1H NMR studies of transfer RNA III: the observed and the computed spectra of the hydrogen-bonded NH resonances of baker''s yeast transfer-RNA Phe.

The hydrogen-bonded NH resonances of Baker's yeast tRNAphe in H2O solution with Mg++ have been measured by a 360 MHz spectrometer at 23 degrees C. Totally, fifteen peaks and one shoulder can be resolved which represent 25 +/- 1 protons. Based on the refined atomic coordinates of the tRNAphe in the orthorhombic crystal, on the recent advances in the distance dependence of the ring-current magnetic field effects and on the adopted values for the isolated hydrogen-bonded NH resonances, a computed spectrum consisting of 23 protons was constructed. A quantitative comparison by computer was made between the computed spectrum and the spectrum simulated from the observed spectrum. These two spectra are closely similar but not identical. We suggest that the conformation of yeast tRNAphe in aqueous solution is closely similar but not identical to that found in the crystal, especially in the T psi C region and D region. Also the NH resonances in 3-4 proposed hydrogen bonds (most likely for tertiary structure) may exchange very rapidly in aqueous solution.     

Study of transfer ribonucleic acid unfolding by dynamic nuclear magnetic resonance

Nuclear magnetic resonance (NMR) measurements of proton exchange were performed on yeast tRNAPhe, and in much less detail on Escherichia coli tRNAfMet, over a range of Mg2+ concentrations and temperatures, at neutral pH and 0.1 M NaCl. The resonances studied were those of ring nitrogen protons, resonating between 10 and 15 ppm downfield from sodium 3-(trimethylsilyl)-1-propanesulfonate, which partake in hydrogen bonding between bases of secondary and tertiary pairs. Methods include saturation--recovery, line width, and real-time observation after a change to deuterated solvent. The relevant theory is briefly reviewed. We believe that most of the higher temperature rates reflect major unfolding of the molecule. For E. coli tRNAfMet, the temperature dependence of the rate for the U8--A14 resonance maps well onto previous optical T-jump studies for a transition assigned to tertiary melting. For yeast tRNAPhe, exchange rates of several resolved protons could be studied from 30 to 45 degrees C in zero Mg2+ concentration and had activation energies on the order of 40 kcal/mol. Initially, the tertiary structure melts, followed shortly by the acceptor stem. At high Mg2+ concentration, relatively few exchange rates are measurable below the general cooperative melt at about 60 degrees C; these are attributed to tertiary changes. Real-time observations suggest a change in the exchange mechanism at room temperature with a lower activation energy. The results are compared with those obtained by other methods directed toward assaying ribonucleic acid dynamics.     

Amide proton exchange rates of a bound pepsin inhibitor determined by isotope-edited proton NMR experiments

From a series of isotope-edited proton NMR spectra, amide proton exchange rates were measured at 20 degrees C, 30 degrees C, and 40 degrees C for a tightly bound 15N-labeled tripeptide inhibitor of porcine pepsin (IC50 = 1.7 X 10(-) M). Markedly different NH exchange rates were observed for the three amide protons of the bound inhibitor. The P1 NH exchanged much more slowly than the P2 NH and P3 NH. These results are discussed in terms of the relative solvent accessibility in the active site and the role of the NH protons of the inhibitor for hydrogen bonding to the enzyme. In this study a useful approach is demonstrated for obtaining NH exchange rates on ligands bound to biomacromolecules, the knowledge of which could be of potential utility in the design of therapeutically useful nonpeptide enzyme inhibitors from peptide leads.     

