Probing the influence on folding behavior of structurally conserved core residues in P. aeruginosa apo-azurin

The effects on folding kinetics and equilibrium stability of core mutations in the apo-mutant C112S of azurin from Pseudomonas aeruginosa were studied. A number of conserved residues within the cupredoxin family were recognized by sequential alignment as constituting a common hydrophobic core: I7, F15, L33, W48, F110, L50, V95, and V31. Of these, I7, V31, L33, and L50 were mutated for the purpose of obtaining information on the transition state and a potential folding nucleus. In addition, residue V5 in the immediate vicinity of the common core, as well as T52, separate from the core, were mutated as controls. All mutants exhibited a nonlinear dependence of activation free energy of folding on denaturant concentration, although the refolding kinetics of the V31A/C112S mutant indicated that the V31A mutation destabilizes the transition state enough to allow folding via a parallel transition state ensemble. Phi-values could be calculated for three of the six mutants, V31A/C112S, L33A/C112S, and L50A/C112S, and the fractional values of 0.63, 0.33, and 0.50 (respectively) obtained at 0.5 M GdmCl suggest that these residues are important for stabilizing the transition state. Furthermore, a linear dependence of ln k(obs)(H2O) on DeltaG(U-N)(H2O) of the core mutations and the putative involvement of ground-state effects suggest the presence of native-like residual interactions in the denatured state that bias this ensemble toward a folding-competent state.     

Kinetic traps in the folding/unfolding of procaspase-1 CARD domain

We have examined the folding and unfolding of the caspase recruitment domain of procaspase-1 (CP1-CARD), a member of the alpha-helical Greek key protein family. The equilibrium folding/unfolding of CP1-CARD is described by a two-state mechanism, and the results show CP1-CARD is marginally stable with a DeltaG(H2O) of 1.1 +/- 0.2 kcal/mole and an m-value of 0.65 +/- 0.06 kcal/mole/M (10 mM Tris-HCl at pH 8.0, 1 mM DTT, 25 degrees C). Consistent with the equilibrium folding data, CP1-CARD is a monomer in solution when examined by size exclusion chromatography. Single-mixing stopped-flow refolding and unfolding studies show that CP1-CARD folds and unfolds rapidly, with no detectable slow phases, and the reactions appear to reach equilibrium within 10 msec. However, double jump kinetic experiments demonstrate the presence of an unfolded-like intermediate during unfolding. The intermediate converts to the fully unfolded conformation with a half-time of 10 sec. Interrupted refolding studies demonstrate the presence of one or more nativelike intermediates during refolding, which convert to the native conformation with a half-time of about 60 sec. Overall, the data show that both unfolding and refolding processes are slow, and the pathways contain kinetically trapped species.     

High stability of a ferredoxin from the hyperthermophilic archaeon A. ambivalens: involvement of electrostatic interactions and cofactors

The ferredoxin from the thermophilic archaeon Acidianus ambivalens is a small monomeric seven-iron protein with a thermal midpoint (T(m)) of 122 degrees C (pH 7). To gain insight into the basis of its thermostability, we have characterized unfolding reactions induced chemically and thermally at various pHs. Thermal unfolding of this ferredoxin, in the presence of various guanidine hydrochloride (GuHCl) concentrations, yields a linear correlation between unfolding enthalpies (DeltaH[T(m)]) and T(m) from which an upper limit for the heat capacity of unfolding (DeltaC(P)) was determined to be 3.15 +/- 0.1 kJ/(mole * K). Only by the use of the stronger denaturant guanidine thiocyanate (GuSCN) is unfolding of A. ambivalens ferredoxin at pH 7 (20 degrees C) observed ([GuSCN](1/2) = 3.1 M; DeltaG(U)[H(2)O] = 79 +/- 8 kJ/mole). The protein is, however, less stable at low pH: At pH 2.5, T(m) is 64 +/- 1 degrees C, and GuHCl-induced unfolding shows a midpoint at 2.3 M (DeltaG(U)[H(2)O] = 20 +/- 1 kJ/mole). These results support that electrostatic interactions contribute significantly to the stability. Analysis of the three-dimensional molecular model of the protein shows that there are several possible ion pairs on the surface. In addition, ferredoxin incorporates two iron-sulfur clusters and a zinc ion that all coordinate deprotonated side chains. The zinc remains bound in the unfolded state whereas the iron-sulfur clusters transiently form linear three-iron species (in pH range 2.5 to 10), which are associated with the unfolded polypeptide, before their complete degradation.     

