Dynamic studies of proton diffusion in mesoscopic heterogeneous matrix: II. The interbilayer space between phospholipid membranes

The thin water layer, as found in chloroplast or mitochondria, is confined between low dielectric amphypathic surfaces a few nm apart.

The physical properties of this mesoscopic space, and how its dimensions affect the rate of chemical reactions proceeding in it, is the subject for this study.

The method selected for this purpose is time resolved fluorometry which can monitor the reversible dissociation of a proton from excited molecule of pyranine (8 hydroxy pyrene 1,3,6 tri sulfonate) trapped in thin water layers of a multilamellar vesicle made of neutral or slightly charged phospholipids.

The results were analyzed by a computer program of N. Agmon (Pines, E., D. Huppert, and N. Agmon. 1988. J. Am. Chem. Soc. 88:5620-5630) that simulates the diffusion of a proton, subjected to electrostatic attraction, in a thin water layer enclosed between low affinity, proton binding surfaces. The analysis determines the diffusion coefficient of the proton, the effective dielectric constant of the water and the water accessibility of the phosphomoieties of the lipids.

These parameters were measured for various lipids [egg-phosphatidylcholine (egg PC), dipalmitoyl phosphatidylcholine (DPPC), cholesterol + DPPC (1:1) and egg PC plus phosphatidyl serine (9:1)] and under varying osmotic pressure which reduces the width of the water layer down to ~10 ~ across.

We found that: (a) The effective dielectric constant of the aqueous layer, depending on the lipid composition, is ~40. (b) The diffusion coefficient of the proton in the thin layer (30-10 ~ across) is that measured in bulk water D = 9.3 10^-5 cm²/s, indicating that the water retains its normal liquid state even on contact with the membrane. (c) The reactivity of the phosphomoiety, quantitated by rate of its reaction with proton, diminishes under lateral pressure which reduces the surface area per lipid.

We find no evidence for abnormal dynamics of proton transfer at the lipid water interface which, by any mechanism, accelerates its diffusion.

     

Azide binding to the cytochrome c ferric heme octapeptide. A model for anion binding to the active site of high spin ferric heme proteins.

Equilibrium constants for the binding of azide to the ferric heme c octapeptide in 50% ethylene glycol 50% buffer were measured spectrophotometrically. The equilibrium constant for azide binding at 20 degrees C and pH* 7.4 is 29.2, which is approximately 3 to 4 orders of magnitude lower than that observed for azide binding to various ferric hemeproteins. The equilibrium constant was indepent of pH* in the range from 7 to 8. Equilibrium constants at several temperatures exhibited an apparent van't Hoff relationship yielding thermodynamic values of delta H0 = -26,100 J/mol (-6240 cal/mol) and delta S0 = -61.5 J/0K mol (-14.7 e.u.). Comparison of these values to the values for the heme proteins enables one to explain the differences in equiliberium constants in terms of differences in the polarity of the heme environments. The results are consistent with the concept that the oxygen affinity of heme complexes increases with the polarity of the heme environment. The data also suggest that an increase in the polarity of the heme environment should result in a corresponding increase in the susceptibility of ferrous heme dioxygen complexes toward oxidation by the dioxygen.     

Quantitation of physical-chemical properties of the aqueous phase inside the phoE ionic channel.

The anion-specific channel of the phoE porine is a miniature body of water surrounded by peptide walls. The physical and chemical properties of the water in such a microscopic space were measured by monitoring the dynamics of a well-studied reaction--the protolytic dissociation of a strong acid. To attain this purpose, we allowed pyranine (8-hydroxypyrene-1,3,6-trisulfonate) to bind to the anion-specific channel. The dye is bound, with a 1:1 stoichiometry, with a delta G = -9.5 kcal/mol. Photoexcitation of the dye, to its first electronic singlet state (phi OH*), renders it very acidic and the hydroxyl proton dissociates to H+ and excited anion (phi O*-). We employed single photon-counting time-resolved fluorimetry, to monitor the reversible dissociation of pyranine as it proceeds within the channel and reconstructed the observed signal by a numerical integration of the differential diffusion equation pertinent for a proton within the channel. The most characteristic feature of the water-filled channel, is the intensified electrostatic interactions attained by the low dielectric constant of the diffusion space, epsilon eff = 24. For this reason, the electric field of a few positive charges is sufficient to ensure that an anion entering the channel will be effectively sucked in. The interaction of the water molecules with the peptide structure forming the channel affects the physical properties of the water. Their capacity to conduct proton, quantitated by the protons diffusion coefficient (4.5.10(-5) cm2/s), is reduced by 50% with respect to that of bulk water. The activity of the water in the channel is reduced to alpha H2O = 0.966. These observation are in accord with our previous studies of water in small defined cavities in proteins.     