Measurement of the helix opening rate in Z-DNA by 1H nuclear magnetic resonance relaxation spectroscopy

The exchange rate of the hydrogen-bonded guanine imino protons N(1) in the high-salt form of Poly(dG-dC) was measured by following the non-selective inversion-recovery of their 1H NMR signal at 360 MHz, in the temperature range between 77 degrees C and 90 degrees C. In a 4.5M NaCl solution, Poly(dG-dC) is believed to adapt the left-handed Z-conformation, and the results reported here represent the first quantitative measurements of this rate process for Z-DNA by Nuclear Magnetic Resonance, complementing previous measurements made by tritium exchange at 0 degrees C (Ramstein, J. and Leng, M. (1980) Nature 288, 413-414). The results confirm that this process is much slower in the Z-form, compared to the B-structure, and that this difference in rates results mainly from a large decrease in the entropy of activation for Z-DNA.     

Proton exchange rates in transfer RNA as a function of spermidine and magnesium

Solvent exchange rates of selected protons were measured by NMR saturation recovery for E. coli tRNAVal, E. colifMet and yeast tRNAPhe, at temperatures from 20 to 40 degrees C, in the presence of 0.12M Na+ and various levels of added spermidine. tRNAVal was also studied with added Mg++. The exchange rates in zero spermidine and Mg++ indicate early melting of the U8 A14 interaction, in accord with thermodynamic melting studies. Exchange rates for secondary protons suggest early melting of the T stem in tRNAfMet and the acceptor stem in tRNAPhe, in contradiction with melting transition assignments from thermodynamic work. Addition of 10 spermidines per tRNA stabilizes the secondary and tertiary interactions more effectively than added Na+, but less so than Mg++. Added spermidine has the curious effect of increasing the exchange rate of the psi 55 N1 proton, while protecting the psi 55 N3 proton from exchange in all three tRNA's. Added Mg++ has the same effect on tRNAVal.     

Conformation and dynamics of the Pribnow box region of the self-complementary d(C-G-A-T-T-A-T-A-A-T-C-G) duplex in solution

Nuclear magnetic resonance (NMR) has been used to monitor the conformation and dynamics of the d(C1-G2-A3-T4-T5-A6-T6-A5-A4-T3-C2-G1) self-complementary dodecanucleotide duplex (henceforth called Pribnow 12-mer), which contains a TATAAT Pribnow box and a central core of eight dA X dT base pairs. The exchangeable imino and nonexchangeable base protons have been assigned from one-dimensional intra and inter base pair nuclear Overhauser effect (NOE) measurements. Premelting conformational changes are observed at all the dA X dT base pairs in the central octanucleotide core in the Pribnow 12-mer duplex with the duplex to strand transition occurring at 55 degrees C in 0.1 M phosphate solution. The magnitude of the NOE measurements between minor groove H-2 protons of adjacent adenosines demonstrates that the base pairs are propeller twisted with the same handedness as observed in the crystalline state. The thymidine imino proton hydrogen exchange at the dA X dT base pairs has been measured from saturation recovery measurements as a function of temperature. The exchange rates and activation barriers show small variations among the four different dA X dT base pairs in the Pribnow 12-mer duplex.(ABSTRACT TRUNCATED AT 250 WORDS)     

Hydrogen exchange kinetics of core peptide protons in Streptomyces subtilisin inhibitor

The hydrogen isotope exchange kinetics of the 10 slowest exchanging resonances in the 1H NMR spectrum of Streptomyces subtilisin inhibitor (SSI) have been determined at pH 7-11 and 30-60 degrees C. These resonances are assigned to peptide amide protons in the beta-sheet core that comprises the extensive protein-protein interface of the tightly bound SSI dimer. The core protons are atypical in that their exchange rates are orders of magnitude slower than those for all other SSI protons. When they do exchange at temperatures greater than 50 degrees C, they do so as a set and with a very high temperature coefficient. The pH dependence of the exchange rate constants is also atypical. Exchange rates are approximately first order in hydroxyl ion dependence at pH less than 8.5 and greater than 9.5 and pH independent between pH 8.5 and 9.5. The pH dependence and temperature dependence of the SSI proton exchange rates are interpreted by the two-process model [Woodward, C. K., & Hilton, B. D. (1980) Biophys. J. 32, 561-575]. The results suggest that in the average solution structure of SSI, an unusual mobility of secondary structural elements at the protein surface is, in a sense, compensated by an unusual rigidity and inaccessibility of the beta-sheet core at the dimer interface.     

