons inside the vesicles appear to persist as the pH is raised, while those on the outside disappear. Solvent catalized proton conduction along the surface is proposed, with an effective -NH₂ to -NH₃ transfer rate of about 8 × 10⁵ sec^?1 at 25°C.     

Exchange mechanisms for hydrogen bonding protons of cytidylic and guanylic acids.

The pH dependence of buffer catalysis of exchange of the C-4 amino protons of cyclic cytosine 2',3'-monophosphate (cCMP) and the N-1 proton of cyclic guanosine 2',3'-monophosphate (cGMP) conforms to an exchange mechanism, in which protonation of the nucleobases at C(N-3) AND G(N-7) establishes the important intermediates at neutral to acidic pH. Rate constants for transfer of the G(N-1) proton to H2O, OH-, phosphate, acetate, chloracetate, lactate, and cytosine (N-3) were obtained from 1H nuclear magnetic resonance line width measurements at 360 MHz and were used to estimate the pK or acidity of the exchange site in both the protonated and unprotonated nucleobase. These estimates reveal an increase in acidity of the G(N-1) site corresponding to 2 to 3 pK units as the G(N-7) site is protonated: At neutral pH the G(N-1) site of the protonated purine would be ionized (pK = 6.3). Determinations of phosphate, imidazole, and methylimidazole rate constants for transfer of the amino protons of cCMP provide a more approximate estimate of pK = 7 to 9 for the amino of the protonated pyrimidine. A comparison of the intrinsic amino acidity in the neutral and protonated cytosine is vitiated by the observation that OH- catalyzed exchange in the neutral base is not diffusion limited. This leads to the conclusion that protonation of the nucleobase effects a qualitative increase in the ability of the amino protons to form hydrogen bonds: from very poor in the neutral base to "normal" in the conjugate acid.     

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.     

Study of structure, base-pair opening kinetics and proton exchange mechanism of the d-(AATTGCAATT) self-complementary oligodeoxynucleotide in solution.

Using proton magnetic resonance, we have investigated the structure and the base-pair opening kinetics of the d-(AATTGCAATT) self-complementary duplex. All the non-exchangeable (except H5',5") and most exchangeable proton resonances have been assigned. The structure belongs to the B family. Imino proton exchange, measured by line broadening, longitudinal relaxation and magnetization transfer from water, is catalyzed by proton acceptors. The base-pair lifetimes, obtained by extrapolation of the exchange times to infinite concentration of ammonia are 2 and 3 milliseconds for internal A.Ts and 18 ms for G.C at 15 degrees C. In the absence of added catalysts, the imino proton of the first A.T base pair exchanges faster than that of the unpaired thymidine of the duplex formed by the sequence d-(AATTGCAATTT). This gives strong evidence for intrinsic exchange catalysis. The exchange of adenine amino protons from the closed state has been observed. Hence amino proton exchange is ill-suited for the investigation of base-pair opening kinetics.     

Backbone dynamics of plastocyanin in both oxidation states. Solution structure of the reduced form and comparison with the oxidized state

A model-free analysis based on (15)N R(1), (15)N R(2), and (15)N-(1)H nuclear Overhauser effects was performed on reduced (diamagnetic) and oxidized (paramagnetic) forms of plastocyanin from Synechocystis sp. PCC6803. The protein backbone is rigid, displaying a small degree of mobility in the sub-nanosecond time scale. The loops surrounding the copper ion, involved in physiological electron transfer, feature a higher extent of flexibility in the longer time scale in both redox states, as measured from D(2)O exchange of amide protons and from NH-H(2)O saturation transfer experiments. In contrast to the situation for other electron transfer proteins, no significant difference in the dynamic properties is found between the two redox forms. A solution structure was also determined for the reduced plastocyanin and compared with the solution structure of the oxidized form in order to assess possible structural changes related to the copper ion redox state. Within the attained resolution, the structure of the reduced plastocyanin is indistinguishable from that of the oxidized form, even though small chemical shift differences are observed. The present characterization provides information on both the structural and dynamic behavior of blue copper proteins in solution that is useful to understand further the role(s) of protein dynamics in electron transfer processes.     