Microcalorimetric investigation of the interactions in the ternary complex calmodulin-calcium-melittin

Flow microcalorimetric titrations of calmodulin with melittin at 25 degrees C revealed that the formation of the high-affinity one-to-one complex in the presence of Ca2+ (Comte, M., Maulet, Y., and Cox, J. A. (1983) Biochem, J. 209, 269-272) is entirely entropy driven (delta H0 = 30.3 kJ X mol-1; delta S0 = 275 J X K-1 X mol-1). Neither the proton nor the Mg2+ concentrations have any significant effect on the strength of the complex. In the absence of Ca2+, a nonspecific calmodulin-(melittin)n complex is formed; the latter is predominantly entropy driven, accompanied by a significant uptake of protons and fully antagonized by Mg2+. Enthalpy titrations of metal-free calmodulin with Ca2+ in the presence of an equimolar amount of melittin were carried out at pH 7.0 in two buffers of different protonation enthalpy. The enthalpy and proton release profiles indicate that: protons, absorbed by the nonspecific calmodulin-melittin complex, are released upon binding of the first Ca2+; Ca2+ binding to the high-affinity configuration of the calmodulin-melittin complex displays an affinity constant greater than or equal to 10(7) M-1, i.e. 2 orders of magnitude higher than that of free calmodulin; the latter is even more entropy driven (delta H0 = 7.2 kJ X site-1; delta S0 = 158 J X K-1 X site-1) than binding to free calmodulin (delta H0 = 4.7 kJ X site-1; delta S0 = 112 J X K-1 X site-1), thus underlining the importance of hydrophobic forces in the free energy coupling involved in the ternary complex.     

Gaugement of the inner space of the apomyoglobin's heme binding site by a single free diffusing proton. II. Interaction with a bulk proton.

The reaction mechanism and the dynamic aspects of protonation of a defined moiety located inside an aqueous cavity in a protein were monitored by time resolved spectroscopy using the pyranine apomyoglobin complex as a model (Shimoni, Tsfadia, Nachliel, and Gutman, 1993, Biophys. J. 64:472-479). The reaction was synchronized by a short laser pulse and the reprotonation of the ground state pyranine anion (phi O-) was monitored, in the microsecond time scale, by its transient absorption at 457 nm. The observed signal was reconstructed by a numeric solution of nonlinear, coupled differential equations which account for the direct reaction of phi O- with bulk proton and by proton transfer from the nearby amino acids: His 64, Asp 44, Asp 60, and Glu 59. A unique combination of rate constant was obtained which quantitates the contribution of each pathway to the overall relaxation process. In the first phase of the dynamics phi O- abstracts a proton from the nearby protonated histidine. The bulk proton interacts preferentially with the cluster of three carboxylates and immediately shuttled to the deprotonated histidine. The high proximity of the reactive groups and the strong electrostatic forces operating inside the heme binding cavity render the rate of proton transfer in the site ultrafast.     

Cyanide binding to the cytochrome c ferric heme octapeptide. A model for anion binding to the active site of high spin ferric heme proteins

Equilibrium constants for the binding of cyanide to the ferric heme c octapeptide in 20% ethylene glycol, 50% buffer were measured spectrophotometrically. The equilibrium constant for cyanide binding at 20 degrees C and pH 7.4 is 3.47 X 10(7), which is approximately 15-fold lower than that observed for cyanide binding to methemoglobin or metmyoglobin. Equilibrium constants at several temperatures exhibited an apparent van't Hoff relationship, yielding thermodynamic values of delta H degrees = -79,000 J/mol (-18,900 cal/mol) and delta S degrees = J/degrees K mol (-30.1 e.u.). Comparison of the ratio of equilibrium constants for cyanide ligation to methemoglobin the heme octapeptide with the ratio of equilibrium constants for azide ligation to methemoglobin and the heme octapeptide suggests that cyanide binding to the methemoproteins is much smaller than expected by comparison to azide binding. The differences in the ratios, the thermodynamic values, and the preferred binding geometries suggest that CN- ligation, like CO ligation, is sterically hindered. A comparison of these ratios to similar ratios for CO, O2, and NO binding suggests that the Fe-CN bond angle is less subject to distortion than the Fe-CO bond and/or additional binding interactions contribute to N3- but not to CN-binding to the protein.     

