Kinetics of open complex formation between Escherichia coli RNA polymerase and the lac UV5 promoter. Evidence for a sequential mechanism involving three steps

The forward and reverse kinetics of open complex formation between Escherichia coli RNA polymerase and the lac UV5 promoter have been studied in the temperature range of 15-42 degrees C. The standard two-step model, involving the formation of a closed intermediate, RPc, followed by an isomerization that leads to the active complex RPo, could not account for the present data. The promoter-enzyme lifetime measurements showed an inverse temperature dependence (apparent activation energy, -35 kcal/mol). A third step, which is very temperature dependent and which is very rapid at 37 degrees C, was postulated to involve the unstacking of DNA base pairs that immediately precedes open complex formation. Evidence for incorporating a new binary complex, RPi, in the pathway was provided by experiments that distinguished between stably bound species and active promoter after temperature-jump perturbations. These experiments allowed measurement of the rate of reequilibration between the stably bound species and determination of the corresponding equilibrium constant. They indicated that the third step became rate limiting below 20 degrees C; this prediction was checked by an analysis of the forward kinetics. A quantitative evaluation of the parameters involved in this three-step model is provided. Similar experiments were performed on a negatively supercoiled template: in this case the third equilibrium was driven toward formation of the open complex even at low temperature, and the corresponding step was not rate limiting.     

Spectroscopic analysis of DNA base-pair opening by Escherichia coli RNA polymerase. Temperature and ionic strength effects

The interaction of Escherichia coli RNA polymerase with poly[d(A-T)] and poly[d-(I-C)] was studied by difference absorption spectroscopy at temperatures, from 5 to 45 degrees C in the absence and presence of Mg2+. The effect of KCl concentration, at a fixed temperature, was studied from 12.5 to 400 mM. Difference absorption experiments permitted calculation of the extent of DNA opening induced by RNA polymerase and estimation of the equilibrium constant associated with the isomerization from a closed to an open RNA polymerase-DNA complex. delta H0 and delta S0 for the closed-to-open transition with poly[d(A-T)] or poly[d(I-C)] complexed with RNA polymerase are significantly lower than the values associated with the helix-to-coil transition for the free polynucleotides. For the RNA polymerase complexes with poly[d(A-T)] and poly[d(I-C)] in 50 mM KCl, delta H0 approximately 15-16 kcal/mol (63-67 kJ/mol) and delta S0 approximately 50-57 cal/K per mol (209-239 J/K per mol). The presence of Mg2+ does not change these parameters appreciably for the RNA polymerase-poly[d(A-T)] complex, but for the RNA polymerase-poly[d(I-C)] complex in the presence of Mg2+, the delta H0 and delta S0 values are larger and temperature-dependent, with delta H0 approximately 22 kcal/mol (92 kJ/mol) and delta S0 approximately 72 cal/K per mol (approx. 300 J/K per mol) at 25 degrees C, and delta Cp0 approximately 2 kcal/K per mol (approx. 8.3 kJ/K per mol). The circular dichroism (CD) changes observed for helix opening induced by RNA polymerase are qualitatively consistent with the thermally induced changes observed for the free polynucleotides, supporting the difference absorption method. The salt-dependent studies indicate that two monovalent cations are released upon helix opening. For poly[d(A-T)], the temperature-dependence of enzyme activity correlates well with the helix opening, implying this step to be the rate-determining step. In the case of poly[d(I-C)], the same is not true, and so the rate-determining step must be a process subsequent to helix opening.     

Thermodynamics of ribonuclease T1 denaturation.

Differential scanning calorimetry has been used to investigate the thermodynamics of denaturation of ribonuclease T1 as a function of pH over the pH range 2-10, and as a function of NaCl and MgCl2 concentration. At pH 7 in 30 mM PIPES buffer, the thermodynamic parameters are as follows: melting temperature, T1/2 = 48.9 +/- 0.1 degrees C; enthalpy change, delta H = 95.5 +/- 0.9 kcal mol-1; heat capacity change, delta Cp = 1.59 kcal mol-1 K-1; free energy change at 25 degrees C, delta G degrees (25 degrees C) = 5.6 kcal mol-1. Both T1/2 = 56.5 degrees C and delta H = 106.1 kcal mol-1 are maximal near pH 5. The conformational stability of ribonuclease T1 is increased by 3.0 kcal/mol in the presence of 0.6 M NaCl or 0.3 M MgCl2. This stabilization results mainly from the preferential binding of cations to the folded conformation of the protein. The estimates of the conformational stability of ribonuclease T1 from differential scanning calorimetry are shown to be in remarkably good agreement with estimates derived from an analysis of urea denaturation curves.     