Role of arginine 67 in the stabilization of chymotrypsin inhibitor 2: examination of amide proton exchange rates and denaturation thermodynamics of an engineered protein

We have examined the contribution to protein stability of an interaction involving a charged hydrogen bond from an arginyl side chain (Arg67) in the serine proteinase inhibitor chymotrypsin inhibitor 2 (CI-2), by replacing this side chain with an alanyl residue by protein engineering. Using nuclear magnetic resonance spectroscopy (NMR), we have examined the effect of this mutation on the hydrogen-deuterium exchange rates of several backbone amide protons in the native and engineered proteins at 50 degrees C. These exchange rates provide a localized probe at multiple discrete sites throughout the protein and from comparison of native and mutant exchange rates allow calculation of the difference in free energy of exchange (delta delta Gex) resulting from the mutation. The results show that for the majority of amides observed this mutation results in delta delta Gex of ca. 1.7 kcal mol-1 over the whole CI-2 molecule. However, for two relatively exposed amide protons the exchange rates are found to be far less perturbed, implying that local unfolding mechanisms predominate for these protons. Direct measurement of the stability of both proteins to denaturation by guanidinum hydrochloride shows that the interaction contributes 1.4 kcal mol-1 to the stability of the molecule. This value is comparable to those obtained from the NMR exchange measurements and indicates that the exchange processes reflect the differences in stability between the native and mutant proteins.(ABSTRACT TRUNCATED AT 250 WORDS)     

The effect of cytochrome P-450cam on the NMR relaxation rate of water protons.

Cytochrome P-450cam in the native, substrate-free state (Fe3+, S = 1/2) substantially reduces the NMR relaxation times, T1 and T2, of water protons. Temperature and frequency dependences of T1 and T2 were measured; they are consistent with a model of one or two protons exchanging between a binding site on a heme ligand and bulk water. The relevant parameters of this model have been deduced from the data. The spin relaxation time of the heme iron, tau S similar to 0.5 ns at 25 degrees C, is unusually long for a low spin ferric heme protein but is compatible with the line widths measured for paramagnetically shifted heme resonances. The proton residence time on the ligand, tau M similar to 1 microsecond at 25 degrees C, follows an Arrhenius law with activation energy EM similar to 15 kcal/mol. A scalar hyperfine interaction A/h = 2.2 MHz (3.1 MHz for one-proton exchange) of the found proton(s) with the heme iron is deduced from the difference between T1 and T2 observed in the fast exchange limit. The iron-proton distance is found to be 2.9 A (2.6 A for one-proton exchange). Variation of pH between pH 6.4 and 8.6 does not affect T1. The bearing of these results on the question of the axial heme ligand is discussed.     

"Asymmetric" opening reaction mechanism of Z-DNA base pairs: a hydrogen exchange study

With the tritium-Sephadex method, the hydrogen-exchange kinetics of the five NH protons of guanine and cytosine residues in Z-form poly(dG-dC) X poly (dG-dC) were measured as a function of temperature and catalyst concentration. Over the measured temperature range from 0 to 34 degrees C, two classes of protons with constant amplitudes are found. The three protons of the fast class, which were assigned to the guanine amino and imino protons, have an exchange half-time in the minute time range (at 20 degrees C the half-time is 2.5 min) and an activation energy of 18 kcal mol-1. Since these two types of protons exchange at the same rate in spite of their grossly different pK values, the exchange of these protons must be limited by the same nucleic acid conformational change. The two cytosine amino protons of the slow class are especially slow with exchange half-times in the hour time range (at 20 degrees C the exchange half-time is 1 h) and the activation energy is 20 kcal mol-1. The exchange of these two protons is not limited by some nucleic acid conformational change as shown by the marked exchange acceleration of these protons upon addition of 0.2 M imidazole. In addition, we have also reexamined the hydrogen-deuterium exchange kinetics of the amino protons of guanosine cyclic 2',3'-monophosphate by a spectral difference method using a stopped-flow spectrophotometer. The measured kinetic process is monophasic with a rate constant of 3 s-1 at 20 degrees C, which is in the same range as the predicted rate constant of the guanine amino protons.(ABSTRACT TRUNCATED AT 250 WORDS)     

