Effect of solution viscosity on intraprotein electron transfer between the FMN and heme domains in inducible nitric oxide synthase

The FMN-heme intraprotein electron transfer (IET) kinetics in a human inducible NOS (iNOS) oxygenase/FMN construct were determined by laser flash photolysis as a function of solution viscosity (1.0-3.0 cP). In the presence of ethylene glycol or sucrose, an appreciable decrease in the IET rate constant value was observed with an increase in the solution viscosity. The IET rate constant is inversely proportional to the viscosity for both viscosogens. This demonstrates that viscosity, and not other properties of the added viscosogens, causes the dependence of IET rates on the solvent concentration. The IET kinetics results indicate that the FMN-heme IET in iNOS is gated by a large conformational change of the FMN domain. The kinetics and NOS flavin fluorescence results together indicate that the docked FMN/heme state is populated transiently.     

Pressure-jump study of the kinetics of ethidium bromide binding to DNA

Pressure-jump chemical relaxation has been used to investigate the kinetics of ethidium bromide binding to the synthetic double-stranded polymers poly[d(G-C)] and poly[d(A-T)] in 0.1 M NaCl, 10 mM tris(hydroxymethyl)aminomethane hydrochloride, and 1 mM ethylenediaminetetraacetic acid, pH 7.2, at 24 degrees C. The progress of the reaction was followed by monitoring the fluorescence of the intercalated ethidium at wavelengths greater than 610 nm upon excitation at 545 nm. The concentration of DNA was varied from 1 to 45 microM and the ethidium bromide concentration from 0.5 to 25 microM. The data for both polymers were consistent with a single-step bimolecular association of ethidium bromide with a DNA binding site. The necessity of a proper definition of the ethidium bromide binding site is discussed: it is shown that an account of the statistically excluded binding phenomenon must be included in any adequate representation of the kinetic data. For poly[d(A-T)], the bimolecular association rate constant is k1 = 17 X 10(6) M-1 s-1, and the dissociation rate constant is k-1 = 10 s-1; in the case of poly[d(G-C)], k1 = 13 X 10(6) M-1 s-1, and k-1 = 30 s-1. From the analysis of the kinetic amplitudes, the molar volume change, delta V0, of the intercalation was calculated. In the case of poly[d(A-T)], delta V0 = -15 mL/mol, and for poly[d(G-C)], delta V0 = -9 mL/mol; that is, for both polymers, intercalation is favored as the pressure is increased.(ABSTRACT TRUNCATED AT 250 WORDS)     

Kinetics of phloretin binding to phosphatidylcholine vesicle membranes

The submillisecond kinetics for phloretin binding to unilamellar phosphatidylcholine (PC) vesicles was investigated using the temperature-jump technique. Spectrophotometric studies of the equilibrium binding performed at 328 nm demonstrated that phloretin binds to a single set of independent, equivalent sites on the vesicle with a dissociation constant of 8.0 microM and a lipid/site ratio of 4.0. The temperature of the phloretin-vesicle solution was jumped by 4 degrees C within 4 microseconds producing a monoexponential, concentration-dependent relaxation process with time constants in the 30--200-microseconds time range. An analysis of the concentration dependence of relaxation time constants at pH 7.30 and 24 degrees C yielded a binding rate constant of 2.7 X 10(8) M-1 s-1 and an unbinding constant of 2,900 s-1; approximately 66 percent of total binding sites are exposed at the outer vesicle surface. The value of the binding rate constant and three additional observations suggest that the binding kinetics are diffusion limited. The phloretin analogue, naringenin, which has a diffusion coefficient similar to phloretin yet a dissociation constant equal to 24 microM, bound to PC vesicle with the same rate constant as phloretin did. In addition, the phloretin-PC system was studied in buffers made one to six times more viscous than water by addition of sucrose or glycerol to the differ. The equilibrium affinity for phloretin binding to PC vesicles is independent of viscosity, yet the binding rate constant decreases with the expected dependence (kappa binding alpha 1/viscosity) for diffusion-limited processes. Thus, the binding rate constant is not altered by differences in binding affinity, yet depends upon the diffusion coefficient in buffer. Finally, studies of the pH dependence of the binding rate constant showed a dependence (kappa binding alpha [1 + 10pH-pK]) consistent with the diffusion-limited binding of a weak acid.     

