Kinetics of Na(+)-dependent conformational changes of rabbit kidney Na+,K(+)-ATPase.

The kinetics of Na(+)-dependent partial reactions of the Na+,K(+)-ATPase from rabbit kidney were investigated via the stopped-flow technique, using the fluorescent labels N-(4-sulfobutyl)-4-(4-(p-(dipentylamino)phenyl)butadienyl)py ridinium inner salt (RH421) and 5-iodoacetamidofluorescein (5-IAF). When covalently labeled 5-IAF enzyme is mixed with ATP, the two labels give almost identical kinetic responses. Under the chosen experimental conditions two exponential time functions are necessary to fit the data. The dominant fast phase, 1/tau 1 approximately 155 s-1 for 5-IAF-labeled enzyme and 1/tau 1 approximately 200 s-1 for native enzyme (saturating [ATP] and [Na+], pH 7.4 and 24 degrees C), is attributed to phosphorylation of the enzyme and a subsequent conformational change (E1ATP(Na+)3-->E2P(Na+)3 + ADP). The smaller amplitude slow phase, 1/tau 2 = 30-45 s-1, is attributed to the relaxation of the dephosphorylation/rephosphorylation equilibrium in the absence of K+ ions (E2P<==>E2). The Na+ concentration dependence of 1/tau 1 showed half-saturation at a Na+ concentration of 6-8 mM, with positive cooperatively involved in the occupation of the Na+ binding sites. The apparent dissociation constant of the high-affinity ATP-binding site determined from the ATP concentration dependence of 1/tau 1 was 8.0 (+/- 0.7) microM. It was found that P3-1-(2-nitrophenyl)ethyl ATP, tripropylammonium salt (NPE-caged ATP), at concentrations in the hundreds of micromolar range, significantly decreases the value of 1/tau 1, observed. This, as well as the biexponential nature of the kinetic traces, can account for previously reported discrepancies in the rates of the reactions investigated.     

Two adaptor proteins differentially modulate the phosphorylation and biophysics of Kv1.3 ion channel by SRC kinase.

The Shaker family K(+) channel protein, Kv1.3, is tyrosine phosphorylated by v-Src kinase at Tyr(137) and Tyr(449) to modulate current magnitude and kinetic properties. Despite two proline rich sequences and these phosphotyrosines contained in the carboxyl and amino terminals of the channel, v-Src kinase fails to co-immunoprecipitate with Kv1.3 as expressed in HEK 293 cells, indicating a lack of direct Src homology 3- or Src homology 2-mediated protein-protein interaction between the channel and the kinase. We show that the adaptor proteins, n-Shc and Grb10, are expressed in the olfactory bulb, a region of the brain where Kv1.3 is highly expressed. In HEK 293 cells, co-expression of Kv1.3 plus v-Src with Grb10 causes a decrease in v-Src-induced Kv1.3 tyrosine phosphorylation and a reversal of v-Src-induced Kv1.3 current suppression, increase in inactivation time constant (tau(inact)), and disruption of cumulative inactivation properties. Co-expression of Kv1.3 plus v-Src with n-Shc did not significantly alter v-Src-induced Kv1.3 current suppression but reversed v-Src induced increased tau(inact) and restored the right-shifted voltage at half-activation (V(1/2)) induced by v-Src. The v-Src-induced shift in V(1/2) and increased tau(inact) was retained when Tyr(220), Tyr(221), and Tyr(304) in the CH domain of n-Shc were mutated to Phe (triple Shc mutant) but was reversed back to control values when either wild-type Shc or the family member Sck, which is not a substrate for Src kinase, was substituted for the triple Shc mutant. Thus the portion of the CH domain that includes Tyr(220), Tyr(221), and Tyr(304) may regulate a shift in Kv1.3 voltage dependence and inactivation kinetics produced by n-Shc in the presence of v-Src. Collectively these data indicate that Grb10 and n-Shc adaptor molecules differentially modulate the degree of Kv1.3 tyrosine phosphorylation, the channel's biophysical properties, and the physical complexes associated with Kv1.3 in the presence of Src kinase.     

