Myoglobin with chlorophyllous chromophores: Influence on protein stability

The stabilities of myoglobin, apo-myoglobin, and of two myoglobins with chlorophyllous chromophores (Zn-pheophorbide a and Zn-bacteriopheophorbide a), have been studied by thermal and chemical denaturation. With guanidinium chloride, the stability order is myoglobin > Zn-pheophorbide-myoglobin > Zn-bacteriopheophorbide-myoglobin ∼ apo-myoglobin. The thermal behavior is more complex. The transition temperature of thermal unfolding of the apoprotein (62.4 °C) is increased by Zn-pheophorbide a (83.9 °C) and Zn-bacteriopheophorbide a (82.6 °C) to a similar degree as by the native chromophore, heme (83.5 °C). The recovery with Zn-pheophorbide (92-98%) is even higher than with heme (74-76%), while with Zn-bacteriopheophorbide (40%) it is as low as with the apoprotein (42%). Recovery also depends on the rates of heating, and in particular the time spent at high temperatures. It is concluded that irreversibility of unfolding is related to loss of the chromophores, which are required for proper re-folding.     

Thermal and conformational stability of seed coat soybean peroxidase

Soybean peroxidase (SBP) obtained from the soybean seed coats belongs to class III of the plant peroxidase superfamily. Detailed circular dichroism and steady state fluorescence studies have been carried out to monitor thermal as well as denaturant-induced unfolding of SBP and apo-SBP. Melting of secondary and tertiary structures of SBP occurs with characteristic transition midpoints, T(m), of 86 and 83.5 degrees C, respectively, at neutral pH. Removal of heme resulted in greatly decreased thermal stability of the protein (T(m) = 38 degrees C). The deltaG degrees (H2O) determined from guanidine hydrochloride-induced denaturation at 25 degrees C and at neutral pH is 43.3 kJ mol(-1) for SBP and 9.0 kJ mol(-1) for apo-SBP. Comparison with the reported unfolding data of the homologous enzyme, horseradish peroxidase (HRP-C), showed that SBP exhibits significantly high thermal and conformational stability. We show that this enhanced structural stability of SBP relative to HRP-C arises due to the unique nature of their heme binding. A stronger heme-apoprotein affinity probably due to the interaction between Met37 and the C8 heme vinyl substituent contributes to the unusually high structural stability of SBP.     

Myoglobin with modified tetrapyrrole chromophores: binding specificity and photochemistry

Complexes were prepared of horse heart myoglobin with derivatives of (bacterio)chlorophylls and the linear tetrapyrrole, phycocyanobilin. Structural factors important for binding are (i) the presence of a central metal with open ligation site, which even induces binding of phycocyanobilin, and (ii) the absence of the hydrophobic esterifying alcohol, phytol. Binding is further modulated by the stereochemistry at the isocyclic ring. The binding pocket can act as a reaction chamber: with enolizable substrates, apo-myoglobin acts as a 13(2)-epimerase converting, e.g., Zn-pheophorbide a' (13(2)S) to a (13(2)R). Light-induced reduction and oxidation of the bound pigments are accelerated as compared to solution. Some flexibility of the myoglobin is required for these reactions to occur; a nucleophile is required near the chromophores for photoreduction (Krasnovskii reaction), and oxygen for photooxidation. Oxidation of the bacteriochlorin in the complex and in aqueous solution continues in the dark.     

Myoglobin with modified tetrapyrrole chromophores: Binding specificity and photochemistry

Complexes were prepared of horse heart myoglobin with derivatives of (bacterio)chlorophylls and the linear tetrapyrrole, phycocyanobilin. Structural factors important for binding are (i) the presence of a central metal with open ligation site, which even induces binding of phycocyanobilin, and (ii) the absence of the hydrophobic esterifying alcohol, phytol. Binding is further modulated by the stereochemistry at the isocyclic ring. The binding pocket can act as a reaction chamber: with enolizable substrates, apo-myoglobin acts as a 13²-epimerase converting, e.g., Zn-pheophorbide a' (13²S) to a (13²R). Light-induced reduction and oxidation of the bound pigments are accelerated as compared to solution. Some flexibility of the myoglobin is required for these reactions to occur; a nucleophile is required near the chromophores for photoreduction (Krasnovskii reaction), and oxygen for photooxidation. Oxidation of the bacteriochlorin in the complex and in aqueous solution continues in the dark.     

