Design and structural analysis of an engineered thermostable chicken lysozyme.

A hyperstable (hs) variant of chicken egg-white lysozyme with enhanced thermal (delta Tm approximately +10.5 degrees C) and chemical (delta Cm for guanidine hydrochloride denaturation = +1.3 M) stabilities relative to wild-type (WT) was constructed by combining several individual stabilizing substitutions. The free energy difference between the native and denatured states of the hs variant is 3.1 (GdnHCl, 25 degrees C) to 4.0 (differential scanning calorimetry, 74 degrees C) kcal mol-1 greater than that of WT. The specific activity of the hs variant is 2.5-fold greater than that of WT. The choice of mutations came from diverse sources: (1) The I55L/S91T core construct with delta Tm = 3.3 degrees C from WT was available from the accompanying study (Shih P, Holland DR, Kirsch JF, 1995, Protein Sci 4:2050-2062). (2) The A31V mutation was suggested by the better atomic packing in the human lysozyme structure where the Ala 31 equivalent is Leu. (3) The H15L and R114H substitutions were selected on the basis of sequence comparisons with pheasant lysozymes that are more stable than the chicken enzyme. (4) The D101S variant was identified from a screen of mutants previously prepared in this laboratory. The effects of the individual mutations on stability are cumulative and nearly additive.     

Destabilizing effect of proline substitutions in two helical regions of T4 lysozyme: leucine 66 to proline and leucine 91 to proline.

A class of temperature-sensitive (ts) mutants of T4 lysozyme with reduced activity at 30 degrees C and no activity at 43 degrees C has been selected. These mutants, designated "tight" ts mutants, differ from most other T4 lysozyme mutants that are active at 43 degrees C, but only manifest their ts lesion by a reduced halo size around phage plaques after exposure of the growth plates to chloroform vapors. For example, in the series of T4 lysozyme mutants at position 157, the original randomly selected mutant, T1571, is the least stable of the series, yet, apart from the halo assay and subsequent in vitro protein stability measurements, this mutant is indistinguishable from wild type (WT) even at 43 degrees C. Two mutants were identified: L91P and L66P. Both insert proline residues into alpha-helical regions of the WT protein structure. The stabilities (delta delta G) as determined by urea denaturation are 8.2 kcal/mol for L91P and 7.1 kcal/mol for L66P. CD spectra indicate that no major conformational changes have occurred in the mutant structures. The structures of the mutants were modeled with a 40-ps molecular dynamics simulation using explicit solvent. For L91P, the reduction of stability appears to be due to an unsatisfied hydrogen bond in the alpha-helix and to a new buried cavity. For L66P, the reduction of stability appears to be due to a disruption of the interdomain alpha-helix, at least two unsatisfied hydrogen bonds, and a newly formed solvent-filled pocket that protrudes into the hydrophobic core, possibly reducing the stabilizing contribution of a partially buried intrachain salt bridge.     

Quantification of the thermodynamically linked quaternary and tertiary structural stabilities of transthyretin and its disease-associated variants: the relationship between stability and amyloidosis