Stability mutants of staphylococcal nuclease: large compensating enthalpy-entropy changes for the reversible denaturation reaction

By use of intrinsic fluorescence to determine the apparent equilibrium constant Kapp as a function of temperature, the midpoint temperature Tm and apparent enthalpy change delta Happ on reversible thermal denaturation have been determined over a range of pH values for wild-type staphylococcal nuclease and six mutant forms. For wild-type nuclease at pH 7.0, a Tm of 53.3 +/- 0.2 degrees C and a delta Happ of 86.8 +/- 1.4 kcal/mol were obtained, in reasonable agreement with values determined calorimetrically, 52.8 degrees C and 96 +/- 2 kcal/mol. The heat capacity change on denaturation delta Cp was estimated at 1.8 kcal/(mol K) versus the calorimetric value of 2.2 kcal/(mol K). When values of delta Happ and delta Sapp for a series of mutant nucleases that exhibit markedly altered denaturation behavior with guanidine hydrochloride and urea were compared at the same temperature, compensating changes in enthalpy and entropy were observed that greatly reduce the overall effect of the mutations on the free energy of denaturation. In addition, a correlation was found between the estimated delta Cp for the mutant proteins and the d(delta Gapp)/dC for guanidine hydrochloride denaturation. It is proposed that both the enthalpy/entropy compensation and this correlation between two seemingly unrelated denaturation parameters are consequences of large changes in the solvation of the denatured state that result from the mutant amino acid substitutions.     

Thermodynamic analyses of triplex formation with homopurine oligonucleotide.

We analyzed the thermodynamics of purine motif triplex formation by isothermal titration calorimetry. The signs of calorimetric enthalpy change, delta Hcal, and entropy change, delta S, of the triplex formation were negative in the temperature range between 15 and 35 degrees C. Since an observed negative delta S was unfavorable for the triplex formation, the triplex formation was driven by a large negative delta Hcal. delta Hcal decreased with increasing temperature, yielding a negative heat capacity change, delta Cp, of approximately -1.2 kcal mol-1 K-1. We found that the binding constant, Ka, increased with increasing temperature, leading to an apparent positive van't Hoff enthalpy change, delta Hvh, which was in sharp contrast with the large negative delta Hcal. The analyses of the observed temperature dependence of Ka and delta Hcal and the negative delta Cp suggest that the purine motif triplex formation near room temperature is not a simple two-state binding process but exhibits multiple states, which was previously observed for the pyrimidine motif triplex formation near room temperature.     

Binding to tubulin of the colchicine analog 2-methoxy-5-(2', 3', 4'-trimethoxyphenyl)tropone. Thermodynamic and kinetic aspects

The thermodynamics and kinetics of the binding to tubulin of the colchicine analog 2-methoxy-5-(2', 3', 4'-trimethoxyphenyl) tropone (termed AC because it lacks the B-ring of colchicine) have been characterized by fluorescence techniques. The fluorescence of AC is weak in aqueous solution and is enhanced 250-fold upon binding to tubulin. The following thermodynamic values were obtained for the interaction at 37 degrees C: K = 3.5 X 10(5) M-1; delta G0 = -7.9 kcal/mol; delta H0 = -6.8 kcal/mol; delta S0 = 3.6 entropy units. The AC-tubulin complex is 1-2 kcal/mol less stable than the colchicine-tubulin complex. The change in fluorescence of AC was employed to measure the kinetics of the association process, and quenching of protein fluorescence was used to measure both association and dissociation. The association process, like that of colchicine, could be resolved into a major fast phase and a minor slow phase. The apparent second order rate constant for the fast phase was found to be 5.2 X 10(4) M-1 S-1 at 37 degrees C, and the activation energy was 13 kcal/mol. This activation energy is 7-11 kcal/mol less than that for the binding of colchicine to tubulin. The difference in activation energies can most easily be rationalized by a mechanism involving a tubulin-induced conformational change in the ligand ( Detrich , H. W., III, Williams, R. C., Jr., Macdonald, T. L., Wilson, L., and Puett , D. (1981) Biochemistry 20, 5999-6005). Such a change would be expected to have a small activation energy in AC because it possesses a freely rotating single bond in place of the B-ring of colchicine.     