Adenosine deaminase: viscosity studies and the mechanism of binding of substrate and of ground- and transition-state analogue inhibitors

We have studied the effects of viscosogenic agents, sucrose and ficoll, on (1) the hydrolysis of adenosine and of 6-methoxypurine riboside catalyzed by adenosine deaminase and (2) the rates of association and dissociation of ground-state and transition-state analogue inhibitors. For adenosine, Vmax/Km is found to be inversely proportional to the relative viscosity with sucrose, an agent affecting the microscopic viscosity, while no effect is found with ficoll, an agent affecting the macroscopic viscosity. Viscosogenic agents have no effect on the kinetic constants for 6-methoxypurine riboside. Thus, the bimolecular rate constant, Vmax/Km = 11.2 +/- 0.8 microM-1 s-1, for the reaction with adenosine is found to be at the encounter-controlled limit while that for the reaction with the poor substrate 6-methoxypurine riboside, 0.040 +/- 0.004 microM-1 s-1, is limited by some other process. Viscosity-dependent processes do not make a significant (less than 10%) contribution to Vmax. The dissociation constants for inhibitors are unaffected by viscosity. The ground-state analogue inhibitor purine riboside appears to bind at a rate comparable to that of adenosine. However, the slower rates of association (0.16-2.5 microM-1 s-1) and dissociation (5 X 10(-6) to 12 s-1) of transition-state analogue inhibitors are affected by the viscosity of the medium to approximately the same extent as the encounter-controlled rates of association and dissociation of adenosine.(ABSTRACT TRUNCATED AT 250 WORDS)     

Dissociation of calcium from the phosphorylated calcium-transporting adenosine triphosphatase of sarcoplasmic reticulum: kinetic equivalence of the calcium ions bound to the phosphorylated enzyme.

The internalization of 45Ca by the calcium-transporting ATPase into sarcoplasmic reticulum vesicles from rabbit muscle was measured during a single turnover of the enzyme by using a quench of 7 mM ADP and EGTA (25 degrees C, 5 mM MgCl2, 100 mM KCl, 40 mM MOPS.Tris, pH 7.0). Intact vesicles containing either 10-20 microM or 20 mM Ca2+ were preincubated with 45Ca for approximately 20 s and then mixed with 0.20-0.25 mM ATP and excess EGTA to give 70% phosphorylation of Etot with the rate constant k = 300 s-1. The two 45Ca ions bound to the phosphoenzyme (EP) become insensitive to the quench with ADP as they are internalized in a first-order reaction with a rate constant of k = approximately 30 s-1. The first and second Ca2+ ions that bind to the free enzyme were selectively labeled by mixing the enzyme and 45Ca with excess 40Ca, or by mixing the enzyme and 40Ca with 45Ca, for 50 ms prior to the addition of ATP and EGTA. The internalization of each ion into loaded or empty vesicles follows first-order kinetics with k = approximately 30 s-1; there is no indication of biphasic kinetics or an induction period for the internalization of either Ca2+ ion. The presence of 20 mM Ca2+ inside the vesicles has no effect on the kinetics or the extent of internalization of either or both of the individual ions. The Ca2+ ions bound to the phosphoenzyme are kinetically equivalent. A first-order reaction for the internalization of the individual Ca2+ ions is consistent with a rate-limiting conformational change of the phosphoenzyme with kc = 30 s-1, followed by rapid dissociation of the Ca2+ ions from separate independent binding sites on E approximately P.Ca2; lumenal calcium does not inhibit the dissociation of calcium from these sites. Alternatively, the Ca2+ ions may dissociate sequentially from E approximately P.Ca2 following a rate-limiting conformational change. However, the order of dissociation of the individual ions can not be distinguished. An ordered-sequential mechanism for dissociation requires that the ions dissociate much faster (k greater than or equal to 10(5) s-1) than the forward and reverse reactions for the conformational change (k-c = approximately 3000 s-1). Finally, the Ca2+ ions may exchange their positions rapidly on the phosphoenzyme (kmix greater than or equal to 10(5) s-1) before dissociating. A Hill slope of nH = 1.0-1.2, with K0.5 = 0.8-0.9 mM, for the inhibition of turnover by binding of Ca2+ to the low-affinity transport sites of the phosphoenzyme was obtained from rate measurements at six different concentrations of Mg2+.     