Urea denaturation studies were carried out as a function of transthyretin (TTR) concentration to quantify the thermodynamically linked quaternary and tertiary structural stability and to improve our understanding of the relationship between mutant folding energetics and amyloid disease phenotype. Urea denaturation of TTR involves at least two equilibria: dissociation of tetramers into folded monomers and monomer unfolding. To deal with the thermodynamic linkage of these equilibria, we analyzed concentration-dependent denaturation data by globally fitting them to an equation that simultaneously accounts for the two-step denaturation process. Using this method, the quaternary and tertiary structural stabilities of well-behaved TTR sequences, wild-type (WT) TTR and the disease-associated variant V122I, were scrutinized. The V122I variant is linked to late onset familial amyloid cardiomyopathy, the most common familial TTR amyloid disease. V122I TTR exhibits a destabilized quaternary structure and a stable tertiary structure relative to those of WT TTR. Three other variants of TTR were also examined, L55P, V30M, and A25T TTR. The L55P mutation is associated with the most aggressive familial TTR amyloid disease. L55P TTR has a complicated denaturation pathway that includes dimers and trimers, so globally fitting its concentration-dependent urea denaturation data yielded error-laden estimates of stability parameters. Nevertheless, it is clear that L55P TTR is substantially less stable than WT TTR, primarily because its tertiary structure is unstable, although its quaternary structure is destabilized as well. V30M is the most common mutation associated with neuropathic forms of TTR amyloid disease. V30M TTR is certainly destabilized relative to WT TTR, but like L55P TTR, it has a complex denaturation pathway that cannot be fit to the aforementioned two-step denaturation model. Literature data suggest that V30M TTR has stable quaternary structure but unstable tertiary structure. The A25T mutant, associated with central nervous system amyloidosis, is highly aggregation-prone and exhibits drastically reduced quaternary and tertiary structural stabilities. The observed differences in stability among the disease-associated TTR variants highlight the complexity and heterogeneity of TTR amyloid disease, an observation that has important implications for the treatment of these maladies.     

Mechanism of the stabilization of ribonuclease A by sorbitol: preferential hydration is greater for the denatured then for the native protein.

The effect of interactions of sorbitol with ribonuclease A (RNase A) and the resulting stabilization of structure was examined in parallel thermal unfolding and preferential binding studies with the application of multicomponent thermodynamic theory. The protein was stabilized by sorbitol both at pH 2.0 and pH 5.5 as the transition temperature, Tm, was increased. The enthalpy of the thermal denaturation had a small dependence on sorbitol concentration, which was reflected in the values of the standard free energy change of denaturation, delta delta G(o) = delta G(o) (sorbitol) - delta G(o)(water). Measurements of preferential interactions at 48 degrees C at pH 5.5, where protein is native, and pH 2.0 where it is denatured, showed that sorbitol is preferentially excluded from the denatured protein up to 40%, but becomes preferentially bound to native protein above 20% sorbitol. The chemical potential change on transferring the denatured RNase A from water to sorbitol solution is larger than that for the native protein, delta mu(2D) > delta mu(2N), which is consistent with the effect of sorbitol on the free energy change of denaturation. The conformity of these results to the thermodynamic expression of the effect of a co-solvent on denaturation, delta G(o)(W) + delta mu(D)(2)delta G(o)(S) + delta mu(2D), indicates that the stabilization of the protein by sorbitol can be fully accounted for by weak thermodynamic interactions at the protein surface that involve water reversible co-solvent exchange at thermodynamically non-neutral sites. The protein structure stabilizing action of sorbitol is driven by stronger exclusion from the unfolded protein than from the native structure.     

Changes in strand 6B and helix B during neuroserpin inhibition: Implication in severity of clinical phenotype

Neuroserpin (NS) is predominantly expressed in brain and inhibits tissue-type plasminogen activator (tPA) with implications in brain development and memory. Nature of conformational change in pathological variants in strand 6B and helix B of NS that cause a relatively mild to severe epilepsy (and/or dementia) remains largely elusive. MD simulation with wild type (WT) NS, strand 6B and helix B variants indicated that substitution in this region affects the conformation of the strands 5B, 5A and reactive centre loop. Therefore, we designed variants of NS in strand 6B (I46D and F48S) and helix B (A54F, L55A and L55P) to investigate their role in tPA inhibition mechanism and propensity to aggregate. An interaction analysis showed disturbance of a hydrophobic patch centered at strands 5B, 6B and helix B in I46D and F48S but not in A54F, L55A, L55P and WT NS. Purified I46D, F48S and L55P variants showed decrease in fluorescence emission intensity but have similar α-helical content, however results of A54F and L55A were comparable to WT NS. Analysis of tPA inhibition showed marginal effect on A54F and L55A variant with tPA-NS complex formation. In contrast, I46D, F48S and L55P variants showed massive decrease in tPA inhibition, with no tPA-NS complex formation. Analysis of native PAGE under under polymerization condition showed prompt conversion of I46D, F48S and L55P to latent conformation but not A54F and L55A variants. Identification of these novel conformational changes will aid in the understanding of variable clinical phenotype of shutter region NS variants and other serpins.     