Copper binding before polypeptide folding speeds up formation of active (holo) Pseudomonas aeruginosa azurin.

Cofactors often stabilize the native state of the proteins; however, their effects on folding dynamics remain poorly understood. To uncover the role of one cofactor, we have examined the folding kinetics of Pseudomonas aeruginosa azurin, a small blue-copper protein with a copper cofactor uniquely coordinated to five protein residues. Copper removal produces apo-azurin which adopts a folded structure identical to that of the holo-form. The folding and unfolding kinetics for apo-azurin follow two-state behavior. The extrapolated folding time in water, tau approximately 7 ms, is in good agreement with the topology-based prediction. Copper uptake by folded apo-azurin, to govern active (holo) protein, is slow (tau approximately 14 min, 50:1 copper-to-protein ratio). In contrast, the formation of active (holo) azurin is much faster when copper is allowed to interact with the unfolded polypeptide. Refolding in the presence of 10:1, 50:1, and 100:1 copper:protein ratios yields identical time-trajectories: active azurin forms in two kinetic phases with folding times, extrapolated to water, of tau = 10 +/- 2 ms (major phase) and tau = 190 +/- 30 ms (minor phase), respectively. Correlating copper-binding studies, with a small peptide derived from the metal-binding region of azurin, support that initial cofactor binding is fast (tau approximately 3.7 ms) and thus not rate-limiting. Taken together, introducing copper prior to protein folding does not speed up the polypeptide-folding rate; nevertheless, it results in much faster (> 4000-fold) formation of active (i.e., holo) azurin. Living systems depend on efficient formation of functional biomolecules; attachment of cofactors prior to polypeptide folding appears to be one method to achieve this.     

Kinetically robust monomeric protein from a hyperthermophile

Equilibrium and kinetic studies were carried out under denaturation conditions to clarify the energetic features of the high stability of a monomeric protein, ribonuclease HII, from a hyperthermophile, Thermococcus kodakaraensis (Tk-RNase HII). Guanidine hydrochloride (GdnHCl)-induced unfolding and refolding were measured with circular dichroism at 220 nm, and heat-induced denaturation was studied with differential scanning calorimetry. Both GdnHCl- and heat-induced denaturation are very reversible. It was difficult to obtain the equilibrated unfolding curve of Tk-RNase HII below 40 degrees C, because of the remarkably slow unfolding. The two-state unfolding and refolding reactions attained equilibrium at 50 degrees C after 2 weeks. The Gibbs energy change of GdnHCl-induced unfolding (DeltaG(H(2)O)) at 50 degrees C was 43.6 kJ mol(-1). The denaturation temperature in the DSC measurement shifted as a function of the scan rate; the denaturation temperature at a scan rate of 90 degrees C h(-1) was higher than at a scan rate of 5 degrees C h(-1). The unfolding and refolding kinetics of Tk-RNase HII were approximated as a first-order reaction. The ln k(u) and ln k(r) values depended linearly on the denaturant concentration between 10 and 50 degrees C. The DeltaG(H(2)O) value obtained from the rate constant in water using the two-state model at 50 degrees C, 44.5 kJ mol(-1), was coincident with that from the equilibrium study, 43.6 kJ mol(-1), suggesting the two-state folding of Tk-RNase HII. The values for the rate constant in water of the unfolding for Tk-RNase HII were much smaller than those of E. coli RNase HI and Thermus thermophilus RNase HI, which has a denaturation temperature similar to that of Tk-RNase HII. In contrast, little difference was observed in the refolding rates among these proteins. These results indicate that the stabilization mechanism of monomeric protein from a hyperthermophile, Tk-RNase HII, with reversible two-state folding is characterized by remarkably slow unfolding.     