Preparation and characterization of a uniformly 2 H/ 15 N-labeled RNA oligonucleotide for NMR studies.

An RNA oligonucleotide that contains the binding site for Escherichia coli ribosomal protein S8 was prepared with uniform 15N isotopic enrichment and uniform deuterium enrichment at all non-exchangeable sites using enzymatic methods. The RNA binding site, which contains 44 nt, forms a hairpin in solution and requires Mg2+for proper folding. The longitudinal magnetization recovery rates of the exchangeable protons were compared for the [2H,15N]-enriched RNA molecule and for the corresponding fully [2H,15N]-enriched RNA hairpin. It was found that 1H-1H dipolar relaxation significantly contributes to the recovery of exchangeable proton longitudinal magnetization. The exchangeable proton resonance line widths were less affected by deuteration, indicating that chemical exchange with H2O remains the dominant mechanism of transverse magnetization relaxation. Nevertheless, deuteration of this RNA hairpin was found to enhance the sensitivity of NOE-based experiments relative to the fully protonated hairpin and to simplify 2D NMR spectra. The increased signal-to-noise ratio facilitated the assignment of the cytidine amino resonances and several of the purine nucleotide amino resonances and permitted the identification of NOE crosspeaks that could not be observed in spectra of the fully protonated RNA hairpin.     

Netropsin specifically recognizes one of the two conformationally equivalent strands of poly(dA).poly(dT). One dimensional NMR study at 500 MHz involving NOE transfer between netropsin and DNA protons

Recent observations that the heteronomous structural model for poly(dA).poly(dT) is not found in solution and that in this DNA, the two strands are conformationally equivalent (J. Biomole. Str. Dyns. 2, 1057 (1985], has added a new dimension to the structural dynamics of DNA-netropsin complex. Does the antibiotic somehow distinguish between the two strands and specifically interact with only one of the conformationally equivalent strands? Model-building studies suggest that netropsin can either bind to the dA-strand in the minor groove such that H-bonds are formed between the imino protons N4-H, N6-H, N8-H of netropsin and N3 atoms of A or can bind to the dT-strand in the minor groove and form H-bonds between the imino-protons N4-H, N6-H, N8-H of netropsin and O2 atoms of T. If netropsin binds to the dA-strand, AH2 atoms of poly(dA).poly(dT) would be in closer proximity to the imino protons N4-H, N6-H, N8-H and pyrrole ring protons C5-H, C11-H of netropsin than they would be, if netropsin binds to the dT-strand. In order to distinguish these possibilities experiments were conducted which involved NOE energy transfer between netropsin and DNA protons in the drug-DNA complex. Difference NOE spectra of netropsin-poly(dA).poly(dT) complex in which AH2 was irradiated indicate that dominant NOEs were observed at the imino and pyrrole ring protons of netropsin. When the netropsin pyrrole ring protons were irradiated, the magnetization transfer was at AH2 of DNA. These observations suggest that netropsin binds to the dA-strand of poly(dA).poly(dT) even though dA/dT strands are conformationally equivalent.     

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)     

Timing of Electron and Proton Transfer in the ba(3) Cytochrome c Oxidase from Thermus thermophilus

Heme-copper oxidases are membrane-bound proteins that catalyze the reduction of O(2) to H(2)O, a highly exergonic reaction. Part of the free energy of this reaction is used for pumping of protons across the membrane. The ba(3) oxidase from Thermus thermophilus presumably uses a single proton pathway for the transfer of substrate protons used during O(2) reduction as well as for the transfer of the protons that are pumped across the membrane. The pumping stoichiometry (0.5 H(+)/electron) is lower than that of most other (mitochondrial-like) oxidases characterized to date (1?H(+)/electron). We studied the pH dependence and deuterium isotope effect of the kinetics of electron and proton transfer reactions in the ba(3) oxidase. The results from these studies suggest that the movement of protons to the catalytic site and movement to a site located some distance from the catalytic site [proposed to be a "proton-loading site" (PLS) for pumped protons] are separated in time, which allows individual investigation of these reactions. A scenario in which the uptake and release of a pumped proton occurs upon every second transfer of an electron to the catalytic site would explain the decreased proton pumping stoichiometry compared to that of mitochondrial-like oxidases.     