X-ray and thermodynamic studies of staphylococcal nuclease variants I92E and I92K: insights into polarity of the protein interior

We have used crystallography and thermodynamic analysis to study nuclease variants I92E and I92K, in which an ionizable side-chain is placed in the hydrophobic core of nuclease. We find that the energetic cost of burying ionizable groups is rather modest. The X-ray determinations show water molecules solvating the buried glutamic acid under cryo conditions, but not at room temperature. The lysine side-chain does not appear solvated in either case. Guanidine hydrochloride (GnHCl) denaturation of I92E and I92K, done as a function of pH and monitored by tryptophan fluorescence, showed that I92E and I92K are folded in the pH range pH 3.5-9.0 and pH 5.5-9.5, respectively. The stability of the parental protein is independent of pH over a broad range. In contrast, the stabilities of I92E and I92K exhibit a pH dependence, which is quantitatively explained by thermodynamic analysis: the PK(a) value of the buried K92 is 5.6, while that of the buried E92 is 8.65. The free energy difference between burying the uncharged and charged forms of the groups is modest, about 6 kcal/mol. We also found that epsilon(app) for I92K and I92E is in the range approximately 10-12, instead of 2-4 commonly used to represent the protein interior. Side-chains 92E and 92K were uncharged under the conditions of the X-ray experiment. Both are buried completely inside the well-defined hydrophobic core of the variant proteins without forming salt-bridges or hydrogen bonds to other functional groups of the proteins. Under cryo conditions 92E shows a chain of four water molecules, which hydrate one oxygen atom of the carboxyl group of the glutamic acid. Two other water molecules, which are present in the wild-type at all temperatures, are also connected to the water ring observed inside the hydrophobic core. The ready burial of water with an uncharged E92 raises the possibility that solvent excursions into the interior also take place in the wild-type protein, but in a random, dynamic way not detectable by crystallography. Such transient excursions could increase the average polarity, and thus epsilon(app), of the protein interior.     

Thermodynamic characterization of an artificially designed amphiphilic alpha-helical peptide containing periodic prolines: observations of high thermal stability and cold denaturation.

To investigate the structural stability of proteins, we analyzed the thermodynamics of an artificially designed 30-residue peptide. The designed peptide, NH2-EELLPLAEALAPLLEALLPLAEALAPLLKK-COOH (PERI COIL-1), with prolines at i + 7 positions, forms a pentameric alpha-helical structure in aqueous solution. The thermal denaturation curves of the CD at 222 nm (pH 7.5) show an unusual cold denaturation occurring well above 0 degrees C and no thermal denaturation is observable under 90 degrees C. This conformational change is reversible and depends on peptide concentration. A 2-state model between the monomeric denatured state (5D) and the pentameric helical state (H5) was sufficient to analyze 5 thermal denaturation curves of PERI COIL-1 with concentrations between 23 and 286 microM. The analysis was carried out by a nonlinear least-squares method using 3 fitting parameters: the midpoint temperature, Tm, the enthalpy change, delta H(Tm), and the heat capacity change, delta Cp. The association number (n = 5) was determined by sedimentation equilibrium and was not used as a fitting parameter. The heat capacity change suggests that the hydrophobic residues are buried in the helical state and exposed in the denatured one, as it occurs normally for natural globular proteins. On the other hand, the enthalpy and the entropy changes have values close to those found for coiled-coils and are quite distinct from typical values reported for natural globular proteins. In particular, the enthalpy change extrapolated at 110 degrees C is about 3 kJ/mol per amino acid residue, i.e., half of the value found for globular proteins.(ABSTRACT TRUNCATED AT 250 WORDS)     

Contribution of polar groups in the interior of a protein to the conformational stability