Pre-steady-state charge translocation in NaK-ATPase from eel electric organ

Time-resolved measurements of charge translocation and phosphorylation kinetics during the pre-steady state of the NaK-ATPase reaction cycle are presented. NaK-ATPase-containing microsomes prepared from the electric organ of Electrophorus electricus were adsorbed to planar lipid bilayers for investigation of charge translocation, while rapid acid quenching was used to study the concomitant enzymatic partial reactions involved in phosphoenzyme formation. To facilitate comparison of these data, conditions were standardized with respect to pH (6.2), ionic composition, and temperature (24 degrees C). The different phases of the current generated by the enzyme are analyzed under various conditions and compared with the kinetics of phosphoenzyme formation. The slowest time constant (tau 3(-1) approximately 8 s-1) is related to the influence of the capacitive coupling of the adsorbed membrane fragments on the electrical signal. The relaxation time associated with the decaying phase of the electrical signal (tau 2(-1) = 10-70 s-1) depends on ATP and caged ATP concentration. It is assigned to the ATP and caged ATP binding and exchange reaction. A kinetic model is proposed that explains the behavior of the relaxation time at different ATP and caged ATP concentrations. Control measurements with the rapid mixing technique confirm this assignment. The rising phase of the electrical signal was analyzed with a kinetic model based on a condensed Albers-Post cycle. Together with kinetic information obtained from rapid mixing studies, the analysis suggests that electroneutral ATP release, ATP and caged ATP binding, and exchange and phosphorylation are followed by a fast electrogenic E1P-->E2P transition. At 24 degrees C and pH 6.2, the rate constant for the E1P-- >E2P transition in NaK-ATPase from eel electric organ is > or = 1,000 s- 1.     

Some kinetic and steady-state properties of sodium channels after removal of inactivation

To study the kinetic and steady-state properties of voltage-dependent sodium conductance activation, squid giant axons were perfused internally with either pronase or N-bromoacetamide and voltage clamped. Parameters of activation, tau m and gNa(V), and deactivation, tau Na, were measured and compared with those obtained from control axons under the assumption that gNa oc m3h of the Hodgkin-Huxley scheme. tau m(V) values obtained from the turn-on of INa agree well with control axons and previous determinations by others. tau Na(V) values derived from Na tail currents were also unchanged by pronase treatment and matched fairly well previously published values. tau m(V) obtained from 3 x tau Na(V) were much larger than tau m(V) obtained from INa turn-on at the same potentials, resulting in a discontinuous distribution. Steady-state In (gNa/gNa max - gNa) vs. voltage was not linear and had a limiting logarithmic slope of 5.3 mV/e-fold gNa. Voltage step procedures that induce a second turn-on of INa during various stages of the deactivation (Na tail current) process reveal quasiexponential activation at early stages that becomes increasingly sigmoid as deactivation progresses. For moderate depolarizations, primary and secondary activation kinetics are superimposable. These data suggest that, although m3 can describe the shape of INa turn-on, it cannot quantitatively account for the kinetics of gNa after repolarization. Kinetic schemes for gNa in which substantial deactivation occurs by a unique pathway between conducting and resting states are shown to be unlikely. It appears that the rate-limiting step in linear kinetic models of activation may be between a terminal conducting state and the adjacent nonconducting intermediate.     

Extracellular K+ elevates outward currents through Kir2.1 channels by increasing single-channel conductance

Outward currents through inward rectifier K+ channels (Kir) play a pivotal role in determining resting membrane potential and in controlling excitability in many cell types. Thus, the regulation of outward Kir current (IK1) is important for appropriate physiological functions. It is known that outward IK1 increases with increasing extracellular K+ concentration ([K+]o), but the underlying mechanism is not fully understood. A "K+-activation of K+-channel" hypothesis and a "blocking-particle" model have been proposed to explain the [K+]o-dependence of outward IK1. Yet, these mechanisms have not been examined at the single-channel level. In the present study, we explored the mechanisms that determine the amplitudes of outward IK1 at constant driving forces [membrane potential (Vm) minus reversal potential (EK)]. We found that increases in [K+]o elevated the single-channel current to the same extent as macroscopic IK1 but did not affect the channel open probability at a constant driving force. In addition, spermine-binding kinetics remained unchanged when [K+]o ranged from 1 to 150 mM at a constant driving force. We suggest the regulation of K+ permeation by [K+]o as a new mechanism for the [K+]o-dependence of outward IK1.     