Diffusional barrier in the unfolding of a small protein

To determine how the dynamics of the polypeptide chain in a protein molecule are coupled to the bulk solvent viscosity, the unfolding by urea of the small protein barstar was studied in the presence of two viscogens, xylose and glycerol. Thermodynamic studies of unfolding show that both viscogens stabilize barstar by a preferential hydration mechanism, and that viscogen and urea act independently on protein stability. Kinetic studies of unfolding show that while the rate-limiting conformational change during unfolding is dependent on the bulk solvent viscosity, eta, its rate does not show an inverse dependence on eta, as expected by Kramers' theory. Instead, the rate is found to be inversely proportional to an effective viscosity, eta + xi, where xi is an adjustable parameter which needs to be included in the rate equation. xi is found to have a value of -0.7 cP in xylose and -0.5 cP in glycerol, in the case of unfolding, at constant urea concentration as well as under isostability conditions. Hence, the unfolding protein chain does not experience the bulk solvent viscosity, but instead an effective solvent viscosity, which is lower than the bulk solvent viscosity by either 0.7 cP or 0.5 cP. A second important result is the validation of the isostability assumption, commonly used in protein folding studies but hitherto untested, according to which if a certain concentration of urea can nullify the effect of a certain concentration of viscogen on stability, then the same concentrations of urea and viscogen will also not perturb the free energy of activation of the unfolding of the protein.     

Kinetics of the helix-coil transition in DNA

The kinetics of the helix-coil transition have been investigated for T2 and T7 phage DNA in a formamide-water-salt mixed solvent using a slow temperature perturbation technique (applicable to kinetic processes with rate constants ? 3 min^?1). In this solvent degradation of the DNA is effectively suppressed. Complex kinetic curves are observed by absorbance and viscosity measurements for the response to denaturing perturbations in the transition region. Analysis of the decay curves indicates that the denaturation reaction in this time range can be treated as a first-order reaction with a variable first-order rate parameter, k, the derivative of the logarithm of the absorbance or viscosity change with respect to time. In the approach to denaturation equilibrium in the transition region, the rate parameter is determined only by the instantaneous extent of denaturation of the molecules. Near equilibrium, the rate parameter assumes a constant value characteristic of the equilibrium state. In this region, where the denaturation reaction proceeds as a simple first-order process, both the decay of absorbance (reflected local conformational change) and the decay of solution viscosity (reflecting macromolecular conformational change) are characterized by the same constant value of k. In 83% formamide, 0.3M Na⁺, the rate parameter k for T2 DNA decreases from an extrapolated value of 2.0 min^?1 at 0% denaturation to 0.11 min^?1 at 90% denaturation. Rate parameters determined for T7 DNA at the same counterion concentration and fraction of denaturation are approximately five times as large as those cited for T2 DNA, indicating an inverse proportionality of rate constant to molecular length. On the other hand, simple first-order kinetic responses with constant k are obtained for renaturing perturbations within the transition, indicating that the mechanism of rewinding differs, in most cases, from that of unwinding. Only in the limit of very small perturbations about a given equilibrium position are the rate constants k obtained from denaturing and renaturing perturbations equal. For perturbations of finite size, it appears possible that an intramolecular initiation or nucleation event may precede rewinding and limit the rate of this reaction. The rate parameters again are approximately inversely proportional to molecular weight. The one exception to the first-power dependence on molecular weight appears when temperature jumps are made upward into the post-transition region. Here the molecular-weight dependence is second power, but complications arising from the different strand-separation properties of T2 and T7 DNA's make interpretation difficult. The previously used model of friction-limited unwinding appears to fit all the observations except for the molecular-weight dependence.     