Folding of horse cytochrome c in the reduced state

Equilibrium and kinetic folding studies of horse cytochrome c in the reduced state have been carried out under strictly anaerobic conditions at neutral pH, 10 degrees C, in the entire range of aqueous solubility of guanidinium hydrochloride (GdnHCl). Equilibrium unfolding transitions observed by Soret heme absorbance, excitation energy transfer from the lone tryptophan residue to the ferrous heme, and far-UV circular dichroism (CD) are all biphasic and superimposable, implying no accumulation of structural intermediates. The thermodynamic parameters obtained by two-state analysis of these transitions yielded DeltaG(H2O)=18.8(+/-1.45) kcal mol(-1), and C(m)=5.1(+/-0.15) M GdnHCl, indicating unusual stability of reduced cytochrome c. These results have been used in conjunction with the redox potential of native cytochrome c and the known stability of oxidized cytochrome c to estimate a value of -164 mV as the redox potential of the unfolded protein. Stopped-flow kinetics of folding and unfolding have been recorded by Soret heme absorbance, and tryptophan fluorescence as observables. The refolding kinetics are monophasic in the transition region, but become biphasic as moderate to strongly native-like conditions are approached. There also is a burst folding reaction unobservable in the stopped-flow time window. Analyses of the two observable rates and their amplitudes indicate that the faster of the two rates corresponds to apparent two-state folding (U<-->N) of 80-90 % of unfolded molecules with a time constant in the range 190-550 micros estimated by linear extrapolation and model calculations. The remaining 10-20 % of the population folds to an off-pathway intermediate, I, which is required to unfold first to the initial unfolded state, U, in order to refold correctly to the native state, N (I<-->U<-->N). The slower of the two observable rates, which has a positive slope in the linear functional dependence on the denaturant concentration indicating that an unfolding process under native-like conditions indeed exists, originates from the unfolding of I to U, which rate-limits the overall folding of these 10-20 % of molecules. Both fast and slow rates are independent of protein concentration and pH of the refolding milieu, suggesting that the off-pathway intermediate is not a protein aggregate or trapped by heme misligation. The nature or type of unfolded-state heme ligation does not interfere with refolding. Equilibrium pH titration of the unfolded state yielded coupled ionization of the two non-native histidine ligands, H26 and H33, with a pK(a) value of 5.85. A substantial fraction of the unfolded population persists as the six-coordinate form even at low pH, suggesting ligation of the two methionine residues, M65 and M80. These results have been used along with the known ligand-binding properties of unfolded cytochrome c to propose a model for heme ligation dynamics. In contrast to refolding kinetics, the unfolding kinetics of reduced cytochrome c recorded by observation of Soret absorbance and tryptophan fluorescence are all slow, simple, and single-exponential. In the presence of 6.8 M GdnHCl, the unfolding time constant is approximately 300(+/-125) ms. There is no burst unfolding reaction. Simulations of the observed folding-unfolding kinetics by numerical solutions of the rate equations corresponding to the three-state I<-->U<-->N scheme have yielded the microscopic rate constants.     

Protein thermal aggregation involves distinct regions: sequential events in the heat-induced unfolding and aggregation of hemoglobin

Protein thermal aggregation plays a crucial role in protein science and engineering. Despite its biological importance, little is known about the mechanism and pathway(s) involved in the formation of aggregates. In this report, the sequential events occurring during thermal unfolding and aggregation process of hemoglobin were studied by two-dimensional infrared correlation spectroscopy. Analysis of the infrared spectra recorded at different temperatures suggested that hemoglobin denatured by a two-stage thermal transition. At the initial structural perturbation stage (30-44 degrees C), the fast red shift of the band from alpha-helix indicated that the native helical structures became more and more solvent-exposed as temperature increased. At the thermal unfolding stage (44-54 degrees C), the unfolding of solvent-exposed helical structures dominated the transition and was supposed to be responsible to the start of aggregation. At the thermal aggregation stage (54-70 degrees C), the transition was dominated by the formation of aggregates and the further unfolding of the buried structures. A close inspection of the sequential events occurring at different stages suggested that protein thermal aggregation involves distinct regions.     