Effects of sulphate and urea on the stability and reversible unfolding of beta-lactamase from Staphylococcus aureus. Implications for the folding pathway of beta-lactamase

The reversible denaturation by urea of beta-lactamase from Staphylococcus aureus was followed in the presence and absence of ammonium sulphate by circular dichroism studies, difference absorption spectroscopy and measurement of enzyme activity. The multiple unfolding and refolding transitions demonstrate the existence of a thermodynamically stable state of intermediate conformation in equilibrium with the native (N) and fully unfolded (U) states. Its physical properties show that it is identical to the state H found on denaturation by guanidinium chloride. State H is 10.1 (+/-1.5) kJ mol-1 less stable than the native state and 10.1 (+/-1.6) kJ mol-1 more stable than the unfolded state. Ammonium sulphate shifts both the N in equilibrium H and H in equilibrium U transitions to concentrations of urea higher by 5.3 M per mole of sulphate. It has markedly different effects on the thermodynamic stabilities of states N and H, making delta G'N-H, O and delta G'H-U, O more negative by 41 kJ mol and 20 kJ mole, respectively, per mole of ammonium sulphate. The change in equilibrium constant for the N-H transition is reflected almost exclusively in a dramatic change of the unfolding rate constant, which is decreased by a factor of 10(11) on addition of 1.4 M-sulphate. The presence of the substrate benzyl penicillin has little effect on the equilibria or kinetics of the N-H transition. The results are discussed in terms of the nature of the N-H transition and of the ordering of intermediate states on the folding pathway.     

The effect of pressure and guanidine hydrochloride on azurins mutated in the hydrophobic core.

The unfolding of the blue-copper protein azurin from Pseudomonas aeruginosa by guanidine hydrochloride, under nonreducing conditions, has been studied by fluorescence techniques and circular dichroism. The denaturation transition may be fitted by a simple two-state model. The total free energy change from the native to the unfolded state was 9.4 +/- 0.4 kcal.mol-1, while a lower value (6.4 +/- 0.4 kcal.mol-1) was obtained for the metal depleted enzyme (apo-azurin) suggesting that the copper atom plays an important stabilization role. Azurin and apo-azurin were practically unaffected by hydrostatic pressure up to 3000 bar. Site-directed mutagenesis has been used to destabilize the hydrophobic core of azurin. In particular either hydrophobic residue Ile7 or Phe110 has been substituted with a serine. The free energy change of unfolding by guanidinium hydrochloride, resulted to be 5.8 +/- 0.3 kcal.mol-1 and 4.8 +/- 0.3 kcal.mol-1 for Ile7Ser and Phe110Ser, respectively, showing that both mutants are much less stable than the wild-type protein. The mutated apoproteins could be reversible denatured even by high pressure, as demonstrated by steady-state fluorescence measurements. The change in volume associated to the pressure-induced unfolding was estimated to be -24 mL.mol-1 for Ile7Ser and -55 mL.mol-1 for Phe110Ser. These results show that the tight packing of the hydrophobic residues that characterize the inner structure of azurin is fundamental for the protein stability. This suggests that the proper assembly of the hydrophobic core is one of the earliest and most crucial event in the folding process, bearing important implication for de novo design of proteins.     