Kinetic studies and structural models of the association of E. coli sigma(70) RNA polymerase with the lambdaP(R) promoter: large scale conformational changes in forming the kinetically significant intermediates

The kinetics of interaction of Esigma(70) RNA polymerase (R) with the lambdaP(R) promoter (P) were investigated by filter binding over a broad range of temperatures (7.3-42 degrees C) and concentrations of RNA polymerase (1-123 nM) in large excess over promoter DNA. Under all conditions examined, the kinetics of formation of competitor-resistant complexes (I(2), RP(o)) are single-exponential with first order rate constant beta(CR). Interpretation of the polymerase concentration dependence of beta(CR) in terms of the three step mechanism of open complex formation yields the equilibrium constant K(1) for formation of the first kinetically significant intermediate (I(1)) and the forward rate constant (k(2)) for the conformational change converting I(1) to the second kinetically significant intermediate I(2): R + P-->(K(1))<--I(1)(k(2))-->I(2). Use of rapid quench mixing allows K(1) and k(2) to be individually determined over the entire temperature range investigated, previously not possible at this promoter using manual mixing. Given the large (>60 bp) interface formed in I(1), its relatively small binding constant K(1) at 37 degrees C at this [salt] (approximately 6 x 10(6) M(-1)) strongly argues that binding free energy is used to drive large-scale structural changes in polymerase and/or promoter DNA or other coupled processes. Evidence for coupling of protein folding is provided by the large and negative activation heat capacity of k(a)[DeltaC(o,++)(a)= -1.5(+/-0.2)kcal K(-1)], now shown to originate directly from formation of I(1) [DeltaC(o)(1)= -1.4(+/-0.3)kcal K(-1)] rather than from the formation of I(2) as previously proposed. The isomerization I(1)-->I(2) exhibits relatively slow kinetics and has a very large temperature-independent Arrhenius activation energy [E(act)(2)= 34(+/-2)kcal]. This kinetic signature suggests that formation of the transition state (I(1)-I(2)++ involves large conformational changes dominated by changes in the exposure of polar and/or charged surface to water. Structural and biochemical data lead to the following hypotheses to interpret these results. We propose that formation of I(1) involves coupled folding of unstructured regions of polymerase (beta, beta' and sigma(70)) and bending of promoter DNA (in the -10 region). We propose that interactions with region 2 of sigma(70) and possibly domain 1 of beta induce a kink at the -11/-12 base pairs of the lambdaP(R) promoter which places the downstream DNA (-5 to +20) in the jaws of the beta and beta' subunits of polymerase in I(1). These early interactions of beta and beta' with the DNA downstream of position -5 trigger jaw closing (with coupled folding) and subsequent steps of DNA opening.     

