Structurally homologous toxins isolated from the Taiwan cobra (Naja naja atra) differ significantly in their structural stability

Cardiotoxin and neurotoxin analogues isolated from snake venom sources are highly homologous proteins (>50% homology) with similar three-dimensional structures but exhibit drastically different biological properties. In the present study, we compare the conformational stability of cardiotoxin analogue III (CTX III) and cobrotoxin (CBTX), a neurotoxin analogue, from the Taiwan cobra (Naja naja atra), using circular dichroism spectroscopy and hydrogen-deuterium (H/D) exchange techniques in conjunction with two-dimensional NMR methods. Contrary to expectations, it is found that CTX III and CBTX differ significantly in their structural stabilities. The three-dimensional structure of CBTX is less stable than that of CTX III. The amide protons of residues at the N- and C-terminal ends of the CTX III molecule are strongly protected against H/D exchange, implying that the terminal ends of the molecule are bridged together by significant numbers of hydrogen bonds. However, in CBTX, amide protons at the terminal ends of the molecule do not exhibit an significant protection against H/D exchange. Comparison of the protection factors of the various amide protons in CTX III and CBTX reveals that the extraordinary stability of CTX III stems from the strong network of interactions among the residues at the N- and C-terminal ends and also due to the tight and ordered packing of the nonpolar residues involved in the triple-stranded, anti-parallel, beta-sheet segment of the molecule.     

Comparison of the structural stability of two homologous toxins isolated from the Taiwan cobra (Naja naja atra) venom

Cardiotoxin analogue III (CTX III) and cobrotoxin (CBTX) isolated from the Taiwan cobra venom (Naja naja atra) are structurally homologous, small molecular weight, all-beta-sheet proteins, cross-linked by four disulfide bonds at identical positions. The conformational stabilities of these toxins are compared based on temperature-dependent chemical shifts and amide proton exchange kinetics using two-dimensional NMR spectroscopy. The structure of CTX III is found to be significantly more stable than that of CBTX. In both the toxins, beta-strand III appears to constitute the stability core. In CTX III, the stability of the triple-stranded beta-sheet domain is observed to be markedly higher than the double-stranded beta-sheet segment. In contrast, in CBTX, both structural domains (double- and triple-stranded beta-sheet domains) appear to contribute equally to the stability of the protein. Estimation of the free energy of exchange (Delta G(ex)) of residues in CBTX and CTX III reveals that the enhanced stability of the structure of CTX III stems from the strong interactions among the beta-strands constituting the triple-stranded beta-sheet domain and also the molecular forces bridging the residues at the N- and C-terminal ends of the molecule.     

Apparent local stability of the secondary structure of Azotobacter vinelandii holoflavodoxin II as probed by hydrogen exchange: implications for redox potential regulation and flavodoxin folding.

As a first step to determine the folding pathway of a protein with an alpha/beta doubly wound topology, the 1H, 13C, and 15N backbone chemical shifts of Azotobacter vinelandii holoflavodoxin II (179 residues) have been determined using multidimensional NMR spectroscopy. Its secondary structure is shown to contain a five-stranded parallel beta-sheet (beta2-beta1-beta3-beta4-beta5) and five alpha-helices. Exchange rates for the individual amide protons of holoflavodoxin were determined using the hydrogen exchange method. The amide protons of 65 residues distributed throughout the structure of holoflavodoxin exchange slowly at pH* 6.2 [kex < 10(-5) s(-1)] and can be used as probes in future folding studies. Measured exchange rates relate to apparent local free energies for transient opening. We propose that the amide protons in the core of holoflavodoxin only exchange by global unfolding of the apo state of the protein. The results obtained are discussed with respect to their implications for flavodoxin folding and for modulation of the flavin redox potential by the apoprotein. We do not find any evidence that A. vinelandii holoflavodoxin II is divided into two subdomains based on its amide proton exchange rates, as opposed to what is found for the structurally but not sequentially homologous alpha/beta doubly wound protein Che Y.     

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

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

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.     