Hydrogen exchange behavior of [U-15N]-labeled oxidized and reduced iso-1-cytochrome c

Heteronuclear NMR spectroscopy was used to measure the hydrogen-deuterium exchange rates of backbone amide hydrogens in both oxidized and reduced [U-15N]iso-1-cytochrome c from the yeast Saccharomyces cerevisiae. The exchange data confirm previously reported data [Marmorino et al. (1993) Protein Sci. 2, 1966-1974], resolve several inconsistencies, and provide more thorough coverage of exchange rates throughout the cytochrome c protein in both oxidation states. Combining the data previously collected on unlabeled C102T with the current data collected on [U-15N]C102T, exchange rates for 53 protons in the oxidized state and 52 protons in the reduced state can now be reported. Most significantly, hydrogen exchange measurements on [U-15N]iso-1-cytochrome c allowed the observation of exchange behavior of the secondary structures, such as large loops, that are not extensively hydrogen-bonded. For the helices, the most slowly exchanging protons are found in the middle of the helix, with more rapidly exchanging protons at the helix ends. The observation for the Omega-loops in cytochrome c is just the opposite. In the loops, the ends contain the most slowly exchanging protons and the loop middles allow more rapid exchange. This is found to be true in cytochrome c loops, even though the loop ends are not attached to any regular secondary structures. Some of the exchange data are strikingly inconsistent with data collected on the C102S variant at a different pH, which suggests pH-dependent dynamic differences in the protein structure. This new hydrogen exchange data for loop residues could have implications for the substructure model of eukaryotic cytochrome c folding. Isotopic labeling of variant forms of cytochrome c can now be used to answer many questions about the structure and folding of this model protein.     

Exchange behavior of the H-bonded amide protons in the 3 to 13 helix of ribonuclease S

The preceding article shows that there are eight highly protected amide protons in the S-peptide moiety of RNAase S at pH 5, 0 degrees C. The residues with protected NH protons are 7 to 13, whose amide protons are H-bonded in the 3 to 13 alpha-helix, and Asp 14, whose NH proton is H-bonded to the CO group of Val47. We describe here the exchange behavior of these eight protected protons as a function of pH. Exchange rates of the individual NH protons are measured by 1H nuclear magnetic resonance in D2O. A procedure is used for specifically labeling with 1H only these eight NH protons. The resonance assignments of the eight protons are made chiefly by partial exchange, through correlating the resonance intensities in spectra taken when the peptide is bound and when it is dissociated from S-protein in 3.5 M-urea-d4, in D2O, pH 2.3, -4 degrees C. The two remaining assignments are made and some other assignments are checked by measurements of the nuclear Overhauser effect between adjacent NH protons of the alpha-helix. There is a transition in exchange behavior between pH 3, where the helix is weakly protected against exchange, and pH 5 where the helix is much more stable. At pH 3.1, 20 degrees C, exchange rates are uniform within the helix within a factor of two, after correction for different intrinsic exchange rates. The degree of protection within the helix is only 10 to 20-fold at this pH. At pH 5.1, 20 degrees C, the helix is more stable by two orders of magnitude and exchange occurs preferentially from the N-terminal end. At both pH values the NH proton of Asp 14, which is just outside the helix, is less protected by an order of magnitude than the adjacent NH protons inside the helix. Opening of the helix can be observed below pH 3.7 by changes in chemical shifts of the NH protons in the helix. At pH 2.4 the changes are 25% of those expected for complete opening. Helix opening is a fast reaction on the n.m.r. time scale (tau much less than 1 ms) unlike the generalized unfolding of RNAase S which is a slow reaction. Dissociation of S-peptide from S-protein in native RNAase S at pH 3.0 also is a slow reaction. Opening of the helix below pH 3.7 is a two-state reaction, as judged by comparing chemical shifts with exchange rates. The exchange rates at pH 3.1 are predicted correctly from the changes in chemical shift by assuming that helix opening is a two-state reaction. At pH values above 3.7, the nature of the helix opening reaction changes. These results indicate that at least one partially unfolded state of RNAase S is populated in the low pH unfolding transition.     