Stability and cooperativity of individual tertiary contacts in RNA revealed through chemical denaturation

For proteins, understanding tertiary interactions involved in local versus global unfolding has become increasingly important for understanding the nature of the native state ensemble, the mechanisms of unfolding, and the stability of both the native and intermediate states in folding. In this work we have addressed related questions with respect to RNA structure by combining chemical denaturation and hydroxyl radical footprinting methods. We have determined unfolding isotherms for each of 26 discrete sites of protection located throughout the Tetrahymena thermophila group I ribozyme. The cooperativity of folding, m-value, and the free energy, DeltaG degrees N-U, associated with formation of each tertiary contact was determined by analysis of the isotherms. The DeltaG degrees N-U values measured in this study vary from 1.7 +/- 0.2 to 7. 6 +/- 1.2 kcal mol-1. Thus, the stability of these discrete tertiary contacts vary by almost 104. In addition, an intradomain contact and three interdomain contacts show high cooperativity (m-values of 1.1 +/- 0.2 to 1.7 +/- 0.3 kcal mol-1 M-1) indicating that these contacts exhibit global cooperatively in their folding behavior. This new approach to examining RNA stability provides an exciting comparison to our understanding of protein structure and folding mechanisms.     

Equilibrium unfolding of dimeric desulfoferrodoxin involves a monomeric intermediate: iron cofactors dissociate after polypeptide unfolding

Here we report the conformational stability of homodimeric desulfoferrodoxin (dfx) from Desulfovibrio desulfuricans (ATCC 27774). The dimer is formed by two dfx monomers linked through beta-strand interactions in two domains; in addition, each monomer contains two different iron centers: one Fe-(S-Cys)(4) center and one Fe-[S-Cys+(N-His)(4)] center. The dissociation constant for dfx was determined to be 1 microM (DeltaG = 34 kJ/mol of dimer) from the concentration dependence of aromatic residue emission. Upon addition of the chemical denaturant guanidine hydrochloride (GuHCl) to dfx, a reversible fluorescence change occurred at 2-3 M GuHCl. This transition was dependent upon protein concentration, in accord with a dimer to monomer reaction [DeltaG(H(2)O) = 46 kJ/mol of dimer]. The secondary structure did not disappear, according to far-UV circular dichroism (CD), until 6 M GuHCl was added; this transition was reversible (for incubation times of < 1 h) and independent of dfx concentration [DeltaG(H(2)O) = 50 kJ/mol of monomer]. Thus, dfx equilibrium unfolding is at least three-state, involving a monomeric intermediate with native-like secondary structure. Only after complete polypeptide unfolding (and incubation times of > 1 h) did the iron centers dissociate, as monitored by disappearance of ligand-to-metal charge transfer absorption, fluorescence of an iron indicator, and reactivity of cysteines to Ellman's reagent. Iron dissociation took place over several hours and resulted in an irreversibly denatured dfx. It appears as if the presence of the iron centers, the amino acid composition, and, to a lesser extent, the dimeric structure are factors that aid in facilitating dfx's unusually high thermodynamic stability for a mesophilic protein.     

Novel direct access to enantiomerization barriers from peak profiles in enantioselective dynamic chromatography: enantiomerization of dialkyl-1,3-allenedicarboxylates

The axially chiral allenes dimethyl-1,3-allenedicarboxylate 1 and diethyl-1,3-allenedicarboxylate 2 show characteristic plateau formation during enantioselective GC separation on the chiral stationary liquid phase Chirasil-beta-Dex. The elution profiles, obtained from temperature-dependent dynamic GC (DGC) experiments (1: 100-140 degrees C; 2: 110-150 degrees C) were evaluated with the recently derived approximation function (AF) k1(approx) = f(t(R)(A),t(R)(B),w(h)(A),h(plateau), N) to yield the enantiomerization rate constant directly k(1). These values were compared with those obtained by computer-aided simulation with ChromWin. The Eyring activation parameters of the experimental interconversion profiles were determined to be: DeltaG(#)(298.15 K) = 103.6 +/- 0.9 kJ mol(-1), DeltaH(#) = 44.7 +/- 0.4 kJ mol(-1), DeltaS(#) = -198 +/- 7 J K(1) mol(-1) for dimethyl-1,3-allenedicarboxylate 1, and DeltaG(#)(298.15 K) = 103.5 +/- 1.1 kJ mol(-1), DeltaH(#) = 44.7 +/- 0.5 kJ mol(-1), DeltaS(#) = -197 +/- 9 J K(-1) mol(-1) for diethyl-1,3-allenedicarboxylate 2. The approximation function (AF) presented here allows the fast determination of rate constants k(1) and activation barriers of enantiomerization DeltaG(#) from chromatographic parameters without extensive computer simulation.     