Amide proton hydrogen exchange rates for sperm whale myoglobin obtained from 15N-1H NMR spectra

The hydrogen exchange behavior of exchangeable protons in proteins can provide important information for understanding the principles of protein structure and function. The positions and exchange rates of the slowly-exchanging amide protons in sperm whale myoglobin have been mapped using 15N-1H NMR spectroscopy. The slowest-exchanging amide protons are those that are hydrogen bonded in the longest helices, including members of the B, E, and H helices. Significant protection factors were observed also in the A, C, and G helices, and for a few residues in the D and F helices. Knowledge of the identity of slowly-exchanging amide protons forms the basis for the extensive quench-flow kinetic folding experiments that have been performed for myoglobin, and gives insights into the tertiary interactions and dynamics in the protein.     

Dihydrofolate reductase: sequential resonance assignments using 2D and 3D NMR and secondary structure determination in solution

Three-dimensional (3D) heteronuclear NMR techniques have been used to make sequential 1H and 15N resonance assignments for most of the residues of Lactobacillus casei dihydrofolate reductase (DHFR), a monomeric protein of molecular mass 18,300 Da. A uniformly 15N-labeled sample of the protein was prepared and its complex with methotrexate (MTX) studied by 3D 15N/1H nuclear Overhauser-heteronuclear multiple quantum coherence (NOESY-HMQC), Hartmann-Hahn-heteronuclear multiple quantum coherence (HOHAHA-HMQC), and HMQC-NOESY-HMQC experiments. These experiments overcame most of the spectral overlap problems caused by chemical shift degeneracies in 2D spectra and allowed the 1H-1H through-space and through-bond connectivities to be identified unambiguously, leading to the resonance assignments. The novel HMQC-NOESY-HMQC experiment allows NOE cross peaks to be detected between NH protons even when their 1H chemical shifts are degenerate as long as the amide 15N chemical shifts are nondegenerate. The 3D experiments, in combination with conventional 2D NOESY, COSY, and HOHAHA experiments on unlabelled and selectively deuterated DHFR, provide backbone assignments for 146 of the 162 residues and side-chain assignments for 104 residues of the protein. Data from the NOE-based experiments and identification of the slowly exchanging amide protons provide detailed information about the secondary structure of the binary complex of the protein with methotrexate. Sequential NHi-NHi+1 NOEs define four regions with helical structure. Two of these regions, residues 44-49 and 79-89, correspond to within one amino acid to helices C and E in the crystal structure of the DHFR.methotrexate.NADPH complex [Bolin et al. (1982) J. Biol. Chem. 257, 13650-13662], while the NMR-determined helix formed by residues 26-35 is about one turn shorter at the N-terminus than helix B in the crystal structure, which spans residues 23-34. Similarly, the NMR-determined helical region comprising residues 102-110 is somewhat offset from the crystal structure's helix F, which encompasses residues 97-107. Regions of beta-sheet structure were characterized in the binary complex by strong alpha CHi-NHi+1 NOEs and by slowly exchanging amide protons. In addition, several long-range NOEs were identified linking together these stretches to form a beta-sheet. These elements align perfectly with corresponding elements in the crystal structure of the DHFR.methotrexate.NADPH complex, which contains an eight-stranded beta-sheet, indicating that the main body of the beta-sheet is preserved in the binary complex in solution.     

Structure and dynamics of the potato carboxypeptidase inhibitor by 1H and 15N NMR

The solution structure and backbone dynamics of the recombinant potato carboxypeptidase inhibitor (PCI) have been characterized by NMR spectroscopy. The structure, determined on the basis of 497 NOE-derived distance constraints, is much better defined than the one reported in a previous NMR study, with an average pairwise backbone root-mean-square deviation of 0.5 A for the well-defined region of the protein, residues 7-37. Many of the side-chains show now well-defined conformations, both in the hydrophobic core and on the surface of the protein. Overall, the solution structure of free PCI is similar to the one that it shows in the crystal of the complex with carboxypeptidase A. However, some local differences are observed in regions 15-21 and 27-29. In solution, the six N-terminal and the two C-terminal residues are rather flexible, as shown by 15N backbone relaxation measurements. The flexibility of the latter segment may have implications in the binding of the inhibitor by the enzyme. All the remaining residues in the protein are essentially rigid (S2 > 0.8) with the exception of two of them at the end of a short 3/10 helix. Despite the small size of the protein, a number of amide protons are protected from exchange with solvent deuterons. The slowest exchanging protons are those in a small two-strand beta-sheet. The unfolding free energies, as calculated from the exchange rates of these protons, are around 5 kcal/mol. Other protected amide protons are located in the segment 7-12, adjacent to the beta-sheet. Although these residues are not in an extended conformation in PCI, the equivalent residues in structurally homologous proteins form a third strand of the central beta-sheet. The amide protons in the 3/10 helix are only marginally protected, indicating that they exchange by a local unfolding mechanism, which is consistent with the increase in flexibility shown by some of its residues. Backbone alignment-based programs for folding recognition, as opposite to disulfide-bond alignments, reveal new proteins of unrelated sequence and function with a similar structure.     