Photoactive yellow protein from the purple phototrophic bacterium, Ectothiorhodospira halophila. Quantum yield of photobleaching and effects of temperature, alcohols, glycerol, and sucrose on kinetics of photobleaching and recovery.

A water-soluble yellow protein from E. halophila was previously shown to be photoactive (Meyer, T. E., E. Yakali, M. A. Cusanovich, and G. Tollin. 1987. Biochemistry. 26:418-423). Pulsed laser excitation in the protein visible absorption band (maximum at 445 nm) causes a rapid bleach of color (k = 7.5 x 10(3) s-1) followed by a slower dark recovery (k = 2.6 s-1). This is analogous to the photocycle of sensory rhodopsin II from Halobacterium (which also has k = 2.6 s-1 for recovery). We have now determined the quantum yield of the photobleaching process to be 0.64, which is comparable with that of bacteriorhodopsin (0.25), and is thus large enough to be biologically significant. Although the photoreactions of yellow protein were previously shown to be relatively insensitive to pH, ionic strength and the osmoregulator betaine, the present experiments demonstrate that temperature, glycerol, sucrose, and various alcohol-water mixtures strongly influence the kinetics of photobleaching and recovery. The effect of temperature follows normal Arrhenius behavior for the bleach reaction (Ea = 15.5 kcal/mol). The rate constant for the recovery reaction increases with temperature between 5 degrees C and 35 degrees C, but decreases above 35 degrees C indicating alternate conformations with differing kinetics. There is an order of magnitude decrease in the rate constant for photobleaching in both glycerol and sucrose solutions that can be correlated with the changes in viscosity. We conclude from this that the protein undergoes a conformational change as a consequence of the photoinduced bleach. Recovery kinetics are affected by glycerol and sucrose to a much smaller extent and in a more complicated manner.(ABSTRACT TRUNCATED AT 250 WORDS)     

The association reaction of yeast alcohol dehydrogenase with coenzyme is partly diffusion-controlled in solvents of increased viscosity

The steady-state kinetics of the yeast and liver alcohol dehydrogenase catalyzed reduction of aldehydes were examined in solvent mixtures of increased viscosity. This was done to investigate the effects of diffusion control on the fast association of NADH with the enzymes. Both glycerol and sucrose were unsatisfactory as viscosogens, as they inhibited the enzyme, but poly(ethylene glycol)/water mixtures were satisfactory. The 5-fold faster reaction of yeast alcohol dehydrogenase with NADH is partly diffusion controlled, whereas the slower liver alcohol dehydrogenase reaction showed no diffusion effects. These results are consistent with a yeast alcohol dehydrogenase active site that has relatively little steric hindrance to NADH binding. It is estimated that contributions to this association reaction from diffusion control and chemical activation control are equal at a solvent viscosity of 10 cP. Thus, under physiological conditions of increased viscocity the NADH association may be significantly affected by diffusion effects. In order to estimate accurately the maximum diffusion-controlled rate constant from diffusion theory, the diffusion coefficients of NADH were measured in poly(ethylene glycol)/water mixtures and were found to vary inversely as the solvent viscosity raised to the power of 0.5. The non-Stokesian behaviour of molecules as large as NADH in polymer/water mixtures may be a serious limitation to the routine use of poly(ethylene glycol) as a viscosogen for diffusion studies.     