Crystal structures of the NO- and CO-bound heme oxygenase from Neisseriae meningitidis. Implications for O2 activation

Heme oxygenases catalyze the oxidation of heme to biliverdin, carbon monoxide, and free iron while playing a critical role in mammalian heme homeostasis. Pathogenic bacteria such as Neisseriae meningitidis also produce heme oxygenase as part of a mechanism to mine host iron. The key step in heme oxidation is the regioselective oxidation of the heme alpha-meso-carbon by an activated Fe(III)-OOH complex. The structures of various diatomic ligands bound to the heme iron can mimic the dioxygen complex and provide important insights on the mechanism of O2 activation. Here we report the crystal structures of N. meningitidis heme oxygenase (nm-HO) in the Fe(II), Fe(II)-CO, and Fe(II)-NO states and compare these to the NO complex of human heme oxygenase-1 (Lad, L., Wang, J., Li, H., Friedman, J., Bhaskar, B., Ortiz de Montellano, P. R., and Poulos, T. L. (2003) J. Mol. Biol. 330, 527-538). Coordination of NO or CO results in a reorientation of Arg-77 that enables Arg-77 to participate in an active site H-bonded network involving a series of water molecules. One of these water molecules directly H-bonds to the Fe(II)-linked ligand and very likely serves as the proton source required for oxygen activation. Although the active site residues differ between nm-HO and human HO-1, the close similarity in the H-bonded water network suggests a common mechanism shared by all heme oxygenases.     

Gauging of the PhoE channel by a single freely diffusing proton

In the present study we combined a continuum approximation with a detailed mapping of the electrostatic potential inside an ionic channel to define the most probable trajectory for proton propagation through the channel (propagation along a structure-supported trajectory (PSST)). The conversion of the three-dimensional diffusion space into propagation along a one-dimensional pathway permits reconstruction of an ion motion by a short calculation (a few seconds on a state-of-the-art workstation) rather than a laborious, time-consuming random walk simulations. The experimental system selected for testing the accuracy of this concept was the reversible dissociation of a proton from a single pyranine molecule (8-hydroxypyrene-1,2,3-trisulfonate) bound by electrostatic forces inside the PhoE ionic channel of the Escherichia coli outer membrane. The crystal structure coordinates were used for calculation of the intra-cavity electrostatic potential, and the reconstruction of the observed fluorescence decay curve was carried out using the dielectric constant of the intra-cavity space as an adjustable parameter. The fitting of past experimental observations (Shimoni, E., Y. Tsfadia, E. Nachliel, and M. Gutman. 1993. Biophys. J. 64:472-479) was carried out by a modified version of the Agmon geminate recombination program (Krissinel, E. B., and N. Agmon. 1996. J. Comp. Chem. 17:1085-1098), where the gradient of the electrostatic potential and the entropic terms were calculated by the PSST program. The best-fitted reconstruction of the observed dynamics was attained when the water in the cavity was assigned epsilon 相似文献   

NMR study of Galeorhinus japonicus myoglobin. 1H-NMR evidence for a structural alteration on the active site of G. japonicus myoglobin upon azide ion binding