Structural stability of the PsbQ protein of higher plant photosystem II

We have characterized the stability and folding behavior of the isolated extrinsic PsbQ protein of photosystem II (PSII) from a higher plant, Spinacia oleracea, using intrinsic protein fluorescence emission and near- and far-UV circular dichroism (CD) spectroscopy in combination with differential scanning calorimetry (DSC). Experimental results reveal that both chemical denaturation using guanidine hydrochloride (GdnHCl) and thermal unfolding of PsbQ proceed as a two-state reversible process. The denaturation free-energy changes (DeltaG(D)) at 20 degrees C extrapolated from GdnHCl (4.0 +/- 0.6 kcal mol(-1)) or thermal unfolding (4.4 +/- 0.8 kcal mol(-1)) are very close. Moreover, the far-UV CD spectra of the denatured PsbQ registered at 90 degrees C in the absence and presence of 6.0 M GdnHCl superimpose, leading us to conclude that both denatured states of PsbQ are structurally and energetically similar. The thermal unfolding of PsbQ has been also characterized by CD and DSC over a wide pH range. The stability of PsbQ is at its maximum at pH comprised between 5 and 8, being wider than the optimal pH for oxygen evolution in the lumen of thylakoid membranes. In addition, no significant structural changes were detected in PsbQ between 50 and 55 degrees C in the pH range of 3-8, suggesting that PsbQ behaves as a soluble and stable particle in the lumen when it detaches from PSII under physiological stress conditions such as high temperature (45-50 degrees C) or low pH (<5.0). Sedimentation experiments showed that, in solution at 20 degrees C, the PsbQ protein is a monomer with an elongated shape.     

Infrared spectroscopic discrimination between the loop and alpha-helices and determination of the loop diffusion kinetics by temperature-jump time-resolved infrared spectroscopy for cytochrome c

The infrared (IR) absorption of the amide I band for the loop structure may overlap with that of the alpha-helices, which can lead to the misassignment of the protein secondary structures. A resolution-enhanced Fourier transform infrared (FTIR) spectroscopic method and temperature-jump (T-jump) time-resolved IR absorbance difference spectra were used to identify one specific loop absorption from the helical IR absorption bands of horse heart cytochrome c in D2O at a pD around 7.0. This small loop consists of residues 70-85 with Met-80 binding to the heme Fe(III). The FTIR spectra in amide I' region indicate that the loop and the helical absorption bands overlap at 1653 cm(-1) at room temperature. Thermal titration of the amide I' intensity at 1653 cm(-1) reveals that a transition in loop structural change occurs at lower temperature (Tm=45 degrees C), well before the global unfolding of the secondary structure (Tm approximately 82 degrees C). This loop structural change is assigned as being triggered by the Met-80 deligation from the heme Fe(III). T-jump time-resolved IR absorbance difference spectra reveal that a T-jump from 25 degrees C to 35 degrees C breaks the Fe-S bond between the Met-80 and the iron reversibly, which leads to a loop (1653 cm(-1), overlap with the helical absorption) to random coil (1645 cm(-1)) transition. The observed unfolding rate constant interpreted as the intrachain diffusion rate for this 16 residue loop was approximately 3.6x10(6) s(-1).     