Thermodynamics of follitropin binding to solubilized calf testis receptor

Thermodynamic parameters of follitropin binding to solubilized testicular receptors were measured in order to assess the forces involved in the binding reaction. Reversibility of follitropin binding to solubilized receptor decreased only 20% over the temperature range 4-24 degrees C, whereas earlier studies indicated reversibility of binding to membrane-bound receptor decreased by more than 40% over the same range [Anderson, T. T., Curatolo, L. M., & Reichert, L. E., Jr. (1983) Mol. Cell. Endocrinol. 33, 37-52]. Thermodynamic analysis of follitropin binding to solubilized receptors showed that the hydrophobic effect was important in the binding reaction. The mean values, at 25 degrees C, for delta H and delta S were -31.8 kcal/mol and -66.0 cal mol-1 K-1, respectively, and delta Cp was -3.0 kcal mol-1 K-1. This is an unusually large heat capacity for protein-protein association reactions, indicating an enhanced role for the hydrophobic effect with the solubilized (compared to membrane-bound) receptor. Since glycerol was necessary to stabilize the solubilized receptor, we determined whether glycerol affected the thermodynamic parameters measured for the binding reaction. Control experiments, performed with membrane-bound receptor in the presence or absence of glycerol, indicated that delta Cp actually decreased upon addition of glycerol (-0.8 kcal mol-1 K-1 in the presence of glycerol compared to -2.3 kcal mol-1 K-1 in the absence of glycerol). Thus, the large negative delta Cp observed for the soluble receptor was a result of its removal from the membrane and was not due to the presence of glycerol.(ABSTRACT TRUNCATED AT 250 WORDS)     

Physicochemical studies of processes involving potential photodynamic drugs on route to their targets: self-aggregation and membrane-binding of Zn-hematoporphyrin

The thermodynamics of zinc hematoporphyrin (ZnHP) dimerization and ZnHP-membrane binding were studied. The dimerization equilibrium was determined over the temperature range 19-40 degrees C, using fluorometric techniques. The dimerization constant obtained at 37 degrees C (neutral pH in phosphate-buffered saline) is 4.6 (+/- 0.6) X 10(4) M-1. The dimerization was found to decrease with temperature over the range 19-36 degrees C, the data allowing the extraction of the following thermodynamic parameters for the temperature range 19-31 degrees C: delta G0 = -9.3 kcal/mol, delta H0 = -7.4 kcal/mol, delta S0 = -6.4 eu. For temperatures above 36 degrees C the dimerization was found to be temperature independent, giving the following parameters: delta G0 = -6.6 kcal/mol, delta H0 = 0 kcal/mol, delta S0 = 21.2 eu. On the basis of the data the case is made for the existence of two types of ZnHP dimers, differing in the location of the fifth Zn2+ ligand and in the nature of the contribution of the solvent to the dimerization. For the membrane binding, large unilamellar liposomes served to model biological membranes. The binding of ZnHP to the liposomes was found to be similar, quantitatively, to the corresponding metal-free molecule, namely, fitting a case of one type of site and giving a binding constant of 1600 +/- 160 M (neutral pH and 37 degrees C) which is independent of the length of the porphyrin-liposome.     

Elementary steps in the formation of horseradish peroxidase compound I: direct observation of compound 0, a new intermediate with a hyperporphyrin spectrum

The reaction of horseradish peroxidase (HRP) with H2O2 has been studied in 50% v/v methanol/water over the 25.0 to -36.0 degrees C temperature range by using the low-temperature stopped-flow technique. All reactions were carried out under pseudo-first-order conditions with [H2O2] much greater than [HRP]. Arrhenius plots for the pseudo-first-order rate constant kobs were linear over the 17.6 to -36.0 degrees C temperature range studied with an activation energy of 4.8 +/- 0.5 kcal/mol. Above 0 degrees C, kobs varies linearly with peroxide concentration. However, saturation kinetics are observed below -16.0 degrees C, indicating that there is at least one reversible elementary step in this reaction. Double-reciprocal plots at -26.0 degrees C at pH* 7.3 for the reaction give kappa max(obs) = 163 s-1 and KM = 0.190 mM. Rapid-scan optical studies carried out at -35.0 degrees C with [H2O2] much greater than KM reveal the presence of a transient intermediate referred to as compound 0 whose conversion to compound I is rate limiting. The Soret region of the optical spectrum of compound 0 resembles that of a "hyperporphyrin" with prominent bands near 330 and 410 nm. The temperature dependencies of kappa max(obs) and KM have been measured over the -16.0 to -26.0 degrees C range and give an activation energy for kappa max(obs) of 1.6 +/- 0.7 kcal/mol and an enthalpy of formation for compound 0 of 4.0 +/- 0.7 kcal/mol.     