Unfolding and folding kinetics of amyotrophic lateral sclerosis-associated mutant Cu,Zn superoxide dismutases

More than 110 mutations in dimeric, Cu,Zn superoxide dismutase (SOD) have been linked to the fatal neurodegenerative disease, amyotrophic lateral sclerosis (ALS). In both human patients and mouse model studies, protein misfolding has been implicated in disease pathogenesis. A central step in understanding the misfolding/aggregation mechanism of this protein is the elucidation of the folding pathway of SOD. Here we report a systematic analyses of unfolding and folding kinetics using single- and double-jump experiments as well as measurements as a function of guanidium chloride, protein, and metal concentration for fully metallated (holo) pseudo wild-type and ALS-associated mutant (E100G, G93R, G93A, and metal binding mutants G85R and H46R) SODs. The kinetic mechanism for holo SODs involves native dimer, monomer intermediate, and unfolded monomer, with variable metal dissociation from the monomeric states depending on solution conditions. The effects of the ALS mutations on the kinetics of the holoproteins in guanidium chloride are markedly different from those observed previously for acid-induced unfolding and for the unmetallated (apo) forms of the proteins. The mutations decrease the stability of holo SOD mainly by increasing unfolding rates, which is particularly pronounced for the metal-binding mutants, and have relatively smaller effects on the observed folding kinetics. Mutations also seem to favour increased formation of a Zn-free monomer intermediate, which has been implicated in the formation of toxic aggregates. The results reveal the kinetic basis for the extremely high stability of wild-type holo SOD and the possible consequences of kinetic changes for disease.     

Evolutionally conserved intermediates between ubiquitin and NEDD8

The investigation of common structural motifs provides additional information on why proteins conserve similar topologies yet may have non-conserved amino acid sequences. Proteins containing the ubiquitin superfold have similar topologies, although the sequence conservation is rather poor. Here, we present novel similarities and differences between the proteins ubiquitin and NEDD8. They have 57% identical sequence, almost identical backbone topology and similar functional strategy, although their physiological functions are mutually different. Using variable pressure NMR spectroscopy, we found that the two proteins have similar conformational fluctuation in the evolutionary conserved enzyme-binding region and contain a structurally similar locally disordered conformer (I) in equilibrium with the basic folded conformer (N). A notable difference between the two proteins is that the equilibrium population of I is far greater for NEDD8 (DeltaG(0)(NI)<5 kJ/mol) than for ubiquitin (DeltaG(0)(NI)=15.2(+/-1.0) kJ/mol), and that the tendency for overall unfolding (U) is also far higher for NEDD8 (DeltaG(0)(NU)=11.0(+/-1.5) kJ/mol) than for ubiquitin (DeltaG(0)(NU)=31.3(+/-4.7) kJ/mol). These results suggest that the marked differences in thermodynamic stabilities of the locally disordered conformer (I) and the overall unfolding species (U) are a key to determine the functional differences of the two structurally similar proteins in physiology.     

Thermodynamic effects of the hydrophobic surfactant proteins on the early adsorption of pulmonary surfactant