Dynamic behavior of the imino protons of the gamma OR3 17mer in H2O solution studied by high-resolution NMR

The imino proton resonances of gamma OR3 17mer in water were observed at 500 MHz with the time-shared Redfield pulse train. All of the 17 imino proton resonances could be assigned specifically to individual base pairs by utilizing the trace of NOE connectivities between the imino and adenine C2H protons and between imino protons themselves. AT1 and 17 showed abnormally high chemical shifts in comparison with the other AT pairs. On raising the temperature, broadening of the signal occurred in a sequential manner from the terminals except for AT10 and AT11, which were broadened at a lower temperature than GC12. The relaxation rates of the imino protons were measured by the inversion recovery method. The rates at higher temperatures represent the exchange rates of the imino protons. From the temperature dependences, activation energies of about 15 kcal/mol for the AT imino protons and 23-26 kcal/mol for the GC imino protons were obtained.     

Hydrogen isotope exchange kinetics of single protons in bovine pancreatic trypsin inhibitor.

The exchange kinetics of the slowest exchanging BPTI beta-sheet protons are complex compared to model peptides; the activation energy, E alpha, and the pH dependence are temperature dependent. We have measured the exchange kinetics in the range pH 1--11, 33--71 degrees C, particularly the temperature dependence. The data are fit to a model in which exchange of each proton is determined by two discrete dynamical processes, one with E alpha approximately 65 kcal/mol and less than first order dependence on catalyst ion, and one with E alpha 20--30 kcal/mol and approaching first order in catalyst ion. The low activation energy process is the mechanism of interest in the native conformation of globular proteins and involves low energy, small amplitude fluctuations; the high activation energy process involves major unfolding. The model is simple, has a precedent in the hydrogen exchange literature, and explains quantitatively the complex feature of the exchange kinetics of single protons in BPTI, including the following. For the slowest exchanging protons, in the range 36 degrees--68 degrees C, E alpha is approximately 65 kcal/mol at pH approximately 4, 20--30 kcal/mol at pH greater than 10, and rises to approximately 65 kcal/mol with increasing temperature at pH 6--10; the Arrhenius plots converge around 70 degrees C; the pH of minimum rate, pHmin, is greater than 1 pH unit higher at 68 degrees C than for model compounds; and at high pH, the pH-rate profiles shift to steeper slope; the exchange rates around pHmin are correlated to the thermal unfolding temperature in BPTI derivatives (Wagner and Wüthrich, 1979, J. Mol. Biol. 130:31). For the more rapidly exchanging protons in BPTI the model accounts for the observation of normal pHmin and E alpha of 20--30 kcal/mol at all pH's. The important results of our analysis are (a) rates for exchange from the folded state of proteins are not correlated to thermal lability, as proposed by Wuthrich et al. (1979, J. Mol. Biol. 134:75); (b) the unfolding rate for the BPTI cooperative thermal transition is equal to the observed exchange rates of the slowest exchanging protons between pH 8.4--9.6, 51 degrees C; (c) the rates for exchange of single protons from folded BPTI are consistent with our previous hydrogen-tritium exchange results and with a penetration model of the dynamic processes limiting hydrogen exchange.     