Three classes of epidermal growth factor receptors on HeLa cells

The kinetics of 125I-labeled epidermal growth factor (EGF) binding to receptors on HeLa cells were investigated. Scatchard analysis revealed the presence of 22,000 high affinity receptors (Kd = 0.12 nM) and 25,000 low affinity receptors per cell (Kd = 9.2 nM). The kinetic analysis of EGF binding to high affinity receptors was performed with cells pretreated with the monoclonal antibody 2E9, which prevents specifically EGF binding to low affinity receptors. The study of EGF binding to only low affinity receptors was performed with cells pretreated with the phorbol ester phorbol 12-myristate 13-acetate, which induces a conversion of high affinity receptors to low affinity receptors. This kinetic analysis of EGF binding to HeLa cells revealed the presence of three types of receptors. High affinity receptors were found to consist of one receptor type (type I) with a kinetic association constant (kass) of 6.2 x 10(5) M-1.s-1 and a kinetic dissociation constant (kdis) of 3.5 x 10(-4) s-1. The low affinity receptors were found to consist of two kinetic distinguishable sites: type II or fast sites with kass = 3.3 x 10(6) M-1.s-1 and kdis = 8.1 x 10(-3) s-1 and the type III or slow sites with kass = 3.2 x 10(4) M-1.s-1 and kdis = 1.6 x 10(-4) s-1. The regulatory mechanism which may determine the EGF binding characteristics is discussed.     

Molecular basis for the different activation kinetics of the pacemaker channels HCN2 and HCN4

The pacemaker channels HCN2 and HCN4 have been identified in cardiac sino-atrial node cells. These channels differ considerably in several kinetic properties including the activation time constant (tau act), which is fast for HCN2 (144 ms at -140 mV) and slow for HCN4 (461 ms at -140 mV). Here, by analyzing HCN2/4 chimeras and mutants we identified single amino acid residues in transmembrane segments 1 and 2 and the connecting loop between S1 and S2 that are major determinants of this difference. Replacement of leucine 272 in S1 of HCN4 by the corresponding phenylalanine present in HCN2 decreased tau act of HCN4 to 149 ms. Conversely, activation of the fast channel HCN2 was decreased 3-fold upon the corresponding mutation of F221L in the S1 segment. Mutation of N291T and T293A in the linker between S1 and S2 of HCN4 shifted tau act to 275 ms. While residues 272, 291, and 293 of HCN4 affected the activation speed at basal conditions they had no obvious influence on the cAMP-dependent acceleration of activation kinetics. In contrast, mutation of I308M in S2 of HCN4 abolished the cAMP-dependent decrease in tau act. Surprisingly, this mutation also prevented the acceleration of channel activation observed after deletion of the C-terminal cAMP binding site. Taken together our results indicate that the speed of activation of the HCN4 channel is determined by structural elements present in the S1, S1-S2 linker, and the S2 segment.     

Kinetics of the reaction between testosterone and antitestosterone antiserum

In order to characterize from a kinetic viewpoint the antibody population mainly involved in the binding of testosterone by its homologous antiserum, the kinetics of the association reaction between [1,2,6,7-3H]-testosterone and rabbit antiserum anti-testosterone-3-(O-carboxymethyl)oxime-bovine serum albumin (Ab R2603-1) was followed at pH 7.4 and at constant ionic strength, at temperatures ranging from 2 degrees C to 37 degrees C and at concentration near to work conditions for testosterone radioimmunoassay; dextran coated charcoal suspension was used for the bound/free separation. In the examined concentration range, the observed kinetics trends can be explained by assuming the existence of two classes of antibody binding sites, Ab1 and Ab2. The kinetics of the dissociation reaction of the testosterone-antibody complex was also followed after the addition of a large excess of unlabeled testosterone. At 22.0 degrees C, association and dissociation rate constants are 2.1.10(7) s-1M-1 and 3.7.10(-3) s-1, respectively, for the Ab1 class of antibody binding sites, and 3.6.10(6) s-1M-1 and 7.0.10(-4) s-1 for the Ab2 class. Equilibrium constants obtained from kinetic data were very similar for both classes of antibody binding sites and in good agreement with the equilibrium values obtained from linear Scatchard plot. The order of magnitude of the second order rate constants and the high activation enthalpy for the forward and reverse reaction suggest a mechanism more complex than a simple second order.     