Lack of communication between LC2 light chain and the SH1 region of myosin S-1 studied by 19F-NMR

Myosin subfragment-1 (S-1) which contains the LC2 light chain has been labelled with fluorine to allow an 19F-NMR study of the coupling and energetics of structural changes in the myosin head. Two fluorine-containing reagents, N-4-(trifluoromethyl)phenyl iodoacetamide and N-3,5-di(trifluoromethyl)phenyl iodoacetamide, have been used to label the myosin heavy chain at the unusually reactive sulfhydryl-1 (SH1) position. The chemical shift of both reagents on S-1 is sensitive to a structural transition in the region of SH1 which occurs upon increasing the temperature from 0 degrees C to 35 degrees C. The midpoint of the transition in both papain and chymotryptic S-1 is at approximately 11 degrees C at pH 7 (0.1 M CKl). The temperature dependence of the chemical shift may be fit assuming a two-state equilibrium where delta G degree' (T) = 101-110T +0.386 T2 (where T is the temperature in Kelvin). Both delta H degree' (T) and delta S degree' (T) have a small temperature dependence from 0 to 35 degrees C: at 20 degrees C, delta H degree' (T) = -33 kcal/mol. delta S degree' (T) = -116 e.u. and delta Cp = -226 cal/mol per deg (pH 7.0, 0.1 M KCl). The NMR data indicate that the presence of the LC2 light chain in papain S-1 does not modify the structure of S-1 in the vicinity of SH1, nor does it modify the energetics of the structural transition from that seen in its absence with chymotryptic S-1. The presence of calcium which is bound by the LC2 of papain S-1 also does not alter the energetics of the transition. Thus it would appear that the LC2 light chain (on myosin S-1) does not participate in the two-state transition, nor does it interact strongly with regions of the heavy chain which participate in the transition.     

Thermodynamic analysis of the folding of the streptococcal protein G IgG-binding domains B1 and B2: why small proteins tend to have high denaturation temperatures.

We have cloned, expressed, and characterized two naturally occurring variations of the IgG-binding domain of streptococcal protein G. The domain is a stable cooperative folding unit of 56 amino acids, which maintains a unique folded structure without disulfide cross-links or tight ligand binding. We have studied the thermodynamics of the unfolding reaction for the two versions of this domain, designated B1 and B2, which differ by six amino acids. They have denaturation temperatures of 87.5 degrees C and 79.4 degrees C, respectively at pH 5.4, as determined by differential scanning calorimetry. Thermodynamic state functions for the unfolding reaction (delta G, delta H, delta S, and delta Cp) have been determined and reveal several interesting insights into the behavior of very small proteins. First, though the B1 domain has a heat denaturation point close to 90 degrees C, it is not unusually stable at physiologically relevant temperatures (delta G = 25 kJ/mol at 37 degrees C). This behavior occurs because the stability profile (delta G vs temperature) is flat and shallow due to the small delta S and delta Cp for unfolding. Related to this point is the second observation that small changes in the free energy of unfolding of the B-domain due to mutation or change in solvent conditions lead to large shifts in the heat denaturation temperature. Third, the magnitude and relative contributions of hydrophobic vs nonhydrophobic forces (per amino acid residue) to the total free energy of folding of the B-domain are remarkably typical of other globular proteins of much larger size.     

Effects of pH, ionic strength, and temperature on activation by calmodulin an catalytic activity of myosin light chain kinase