It has been generally believed that polar residues are usually located on the surface of protein structures. However, there are many polar groups in the interior of the structures in reality. To evaluate the contribution of such buried polar groups to the conformational stability of a protein, nonpolar to polar mutations (L8T, A9S, A32S, I56T, I59T, I59S, A92S, V93T, A96S, V99T, and V100T) in the interior of a human lysozyme were examined. The thermodynamic parameters for denaturation were determined using a differential scanning calorimeter, and the crystal structures were analyzed by X-ray crystallography. If a polar group had a heavy energy cost to be buried, a mutant protein would be remarkably destabilized. However, the stability (Delta G) of the Ala to Ser and Val to Thr mutant human lysozymes was comparable to that of the wild-type protein, suggesting a low-energy penalty of buried polar groups. The structural analysis showed that all polar side chains introduced in the mutant proteins were able to find their hydrogen bond partners, which are ubiquitous in protein structures. The empirical structure-based calculation of stability change (Delta Delta G) [Takano et al. (1999) Biochemistry 38, 12698--12708] revealed that the mutant proteins decreased the hydrophobic effect contributing to the stability (Delta G(HP)), but this destabilization was recovered by the hydrogen bonds newly introduced. The present study shows the favorable contribution of polar groups with hydrogen bonds in the interior of protein molecules to the conformational stability.     

Thermotropic and mixing behavior of mixed-chain phosphatidylcholines with molecular weights identical with that of L-alpha-dipalmitoylphosphatidylcholine.

The thermotropic phase behavior of 10 mixed-chain phosphatidylcholines, in excess water, has been examined and compared with that of identical-chain C(16):C(16)PC by using high-resolution differential scanning calorimetry (DSC). The molecular weights (MW) of these 11 molecular species are the same, but their delta C/CL values, or the normalized chain length differences, vary considerably, ranging from 0.035 to 0.540. The thermodynamic parameters (Tm, delta H, and delta S) associated with the main phase transitions for these lipid dispersions exhibit biphasic V-shaped curves, when plotted against delta C/CL. Similar characteristic curves have been reported previously for aqueous dispersions of mixed-chain phosphatidylcholines with MW identical with that of C(17):C(17)PC [Lin et al. (1990) Biochemistry 29, 7063-7072]. The initial decrease in Tm (delta H or delta S) with increasing values of delta C/CL is attributed to the progressive increase in the magnitude of the chain-terminal perturbations on the conformational statistics of the adjacent hydrocarbon chains and hence the lateral chain-chain interactions of these mixed-chain phosphatidylcholines in the gel-state bilayer. At delta C/CL approximately equal to 0.42, the chain-end perturbation is presumably at its maximum; beyond this point, the highly asymmetric phosphatidylcholines are proposed to pack, at T less than Tm, into the mixed interdigitated bilayer. In this new packing mode, the methyl ends of the longer acyl chains are relocated at the interfaces between the hydrocarbon core of the bilayer and the aqueous medium. This disposition of the bulky chain ends releases a certain degree of chain-chain packing disorders, leading to an increase in Tm (delta H or delta S) with increasing delta C/CL.(ABSTRACT TRUNCATED AT 250 WORDS)     

Thermodynamics of unfolding for turkey ovomucoid third domain: thermal and chemical denaturation.