31P-NMR spectrum of phosphocreatine: Deuterium-induced splitting of the signal

It has been found in experiments with high resolution ³¹P-NMR spectroscopy (200 MHz) that the phosphocreatine peak is splitted into two different peaks in the mixtures of H₂O and D₂O and is single but with different chemical shifts in pure H₂O and D₂O. This phenomenon is explained by substitution of protons of guanidino group in phosphocreatine by deuterium. The effect of splitting disappeared at extreme pH values (>8.5 or <4.0) and at temperatures higher than 45°C due to accelerated proton-deuterium exchange. Creatine kinase added to phosphocreatine solution also lowered its temperature of peaks' collapse by 5°–10°C. A saturation (spin) transfer method was used to show that the phosphoryl group transfer to ADP in creatine kinase active center is slower with deuterium-substituted phosphocreatine than with H-phosphocreatine. The data are taken to show the importance of the proton transfer step in the creatine kinase reaction mechanism and acceleration of phosphocreatine proton-deuterium exchange by creatine kinase.     

Proton transfer within the active-site cavity of carbonic anhydrase III

The maximal turnover rate of CO2 hydration catalyzed by the carbonic anhydrases is limited by proton transfer steps from the zinc-bound water to solution, steps that regenerate the catalytically active zinc-bound hydroxide. Catalysis of CO2 hydration by wild-type human carbonic anhydrase III (HCA III) (k(cat) = 2 ms (-1)) is the least efficient among the carbonic anhydrases in its class, in part because it lacks an efficient proton shuttle residue. We have used site-directed mutagenesis to test positions within the active-site cavity of HCA III for their ability to carry out proton transfer by replacing various residues with histidine. Catalysis by wild-type HCA III and these six variants was determined from the initial velocity of hydration of CO2 measured by stopped-flow spectrophotometry and from the exchange of 18O between CO2 and H2O at chemical equilibrium by mass spectrometry. The results show that histidine at three positions (Lys64His, Arg67His and Phe131His) have the capacity to transfer protons during catalysis, enhancing maximal velocity of CO2 hydration and 18O exchange from 4- to 15-fold compared with wild-type HCA III. Histidine residues at the other three positions (Trp5His, Tyr7His, Phe20His) showed no firm evidence for proton transfer. These results are discussed in terms of the stereochemistry of the active-site cavity and possible proton transfer pathways.     

31P saturation transfer spectroscopy predicts differential intracellular macromolecular association of ATP and ADP in skeletal muscle

The kinetics of phosphoryl exchange involving ATP and ADP have been investigated successfully by in vivo ³¹P magnetic resonance spectroscopy using magnetization transfer. However, magnetization transfer effects seen on the signals of ATP also could arise from intramolecular cross-relaxation. This relaxation process carries information on the association state of ATP in the cell. To disentangle contributions of chemical exchange and cross-relaxation to magnetization transfer effects seen in ³¹P magnetic resonance spectroscopy of skeletal muscle, we performed saturation transfer experiments on wild type and double-mutant mice lacking the cytosolic muscle creatine kinase and adenylate kinase isoforms. We find that cross-relaxation, observed as nuclear Overhauser effects (NOEs), is responsible for magnetization transfer between ATP phosphates both in wild type and in mutant mice. Analysis of ³¹P relaxation properties identifies these effects as transferred NOEs, i.e. underlying this process is an exchange between free cellular ATP and ATP bound to slowly rotating macromolecules. This explains the β-ATP signal decrease upon saturation of the γ-ATP resonance. Although this usually is attributed to β-ADP ↔ β-ATP phosphoryl exchange, we did not detect an effect of this exchange on the β-ATP signal as expected for free [ADP], derived from the creatine kinase equilibrium reaction. This indicates that in resting muscle, conditions prevail that prevent saturation of β-ADP spins and puts into question the derivation of free [ADP] from the creatine kinase equilibrium. We present a model, matching the experimental result, for ADP ↔ ATP exchange, in which ADP is only transiently present in the cytosol.