Characterization of the structure and dynamics of a near-native equilibrium intermediate in the unfolding pathway of an all beta-barrel protein

The structure and dynamics of equilibrium intermediate in the unfolding pathway of the human acidic fibroblast growth factor (hFGF-1) are investigated using a variety of biophysical techniques including multidimensional NMR spectroscopy. Guanidinium hydrochloride (GdnHCl)-induced unfolding of hFGF-1 proceeds with the accumulation of a stable intermediate state. The transition from the intermediate state to the unfolded state(s) is cooperative without the accumulation of additional intermediate(s). The intermediate state induced maximally in 0.96 m GdnHCl is found to be obligatory in the folding/unfolding pathway of hFGF-1. Most of the native tertiary structure interactions are preserved in the intermediate state. (1)H-(15)N chemical shift perturbation data suggest that the residues in the C-terminal segment including those located in the beta-strands IX, X, and XI undergo the most discernible structural change(s) in the intermediate state in 0.96 m GdnHCl. hFGF-1 in the intermediate state (0.96 m GdnHCl) does not bind to its ligand, sucrose octasulfate. Limited proteolytic digestion experiments and hydrogen-deuterium exchange monitored by (15)N heteronuclear single quantum coherence (HSQC) spectra show that the conformational flexibility of the protein in the intermediate state is significantly higher than in the native conformation. (15)N spin relaxation experiments show that many residues located in beta-strands IX, X, and XI exhibit conformational motions in the micro- to millisecond time scale. Analysis of (15)N relaxation data in conjunction with the amide proton exchange kinetics suggests that residues in the beta-strands II, VIII, and XII possibly constitute the stability core of the protein in the near-native intermediate state.     

Measuring rapid hydrogen exchange in the homodimeric 36 kDa HIV-1 integrase catalytic core domain

Measurements of rapid hydrogen exchange (HX) of water with protein amide sites contain valuable information on protein structure and function, but current NMR methods for measuring HX rates are limited in their applicability to large protein systems. An alternate method for measuring rapid HX is presented that is well-suited for larger proteins, and we apply the method to the deuterated, homodimeric 36 kDa HIV-1 integrase catalytic core domain (CCD). Using long mixing times for water-amide magnetization exchange at multiple pH values, HX rates spanning more than four orders of magnitude were measured, as well as NOE cross-relaxation rates to nearby exchangeable protons. HX protection factors for the CCD are found to be large (>10(4)) for residues along the dimer interface, but much smaller in many other regions. Notably, the catalytic helix (residues 152-167) exhibits low HX protection at both ends, indicative of fraying at both termini as opposed to just the N-terminal end, as originally thought. Residues in the LEDGF/p75 binding pocket also show marginal stability, with protection factors in the 10-100 range (～1.4-2.7 kcal/mol). Additionally, elevated NOE cross-relaxation rates are identified and, as expected, correspond to proximity of the amide proton to a rapidly exchanging proton, typically from an OH side chain. Indirect NOE transfer between H(2) O and the amide proton of I141, a residue in the partially disordered active site of the enzyme, suggests its proximity to the side chain of S147, an interaction seen in the DNA-bound form for a homologous integrase.     

Hydrogen-deuterium exchange in free and prodomain-complexed subtilisin

Residue-specific exchange rates of 223 amide protons in free and prodomain-complexed subtilisin were determined in order to understand how the prodomain binding affects the energetics of subtilisin folding. In free subtilisin, amide protons can be categorized according to exchange rate: 74 fast exchangers (rates > or = 1 h(-1)); 52 medium exchangers (rates between 1 h(-1) and 1 day(-1)); 31 slow exchangers (rates between 1 day(-1) and 0.001 day(-1)). The remaining 66 amide proteins did not exchange detectibly over 9 months (k(obs) < year(-1)) and were denoted as core protons. Core residues occur throughout the main structural elements of subtilisin. Prodomain binding results in high protection factors (100-1000) in the central beta-sheet, particularly in the vicinity of beta-strands S5, S6, and S7 and the connecting loops between them. These connecting loops provide the ligands to the cation at metal site B. Overall, prodomain binding seems to facilitate the organization of the entire central beta-sheet and alpha-helix C in the left-handed crossover connection between beta-strands two and three. It also appears to facilitate the isomerization of multiple prolines late in folding, allowing the formation of metal site B. The gain of stability region around site B comes at the cost of stability in regions more distal to prodomain binding: the C-terminal alpha-helix H and the N-terminal alpha-helices A and B. The acceleration of exchange in these regions by prodomain binding reveals an antagonism between the folding intermediate and the full native structure. This antagonism helps to explain why the prodomain is needed to stabilize the folding intermediate as well as why the unfolding of free subtilisin seldom occurs via this intermediate.     