The reversible association of Ca42+-calmodulin with the inactive catalytic subunit of myosin light chain kinase results in the formation of the catalytically active holoenzyme complex [Blumenthal, D. K., & Stull, J. T. (1980) Biochemistry 19, 5608--5614]. The present study was undertaken in order to determine the effects of pH, temperature, and ionic strength on the processes of activation and catalysis. The catalytic activity of myosin light chain kinase, when fully activated by calmodulin, exhibited a broad pH optimum (greater than 90% of maximal activity from pH 6.5 to pH 9.0), showed only a slight inhibition by moderate ionic strengths (less than 20% inhibition at mu = 0.22), and displayed a marked temperature dependence (Q10 congruent to 2; Ea = 10.4 kcal mol-1). Thermodynamic parameters calculated from Arrhenius plots indicate that the Gibb's energy barrier associated with the rate-limiting step of catalysis is primarily enthalpic. The process of kinase activation by calmodulin had a narrower pH optimum (pH 6.0--7.5) than did catalytic activity, was markedly inhibited by increasing ionic strength (greater than 70% inhibition at mu = 0.22), and exhibited nonlinear van't Hoff plots. Between 10 and 20 degrees C, activation was primarily entropically driven (delta S degrees congruent to 40 cal mol-1 deg-1; delta H degrees = -900 cal mol-1), but between 20 and 30 degrees C, enthalpic factors predominated in driving the activation process (delta S degrees congruent to 10 cal mol-1 deg-1; delta H degrees = -9980 cal mol-1). The apparent change in heat capacity (delta Cp) accompanying activation was estimated to be -910 cal mol-1 deg-1. On the basis of these data we propose that although hydrophobic interactions between calmodulin and the kinase are necessary for the activation of the enzyme, other types of interactions such as hydrogen bonding, ionic, and van der Waals interactions also make significant and probably obligatory contributions to the activation process.     

Thermolysis of coenzymes B12 at physiological temperatures: activation parameters for cobalt-carbon bond homolysis and a quantitative analysis of the perturbation of the homolysis equilibrium by the ribonucleoside triphosphate reductase from Lactobacillus leichmannii

The kinetics of the thermolysis of 5'-deoxyadenosylcobalamin (AdoCbl, coenzyme B12) in aqueous solution, pH 7.5, have been studied in the temperature range 30-85 degrees C using AdoCbl tritiated at the adenine C2 position and the method of initial rates. Combined with a careful analysis of the distribution of adenine-containing products, the results permit the dissection of the competing rate constants for carbon-cobalt bond homolysis and heterolysis. After correction for the temperature-dependent occurrence of the much less reactive base-off species of AdoCbl, the activation parameters for homolysis of the base-on species were found to be delta H++homo,on = 33.8 +/- 0.2 kcal mol-1 and delta S++homo,on = 13.5 +/- 0.7 cal mol-1 K-1, values not significantly different from those determined by Hay and Finke (J. Am. Chem. Soc. 108 (1986) 4820), in the temperature range 85-115 degrees C. In contrast, the heterolysis of base-on AdoCbl was characterized by a much smaller enthalpy of activation (delta H++het,on = 18.5 +/- 0.2 kcal mol-1) and a negative entropy of activation (delta S++het,on = -34.0 +/- 0.7 cal mol-1 K-1) so that heterolysis, which is minor pathway at elevated temperatures, is the dominant pathway for AdoCbl decomposition at physiological temperatures. Using literature values for the rate constant for the reverse reaction, the equilibrium constant for AdoCbl homolysis at 37 degrees C was calculated to be 7.9 x 10(-18). Comparison with the equilibrium constant for this homolysis at the active site of the ribonucleoside triphosphate reductase from Lactobacillus leichmannii shows that the enzymes shifts the equilibrium constant towards homolysis products by a factor of 2.9 x 10(12) (17.7 kcal mol-1) by binding the thermolysis products with an equilibrium constant of 7.1 x 10(16) M-2, compared to the bonding constant for AdoCbl of 2.4 x 10(4) M-1.     

High- and low-temperature unfolding of human high-density apolipoprotein A-2.