Influence of the polyamines spermine and spermidine on yeast tRNAPhe as revealed from its imino proton NMR spectrum.

A comparison of imino proton NMR spectra of yeast tRNAPhe recorded at various solution conditions indicates, that polyamines have a limited effect on the structure of this tRNA molecule. Polyamines are found to catalyse the solvent exchange of several imino protons in yeast tRNAPhe not only of non hydrogen bonded imino protons, but also of imino protons of the GU and of some AU and tertiary base pairs. It is concluded that at low levels of catalysing components the exchange rates of the latter protons are not determined by the base pair lifetime. In the presence of high levels of spermidine the solvent exchange rates of imino protons of several base pairs in the molecule were assessed as a function of the temperature. Apparent activation energies derived from these rates were found to be less than 80 kJ/mol, which is indicative for (transient) independent opening of the corresponding base pairs. In the acceptor helix the GU base pair acts as a dynamic dislocation. The AU base pairs at one side of the GU base pair exhibit faster transient opening than the GC base pairs on the other side of this wobble pair. The base pairs m2GC10 and GC11 from the D stem and GC28 from the anticodon stem show relatively slow opening up to high temperatures. Model studies suggest that 1-methyladenosine, an element of tRNA itself, catalyses imino proton solvent exchange in a way similar to polyamines.     

Proton nuclear magnetic resonance investigation of the conformation and dynamics in the synthetic deoxyribonucleic acid decamers d(ATATCGATAT) and d(ATATGCATAT)

A variety of one-dimensional proton NMR methods have been used to investigate the properties of two synthetic DNA decamers, d(ATATCGATAT) and d(ATATGCATAT). These results, in conjunction with the results of two-dimensional NMR experiments, permit complete assignment of the base proton resonances. Low-field resonances were assigned by sequential "melting" of the A . T base pairs and by comparison of the spectra of the two decamers. Below 20 degree C spin-lattice relaxation is dominated by through-space dipolar interactions. A substantial isotope effect on the G imino proton relaxation is observed in 75% D2O, confirming the importance of the exchangeable amino protons in the relaxation process. A somewhat smaller isotope effect is observed on the T imino proton relaxation. At elevated temperatures spin-lattice relaxation of the imino protons is due to proton exchange with solvent. Apparent activation energies for exchange vary from 36 kcal/base pair for base pairs (3,8) to 64 kcal/mol for the most interior base pairs (5,6), indicating that disruption of part, or all, of the double helix contributes significantly to the exchange of the imino protons in these decamers. By contrast, single base pair opening events are the major low-temperature pathways for exchange from A X T and G X C base pairs in the more stable higher molecular weight DNA examined in other studies. The temperature dependence of the chemical shifts and line widths of certain aromatic resonances indicates that the interconversion between the helix and coil states is not in fast exchange below the melting temperature, Tm. Within experimental error, no differential melting of base pairs was found in either molecule, and both exhibited melting points Tm = 50-52 degrees C. Spin-spin and spin-lattice relaxation rates of the nonexchangeable protons (TH6, AH8, and AH2) are consistent with values calculated by using an isotropic rotor model with a rotational correlation time of 6 ns and interproton distances appropriate for B-family DNA. The faster decay of AH8 compared with GH8 is attributed to an interaction between the thymine methyl protons and the AH8 protons in adjacent adenines (5'ApT3'). The base protons (AH8, GH8, and TH6) appear to be located close (1.9-2.3 A) to sugar H2',2" protons.(ABSTRACT TRUNCATED AT 400 WORDS)     