We have used thermal and chemical denaturation to characterize the thermodynamics of unfolding for turkey ovomucoid third domain (OMTKY3). Thermal denaturation was monitored spectroscopically at a number of wave-lengths and data were subjected to van't Hoff analysis; at pH 2.0, the midpoint of denaturation (Tm) occurs at 58.6 +/- 0.4 degrees C and the enthalpy of unfolding at this temperature (delta Hm) is 40.8 +/- 0.3 kcal/mol. When Tm was perturbed by varying pH and denaturant concentration, the resulting plots of delta Hm versus Tm yield a mean value of 590 +/- 120 cal/(mol.K) for the change in heat capacity upon unfolding (delta Cp). A global fit of the same data to an equation that includes the temperature dependence for the enthalpy of unfolding yielded a value of 640 +/- 110 cal/(mol.K). We also performed a variation of the linear extrapolation method described by Pace and Laurents, which is an independent method for determining delta Cp (Pace, C.N. & Laurents, D., 1989, Biochemistry 28, 2520-2525). First, OMTKY3 was thermally denatured in the presence of a variety of denaturant concentrations. Linear extrapolations were then made from isothermal slices through the transition region of the denaturation curves. When extrapolated free energies of unfolding (delta Gu) were plotted versus temperature, the resulting curve appeared linear; therefore, delta Cp could not be determined. However, the data for delta Gu versus denaturant concentration are linear over an extraordinarily wide range of concentrations. Moreover, extrapolated values of delta Gu in urea are identical to values measured directly.     

Biochemical and structural characterisation of cutinase mutants in the presence of the anionic surfactant AOT

The reactivity, stability and unfolding of wild-type (WT) Fusarium solani pisi cutinase and L153Q, S54D and T179C variants were studied in the absence and presence of the dioctyl sulfosuccinate sodium salt (AOT) surfactant. In the absence of surfactant the S54D variant catalytic activity is similar to that of the WT cutinase, whereas L153Q and T179C variants show a lower activity. AOT addition induces an activity reduction for WT cutinase and its variants, although for low AOT concentrations a small increase of activity was observed for S54D and T179C. The enzyme deactivation in the presence of 0.5 mM AOT is relatively slow for the S54D and T179C variants when compared to wild-type cutinase and L153Q variant. These results were correlated with secondary and tertiary structure changes assessed by the CD spectrum and fluorescence of the single tryptophan and the six tyrosine residues. The WT cutinase and S54D variant have similar secondary and tertiary structures that differ from those of T179C and L153Q variants. L153Q, S54D and T179C mutations prevent the formation of hydrophobic crevices responsible for the unfolding by anionic surfactants, with the consequent decrease of the AOT-cutinase interactions.     

Structure and stability of the P93G variant of ribonuclease A.

The peptide bonds preceding Pro 93 and Pro 114 of bovine pancreatic ribonuclease A (RNase A) are in the cis conformation. The trans-to-cis isomerization of these bonds had been indicted as the slow step during protein folding. Here, site-directed mutagenesis was used to replace Pro 93 or Pro 114 with a glycine residue, and the crystalline structure of the P93G variant was determined by X-ray diffraction analysis to a resolution of 1.7 A. This structure is essentially identical to that of the wild-type protein, except for the 91-94 beta-turn containing the substitution. In the wild-type protein, the beta-turn is of type VIa. In the P93G variant, this turn is of type II with the peptide bond preceding Gly 93 being trans. The thermal stabilities of the P93G and P114G variants were assessed by differential scanning calorimetry and thermal denaturation experiments monitored by ultraviolet spectroscopy. The value of delta deltaGm which reports on the stability lost in the variants, is 1.5-fold greater for the P114G variant than for the P93G variant. The greater stability of the P93G variant is likely due to the relatively facile accommodation of residues 91-94 in a type II turn, which has a preference for a glycine residue in its i + 2 position.     

I. Study of protein aggregation due to heat denaturation: A structural approach using circular dichroism spectroscopy, nuclear magnetic resonance, and static light scattering

The objective of this study was to investigate the relationship between oxidized RNase A protein structure and the occurrence of protein aggregation using several spectroscopic techniques. Circular dichroism spectroscopy (CD) measurements taken at small temperature intervals were used to determine the protein's melting temperature, Tm, of approximately 65 degrees C in deionized water. A more detailed examination of the protein structure was undertaken at several temperatures around Tm using near- and far-UV CD and one-dimensional nuclear magnetic resonance (NMR) measurements. These measurements revealed the presence of folded structures at 55 degrees C and below, while denatured structures appeared at 65 degrees C and above. Concurrent static light scattering (SLS) measurements, employed to detect the presence of RNase A aggregates, showed that RNase A aggregation was observed at 65 degrees C and above, when much of the protein was denatured. Subsequent NMR time-course data demonstrated that aggregates forming at 75 degrees C and pH 7.8 were indeed derived from heat-denatured protein. However, aggregation was also detected at 55 degrees C when the spectroscopic data suggested the protein was present predominantly in the folded configuration. In contrast, heat denaturation did not lead to RNase A aggregation in a very acidic environment. We attribute this phenomenon to the effect of charge-charge repulsion between the highly protonated RNase A molecules in very acidic pH.     