The heme molecular structure of the met-azido form of the myoglobin from the shark Galeorhinus japonicus has been investigated by 1H NMR. A nuclear Overhauser effect (NOE) was clearly observed among the heme peripheral side-chain proton signals of this complex, which undergoes thermal spin equilibrium between high-spin (S = 5/2) and low-spin (S = 1/2) states, and the NOE connectivities provided the assignment of the resonances from the heme C13(1)H2 and C17(1)H2 protons. Chemical shift inequivalence of these proton resonances not only provided information about the orientation of these methylene protons with respect to the heme plane, but also allowed characterization of the time-dependent build-up of the NOE between them, which yields the correlation time for the internal motion of the inter-proton vector. The relatively large mobility found for the C17(1)H2 group suggests that the carboxyl oxygen of the heme C17 propionate is not anchored to the apo-protein by a salt bridge. It has been shown that the ferric high-spin form of G. japonicus Mb possesses a penta-coordinated heme [Suzuki, T. (1987) Biochim. Biophys. Acta 914, 170-176; Yamamoto, Y., Osawa, A., Inoue, Y., Ch?j?, R. & Suzuki, T. (1990) Eur. J. Biochem. 192, 225-229] and that the conformation of both heme propionate groups is fixed with respect to the heme, as well as the apo-protein, by a salt bridge [Yamamoto, Y., Inoue, Y., Ch?j?, R. & Suzuki, T. (1990) Eur. J. Biochem. 189, 567-573]. Therefore the weakening or interruption of the interaction between the C17 propionate and His FG3 upon the changes of the coordination and spin state of the heme iron, during azide ion binding to ferric high-spin G. japonicus Mb, is attributed to the displacement of the FG corner of the apoprotein away from the heme C17 propionate group. A similar structural alteration has been revealed by X-ray structural analyses of unliganded and liganded forms of ferrous hemoproteins [Baldwin, J. & Chothia, C. (1979) J. Mol. Biol. 129, 175-220; Phillips, S.E.V. (1980) J. Mol. Biol. 142, 531-554].     

Time-resolved study of the inner space of lactose permease

Pyranine (8-hydroxy pyrene-1,3,6-trisulfonate) is a commonly used photoacid that discharges a proton when excited to its first electronic singlet state. Follow-up of its dissociation kinetics reveals the physicochemical properties of its most immediate environment. At vanishing ionic strength the dye adsorbs to the Escherichia coli lactose permease with stoichiometry of 1:1 and an association constant of 2.5 x 10(5) M(-1). The reversal of the binding at high ionic strength and the lower pK value of the bound dye imply that positive charge(s) stabilize the dye in its site. The fluorescence decay curve of the bound dye was measured by time-correlated single photon counting and the measured transient was subjected to kinetic analysis based on the geminate recombination model. The analysis indicated that the binding domain is a cleft (between 9 and 17 A deep) characterized by low activity of water (a((water)) = 0.71), reduced diffusivity of protons, and enhanced electrostatic potential. The binding of pyranine and a substrate are not mutually exclusive; however, when the substrate is added, the dye-binding environment is better solvated. These properties, if attributed to the substrate-conducting pathway, may explain some of the forces operating on the substrate in the cavity. The reduced activities of the water strips the substrate from some of its solvation water molecules and replace them by direct interaction with the protein. In parallel, the lower dielectric constant enhances the binding of the proton to the protein, thus keeping a tight seal that prevents protons from diffusing.     

Salicylhydroxamic acid inhibits myeloperoxidase activity.

Salicylhydroxamic and benzohydroxamic acids were found to bind to the resting state of myeloperoxidase and inhibit ligand binding to the heme iron. An ionizable group on the enzyme with pKa = 4 affects salicylhydroxamic acid binding; binding occurs when this group is not protonated. The binding of the heme iron ligands (e.g. cyanide, nitrite, and chloride) is probably controlled by the same ionizable group. The equilibrium dissociation constant of the salicylhydroxamic acid-myeloperoxidase complex is about 2 x 10(-6) M, and the association rate constant is 7.4 x 10(6) M-1.s-1. Salicylhydroxamic acid serves as a donor to the higher oxidation state of myeloperoxidase and thereby inhibits guaiacol oxidation. Salicylhydroxamic acid was also found to bind to intestinal peroxidase and lactoperoxidase. Salicylhydroxamic acid binding to all three mammalian peroxidases was about 3 orders of magnitude stronger than benzohydroxamic acid binding. We conclude that the salicylhydroxamic and benzohydroxamic acids bind in the distal heme cavity of these peroxidases and interact with the heme ligand binding site.     

Heme-pocket-hydration change during the inactivation of cytochrome P-450camphor by hydrostatic pressure.