Temperature dependence of ADP/ATP translocation in mitochondria

The temperature dependence of the adenine nucleotide exchange in mitochondria has been determined by employing a rapid mixing, quenching and sampling apparatus and the inhibitor quench-back exchange method. Thus the exchange is resolved down to 0.1 s. Rates are evaluated from accumulating the time-dependent progress at about 10 points. The exchange rate in liver mitochondria was determined from -10 degrees C to + 10 degrees C in the presence of 20% glycol, from 0 degrees C to 25 degrees C, and from 20 degrees C to 40 degrees C under partial inhibition by carboxyatractylate. The total range between -10 degrees C to + 40 degrees C has only one temperature break at 13 degrees C. From the Arrhenius plot between -10 degrees C to + 13 degrees C, EA approximately equal to 140 kJ and above 13 degrees C, EA approximately equal to 56 kJ is evaluated, corresponding to a Q10 of 8 and 2 respectively. In beef heart mitochondria the exchange rate was measured between 0 degrees C and 20 degrees C, and between 15 degrees C and 30 degrees C under partial inhibition with carboxyatractylate. There is a temperature break around 14 degrees C with EA approximately equal to 143 kJ between 0 degrees C and 14 degrees C and EA approximately equal to 60 kJ from 15 degrees C to 30 degrees C. The extrapolated translocation rates at 37 degrees C are 500 and 1800 mumol min-1 (g protein)-1 for rat liver and for beef heart mitochondria respectively. The temperature break is suggested to reflect a conformation change since there is no reversed break at low temperature, the temperature break changes in sonic particles and no lipid phase transition at 14 degrees C in mitochondria has been reported.     

Hydrogen exchange in native and denatured states of hen egg-white lysozyme.

The hydrogen exchange kinetics of 68 individual amide protons in the native state of hen lysozyme have been measured at pH 7.5 and 30 degrees C by 2D NMR methods. These constitute the most protected subset of amides, with exchange half lives some 10(5)-10(7) times longer than anticipated from studies of small model peptides. The observed distribution of rates under these conditions can be rationalized to a large extent in terms of the hydrogen bonding of individual amides and their burial from bulk solvent. Exchange rates have also been measured in a reversibly denatured state of lysozyme; this was made possible under very mild conditions, pH 2.0 35 degrees C, by lowering the stability of the native state through selective cleavage of the Cys-6-Cys-127 disulfide cross-link (CM6-127 lysozyme). In this state the exchange rates for the majority of amides approach, within a factor of 5, the values anticipated from small model peptides. For a few amides, however, there is evidence for significant retardation (up to nearly 20-fold) relative to the predicted rates. The pattern of protection observed under these conditions does not reflect the behavior of the protein under strongly native conditions, suggesting that regions of native-like structure do not persist significantly in the denatured state of CM6-127 lysozyme. The pattern of exchange rates from the native protein at high temperature, pH 3.8 69 degrees C, resembles that of the acid-denatured state, suggesting that under these conditions the exchange kinetics are dominated by transient global unfolding. The rates of folding and unfolding under these conditions were determined independently by magnetization transfer NMR methods, enabling the intrinsic exchange rates from the denatured state to be deduced on the basis of this model, under conditions where the predominant equilibrium species is the native state. Again, in the case of most amides these rates showed only limited deviation from those predicted by a simple random coil model. This reinforces the view that these denatured states of lysozyme have little persistent residual order and contrasts with the behavior found for compact partially folded states of proteins, including an intermediate detected transiently during the refolding of hen lysozyme.     

Physicochemical characterization of 1,2-diphytanoyl-sn-glycero-3-phosphocholine in model membrane systems.