Structural and thermodynamic analysis of the packing of two alpha-helices in bacteriophage T4 lysozyme

Packing interactions in bacteriophage T4 lysozyme were explored by determining the structural and thermodynamic effects of substitutions for Ala98 and neighboring residues. Ala98 is buried in the core of T4 lysozyme in the interface between two alpha-helices. The Ala98 to Val (A98V) replacement is a temperature-sensitive lesion that lowers the denaturation temperature of the protein by 15 degrees C (pH 3.0, delta delta G = -4.9 kcal/mol) and causes atoms within the two helices to move apart by up to 0.7 A. Additional structural shifts also occur throughout the C-terminal domain. In an attempt to compensate for the A98V replacement, substitutions were made for Val149 and Thr152, which make contact with residue 98. Site-directed mutagenesis was used to construct the multiple mutants A98V/T152S, A98V/V149C/T152S and the control mutants T152S, V149C and A98V/V149I/T152S. These proteins were crystallized, and their high-resolution X-ray crystal structures were determined. None of the second-site substitutions completely alleviates the destabilization or the structural changes caused by A98V. The changes in stability caused by the different mutations are not additive, reflecting both direct interactions between the sites and structural differences among the mutants. As an example, when Thr152 in wild-type lysozyme is replaced with serine, the protein is destabilized by 2.6 kcal/mol. Except for a small movement of Val94 toward the cavity created by removal of the methyl group, the structure of the T152S mutant is very similar to wild-type T4 lysozyme. In contrast, the same Thr152 to Ser replacement in the A98V background causes almost no change in stability. Although the structure of A98V/T152S remains similar to A98V, the combination of T152S with A98V allows relaxation of some of the strain introduced by the Ala98 to Val replacement. These studies show that removal of methyl groups by mutation can be stabilizing (Val98----Ala), neutral (Thr152----Ser in A98V) or destabilizing (Val149----Cys, Thr152----Ser). Such diverse thermodynamic effects are not accounted for by changes in buried surface area or free energies of transfer of wild-type and mutant side-chains. In general, the changes in protein stability caused by a mutation depend not only on changes in the free energy of transfer associated with the substitution, but also on the structural context within which the mutation occurs and on the ability of the surrounding structure to relax in response to the substitution.(ABSTRACT TRUNCATED AT 400 WORDS)     

Contribution of conformational stability and reversibility of unfolding to the increased thermostability of human and bovine superoxide dismutase mutated at free cysteines