Properties of an aldose reductase from pig lens. Comparative studies of an aldehyde reductase from pig lens

THe characteristic feature of the crystal structure of erabutoxin b, a short neurotoxin from Laticauda semifasciata, and alpha-cobratoxin, a long neurotoxin from Naja naja siamensis, is the presence of a triple-stranded antiparallel pleated beta-sheet structure formed by the central and the third peptide loops. In the present study, we have studied the assignment of slowly exchangeable amide protons of Laticauda semifasciata III from L. semifasciata, using nuclear Overhauser effects (NOE) and spin-decoupling methods. The results show that nearly all of the slowly exchangeable amide protons are to be assigned to the back-bone amide protons, involved in the triple-stranded antiparallel pleated beta-sheet structure, indicating that this sheet is stable in 2H2O solution. In contrast, the amide protons in short neurotoxins are readily exchangeable under the same experimental condition, suggesting that long neurotoxins have a more rigid sheet structure than short ones. This rigidity may come from the hydrophobic and hydrogen bond interaction between the central loop and the tail, which is not present in short neurotoxins. Since the functionally important residues are located on this beta-sheet, the different kinetic properties of the neurotoxins are well correlated with the difference in the rigidity of the beta-sheet.     

Mapping the core of the beta(2)-microglobulin amyloid fibril by H/D exchange

Despite numerous efforts, the lack of detailed structural information on amyloid fibrils has hindered clarification of the mechanism of their formation. Here, we describe a novel procedure for characterizing the conformational flexibility of beta(2)-microglobulin amyloid fibrils at single-residue resolution that uses H/D exchange of amide protons combined with NMR analysis. The results indicate that most residues in the middle region of the molecule, including the loop regions in the native structure, form a rigid beta-sheet core, whereas the the N- and C-termini are excluded from this core. The extensively hydrogen-bonded beta-sheet core explains the remarkable rigidity and stability of amyloid fibrils. The present method could be used to obtain residue-specific conformational information of various amyloid fibrils, even though it does not provide a high resolution three-dimensional structure.     

Stable intermediate states and high energy barriers in the unfolding of GFP

We present a study of the denaturation of a truncated, cycle3 variant of green fluorescent protein (GFP). Chemical denaturation is used to unfold the protein, with changes in structure being monitored by the green fluorescence, tyrosine fluorescence and far-UV circular dichroism. The results show that the denaturation behaviour of GFP is complex compared to many small proteins: equilibrium is established only very slowly, over the time course of weeks, suggesting that there are high folding/unfolding energy barriers. Unfolding kinetics confirm that the rates of unfolding at low concentrations of denaturant are very low, consistent with the slow establishment of the equilibrium. In addition, we find that GFP significantly populates an intermediate state under equilibrium conditions, which is compact and stable with respect to the unfolded state (m(IU)=4.6 kcal mol(-1) M(-1) and Delta G(IU)=12.5 kcal mol(-1)). The global and local stability of GFP was probed further by measuring the hydrogen/deuterium (H/D) NMR exchange rates of more than 157 assigned amide protons. Analysis at two different values of pH showed that amide protons within the beta-barrel structure exchange at the EX2 limit, consequently, free energies of exchange could be calculated and compared to those obtained from the denaturation-curve studies providing further support for the three-state model and the existence of a stable intermediate state. Analysis reveals that amide protons in beta-strands 7, 8, 9 and 10 have, on average, higher exchange rates than others in the beta-barrel, suggesting that there is greater flexibility in this region of the protein. Forty or so amide protons were found which do not undergo significant exchange even after several months and these are clustered into a core region encompassing most of the beta-strands, at least at one end of the barrel structure. It is likely that these residues play an important role in stabilizing the structure of the intermediate state. The intermediate state observed in the chemical denaturation studies described here, is similar to that observed at pH 4 in other studies.     