Fourier transform infrared spectroscopy suggests unfolding of loop structures precedes complete unfolding of pig citrate synthase

Pig citrate synthase (PCS) can be used as a model enzyme to gain some insight into the structural basis of protein thermostability. The thermal unfolding characteristics of the specific secondary structure elements within PCS were monitored in detail by following changes in its amide I band components. The result of our study indicates that PCS undergoes irreversible thermal denaturation. Detailed analysis reveals that the different secondary structures display a multistep transition with a major and a minor transition at different temperatures and a very small initial transition at the same temperature (30 degrees C). A plot of temperature-induced changes in (1)H-(2)H exchange, the decrease in the absorbance of the alpha-helical structures, and the increase in the absorbance of aggregated structures all have in common a multistep transition, the minor one centered at 45 degrees C and the major one around 59 degrees C. In contrast, a band that is tentatively assigned to loop structures displays these same minor and major transitions but at lower temperatures (39 and 52 degrees C, respectively). The transition, which occurs at 39-45 degrees C, is not associated with the appearance of aggregated structures. This transition may reflect a change in the tertiary structure of the protein. However, the final transition, which occurs at a higher temperature (52-59 degrees C), reflects unfolding and aggregation of the polypeptide chains. The Fourier transform infrared (FTIR) analysis suggests that PCS has a thermolabile region that unfolds first, some 7 degrees C below the main unfolding of the protein. We propose that this reflects the unfolding of the highly flexible loop segments, which in turn triggers the unfolding of the predominantly helical core structure of PCS.     

Thermal unfolding mechanism of lipocalin-type prostaglandin D synthase

Lipocalin-type prostaglandin (PG) D synthase (L-PGDS) is a dual-functioning protein in the lipocalin family, acting as a PGD(2)-synthesizing enzyme and as an extracellular transporter for small lipophilic molecules. We earlier reported that denaturant-induced unfolding of L-PGDS follows a four-state pathway, including an activity-enhanced state and an inactive intermediate state. In this study, we investigated the thermal unfolding mechanism of L-PGDS by using differential scanning calorimetry (DSC) and CD spectroscopy. DSC measurements revealed that the thermal unfolding of L-PGDS was a completely reversible process at pH 4.0. The DSC curves showed no concentration dependency, demonstrating that the thermal unfolding of L-PGDS involved neither intermolecular interaction nor aggregation. On the basis of a simple two-state unfolding mechanism, the ratio of van't Hoff enthalpy (DeltaH(vH)) to calorimetric enthalpy (DeltaH(cal)) was below 1, indicating the presence of an intermediate state (I) between the native state (N) and unfolded state (U). Then, statistical thermodynamic analyses of a three-state unfolding process were performed. The heat capacity curves fit well with a three-state process; and the estimated transition temperature (T(m)) and enthalpy change (DeltaH(cal)) of the N<-->I and I<-->U transitions were 48.2 degrees C and 190 kJ.mol(-1), and 60.3 degrees C and 144 kJ.mol(-1), respectively. Correspondingly, the thermal unfolding monitored by CD spectroscopy at 200, 235 and 290 nm revealed that L-PGDS unfolded through the intermediate state, where its main chain retained the characteristic beta-sheet structure without side-chain interactions.     

The thermal denaturation of ribonuclease A in aqueous-methanol solvents.

Circular dichroism was used to monitor the thermal unfolding of ribonuclease A in 50% aqueous methanol. The spectrum of the protein at temperatures below -10 degrees C (pH* 3.0) was essentially identical to that of native ribonuclease A in aqueous solution. The spectrum of the thermally denatured material above 70 degrees C revealed some residual secondary structure in comparison to protein unfolded by 5 M Gdn.HCl at 70 degrees C in the presence or absence of methanol. The spectra as a function of temperature were deconvoluted to determine the contributions of different types of secondary structure. The position of the thermal unfolding transition as monitored by alpha-helix, with a midpoint at 38 degrees C, was at a much higher temperature than that monitored by beta-sheet, 26 degrees C, which also corresponded to that observed by delta A286, tyrosine fluorescence and hydrodynamic radius (from light scattering measurements). Thus, the loss of beta-sheet structure is decoupled from that of alpha-helix, suggesting a step-wise unfolding of the protein. The transition observed for loss of alpha-helix coincides with the previously measured transition for His-12 by NMR from a partially folded state to the unfolded state, suggesting that the unfolding of the N-terminal helix in RNase A is lost after unfolding of the core beta-sheet during thermal denaturation. The thermally denatured protein was relatively compact, as measured by dynamic light scattering.     