Human plasma apolipoprotein A-2 (apoA-2) is the second major protein of the high-density lipoproteins that mediate the transport and metabolism of cholesterol. Using CD spectroscopy and differential scanning calorimetry, we demonstrate that the structure of lipid-free apoA-2 in neutral low-salt solutions is most stable at approximately 25 degrees C and unfolds reversibly both upon heating and cooling from 25 degrees C. High-temperature unfolding of apoA-2, monitored by far-UV CD, extends from 25-85 degrees C with midpoint Th = 56 +/- 2 degrees C and vant Hoff's enthalpy delta H(Th) = 17 +/- 2 kcal/mol that is substantially lower than the expected enthalpy of melting of the alpha-helical structure. This suggests low-cooperativity apoA-2 unfolding. The apparent free energy of apoA-2 stabilization inferred from the CD analysis of the thermal unfolding, delta G(app)(25 degrees) = 0.82 +/- 0.15 kcal/mol, agrees with the value determined from chemical denaturation. Enhanced low-temperature stability of apoA-2 observed upon increase in Na2HPO4 concentration from 0.3 mM to 50 mM or addition of 10% glycerol may be linked to reduced water activity. The close proximity of the heat and cold unfolding transitions, that is consistent with low delta G(app)(25 degrees), indicates that lipid-free apoA-2 has a substantial hydrophobic core but is only marginally stable under near-physiological solvent conditions. This suggests that in vivo apoA-2 transfer is unlikely to proceed via the lipid-free state. Low delta H(Th) and low apparent delta Cp approximately 0.52 kcal/mol.K inferred from the far-UV CD analysis of apoA-2 unfolding, and absence of tertiary packing interactions involving Tyr groups suggested by near-UV CD, are consistent with a molten globular-like state of lipid-free apoA-2.     

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.     

DSC studies of the conformational stability of barstar wild-type.

The temperature induced unfolding of barstar wild-type of bacillus amyloliquefaciens (90 residues) has been characterized by differential scanning microcalorimetry. The process has been found to be reversible in the pH range from 6.4 to 8.3 in the absence of oxygen. It has been clearly shown by a ratio of delta HvH/delta Hcal near 1 that denaturation follows a two-state mechanism. For comparison, the C82A mutant was also studied. This mutant exhibits similar reversibility, but has a slightly lower transition temperature. The transition enthalpy of barstar wt (303 kJ mol-1) exceeds that of the C82A mutant (276 kJ mol-1) by approximately 10%. The heat capacity changes show a similar difference, delta Cp being 5.3 +/- 1 kJ mol-1 K-1 for the wild-type and 3.6 +/- 1 kJ mol-1 K-1 for the C82A mutant. The extrapolated stability parameters at 25 degrees C are delta G0 = 23.5 +/- 2 kJ mol-1 for barstar wt and delta G0 = 25.5 +/- 2 kJ mol-1 for the C82A mutant.     

Interaction of benzene with bilayers. Thermal and structural studies

The thermal and structural properties of saturated phosphatidylcholine liposomes are significantly altered by benzene. Upon the addition of benzene, the liposomes first swell and then disperse into small multilamellar vesicles. At 20 degrees C these vesicles contain striations or ripples in the plane of the bilayer. Major changes in the thermal behavior of DSPC-benzene liposomes occur near mole ratios of 2:1 and 1:1. At a 2:1 mole ratio, the area under the main endothermic peak, delta Hm, essentially disappears; however, the total heat absorbed, delta Hf, remains approximately equal to that of the control. This occurs because for benzene mole fractions 0.12 less than x less than 0.50, benzene increases the apparent molar heat capacity, Cp, of the gel phase to about 1.2 kcal/(mol . deg). We interpret this increase in heat capacity to be due to an increase in the concentration of defects (or disorder) in the gel phase. At mole fractions of benzene between 0.5 and 0.9, the transition temperature decreases by 20-30 degrees C, and broad, multiple transitions are observed. From 0.5 less than or equal to x less than or equal to 0.9, the apparent molar heat capacity of the liquid-crystal phase increases to that of the defected rippled gel phase. The value of delta Hf approaches the heat of fusion for 2 mol of n-octadecane, suggesting that benzene uncouples the liquid-crystalline acyl chains. The lipids affected by benzene or "boundary lipids" have higher heat capacity than nonperturbed lipids. The apparent molar specific heat, Cp, of 1,2-distearoyl-sn-glycero-3-phosphorylcholine (and 1,2-dipalmitoyl-sn-glycero-3-phosphorylcholine) multilamellar vesicles is 0.20 +/- 0.05 kcal/(mol. deg) in the L beta', P beta, and L alpha phases. Cp fluctuates about this value in all three phases upon repeated phase transitions in the same sample. However, the value of Cp in the P beta (rippled) phase exhibits much greater fluctuations in Cp than that in the L alpha phase. We attribute these fluctuations to crystal packing defects.