New insights into the self-assembly of insulin amyloid fibrils: an H-D exchange FT-IR study

The solvent protection of the amide backbone in bovine insulin fibrils was studied by FT-IR spectroscopy. In the mature fibrils, approximately 85 +/- 2% of amide protons are protected. Of those "trapped" protons, a further 25 +/- 2 or 35 +/- 2% is H-D exchanged after incubation for 1 h at 1 GPa and 25 degrees C or 0.1 MPa and 100 degrees C, respectively. In contrast to the native or unfolded protein, fibrils do not H-D exchange upon incubation at 65 degrees C. A complete deuteration of H(2)O-grown fibrils occurs when the beta-sheet structure is reassembled in a 75 wt % DMSO/D(2)O solution. Our findings suggest a densely packed environment around the amide protons involved in the intermolecular beta-sheet motive. In disagreement with the concept of "amyloid fibers as water-filled nanotubes" [Perutz, M. F., et al. (2002) Proc. Natl. Acad. Sci. U.S.A. 99, 5591-5595], elution of D(2)O-grown fibrils with H(2)O is complete, which is reflected by the vanishing of D(2)O bending vibrations at 1214 cm(-)(1). This implies the absence of "trapped water" within insulin fibrils. The rigid conformations of the native and fibrillar insulin contrast with transient intermediate states docking at the fibrils' ends. Room-temperature seeding is accompanied by an accelerated H-D exchange in insulin molecules in the act of docking and integrating with the seeds, proving that the profound structural disruption is the sine qua non of forming an aggregation-competent conformation.     

Hydrogen bonding and equilibrium protium-deuterium fractionation factors in the immunoglobulin G binding domain of protein G

Protium-deuterium fractionation factors (phi) were determined for more than 85% of the backbone amide protons in the IgG binding domains of protein G, GB1 and GB2, from NMR spectra recorded over a range of H2O/D2O solvent ratios. Previous studies suggest a correlation between phi and hydrogen bond strength; amide and hydroxyl groups in strong hydrogen bonds accumulate protium (phi < 1), while weak hydrogen bonds accumulate deuterium (phi > 1). Our results show that the alpha-helical residues have slightly lower phi values (1.03 +/- 0.05) than beta-sheet residues (1.12 +/- 0.07), on average. The lowest phi value obtained (0.65) does not involve a backbone amide but rather is for the interaction between two side chains, Y45 and D47. Fractionation factors for solvent-exposed residues are between the alpha-helix and beta-sheet values, on average, and are close to those for random coil peptides. Further, the difference in phiav between alpha-helix and solvent-exposed residues is small, suggesting that differences in hydrogen bond strength for intrachain hydrogen bonds and amide...water hydrogen bonds are also small. Overall, the enrichment for deuterium suggests that most backbone...backbone hydrogen bonds are weak.     

The pH dependence of hydrogen-deuterium exchange in trp repressor: the exchange rate of amide protons in proteins reflects tertiary interactions,not only secondary structure.

The pH dependence of amide proton exchange rates have been measured for trp-repressor. One class of protons exchanges too fast to be measured in these experiments. Among the protons that have measurable hydrogen-deuterium exchange rates, two additional classes may be distinguished. The second class of protons are in elements of secondary structure that are mostly on the surface of the protein, and exchange linearly with increasing base concentration (log kex versus pH). The third class of amide protons is characterized by much higher protection against exchange at higher pH. These protons are located in the core of the protein, in helices B and C. The exchange rate in the core region does not increase linearly with pH, but rather goes through a minimum around pH 6. The mechanism of exchange for the slowly exchanging core protons is interpreted in terms of the two-process model of Hilton and Woodward (1979, Biochemistry 18:5834-5841), i.e., exchange through both a local mechanism that does not require unfolding of the protein, and a mechanism involving global unfolding of the protein. The increase in exchange rates at low pH is attributed to a partial unfolding of the repressor. It is concluded that the formation of secondary structure alone is insufficient to account for the high protection factors seen in the core of native proteins at higher pH, and that tertiary interactions are essential to stabilize the structure.     