Structural and conformational stability of horseradish peroxidase: effect of temperature and pH

Detailed circular dichroism and fluorescence studies at different pHs have been carried out to monitor thermal unfolding of horseradish peroxidase isoenzyme c (HRPc). The change in CD in the 222 nm region corresponds to changes in the overall secondary structure of the enzyme, while that in the 400 nm region (Soret region) corresponds to changes in the tertiary structure around the heme in the enzyme. The temperature dependence of the tertiary structure around the heme also affected the intrinsic tryptophan fluorescence emission spectrum of the enzyme. The results suggested that melting of the tertiary structure to a pre-molten globule form takes place at 45 degrees C, which is much lower than the temperature (T(m) = 74 degrees C) at which depletion of heme from the heme cavity takes place. The melting of the tertiary structure was found to be associated with a pK(a) of approximately 5, indicating that this phase possibly involves breaking of the hydrogen-bonding network of the heme pocket, keeping the heme moiety still inside it. The stability of the secondary structure of the enzyme was also found to decrease at pH below 4.5. A 'high temperature' unfolding phase was observed which was, however, independent of pH. The stability of the secondary structure was found to drastically decrease in the presence of DTT (dithiothreitol), indicating that the 'high temperature' form is possibly stabilized due to interhelical disulfide bonds. Depletion of Ca(2+) ions resulted in a marked decrease in the stability of the secondary structure of the enzyme.     

Unfolding transitions of fibronectin and its domains. Stabilization and structural alteration of the N-terminal domain by heparin.

Changes in the conformational state of human plasma fibronectin and several of its fragments were studied by fluorescence emission, intrinsic fluorescence polarization and c.d. spectroscopy under conditions of guanidinium chloride-and temperature-induced unfolding. Fragments were chosen to represent all three types of internal structural homology in the protein. Low concentration (less than 2 M) of guanidinium chloride induced a gradual transition in the intact protein that was not characteristic of any of the isolated domains, suggesting the presence of interdomain interactions within the protein. Intermediate concentrations of guanidinium chloride (2-3 M) and moderately elevated temperatures (55-60 degrees C) induced a highly co-operative structural transition in intact fibronectin that was attributable to the central 110 kDa cell-binding domain. High temperatures (greater than 60 degrees C) produced a gradual unfolding in the intact protein attributable to the 29 kDa N-terminal heparin-binding and 40 kDa collagen-binding domains. Binding of heparin to intact fibronectin and to its N-terminal fragment stabilized the proteins against thermal unfolding. This was reflected in increased delta H for the unfolding transitions of the heparin-bound N-terminal fragment, as well as decreased accessibility to solvent perturbants of internal chromophores in this fragment when bound to heparin. These results help to account for the biological efficacy of the interaction between the fibronectin N-terminal domain and heparin, despite its relatively low affinity.     

Thermodynamic characterization of an intermediate state of human growth hormone.

The thermal denaturation of recombinant human growth hormone (rhGH) was studied by differential scanning calorimetry and circular dichroism spectroscopy (CD). The thermal unfolding is reversible only below pH 3.5, and under these conditions a single two-state transition was observed between 0 and 100 degrees C. The magnitudes of the deltaH and deltaCp of this transition indicate that it corresponds to a partial unfolding of rhGH. This is also supported by CD data, which show that significant secondary structure remains after the unfolding. Above pH 3.5 the thermal denaturation is irreversible due to the aggregation of rhGH upon unfolding. This aggregation is prevented in aqueous solutions of alcohols such as n-propanol, 2-propanol, or 1,2-propanediol (propylene glycol), which suggests that the self-association of rhGH is caused by hydrophobic interactions. In addition, it was found that the native state of rhGH is stable in relatively high concentrations of propylene glycol (up to 45% v/v at pH 7-8 or 30% at pH 3) and that under these conditions the thermal unfolding is cooperative and corresponds to a transition from the native state to a partially folded state, as observed at acidic pH in the absence of alcohols. In higher concentrations of propylene glycol, the tertiary structure of rhGH is disrupted and the cooperativity of the unfolding decreases. Moreover, the CD and DSC data indicate that a partially folded intermediate with essentially native secondary structure and disordered tertiary structure becomes significantly populated in 70-80% propylene glycol.     