Dissection of the pathway of molecular recognition by calmodulin

Amide hydrogen exchange has been used to examine the structural dynamics and energetics of the interaction of a peptide corresponding to the calmodulin-binding domain of smooth muscle myosin light chain kinase (smMLCKp) with calcium-saturated calmodulin. Heteronuclear NMR (15)N-(1)H correlation spectroscopy was used to quantify amide proton exchange rates of the uniformly (15)N-labeled domain bound to calmodulin. A key feature of a proposed model for molecular recognition by calmodulin [Ehrhardt et al. (1995) Biochemistry 34, 2731-2738] is tested by examination of the dependence of amide hydrogen exchange on applied hydrostatic pressure. Hydrogen exchange rates and corresponding protection factors (1/K(op)) for individual amide protons of the bound smMLCKp domain span 5 orders of magnitude at ambient pressure. Individual protection factors decrease significantly in a linear fashion with increasing hydrostatic pressure. A common pressure dependence is revealed by a constant large negative volume change across the residues comprising the core of the bound helical domain. The pattern of protection factors and their response to hydrostatic pressure is consistent with a structural reorganization that results in the concerted disruption of ion pairs between calmodulin and the bound domain. These observations reinforce a model for the molecular recognition pathway where formation of the initial encounter complex is followed by helix-coil transitions in the bound state and subsequent concerted formation of the extensive ion pair network defining the intermolecular contact surface between CaM and the target domain in the final, compact complex structure.     

Investigation of the structural stability of cardiotoxin analogue III from the Taiwan cobra by hydrogen-deuterium exchange kinetics.

The conformational stability of a small ( approximately 7 kDa), all beta-sheet protein, cardiotoxin analogue III (CTX III), from the venom of the Taiwan cobra has been investigated by hydrogen-deuterium (H/D) exchange using two-dimensional NMR spectroscopy. The H/D exchange kinetics of backbone amide protons in CTX III has been monitored at pD 3.6 and 6.6 (at 25 degrees C), for over 5000 h. Examination of H/D exchange kinetics in the protein showed that a number of slowly exchanging residues are in the hydrophobic core of the protein. The average protection factor of the amide protons of residues belonging to the triple-stranded beta-sheet domain is about 20 times greater than that of those in the double-stranded beta-sheet segment. The residues in the C-terminal tail of the molecule, though structureless, have been found to exhibit significant protection against H/D exchange. Comparison of the quenched-flow H/D exchange data on CTX III with those obtained in the present study reveals that the most slowly exchanging portion constitutes the folding core of the protein.     

Structural events during the refolding of an all beta-sheet protein

The refolding kinetics of the 140-residue, all beta-sheet, human fibroblast growth factor (hFGF-1) is studied using a variety of biophysical techniques such as stopped-flow fluorescence, stopped-flow circular dichroism, and quenched-flow hydrogen exchange in conjunction with multidimensional NMR spectroscopy. Urea-induced unfolding of hFGF-1 under equilibrium conditions reveals that the protein folds via a two-state (native <--> unfolded) mechanism without the accumulation of stable intermediates. However, measurement of the unfolding and refolding rates in various concentrations of urea shows that the refolding of hFGF-1 proceeds through accumulation of kinetic intermediates. Results of the quenched-flow hydrogen exchange experiments reveal that the hydrogen bonds linking the N- and C-terminal ends are the first to form during the refolding of hFGF-1. The basic beta-trefoil framework is provided by the simultaneous formation of beta-strands I, IV, IX, and X. The other beta-strands comprising the beta-barrel structure of hFGF-1 are formed relatively slowly with time constants ranging from 4 to 13 s.     