Hydrostatic pressure has been used to convert cytochrome P-450camphor to cytochrome P-420. The latter is an inactivated but soluble and undenaturated form of cytochrome P-450camphor. Using camphor analogues as probes of the active site we show that the inactivation volume change is directly correlated to the initial degree of hydration of the heme pocket. The values range between -73 ml/mol and -197 ml/mol [Di Primo, C., Hui Bon Hoa, G., Douzou, P. & Sligar, S. G. (1990) Eur. J. Biochem. 193, 383-386] for a totally hydrated (substrate-free, low-spin, six coordinated heme iron) and a non-hydrated (camphor-bound, high-spin, five coordinated heme iron) heme pocket. These results suggest that the larger value, -197 ml/mol, for the inactivation volume change is due to a hydration change of the heme pocket resulting from the displacement of the substrate during the compression and the subsequent entrance of water molecules. Similarly, the stability of the protein against compression is correlated with water accessibility to the active site. Increase in substrate mobility by loss of specific interactions with both regions of well defined secondary structure of cytochrome P-450camphor results in an increase of water accessibility and decrease of stability. Thus for camphor and adamantanone which strongly interact with the protein and exclude water from the active site [Poulos, T. L., Finzel, B. C. & Howard, A. J. (1987) J. Mol. Biol. 195, 687-700; Raag, R. & Poulos, T. L. (1989) Biochemistry 28, 917-922] the increase in stability compared to the free protein is roughly 30 kJ/mol at 20 degrees C. With smaller substrates such as norcamphor, which loosely fits into the active site and does not completely exclude water [Raag, R. & Poulos, T. L. (1989) Biochemistry 28, 917-922], the increase in stability is only 7 kJ/mol. Finally these results suggest that cytochrome P-420 induced by hydrostatic pressure is a unique form where the active site is hydrated and camphor is displaced from its binding site.     

Substitution of the heme binding module in hemoglobin alpha- and beta-subunits. Implication for different regulation mechanisms of the heme proximal structure between hemoglobin and myoglobin

In our previous work, we demonstrated that the replacement of the "heme binding module," a segment from F1 to G5 site, in myoglobin with that of hemoglobin alpha-subunit converted the heme proximal structure of myoglobin into the alpha-subunit type (Inaba, K., Ishimori, K. and Morishima, I. (1998) J. Mol. Biol. 283, 311-327). To further examine the structural regulation by the heme binding module in hemoglobin, we synthesized the betaalpha(HBM)-subunit, in which the heme binding module (HBM) of hemoglobin beta-subunit was replaced by that of hemoglobin alpha-subunit. Based on the gel chromatography, the betaalpha(HBM)-subunit was preferentially associated with the alpha-subunit to form a heterotetramer, alpha(2)[betaalpha(HBM)(2)], just as is native beta-subunit. Deoxy-alpha(2)[betaalpha(HBM)(2)] tetramer exhibited the hyperfine-shifted NMR resonance from the proximal histidyl N(delta)H proton and the resonance Raman band from the Fe-His vibrational mode at the same positions as native hemoglobin. Also, NMR spectra of carbonmonoxy and cyanomet alpha(2)[betaalpha(HBM)(2)] tetramer were quite similar to those of native hemoglobin. Consequently, the heme environmental structure of the betaalpha(HBM)-subunit in tetrameric alpha(2)[betaalpha(HBM)(2)] was similar to that of the beta-subunit in native tetrameric Hb A, and the structural conversion by the module substitution was not clear in the hemoglobin subunits. The contrastive structural effects of the module substitution on myoglobin and hemoglobin subunits strongly suggest different regulation mechanisms of the heme proximal structure between these two globins. Whereas the heme proximal structure of monomeric myoglobin is simply determined by the amino acid sequence of the heme binding module, that of tetrameric hemoglobin appears to be closely coupled to the subunit interactions.     

NMR study of Galeorhinus japonicus myoglobin. 1H-NMR study of molecular structure of the heme cavity

The molecular structure of the active site of myoglobin from the shark, Galeorhinus japonicus, has been studied by 1H-NMR. Some hyperfine-shifted amino acid proton resonances in the met-cyano form of G. japonicus myoglobin have been unambiguously assigned by the combined use of various two-dimensional NMR techniques; they were compared with the corresponding resonances in Physter catodon myoglobin. The orientations of ThrE10 and IleFG5 residues relative to the heme in G. japonicus met-cyano myoglobin were semiquantitatively estimated from the analysis of their shifts using the magnetic susceptibility tensor determined by a method called MATDUHM (magnetic anisotropy tensor determination utilizing heme methyls) [Yamamoto, Y., Nanai, N. & Ch?j?, R. (1990) J. Chem. Soc., Chem. Commun., 1556-1557] and the results were compared with the crystal structure of P. catodon carbonmonoxy myoglobin [Hanson, J. C. & Schoenborn, B. P. (1981) J. Mol. Biol. 153, 117-124]. In spite of a substantial difference in shift between the corresponding amino acid proton resonances for the two proteins, the orientations of these amino acid residues relative to the heme in the active site of both myoglobins were found to be highly alike.     