We determined the influence of the two hydrophobic proteins, SP-B and SP-C, on the thermodynamic barriers that limit adsorption of pulmonary surfactant to the air-water interface. We compared the temperature and concentration dependence of adsorption, measured by monitoring surface tension, between calf lung surfactant extract (CLSE) and the complete set of neutral and phospholipids (N&PL) without the proteins. Three stages generally characterized the various adsorption isotherms: an initial delay during which surface tension remained constant, a fall in surface tension at decreasing rates, and, for experiments that reached approximately 40 mN/m, a late acceleration of the fall in surface tension to approximately 25 mN/m. For the initial change in surface tension, the surfactant proteins accelerated adsorption for CLSE relative to N&PL by more than ten-fold, reducing the Gibbs free energy of transition (DeltaG(O)) from 119 to 112 kJ/mole. For the lipids alone in N&PL, the enthalpy of transition (DeltaH(O), 54 kJ/mole) and entropy (-T. DeltaS, 65 kJ/mole at 37 degrees C) made roughly equal contributions to DeltaG(O). The proteins in CLSE had little effect on -T. DeltaS(O) (68 kJ/mole), but lowered DeltaG(O) for CLSE by reducing DeltaH(O) (44 kJ/mole). Models of the detailed mechanisms by which the proteins facilitate adsorption must meet these thermodynamic constraints.     

Pure-culture growth of fermentative bacteria, facilitated by H2 removal: bioenergetics and H2 production

We used an H2-purging culture vessel to replace an H2-consuming syntrophic partner, allowing the growth of pure cultures of Syntrophothermus lipocalidus on butyrate and Aminobacterium colombiense on alanine. By decoupling the syntrophic association, it was possible to manipulate and monitor the single organism's growth environment and determine the change in Gibbs free energy yield (DeltaG) in response to changes in the concentrations of reactants and products, the purging rate, and the temperature. In each of these situations, H2 production changed such that DeltaG remained nearly constant for each organism (-11.1 +/- 1.4 kJ mol butyrate(-1) for S. lipocalidus and -58.2 +/- 1.0 kJ mol alanine(-1) for A. colombiense). The cellular maintenance energy, determined from the DeltaG value and the hydrogen production rate at the point where the cell number was constant, was 4.6 x 10(-13) kJ cell(-1) day(-1) for S. lipocalidus at 55 degrees C and 6.2 x 10(-13) kJ cell(-1) day(-1) for A. colombiense at 37 degrees C. S. lipocalidus, in particular, seems adapted to thrive under conditions of low energy availability.     

Equilibrium and kinetic folding of an alpha-helical Greek key protein domain: caspase recruitment domain (CARD) of RICK

We have characterized the equilibrium and kinetic folding of a unique protein domain, caspase recruitment domain (CARD), of the RIP-like interacting CLARP kinase (RICK) (RICK-CARD), which adopts a alpha-helical Greek key fold. At equilibrium, the folding of RICK-CARD is well described by a two-state mechanism representing the native and unfolded ensembles. The protein is marginally stable, with a DeltaG(H)()2(O) of 3.0 +/- 0.15 kcal/mol and an m-value of 1.27 +/- 0.06 kcal mol(-1) M(-1) (30 mM Tris-HCl, pH 8, 1 mM DTT, 25 degrees C). While the m-value is constant, the protein stability decreases in the presence of moderate salt concentrations (below 200 mM) and then increases at higher salt concentrations. The results suggest that electrostatic interactions are stabilizing in the native protein, and the favorable Coulombic interactions are reduced at low ionic strength. Above 200 mM salt, the results are consistent with Hofmeister effects. The unfolding pathway of RICK-CARD is complex and contains at least three non-native conformations. The refolding pathway of RICK-CARD also is complex, and the data suggest that the unfolded protein folds via two intermediate conformations prior to reaching the native state. Overall, the data suggest the presence of kinetically trapped, or misfolded, species that are on-pathway both in refolding and in unfolding.     