Phosphorylation of the calcium-transporting adenosinetriphosphatase by lanthanum ATP: rapid phosphoryl transfer following a rate-limiting conformational change

The calcium-transport ATPase (CaATPase) of rabbit sarcoplasmic reticulum preincubated with 0.02 mM Ca2+ (cE.Ca2) is phosphorylated upon the addition of 0.25 mM LaCl3 and 0.3 mM [gamma-32P]ATP with an observed rate constant of 6.5 s-1 (40 mM MOPS, pH 7.0, 100 mM KCl, 25 degrees C). La.ATP binds to cE.Ca2 with a rate constant of 5 X 10(6) M-1 s-1, while ATP, Ca2+, and La3+ dissociate from cE.Ca2.La.ATP at less than or equal to 1 s-1. The reaction of ADP with phosphoenzyme (EP) formed from La.ATP is biphasic. An initial rapid loss of EP is followed by a slower first-order disappearance, which proceeds to an equilibrium mixture of EP.ADP and nonphosphorylated enzyme with bound ATP. The fraction of EP that reacts in the burst (alpha) and the first-order rate constant for the slow phase (kb) increase proportionally with increasing concentrations of ADP to give maximum values of 0.34 and 65 s-1, respectively, at saturating ADP (KADPS = 0.22 mM). The burst represents rapid phosphoryl transfer and demonstrates that ATP synthesis and hydrolysis on the enzyme are fast. The phosphorylation of cE.Ca2 by La.ATP at 6.5 s-1 and the kinetics for the reaction of EP with ADP are consistent with a rate-limiting conformational change in both directions. The conformational change converts cE.Ca2.La.ATP to the form of the enzyme that is activated for phosphoryl transfer, aE.Ca2.La.ATP, at 6.5 s-1; this is much slower than the analogous conformational change at 220 s-1 with Mg2+ as the catalytic ion [Petithory & Jencks (1986) Biochemistry 25, 4493]. The rate constant for the conversion of aE.Ca2.La.ATP to cE.Ca2.La.ATP is 170 s-1. ATP does not dissociate measurably from aE.Ca2.La.ATP. Labeled EP formed from cE.Ca2 and La.ATP with leaky vesicles undergoes hydrolysis at 0.06 s-1. It is concluded that the reaction mechanism of the CaATPase is remarkably similar with Mg.ATP and La.ATP; however, the strong binding of La.ATP slows both the conformational change that is rate limiting for EP formation and the dissociation of La.ATP. An interaction between La3+ at the catalytic site and the calcium transport sites decreases the rate of calcium dissociation by greater than 60-fold. When cE-Ca2 is mixed with 0.3 mM ATP and 1.0 mM Cacl2, the phosphoenzyme is formed with an observed rate constant of 3 s-1. The phosphoenzyme formed from Ca.ATP reacts with 2.0 mM ADP and labeled ATP with a rate constant of 30 s-1; there may be a small burst (alpha less than or equal to 0.05).     

Dynamic aspect of kinetics of reaction catalyzed by lactate dehydrogenase

The influence of solvent viscosity on the kinetic parameters of the pyruvate reduction reaction catalyzed by lactate dehydrogenase has been investigated. The viscosity was adjusted by sucrose and glycerol solutions at concentrations from 0 to 44% and from 0 to 63%, respectively. The reaction rate decreased abruptly with an increase in viscosity. The study of different reaction stages (enzyme-substrate complex formation, catalysis, inhibitory complex decomposition, competitive inhibition by chlorine ions) revealed that the catalysis (and the related conformational changes) is the only stage (of the above mentioned) that depends markedly on the solvent viscosity. The reaction is insensitive to the changes in the dielectric properties of the solution induced by the addition of alcohols and dioxane. The observed power dependence of the rate constant on viscosity is explained in terms of Kramer's theory which considers the proton transition through the activation barrier to be a diffusion in the field of random forces. The influence of solvent viscosity on enzymic kinetics indicates a direct relation between solvent dynamics and relevant protein conformational movements.     

Ligand-induced changes in membrane-bound acetylcholine receptor observed by ethidium fluorescence. 3. Stopped-flow studies with histrionicotoxin.