Cyanate binding to the ferric heme octapeptide from cytochrome c. A model for anion binding to high spin ferric hemoproteins

Equilibrium constants for the binding of cyanate to the ferric heme c octapeptide in 50% ethylene glycol, 50% aqueous buffer were measured spectrophotometrically. Equilibrium constants measured at several temperatures from -20 degrees C to 0 degrees C exhibited an apparent van't Hoff relationship yielding thermodynamic values of delta Ho = -1.3 X 10(3) +/- 0.9 X 10(3) J/mol (-3.1 X 10(2) +/- 2 X 10(2) cal/mol), delta So = -3 +/- 3 J/K X mol (-0.6 +/- 0.8 cal/K X mol). The equilibrium constant for cyanate binding at 25 degrees C and pH 7.4 is 1.21 which is approximately 2 to 3 orders of magnitude lower than that observed for cyanate binding to methemoglobin and metmyoglobin. Krel, the ratio of the hemoprotein to model heme octapeptide binding constants, for NCO- is smaller than Krel for N3- suggesting that hydrogen bonding between the terminal ligand atoms and the distal histidine in hemoglobin and myoglobin does not contribute to the increased protein ligand stabilization observed for these anions relative to the model. A donor-acceptor interaction between the distal histidine and the electrophilic middle atoms of these bound ligands is proposed.     

Kinetics of cyanide binding to Chromatium vinosum ferricytochrome c'

The kinetics of the reversible binding of cyanide by the ferric cytochrome c' from Chromatium vinosum have been studied over the pH range 6.9-9.6. The reaction is extremely slow at neutral pH compared to the reactions of other high-spin ferric heme proteins with cyanide. The observed bimolecular rate constant at pH 7.0 is 2.25 X 10(-3) M-1 s-1, which is approximately 10(7)-fold slower than that for peroxidases, approximately 10(5)-fold slower than those for hemoglobin and myoglobin, and approximately 10(2)-fold to approximately 10(3)-fold slower than that recently reported for the Glycera dibranchiata hemoglobin, which has anomalously slow cyanide rate constants of 4.91 X 10(-1), 3.02 X 10(-1), and 1.82 M-1 s-1 for components II, III, and IV, respectively [Mintorovitch, J., & Satterlee, J. D. (1988) Biochemistry 27, 8045-8050; Mintorovitch, J., Van Pelt, D., & Satterlee, J. D. (1989) Biochemistry 28, 6099-6104]. The unusual ligand binding property of this cytochrome c' is proposed to be associated with a severely hindered heme coordination site. Cyanide binding is also characterized by a nonlinear cyanide concentration dependence of the observed rate constant at higher pH values, which is interpreted as involving a change in the rate-determining step associated with the formation of an intermediate complex between the cytochrome c' and cyanide prior to coordination. The pH dependence of both the binding constant for the formation of the intermediate complex and the association rate constant for the subsequent coordination to the heme can be attributed to the ionization of HCN, where cyanide ion binding is the predominant process.(ABSTRACT TRUNCATED AT 250 WORDS)     

Differences in thermal stability between reduced and oxidized cytochrome b562 from Escherichia coli

The thermal stabilities of ferri- and ferrocytochrome b562 were examined. Thermally induced spectral changes, monitored by absorption and second-derivative spectroscopies, followed the dissociation of the heme moiety and the increased solvation of tyrosine residue(s) located in close proximity to the heme binding site. All observed thermal transitions were independent of the rate of temperature increase (0.5-2 degrees C/min), and the denatured protein exhibited partial to near-complete reversibility upon return to ambient temperature. The extent of renaturation of cytochrome b562 is dependent on the amount of time the unfolded conformer is exposed to temperatures above the transition temperature, Tm. All thermally induced spectra changes fit a simple two-state model, and the thermal transition was assumed to be reversible. The thermal transition for ferrocytochrome b562 yielded Tm and van't Hoff enthalpy (delta HvH) values of 81.0 degrees C and 137 kcal/mol, respectively. In contrast, Tm and delta HvH values obtained for the ferricytochrome were 66.7 degrees C and 110 kcal/mol, respectively. The estimated increase in the stabilization free energy at the Tm of ferricytochrome b562 following the one-electron reduction to the ferrous form, where delta delta G = delta Tm delta Sm [delta Sm = 324 cal/(K.mol), delta Tm = 14.3 degrees C] [Becktel, W. J., & Schellman, J. A. (1987) Biopolymers 26, 1859-1877], is 4.6 kcal/mol.     