Complexes of smooth muscle tropomyosin with F-actin studied by differential scanning calorimetry.

Differential scanning calorimetry (DSC) and light scattering were used to analyze the interaction of duck gizzard tropomyosin (tropomyosin) with rabbit skeletal-muscle F-actin. In the absence of F-actin, tropomyosin, represented mainly by heterodimers, unfolds at 41 degrees C with a sharp thermal transition. Interaction of tropomyosin heterodimers with F-actin causes a 2-6 degrees C shift in the tropomyosin thermal transition to higher temperature, depending on the tropomyosin/actin molar ratio and protein concentration. A pronounced shift of the tropomyosin thermal transition was observed only for tropomyosin heterodimers, and not for homodimers. The most pronounced effect was observed after complete saturation of F-actin with tropomyosin molecules, at tropomyosin/actin molar ratios > 1 : 7. Under these conditions, two well-separated peaks of tropomyosin were observed on the thermogram besides the peak of F-actin, the peak characteristic of free tropomyosin heterodimer, and the peak with a maximum at 45-47 degrees C corresponding to tropomyosin bound to F-actin. By measuring the temperature-dependence of light scattering, we found that thermal unfolding of tropomyosin is accompanied by its dissociation from F-actin. Thermal unfolding of tropomyosin is almost completely reversible, whereas F-actin denatures irreversibly. The addition of tropomyosin has no effect on thermal unfolding of F-actin, which denatures with a maximum at 64 degrees C in the absence and at 78 degrees C in the presence of a twofold molar excess of phalloidin. After the F-actin-tropomyosin complex had been heated to 90 degrees C and then cooled (i.e. after complete irreversible denaturation of F-actin), only the peak characteristic of free tropomyosin was observed on the thermogram during reheating, whereas the thermal transitions of F-actin and actin-bound tropomyosin completely disappeared. Therefore, the DSC method allows changes in thermal unfolding of tropomyosin resulting from its interaction with F-actin to be probed very precisely.     

The mechanism of heme transfer from the cytoplasmic heme binding protein PhuS to the delta-regioselective heme oxygenase of Pseudomonas aeruginosa

The opportunistic pathogen Pseudomonas aeruginosa has evolved two outer membrane receptor-mediated uptake systems (encoded by the phu and has operons) by which it can utilize the hosts heme and hemeproteins as a source of iron. PhuS is a cytoplasmic heme binding protein encoded within the phu operon and has previously been shown to function in the trafficking of heme to the iron-regulated heme oxygenase (pa-HO). While the heme association rate for PhuS was similar to that of myoglobin, a markedly higher rate of heme dissociation (approximately 10(5) s(-1)) was observed, in keeping with a function in heme-trafficking. Additionally, the transfer of heme from PhuS to pa-HO was shown to be specific and unidirectional when compared to transfer to the non-iron regulated heme oxygenase (BphO), in which heme distribution between the two proteins merely reflects their relative intrinsic affinities for heme. Furthermore, the rate of transfer of heme from holo-PhuS to pa-HO of 0.11 +/- 0.01 s(-1) is 30-fold faster than that to apo-myoglobin, despite the significant higher binding affinity of apo-myoglobin for heme (kH = 1.3 x 10(-8) microM) than that of PhuS (0.2 microM). This data suggests that heme transfer to pa-HO is independent of heme affinity and is consistent with temperature dependence studies which indicate the reaction is driven by a negative entropic contribution, typical of an ordered transition state, and supports the notion that heme transfer from PhuS to pa-HO is mediated via a specific protein-protein interaction. In addition, pH studies, and reactions conducted in the presence of cyanide, suggest the involvement of spin transition during the heme transfer process, whereby the heme undergoes spin change from 6-c LS to 6-c HS either in PhuS or pa-HO. On the basis of the magnitudes of the activation parameters obtained in the presence of cyanide, whereby both complexes are maintained in a 6-c LS state, and the biphasic kinetics of heme transfer from holo-PhuS to pa-HO-wt, supports the notion that the spin-state crossover occur within holo-PhuS prior to the heme transfer step. Alternatively, the lack of the biphasic kinetic with pa-HO-G125V, 6-c LS, and with comparable rate of heme transfer as pa-HO is supportive of a mechanism in which the spin-change could occur within pa-HO. The present data suggests either or both of the two pathways proposed for heme transfer may occur under the present experimental conditions. The dissection of which pathway is physiologically relevant is the focus of ongoing studies.     