Rapid kinetic studies of histrionicotoxin interactions with membrane-bound acetylcholine-receptor showed a conformational change in the receptor-histironicotoxin complex as reflected by a decrease in fluorescence intensity of the extrinsic probe ethidium. The simplest kinetic mechanism consistent with the observed data is one in which a rapid preequiliibrium exists between receptor and toxin (K = 3.33 micrometers), followed by a slow conformational change (k1 congruent to 2 X 10(-2) s-1 and k-1 congruent to 1.5 X 10(-3) s-1). The overall equilibrium constant (Kov) determined from a fit of the amplitude dependence on toxin concentration had a value of 0.25 micrometer. The data preclude kinetic mechanisms where histrionicotoxin acts as an effector, shifting equilibria between preexisting, discrete, and slowly interconverting receptor forms.     

Conformational equilibria accompanying the electron transfer between cytochrome c (P551) and azurin from Pseudomonas aeruginosa.

The redox reaction between cytochrome c (Cyt c) (P-551) and the blue copper protein azurin, both from Pseudomonas aeruginosa, was studied using the temperature-jump technique. Two relaxation times were observed in a mechanism assumed to involve three equilibria. The fast relaxation time (0.4 less than tau less than 8 ms) was ascribed to the electron exchange step. The slow relaxation time (tau congruent to 37 ms) was assigned to a conformational equilibrium of the reduced azurin that was coupled through the electron exchange step to a faster conformational equilibrium of the oxidized Cyt c (P551). But because the Cyt c (P551) isomerization, being very rapid, was uncoupled from the two slower equilibria, and was assumed to involve no spectral change, the amplitude of its relaxation time (tau congruent to 0.1 ms) would be zero. At 25 degrees C and pH 7.0 the rate constants for the oxidation and reduction of Cyt c (P551) by azurin were 6.1 X 10(6) and 7.8 X 10(6) M-1 s-1, respectively; for the formation and disappearance of the reactive conformational isomer of azurin they were 12 and 17 s-1, respectively. The rates for the Cyt c (P551) isomerization could only be estimated at approximately 10(4) s-1. The thermodynamic parameters of each reaction step were evaluated from the amplitudes of the relaxations and from Eyring plots of the rate constants. Measurements of the overall equilibrium constant showed it to be temperature independent (5-35 degrees C), i.e. deltaHtot = 0. This zero enthalpy change was found to be compatible with the enthalpies calculated for the individual steps. In the electron exchange equilibrium, the values of the activation enthalpies were two to three times higher than the values published for various low molecular weight reagents in their electron exchange with copper proteins, yet the rate of exchange between Cyt c (P551) and azurin was some hundreds of times faster. This was explained in terms of the measured positive or zero entropies of activation that could result from a high level of specificity between the proteins particularly in areas of complementary charges. The mechanism of electron transfer was considered as essentially an outer sphere reaction, of which the rate could be approximated by the Marcus theory.     

An ATP-linked structural change in protein kinase A precedes phosphoryl transfer under physiological magnesium concentrations

The kinetic mechanism for the catalytic subunit of protein kinase A was evaluated using physiological concentrations of free magnesium (0.5 mM) and a rapid quench flow technique. When the enzyme is pre-equilibrated with ATP, the peptide substrate, LRRASLG (Kemptide), is phosphorylated in a biphasic manner with a rapid, exponential "burst" phase (kb) followed by a slower, linear phase (kL) that corresponds to the steady-state kinetic rate. Both the amplitude and the substrate-rate dependence of the initial, burst phase indicate that the rate of phosphoryl transfer is fast (approximately 500 s-1) and does not limit turnover (45 s-1). Viscosity studies indicate that, while Kemptide is in rapid equilibrium, ATP does not exchange rapidly with the active site and kcat/KATP is limited by the rate constant for nucleotide encounter. When the pre-steady-state kinetic experiments are initiated with ATP, a lag phase is observed at low ATP concentrations consistent with rate-limiting association. At high ATP concentrations (>1 mM), a burst phase is observed but the rate and amplitude are low on the basis of the bimolecular rate constant for ATP association and the rate constant for phosphoryl transfer. The kinetic data indicate that the phosphoryl transfer step is fast at physiological magnesium concentrations, but an ATP-linked conformational change precedes this step, limiting the burst phase rate constant. Simulations of the pre-steady-state kinetic transients indicate that turnover (45 s-1) is limited both by net product release (70 s-1) and by this structural change (170 s-1). This structural change may also occur at high free magnesium concentrations, but it must be significantly faster than 170 s-1 and, consequently, not rate-limiting for turnover (kcat = 20 s-1 at 10 mM free Mg2+). We propose that this conformational event is an obligatory component of the kinetic pathway and includes a movement of the catalytic residues necessary for supporting phosphoryl group donation.     