15N NMR relaxation studies of free and ligand-bound human acidic fibroblast growth factor

15N NMR relaxation data have been used to characterize the backbone dynamics of the human acidic fibroblast growth factor (hFGF-1) in its free and sucrose octasulfate (SOS)-bound states. (15)N longitudinal (R(1)), transverse (R(2)) relaxation rates and (1H)-(15)N steady-state nuclear Overhauser effects were obtained at 500 and 600 MHz (at 25 degrees C) for all resolved backbone amide groups using (1)H- detected two-dimensional NMR experiments. Relaxation data were fit to the extended model free dynamics for each NH group. The overall correlation time (tau(m)) for the free and SOS-bound forms were estimated to be 10.4 +/- 1.07 and 11.1 +/- 1.35 ns, respectively. Titration experiments with SOS reveals that the ligand binds specifically to the C-terminal domain of the protein in a 1:1 ratio. Binding of SOS to hFGF-1 is found to induce a subtle conformational change in the protein. Significant conformational exchange (R(ex)) is observed for several residues in the free form of the protein. However, in the SOS-bound form only three residues exhibit significant R(ex) values, suggesting that the dynamics on the micro- to millisecond time scale in the free form is coupled to the cis-trans-proline isomerization. hFGF-1 is a rigid molecule with an average generalized parameter (S(2)) value of 0.89 +/- 0.03. Upon binding to SOS, there is a marked decrease in the overall flexibility (S(2) = 0.94 +/- 0.02) of the hFGF-1 molecule. However, the segment comprising residues 103-111 shows increased flexibility in the presence of SOS. Significant correlation is found between residues that show high flexibility and the putative receptor binding sites on the protein.     

Proton nuclear magnetic resonance measurement of the amide hydrogen exchange rates of group A streptococcal polysaccharide in H2O

The solvent exchange rates of the acetamido hydrogen of the 2-acetamido-2-deoxy-beta-D-glucopyranosyl unit of group A streptococcal polysaccharide dissolved in H2O have been measured and compared with the corresponding exchange rates in the solvated model compound 1-O-methyl-2-acetamido-2-deoxy-beta-D-glucopyranoside. Amide hydrogen exchange rates were measured at 25 degrees C over a wide pH range by a combination of two separate NMR techniques: the transfer of solvent saturation and the amide hydrogen saturation recovery NMR experiments. The data indicate that the acetamido hydrogen essentially exists in a solvated environment and that its contribution to the conformational stability of this polysaccharide through intramolecular hydrogen bonding is negligible.     

Identification of rare partially unfolded states in equilibrium with the native conformation in an all beta-barrel protein

Human acidic fibroblast growth factor 1 (hFGF-1) is an all beta-barrel protein, and the secondary structural elements in the protein include 12 antiparallel beta-strands arranged into a beta-trefoil fold. In the present study, we investigate the stability of hFGF-1 by hydrogen-deuterium exchange as a function of urea concentration. Urea-induced equilibrium unfolding of hFGF-1 monitored by fluorescence and CD spectroscopy suggests that the protein unfolds by a two-state (native to denatured) mechanism. Hydrogen exchange in hFGF-1, under the experimental conditions used, occurs by the EX2 mechanism. In contrast to the equilibrium unfolding events monitored by optical probes, native state hydrogen exchange data show that the beta-trefoil architecture of hFGF-1 does not behave as a single cooperative unit. There are at least two structurally independent units with differing stabilities in hFGF-1. Beta-strands I, II, III, VI, VII, X, XI, and XII fit into the global unfolding isotherm. By contrast, residues in beta-strands IV, V, VIII, and IX exchange by the subfolding isotherm and could be responsible for the occurrence of high-energy partially unfolded state(s) in hFGF-1. There appears to be a broad continuum of stabilities among the four beta-strands (beta-strands IV, V, VIII, and IX) constituting the subglobal folding unit. The slow exchanging residues in hFGF-1 do not represent the folding nucleus of the protein.     

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.     

Hydrogen exchange of monomeric alpha-synuclein shows unfolded structure persists at physiological temperature and is independent of molecular crowding in Escherichia coli

Amide proton NMR signals from the N-terminal domain of monomeric α-synuclein (αS) are lost when the sample temperature is raised from 10°C to 35°C at pH 7.4. Although the temperature-induced effects have been attributed to conformational exchange caused by an increase in α-helix structure, we show that the loss of signals is due to fast amide proton exchange. At low ionic strength, hydrogen exchange rates are faster for the N-terminal segment of αS than for the acidic C-terminal domain. When the salt concentration is raised to 300 mM, exchange rates increase throughout the protein and become similar for the N- and C-terminal domains. This indicates that the enhanced protection of amide protons from the C-terminal domain at low salt is electrostatic in nature. Cα chemical shift data point to <10% residual α-helix structure at 10°C and 35°C. Conformational exchange contributions to R2 are negligible at both temperatures. In contrast to the situation in vitro, the majority of amide protons are observed at 37°C in ¹H-¹⁵N HSQC spectra of αS encapsulated within living Escherichia coli cells. Our finding that temperature effects on αS NMR spectra can be explained by hydrogen exchange obviates the need to invoke special cellular factors. The retention of signals is likely due to slowed hydrogen exchange caused by the lowered intracellular pH of high-density E. coli cultures. Taken together, our results emphasize that αS remains predominantly unfolded at physiological temperature and pH—an important conclusion for mechanistic models of the association of αS with membranes and fibrils.     