We report here on a series of studies aimed at characterization of the structural and dynamical properties of the synthetic lipid diphytanoyl phosphatidylcholine, in multilamellar dispersions and vesicle suspensions. The lipid exhibits no detectable gel to liquid crystalline phase transition over a large temperature range (-120 degrees C to +120 degrees C). Examination of proton nuclear magnetic resonance (NMR) free induction decays obtained from multilayer dispersions of diphytanoyl phosphatidylcholine provided an estimate of the methylene proton order parameter. The estimated magnitude of 0.21 is comparable to those determined for other phospholipids. Sonication of aqueous dispersions of diphytanoyl phosphatidylcholine led to formation of bilayer vesicles as determined by the measurement of the outer/inner choline methyl proton resonances, vesicle sizes in electron micrographs, and comparison of proton NMR linewidths between multilayer and sonicated dispersions. Ultracentrifugation studies of diphytanoyl phosphatidylcholine vesicles in H2O and 2H2O media yielded a value of 1.013 +/- 0.026 ml/g for the partial specific volume of this lipid. We have measured spin lattice relaxation rates for the methyl and methylenemethyne protons of the hydrocarbon chains of diphytanoyl phosphatidylcholine in bilayer vesicles over a range of temperatures and at two NMR frequencies (100 and 220 MHz). The observed relaxation rates for the methylene protons in this system were approximately twice those previously reported for dipalmitoyl phosphatidylcholine at comparable temperatures and resonance frequencies, whereas the relaxation rates measured for the methyl protons were greater than those of the straight chain lipid by an order of magnitude. Measurement of the spin lattice relaxation rates of the hydrocarbon protons of the diphytanoyl phosphatidylcholine in a 10 mol% mixture of the branched-chain lipid in a deuterated host lipid, diperdeuteropalmitoyl phosphatidylcholine, showed a discontinuity in the temperature dependence of the proton NMR longitudinal relaxation rates of the branched-chain lipid in the region of the gel to liquid crystalline phase transition temperature of the deuterated dipalmitoyl phosphatidylcholine host lipid. This result may be taken as evidence of lateral phase separation of a liquid cyrstalline phase enriched in diphytanoyl phosphatidylcholine from a gel phase enriched in diperdeuteropalmitoyl phosphatidylcholine at temperatures below the phase transition temperature of deuterated host lipid. This conclusion is supported by the observation of an abrupt change in the hydrocarbon methylene linewidth (at 100 MHz) of 10 mol% diphytanoyl phosphatidylcholine in diperdeuteropalmitoyl phosphatidylcholine over the temperature range where lateral phase separation is taking place according to differential thermograms.     

Internal motions of transfer RNA: a study of exchanging protons by magnetic resonance

Proton exchange is a probe of macromolecular structure and kinetics. Its value is enhanced when the exchanging protons can be identified by nmr. After dilution of tRNA-H2O samples in D2O, slowly exchanging imino protons are observed, with exchange times ranging from minutes to days. In many cases they originate from the dihydro-uracil region. Most slow exchangers are sensitive to buffer catalysis. Extrapolation to infinite buffer concentration yields the life-time of the closed form, in a two-state model of each base-pair. As predicted by the model, the lifetime obtained by extrapolation is independent of the buffer. Typical lifetimes are 14 minutes for CG11 of yeast tRNAPhe at 17 degrees C, or 5 minutes for U8-A14 of yeast tRNA(Asp) at 20 degrees C, without magnesium. For most slow exchangers, magnesium increases the lifetime of the closed form, but moderately, by factors never more than five. The exchange rates of other, fast-exchanging, imino protons, as determined by line-broadening, are found to depend on buffer concentration. Base-pair lifetimes are determined as above. For instance UA6 of yeast tRNA(Phe) has a lifetime of 14 ms at 17 degrees C. Base-pairs 4 and 6 have shorter lifetimes than the rest of the acceptor stem. Imidazole is a good catalyst for proton exchange of both the long-and the short-lived base-pairs, whereas phosphate is not. Tris is efficient except for cases where, possibly, access is impeded by its size; magnesium reduces the efficiency of catalysis by tris buffer. From the variation of exchange time vs buffer concentration, one determines the buffer concentration for which the exchange rate from the open state is equal to the closing rate. Remarquably, this concentration takes comparable values for most base-pairs, whether short-lived or long-lived. Buffer effects have also been observed in poly(rA).poly(rU), for which we derive a lifetime of 2.5 ms at 27 degrees C, and in other polynucleotides. Some of the exchange times identified in the literature as base-pair lifetimes may instead reflect incomplete catalysis.