Kinetics and mechanism of bilirubin binding to human serum albumin

The kinetics of bilirubin binding to human serum albumin at pH 7.40, 4 degrees C, was studied by monitoring changes in bilirubin absorbance. The time course of the absorbance change at 380 nm was complex: at least three kinetic events were detected including the bimolecular association (k1 = 3.8 +/- 2.0 X 10(7) M-1 S-1) and two relaxation steps (52 = 40.2 +/- 9.4 s-1 and k3 = 3.8 +/- 0.5 s-1). The presence of the two slow relaxations was confirmed under pseudo-first order conditions with excess albumin. Curve-fitting procedures allowed the assignment of absorption coefficients to the intermediate species. When the bilirubin-albumin binding kinetics was observed at 420 nm, only the two relaxations were seen; apparently the second order association step was isosbestic at this wavelength. The rate of albumin-bound bilirubin dissociation was measured by mixing the pre-equilibrated human albumin-bilirubin complex with bovine albumin. The rate constant for bilirubin dissociation measured at 485 nm was k-3 = 0.01 s-1 at 4 degrees C. A minimum value of the equilibrium constant for bilirubin binding to human albumin determined from the ratio k1/k-3 is therefore approximately 4 X 10(9) M-1.     

Effect of solution viscosity on intramolecular electron transfer in sulfite oxidase

Our previous studies have shown that the rate constant for intramolecular electron transfer (IET) between the heme and molybdenum centers of chicken liver sulfite oxidase varies from approximately 20 to 1400 s(-1) depending upon reaction conditions [Pacheco, A., Hazzard, J. T., Tollin, G., and Enemark, J. H. (1999) J. Biol. Inorg. Chem. 4, 390-401]. These two centers are linked by a flexible polypeptide loop, suggesting that conformational changes, which alter the Mo-Fe distance, may play an important role in the observed IET rates. In this study, we have investigated IET in sulfite oxidase using laser flash photolysis as a function of solution viscosity. The solution viscosity was varied over the range of 1.0-2.0 cP by addition of either polyethylene glycol 400 or sucrose. In the presence of either viscosogen, an appreciable decrease in the IET rate constant value is observed with an increase in the solvent viscosity. The IET rate constant exhibits a linear dependence on the negative 0.7th power of the viscosity. Steady-state kinetics and EPR experiments are consistent with the interpretation that viscosity, and not other properties of the added viscosogens, is responsible for the dependence of IET rates on the solvent composition. The results are consistent with the role of conformational changes on IET in sulfite oxidase, which helps to clarify the inconsistency between the large rate constant for IET between the Mo and Fe centers and the long distance (approximately 32 A) between these two metal centers observed in the crystal structure [Kisker, C., Schindelin, H., Pacheco, A., Wehbi, W., Garnett, R. M., Rajagopalan, K. V., Enemark, J. H., and Rees, D. C. (1997) Cell 91, 973-983].     