A molten globule-like intermediate state detected in the thermal transition of cytochrome c under low salt concentration

To understand the stabilization mechanism of the transient intermediate state in protein folding, it is very important to understand the structure and stability of the molten globule state under a native condition, in which the native state exists stably. The thermal transitions of horse cytochrome c were thermodynamically evaluated by highly precise differential scanning calorimetry (DSC) at pH 3.8-5.0. The heat capacity functions were analyzed using double deconvolution and the nonlinear least-squares method. An intermediate (I) state is clearly confirmed in the thermal native (N)-to-denatured (D) transition of horse cytochrome c. The mole fraction of the intermediate state shows the largest value, 0.4, at nearly 70 degrees C at pH 4.1. This intermediate state was also detected by the circular dichroism (CD) method and was found to have the properties of the molten globule-like structure by three-state analysis of the CD data. The Gibbs free-energy change between N and I, DeltaG(NI), and that between N and D, DeltaG(ND), were evaluated to be 9-22 kJ mol(-1) and 41-45 kJ mol(-1), respectively at 15( ) degrees C and pH 4.1.     

Mutational analysis of the subunit interface of Vibrio harveyi bacterial luciferase

Bacterial luciferase is a heterodimeric (alphabeta) enzyme which catalyzes a light-producing reaction in Vibrio harveyi. In addition to the alphabeta enzyme, the beta subunit can self-associate to form a stable but inactive homodimer [Sinclair, J. F., Ziegler, M. M., and Baldwin, T. O. (1994) Nat. Struct. Biol. 1, 320-326]. The studies reported here were undertaken to explore the role of the subunit interface in the conformational stability of the enzyme. To this end, we constructed four mutant heterodimers in which residues at the subunit interface were changed in an effort to alter the volume of an apparent solvent accessible channel at the interface or to alter H-bonding groups. Equilibrium unfolding data for the heterodimer have been interpreted in terms of a three-state mechanism [Clark, C. A., Sinclair, J. F., and Baldwin, T. O. (1993) J. Biol. Chem. 268, 10773-10779]. However, we found that unfolding for the wild-type and mutant luciferases is better described by a four-state model. This change in the proposed mechanism of unfolding is based on observation of residual structure in the subunits following dissociation of the heterodimeric intermediate. All of the mutants display modest reductions in activity but, surprisingly, no change in the DeltaG2H2O value for subunit dissociation and no measurable change in the equilibrium dissociation constant relative to that of the wild-type heterodimer. However, the DeltaG1H2O value for the formation of the dimeric intermediate that precedes subunit dissociation is reduced for three of the mutants, indicating that mutations at the interface can alter the stability of a region of the alpha subunit that is distant from the interface. We conclude that the interface region communicates with the distal domains of this subunit, probably through the active center region of the enzyme.     

pH-dependent stability and folding kinetics of a protein with an unusual alpha-beta topology: the C-terminal domain of the ribosomal protein L9

The folding kinetics and thermodynamics of the isolated C-terminal domain of the ribosomal protein L9 (CTL9) have been studied as a function of pH. CTL9 is an alpha-beta protein that contains a single beta-sheet with an unusual mixed parallel, anti-parallel topology. The folding is fully reversible and two-state over the entire pH range. Stopped-flow fluorescence and CD experiments yield the same folding rate, and the chevron plots have the characteristic V-shape expected for two-state folding. The values of DeltaG*(H2O) and the m value calculated from the kinetic experiments are in excellent agreement with the equilibrium measurements. The extrapolated initial amplitudes of both the stopped-flow fluorescence and CD measurements show that there is no detectable burst phase intermediate. The domain contains three histidine residues, two of which are largely buried in the native state. They do not participate in salt-bridges or take part in a hydrogen bonded network. NMR measurements reveal that the buried histidine residues have significantly perturbed pK(a) values in the native state. The equilibrium stability and the folding rate are found to be strongly dependent upon their ionization state. There is a linear relationship between the log of the folding rate and DeltaG* (H2O) . The protein is much more stable and folds noticeably faster at pH values above the native state pK(a) values. DeltaG*(H2O) of unfolding increases from 2.90 kcal mol(-1) at pH 5.0 to 6.40 kcal mol(-1) at pH 8.0 while the folding rate increases from 0.60 to 18.7 s(-1). Tanford linkage analysis revealed that the interactions involving the two histidine residues are largely developed in the transition state. The results are compared to other studies of the pH-dependence of folding.