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.     

A two-process model describes the hydrogen exchange behavior of cytochrome c in the molten globule state with various extents of acetylation

Acetylation of Lys residues of horse cytochrome c steadily stabilizes the molten globule state in 18 mM HCl as more Lys residues are acetylated [Goto and Nishikiori (1991) J. Mol. Biol. 222, 679-686]. The dynamic features of the molten globule state were characterized by hydrogen/deuterium exchange of amide protons, monitored by mass spectrometry as each deuteration increased the protein mass by 1 Da. Electrospray mass spectrometry enabled us to monitor simultaneously the exchange kinetics of more than seven species with a different number of acetyl groups. One to four Lys residue-acetylated cytochrome c showed almost no protection of the amide protons from rapid exchange. The transition from the unprotected to the protected state occurred between five and eight Lys residue-acetylated species. For species with more than nine acetylated Lys residues, the exchange kinetics were independent of the extent of acetylation, and 26 amide protons were protected at 60 min of exchange, indicating the formation of a rigid hydrophobic core with hydrogen-bonded secondary structures. The apparent transition to the protected state required a higher degree of acetylation than the conformational transition measured by circular dichroism, which had a midpoint at about four acetylated residues. This difference in the transitions suggested a two-process model in which the exchange occurs either from the protected folded state or from the unprotected unfolded state through global unfolding. On the basis of a two-process model and with the reported values of the exchange and stability parameters, we simulated the exchange kinetics of a series of acetylated cytochrome c species. The simulated kinetics reproduced the observed kinetics well, indicating validity of this model for hydrogen exchange of the molten globule state.     

Hydrogen exchange in a large 29 kD protein and characterization of molten globule aggregation by NMR

The nature of denatured ensembles of the enzyme human carbonic anhydrase (HCA) has been extensively studied by various methods in the past. The protein constitutes an interesting model for folding studies that does not unfold by a simple two-state transition, instead a molten globule intermediate is highly populated at 1.5 M GuHCl. In this work, NMR and H/D exchange studies have been conducted on one of the isozymes, HCA I. The H/D exchange studies, which were enabled by the previously obtained resonance assignment of HCA I, have been used to identify unfolded forms that are accessible from the native state. In addition, the GuHCl-induced unfolded states of HCA I have also been characterized by NMR at GuHCl concentrations in the 0-5 M range. The most important findings in this work are as follows: (1) Amide protons located in the center of the beta-sheet require global unfolding events for efficient H/D exchange. (2) The molten globule and the native state give similar protection against H/D exchange for all of the observable amide protons (i.e., water seems not to efficiently penetrate the interior of the molten globule). (3) At high protein concentrations, the molten globule can form large aggregates, which are not detectable by solution-state NMR methods. (4) The unfolded state (U), present at GuHCl concentrations above 2 M, is composed of an ensemble of conformations having residual structures with different stabilities.     

Comparison of the structure and dynamics of chicken gizzard and rabbit cardiac tropomyosins: 1H NMR spectroscopy and measurement of amide hydrogen exchange rates