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.     

Effects of co-operative ligand binding on protein amide NH hydrogen exchange

Amide protection factors have been determined from NMR measurements of hydrogen/deuterium amide NH exchange rates measured on assigned signals from Lactobacillus casei apo-DHFR and its binary and ternary complexes with trimethoprim (TMP), folinic acid and coenzymes (NADPH/NADP(+)). The substantial sizes of the residue-specific DeltaH and TDeltaS values for the opening/closing events in NH exchange for most of the measurable residues in apo-DHFR indicate that sub-global or global rather than local exchange mechanisms are usually involved. The amide groups of residues in helices and sheets are those most protected in apo-DHFR and its complexes, and the protection factors are generally related to the tightness of ligand binding. The effects of ligand binding that lead to changes in amide protection are not localised to specific binding sites but are spread throughout the structure via a network of intramolecular interactions. Although the increase in protein stability in the DHFR.TMP.NADPH complex involves increased ordering in the protein structure (requiring TDeltaS energy) this is recovered, to a large extent, by the stronger binding (enthalpic DeltaH) interactions made possible by the reduced motion in the protein. The ligand-induced protection effects in the ternary complexes DHFR.TMP.NADPH (large positive binding co-operativity) and DHFR.folinic acid.NADPH (large negative binding co-operativity) mirror the co-operative effects seen in the ligand binding. For the DHFR.TMP.NADPH complex, the ligand-induced protection factors result in DeltaDeltaG(o) values for many residues being larger than the DeltaDeltaG(o) values in the corresponding binary complexes. In contrast, for DHFR.folinic acid.NADPH, the DeltaDeltaG(o) values are generally smaller than many of those in the corresponding binary complexes. The results indicate that changes in protein conformational flexibility on formation of the ligand complex play an important role in determining the co-operativity in the ligand binding.     

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.     

Amide proton exchange in human metallothionein-2 measured by nuclear magnetic resonance spectroscopy

In human metallothionein-2, the exchange rate constants of ten amide protons were found to range from 1.7 x 10(-4) to 1 x 10(-1) min-1 at pH 6.3 and 8 degrees C. Most of these slowly exchanging protons could be associated with hydrogen bonds in secondary structure elements of the alpha-domain. Amide proton exchange rates thus present an additional criterion for the structural characterization of different metallothioneins, which could be particularly valuable for comparisons of different homologous protein preparations containing nuclear magnetic resonance-inactive metal ions, where the metal-polypeptide co-ordinative bonds cannot be identified directly.     

Structural elements involved in proton translocation by cytochrome c oxidase as revealed by backbone amide hydrogen-deuterium exchange of the E286H mutant

Cytochrome c oxidase is the terminal electron acceptor in the respiratory chains of aerobic organisms and energetically couples the reduction of oxygen to water to proton pumping across the membrane. The mechanisms of proton uptake, gating, and pumping have yet to be completely elucidated at the molecular level for these enzymes. For Rhodobacter sphaeroides CytcO (cytochrome aa3), it appears as though the E286 side chain of subunit I is a branching point from which protons are shuttled either to the catalytic site for O2 reduction or to the acceptor site for pumped protons. Amide hydrogen-deuterium exchange mass spectrometry was used to investigate how mutation of this key branching residue to histidine (E286H) affects the structures and dynamics of four redox intermediate states. A functional characterization of this mutant reveals that E286H CytcO retains approximately 1% steady-state activity that is uncoupled from proton pumping and that proton transfer from H286 is significantly slowed. Backbone amide H-D exchange kinetics indicates that specific regions of CytcO, perturbed by the E286H mutation, are likely to be involved in proton gating and in the exit pathway for pumped protons. The results indicate that redox-dependent conformational changes around E286 are essential for internal proton transfer. E286H CytcO, however, is incapable of these specific conformational changes and therefore is insensitive to the redox state of the enzyme. These data support a model where the side chain conformation of E286 controls proton translocation in CytcO through its interactions with the proton gate, which directs the flow of protons either to the active site or to the exit pathway. In the E286H mutant, the proton gate does not function properly and the exit channel is unresponsive. These results provide new insight into the structure and mechanism of proton translocation by CytcO.     

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.     

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)     

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.