Nuclear Overhauser effect studies of the conformations and binding site environments of deoxynucleoside triphosphate substrates bound to DNA polymerase I and its large fragment

The conformations and binding site environments of Mg2+TTP and Mg2+dATP bound to Escherichia coli DNA polymerase I and its large (Klenow) fragment have been investigated by proton NMR. The effect of the large fragment of Pol I on the NMR line widths of the protons of Mg2+TTP detected one binding site for this substrate with a dissociation constant of 300 +/- 100 microM and established simple competitive binding of deoxynucleoside triphosphates at this site in accord with previous equilibrium dialysis experiments with whole Pol I [Englund, P. T., Huberman, J.A., Jovin, T.M., & Kornberg, A. (1969) J. Biol. Chem. 244, 3038]. Primary negative nuclear Overhauser effects were used to calculate interproton distances on enzyme-bound Mg2+dATP and Mg2+TTP. These distances established that each substrate was bound with an anti-glycosidic torsional angle (chi) of 50 +/- 10 degrees for Mg2+dATP and 40 +/- 10 degrees for Mg2+TTP. The sugar pucker of both substrates was predominantly O1'-endo, with a C5'-C4'-C3'-O3' exocyclic torsional angle (delta) of 95 +/- 10 degrees for Mg2+dATP and 100 +/- 10 degrees for Mg2+TTP. The consistency of these conformations with those previously proposed, on the basis of distances from Mn2+ at the active site [Sloan, D. L., Loeb, L. A., Mildvan, A.S., & Feldman, R.J. (1975) J. Biol. Chem. 250, 8913], indicates a unique conformation for each bound nucleotide. The chi and delta values of the bound substrates are appropriate for nucleotide units of B DNA.(ABSTRACT TRUNCATED AT 250 WORDS)     

A thermodynamic study of the interaction of tubulin with colchicine site ligands

The bicyclic colchicine analogue 2-methoxy-5-(2',3',4'-trimethoxyphenyl)-2,4,6-cycloheptatrien-1-on e (MTC) has been used to study the thermodynamics of specific ligand binding to the colchicine site of tubulin, employing isothermal reaction microcalorimetry. The binding of MTC to purified calf brain tubulin, in 10 mM sodium phosphate buffer, pH 7.0, is characterized by delta H degree = -19 +/- 1 kJ.mol-1, delta G degree = -31.8 +/- 0.6 kJ.mol-1, and delta S degree = 43 +/- 5 J.mol-1.K-1 at 298 K, with a slight variation in the temperature range from 283 to 308 K. The binding thermodynamics of colchicine and allocolchicine are similar to MTC under the conditions examined, suggesting related molecular interactions of the three ligands with the protein binding site. The standard enthalpy changes of binding of colchicine and MTC at 308 K coincide within experimental error. Therefore the more favorable free energy change of binding of colchicine must come from a larger binding entropy change (by about 20 J.mol-1.K-1). This difference could be attributed to the presence of the middle ring of colchicine, which is absent in MTC. Consistently, a similar entropy change is observed by the comparison of allocolchicine to MTC binding at several temperatures. In addition, allocolchicine binding is about 6 kJ.mol-1 less exothermic than MTC binding, which could be attributed to the presence in allocolchicine of a substituted phenyl ring instead of the colchicine-MTC tropolone ring. The present results and analysis are fully compatible with the previously proposed bifunctional binding of colchicine and MTC (through their trimethoxybenzene and tropolone moieties) to a bifocal protein binding site, and also with a partial immobilization of intramolecular rotation of MTC upon binding, which in colchicine is already constrained by its middle ring (Andreu, J. M., Gorbunoff, M. J., Lee, J. C., and Timasheff, S. (1984) Biochemistry 23, 1742-1752).