The side chain and backbone mobilities of chicken gizzard tropomyosin (TM) and its nonpolymerizable derivative have been investigated by H NMR spectroscopy and amide hydrogen exchange kinetics and compared to those of rabbit cardiac TM and its nonpolymerizable derivative. Analysis of the 300-MHz H NMR spectra of native chicken gizzard and rabbit cardiac TMs and their nonpolymerizable derivatives showed that the line widths of the aromatic and histidine residues were within a factor of 2 for all four proteins, demonstrating that the side chain mobility of these residues is similar in the different TMs. Direct proton exchange-out kinetics were determined in D2O in the pD range 1.5-3.0 at 25 degrees C by H NMR spectroscopy. Multiple exponential fitting of the exchange data indicated the presence in gizzard TM of at least three kinetically distinct classes of amide hydrogens at pD 1.7 with average population sizes of 147, 74, and 61, whose rates were retarded by a factor of 10, 10(3), and 10(5), respectively, relative to the random-coil peptide poly(DL-alanine). Measurement of the direct exchange kinetics of both rabbit cardiac and nonpolymerizable gizzard TMs showed that their rate constants and population sizes were within experimental error of those for the gizzard protein, except that the fast exchanging class for cardiac TM was increased in size while that of the nonpolymerizable gizzard TM was reduced, relative to that for gizzard TM. Comparison of the exchange-out kinetics for the cardiac and gizzard proteins at pH 2.0 and 55 degrees C, where only the two slowly exchanging amide hydrogen sets are measured, again demonstrated the similarity of their kinetic parameters.(ABSTRACT TRUNCATED AT 250 WORDS)     

Hydrogen exchange in native and alcohol forms of ubiquitin.

Ubiquitin adopts a non-native folded structure in 60% methanol solution at low pH. Two-dimensional nuclear magnetic resonance (2D NMR) was used to measure the hydrogen-exchange rates of backbone amide protons of ubiquitin in both native and methanol forms, and to characterize the structure of ubiquitin in the methanol state. Protection factors (the ratios of experimentally determined exchange rates to the rates calculated for an unfolded polypeptide) for protons in the native form of ubiquitin range from less than 10 to greater than 10(5). Most of the protons that are protected from exchange are located in regions of hydrogen-bonded secondary structure. The most strongly protected backbone amide protons are those of residues comprising the hydrophobic core. Hydrogen exchange from ubiquitin in methanol solution was too rapid to measure directly by 2D NMR, so a labeling scheme was employed, in which exchange with solvent occurred while the protein was in methanol solution. Exchange was quenched by dilution with aqueous buffer after the desired labeling time, and proton occupancies were measured by 1H NMR of the native form of the protein. Protection factors for protons in the methanol form of ubiquitin range from 2.6 to 42, with all protected protons located in hydrogen-bonded structure in the native form. Again, the most strongly protected protons are those of residues in the hydrophobic core. Comparison of the patterns of the hydrogen-exchange rates in the native and methanol forms indicates that almost all of the native secondary structure persists in the methanol form, but that it is almost uniformly destabilized by 4-6 kcal/mol.(ABSTRACT TRUNCATED AT 250 WORDS)     

Three-dimensional solution structure and stability of thioredoxin m from spinach.

Proton NMR spectral resonances of thioredoxin m from spinach have been assigned, and its solution structure has been determined on the basis of 1156 nuclear Overhauser effect- (NOE-) derived distance constraints by using restrained molecular dynamics calculations. The average pairwise root-mean-square deviation (RMSD) for the 25 best NMR structures for the backbone was 1.0 +/- 0.1, when the structurally well-defined residues were considered. The N- and C-terminal segments (1-13 and 118-119) and residues 41-49, comprising the active site, are highly disordered. At the time of concluding this work, a crystal structure of this protein was reported, in which thioredoxin m was found to crystallize as noncovalent dimers. Although the solution and crystal structures are very similar, no evidence was found about the existence of dimers in solution, thus confirming that dimerization is not needed for the regulatory activity of thioredoxin m. The spinach thioredoxin m does not unfold by heat in the range 25-85 degrees C, as revealed by thermal circular dichroic (CD) measurements. However, its unfolding free energy (9.1 +/- 0.8 kcal mol(-1), at pH 5.3 and 25 degrees C) could be determined by extrapolating the free energy values obtained at different concentrations of guanidinium chloride (GdmCl). The folding-unfolding process is two-state as indicated by the coincidence of the CD denaturation curves obtained at far and near UV. The H/D exchange behavior of backbone amide protons was analyzed. The slowest-exchanging protons, requiring a global-unfolding mechanism in order to exchange, are those from beta2, beta3, and beta4, the central strands of the beta-sheet, which constitute the main element of the core of the protein. The free energies obtained from exchange measurements of protons belonging to the alpha-helices are lower than those derived from GdmCl denaturation studies, indicating that those protons exchange by local-unfolding mechanisms.