The conformational stability and reversibility of unfolding of the human dimeric enzyme Cu Zn superoxide dismutase (HSOD) and the three mutant enzymes constructed by replacement of Cys6 by Ala and Cys111 by Ser, singly and in combination, were determined by differential scanning calorimetry. The differential scanning calorimetry profile of wild-type HSOD consists of two components, which probably represent the unfolding of the oxidized and reduced forms of the enzyme, with denaturation temperatures (Tm) of 74.9 and 83.6 degrees C, approximately 7 degrees lower than those for bovine superoxide dismutase (BSOD). The conformational stabilities of the two components of the mutant HSOD's differ only slightly from those of the wild type (delta delta Gs of -0.2 to +0.8 kcal/mol of dimer), while replacement of the BSOD Cys6 by Ala is somewhat destabilizing (delta delta G of -0.7 to -1.3 kcal/mol of dimer). These small alterations in conformational stability do not correlate with the large increases in resistance to thermal inactivation following substitution of free Cys in both HSOD and BSOD (McRee, D.E., Redford, S.M., Getzoff, E.D., Lepock, J.R., Hallewell, R.A., and Tainer, J.A. (1990) J. Biol. Chem. 265, 14234-14241 and Hallewell, R.A., Imlay, K.C., Laria, I., Gallegos, C., Fong, N., Irvine, B., Getzoff, E.D., Tainer, J.A., Cubelli, D.E., Bielski, B.H.J., Olson, P., Mallenbach, G.T., and Cousens, L.S. (1991) Proteins Struct. Funct. Genet., submitted for publication). The reversibility of unfolding was determined by scanning part way through the profile, cooling, rescanning, and calculating the amount of protein irreversibly unfolded by the first scan. The order of reversibility at a constant level of unfolding is the same as the order of resistance to inactivation for both the HSOD and BSOD wild-type and mutant enzymes. Thus, the greater resistance to thermal inactivation of the superoxide dismutase enzymes with free Cys replaced by Ala or Ser is dominated by a greater resistance to irreversible unfolding and relatively unaffected by changes in conformational stability.     

Hydrogen-exchange stabilities of RNase T1 and variants with buried and solvent-exposed Ala --> Gly mutations in the helix

Hydrogen-exchange rates were measured for RNase T1 and three variants with Ala --> Gly substitutions at a solvent-exposed (residue 21) and a buried (residue 23) position in the helix: A21G, G23A, and A21G + G23A. These results were used to measure the stabilities of the proteins. The hydrogen-exchange stabilities (DeltaG(HX)) for the most stable residues in each variant agree with the equilibrium conformational stability measured by urea denaturation (DeltaG(U)), if the effects of D(2)O and proline isomerization are included [Huyghues-Despointes, B. M. P., Scholtz, J. M., and Pace, C. N. (1999) Nat. Struct. Biol. 6, 210-212]. These residues also show similar changes in DeltaG(HX) upon Ala --> Gly mutations (DeltaDeltaG(HX)) as compared to equilibrium measurements (DeltaDeltaG(U)), indicating that the most stable residues are exchanging from the globally unfolded ensemble. Alanine is stabilizing compared to glycine by 1 kcal/mol at a solvent-exposed site 21 as seen by other methods for the RNase T1 protein and peptide helix [Myers, J. K., Pace, C. N., and Scholtz, J. M. (1997) Proc. Natl. Acad. Sci. U.S.A. 94, 3833-2837], while it is destabilizing at the buried site 23 by the same amount. For the A21G variant, only local NMR chemical shift perturbations are observed compared to RNase T1. For the G23A variant, large chemical shift changes are seen throughout the sequence, although X-ray crystal structures of the variant and RNase T1 are nearly superimposable. Ala --> Gly mutations in the helix of RNase T1 at both helical positions alter the native-state hydrogen-exchange stabilities of residues throughout the sequence.     

A D-pathway mutation decouples the Paracoccus denitrificans cytochrome c oxidase by altering the side-chain orientation of a distant conserved glutamate

Asparagine 131, located near the cytoplasmic entrance of the D-pathway in subunit I of the Paracoccus denitrificans aa(3) cytochrome c oxidase, is a residue crucial for proton pumping. When replaced by an aspartate, the mutant enzyme is completely decoupled: while retaining full cytochrome c oxidation activity, it does not pump protons. The same phenotype is observed for two other substitutions at this position (N131E and N131C), whereas a conservative replacement by glutamine affects both activities of the enzyme. The N131D variant oxidase was crystallized and its structure was solved to 2.32-A resolution, revealing no significant overall change in the protein structure when compared with the wild type (WT), except for an alternative orientation of the E278 side chain in addition to its WT conformation. Moreover, remarkable differences in the crystallographically resolved chain of water molecules in the D-pathway are found for the variant: four water molecules that are observed in the water chain between N131 and E278 in the WT structure are not visible in the variant, indicating a higher mobility of these water molecules. Electrochemically induced Fourier transform infrared difference spectra of decoupled mutants confirm that the protonation state of E278 is unaltered by these mutations but indicate a distinct perturbation in the hydrogen-bonding environment of this residue. Furthermore, they suggest that the carboxylate side chain of the N131D mutant is deprotonated. These findings are discussed in terms of their mechanistic implications for proton routing through the D-pathway of cytochrome c oxidase.     