Kinetic mechanism of 1-N6-etheno-2-aza-ATP and 1-N6-etheno-2-aza-ADP binding to bovine ventricular actomyosin-S1 and myofibrils

The fluorescence emission of 1-N6-etheno-2-aza-ATP (epsilon-aza-ATP) at 410-460 nm is enhanced approximately 8-fold upon mixing substoichiometric concentrations of epsilon-aza-ATP with bovine cardiac actomyosin-S1 or myofibrils. The time course of nucleotide fluorescence measured in a front face stopped flow cell upon mixing epsilon-aza-ATP with bovine cardiac myofibrils ([Ca2+] less than 10(-7) M) is essentially the same as that with bovine cardiac actomyosin subfragment-1. In single turnover experiments, the fluorescence rapidly rises to a maximum value, then decreases with a rate constant of 0.04 s-1 at 0 degree C to a final value that is approximately twice the level of the unbound nucleotide. At concentrations of epsilon-aza-ATP greater than 40 microM the kinetics of epsilon-aza-ATP binding is clearly biphasic for both actomyosin-S1 and myofibrils. At 0 degree C, the rate of the more rapid phase is proportional to nucleotide concentration and has a second order rate constant of 1.7 X 10(5) M-1 s-1; the rate of the slower phase extrapolates to a maximum of 4-5 s-1 at high nucleotide concentration. The rate constants for dissociation of epsilon-aza-ADP from bovine cardiac actomyosin-S1 and myofibrils were measured from the decrease in epsilon-aza-ADP fluorescence enhancement observed upon displacement by ATP to be 20 and 18 s-1, respectively, at 0 degree C. These results indicate that most of the cross-bridges in cardiac myofibrils are bound to actin and that the geometric constraints imposed upon the interaction of actin and myosin by the three-dimensional structure of the myofibril do not modify the kinetics of epsilon-aza-ATP binding or epsilon-aza-ADP dissociation.     

Oxidation of (horse) hemoglobin by copper: an intermediate detected by electron spin resonance.

The oxidation of horse hemoglobin by Cu(II) has been followed by the changes in the electron spin resonance spectra of copper. By stopped-flow and freeze-quenching techniques, it is shown that the second-order rate constant for the binding of Cu(II) to hemoglobin is greater than 5 X 10(5) mol-1 s-1 and the apparent first-order rate for the reduction of Cu(II) to Cu(I) is 0.051 s-1. It is also shown that the binding of Cu(II) to hemoglobin is followed by an alteration of the Cu(II) spectrum, decreasing the g values. This process has an apparent rate constant of 17 s-1 and presumably involves a conformational change in the region of the copper binding site. It is also shown that this conformational change is apparently necessary for Cu(II) to oxidize hemoglobin.     

High acetylcholine concentrations cause rapid inactivation before fast desensitization in nicotinic acetylcholine receptors from Torpedo.

By using both a 3 to 4 ms quenched-86Rb+ flux assay and native acetylcholine receptor (AChR) rich electroplaque vesicles on which 50-60% of acetylcholine activation sites were blocked with alpha-BTX, we determined apparent rates of agonist-induced inactivation in AChR from Torpedo under conditions where measured flux response was directly proportional to initial 86Rb+ influx rate. Inactivation kinetics with acetylcholine in both the activating range (10 microM-10 mM) and the self-inhibiting range (15-100 mM) were measured at 4 degrees C. In the presence of 10 microM-1 mM acetylcholine, inactivation is characterized by a single exponential rate constant, kd (fast desensitization). Plots of kd vs. acetylcholine concentration display maximum kds [kd(max)] of 6.6-8.0 s-1, half-maximal kd at 102 +/- 16 microM, and a Hill coefficient of 1.6 +/- 0.3, closely paralleling the initial ion flux response of AChR. Thus, fast desensitization probably occurs from a doubly-liganded preopen state or the open channel state. In the self-inhibiting acetylcholine concentration range, inactivation is biphasic. A "rapid inactivation" phase is complete within 30 ms, followed by fast desensitization at a rate close to kd(max). Both the rate and extent of rapid inactivation increase with acetylcholine concentration, indicating that acetylcholine binds to its self-inhibition site with apparent kon approximately equal to 10(3) M-1s-1 and koff approximately equal to 40 s-1. This slow kon suggests either hindered access to the inhibitory allosteric site or that a fast binding step is followed by a slower conformational change leading to channel inhibition. Overall, our data suggest that acetylcholine binds preferentially to its inhibitory site when the receptor is in the open-channel conformation and that fast desensitization can occur from all multiple-liganded states.