Structural stability and unfolding properties of thermostable bacterial alpha-amylases: a comparative study of homologous enzymes

In a comparative investigation on two thermostable alpha-amylases [Bacillus amyloliquefaciens (BAA), T(m) = 86 degrees C and Bacillus licheniformis (BLA), T(m) = 101 degrees C], we studied thermal and guanidine hydrochloride (GndHCl)-induced unfolding using fluorescence and CD spectroscopy, as well as dynamic light scattering. Depletion of calcium from specific ion-binding sites in the protein structures reduces the melting temperature tremendously for both alpha-amylases. The reduction is nearly the same for both enzymes, namely, in the order of 50 degrees C. Thus, the difference in thermostability between BLA and BAA (DeltaT(m) approximately 15 degrees C) is related to intrinsic properties of the respective protein structures themselves and is not related to the strength of ion binding. The thermal unfolding of both proteins is characterized by a full disappearance of secondary structure elements and by a concurrent expansion of the 3D structure. GndHCl-induced unfolding also yields a fully vanishing secondary structure but with more expanded 3D structures. Both alpha-amylases remain much more compact upon thermal unfolding as compared to the fully unfolded state induced by chemical denaturants. Such rather compact thermal unfolded structures lower the conformational entropy change during the unfolding transition, which principally can contribute to an increased thermal stability. Structural flexibilities of both enzymes, as measured with tryptophan fluorescence quenching, are almost identical for both enzymes in the native states, as well as in the unfolded states. Furthermore, we do not observe any difference in the temperature dependence of the structural flexibilities between BLA and BAA. These results indicate that conformational dynamics on the time scale of our studies seem not to be related to thermal stability or to thermal adaptation.     

Reversible unfolding of beta-sheets in membranes: a calorimetric study

The hexapeptide acetyl-Trp-Leu(5) (AcWL(5)) has the remarkable ability to assemble reversibly and spontaneously into beta-sheets on lipid membranes as a result of monomer partitioning followed by cooperative assembly. This system provides a unique opportunity to study the thermodynamics of protein folding in membranes, which we have done using isothermal titration calorimetry (ITC) and differential scanning calorimetry (DSC). The results, which may represent the first example of reversible thermal unfolding of peptides in membranes, help to define the contribution of hydrogen bonding to the extreme thermal stability of membrane proteins. ITC revealed that the enthalpy change for partitioning of monomeric, unstructured AcWL(5) from water into membranes was zero within experimental error over the temperature range of 5 degrees C to 75 degrees C. DSC showed that the beta-sheet aggregates underwent a reversible, endothermic, and very asymmetric thermal transition with a concentration-dependent transition temperature (T(m)) in the range of 60 degrees C to 80 degrees C. A numerical model of nucleation and growth-dependent assembly of oligomeric beta-sheets, proposed earlier to describe beta-sheet formation in membranes, recreated remarkably well the unusual shape and concentration-dependence of the transition peaks. The enthalpy for thermal unfolding of AcWL(5) beta-sheets in the membrane was found to be about 8(+/-1)kcal mol(-1), or about 1.3(+/-0.2)kcal mol(-1) per residue.     

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.