Polar residues in the protein core of Escherichia coli thioredoxin are important for fold specificity

Most globular proteins contain a core of hydrophobic residues that are inaccessible to solvent in the folded state. In general, polar residues in the core are thermodynamically unfavorable except when they are able to form intramolecular hydrogen bonds. Compared to hydrophobic interactions, polar interactions are more directional in character and may aid in fold specificity. In a survey of 263 globular protein structures, we found a strong positive correlation between the number of polar residues at core positions and protein size. To probe the importance of buried polar residues, we experimentally tested the effects of hydrophobic mutations at the five polar core residues in Escherichia coli thioredoxin. Proteins with single hydrophobic mutations (D26I, C32A, C35A, T66L, and T77V) all have cooperative unfolding transitions like the wild type (wt), as determined by chemical denaturation. Relative to wt, D26I is more stable while the other point mutants are less stable. The combined 5-fold mutant protein (IAALV) is less stable than wt and has an unfolding transition that is substantially less cooperative than that of wt. NMR spectra as well as amide deuterium exchange indicate that IAALV is likely sampling a number of low-energy structures in the folded state, suggesting that polar residues in the core are important for specifying a well-folded native structure.     

A single free cysteine residue and disulfide bond contribute to the thermostability of Aspergillus saitoi 1,2-alpha-mannosidase

Aspergillus saitoi 1,2-alpha-mannosidase contains three conserved cysteine residues (Cys334, Cys363, and Cys443). We showed that Cys334 and Cys363 are involved in a disulfide bond, and that Cys443 contains a free thiol group. The cysteines were not essential for the activity analyzed by site-directed mutagenesis and kinetics. The substitution at each cysteine residue greatly destabilized the enzyme. The T(m) values of WT, C443A, C443G, C443S, and C443T were 55.8, 51.9, 50.2, 50.0, and 52.8 degrees C respectively. The specific activity of these mutants was almost equal to that of WT. Introducing Asp, Leu, Met, or Val at position 443 caused partial denaturation, although the enzymes had some activity. C443F, C443I, C443N, and C443Y were not secreted. These results suggest that the hydrophilic and large side chain causes the destabilization. Molecular modelling showed that the Cys443 residue is buried and surrounded by a hydrophobic environment. Cys334 and Cys363 form a disulfide bond, and Cys443 is involved in a hydrophobic interaction to stabilize the enzyme.     

Stability of yeast iso-1-ferricytochrome c as a function of pH and temperature.

Absorbance-detected thermal denaturation studies of the C102T variant of Saccharomyces cerevisiae iso-1-ferricytochrome c were performed between pH 3 and 5. Thermal denaturation in this pH range is reversible, shows no concentration dependence, and is consistent with a 2-state model. Values for free energy (delta GD), enthalpy (delta HD), and entropy (delta SD) of denaturation were determined as functions of pH and temperature. The value of delta GD at 300 K, pH 4.6, is 5.1 +/- 0.3 kcal mol-1. The change in molar heat capacity upon denaturation (delta Cp), determined by the temperature dependence of delta HD as a function of pH (1.37 +/- 0.06 kcal mol-1 K-1), agrees with the value determined by differential scanning calorimetry. pH-dependent changes in the Soret region indicate that a group or groups in the heme environment of the denatured protein, probably 1 or both heme propionates, ionize with a pK near 4. The C102T variant exhibits both enthalpy and entropy convergence with a delta HD of 1.30 kcal mol-1 residue-1 at 373.6 K and a delta SD of 4.24 cal mol-1 K-1 residue-1 at 385.2 K. These values agree with those for other single-domain, globular proteins.