Comparative kinetic analysis of the activation of human plasminogen by natural and recombinant single-chain urokinase-type plasminogen activator

Single-chain urokinase-type plasminogen activator (scu-PA) may be obtained from conditioned cell culture media (natural scu-PA) or by expression of the cDNA encoding human scu-PA in Escherichia coli (recombinant scu-PA). The activation of Glu-plasminogen by natural and recombinant scu-PA can be described by a sequence of three reactions, each of which obeys Michaelis-Menten kinetics. Initial activation of plasminogen to plasmin by scu-PA (reaction I) occurs with a high affinity (Km below 0.8 microM) for both scu-PAs, while the catalytic rate constant (k2) is 0.017 s-1 for recombinant scu-PA but only 0.0009 s-1 for natural scu-PA. Subsequent conversion of scu-PA to urokinase (two-chain urokinase-type plasminogen activator, tcu-PA) by generated plasmin (reaction II) occurs with a comparable affinity (Km about 5 microM) for natural and recombinant scu-PA and with a k2 of 0.23 s-1 for natural and 1.2 s-1 for recombinant scu-PA. Finally, activation of plasminogen by tcu-PA (reaction III) occurs with low affinity (Km 30-50 microM) but with a high catalytic rate constant (k2 about 5 s-1) for both natural and recombinant tcu-PA. The differences in the kinetic parameters of the activation of plasminogen by natural or recombinant scu-PA are thus mainly due to differences in turnover rate in the first reaction. Indeed, the catalytic rate constant of the first reaction is about 20-times higher for recombinant scu-PA than for natural scu-PA. Thus, surprisingly, the artificial, unglycosylated recombinant scu-PA molecule has a better catalytic efficiency than its natural glycosylated counterpart.     

Conformational change accompanies redox reactions of the tetraheme cytochrome c-554 of Nitrosomonas europaea

Cytochrome c-554 of the ammonia-oxidizing chemolithoautotropic bacteria is thought to mediate electron transfer from hydroxylamine oxidoreductase to a terminal oxidase and/or to ammonia monooxygenase. The cytochrome has four c hemes which interact magnetically and have the same redox potential. We report that the kinetics of reduction of ferric cytochrome c-554 by dithionite or the oxidation of ferrous cytochrome c-554 by O2 or H2O2 are complex and multiphasic. Transient rapid-scan difference spectra indicate discrete maxima at approximately 418 nm, 425 nm and 432 nm. Absorbance changes at all three difference maxima appear to occur in all kinetic phases, although not in equal amounts for each wavelength. Reduction by 20 mM dithionite was biphasic. At pH 7.5 the first phase, which involved approximately 50% of the total absorbance change, had a rate constant (20 degrees C) of 140 s-1 and energy of activation of 20 kJ X mol-1. The slow phase had a rate constant 0.43 s-1 and a relatively high energy of activation, 87 kJ X mol-1, suggesting that a change in protein configuration accompanied the reaction. As the pH of the solution increased, the rate constant for both phases decreased and the fraction of absorbance change in the rapid phase increased. Oxidation of ferrous cytochrome c-554 by O2 involved a discrete rapid phase with a rate constant of 14 s-1, accounting for 6% of the absorbance. The remainder of the reaction was multiphasic with rate constants in the range 0.1-0.01 s-1. With H2O2 as the oxidant, the rapid phase involved 39% of the change in absorbance with a rate constant of 19 s-1. The remainder of the reoxidation was multiphasic with rate constants ranging over 0.4-0.01 s-1.     

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)     

K+ transport properties of K+ channels in the plasma membrane of Vicia faba guard cells

Electrical properties of the plasma membrane of guard cell protoplasts isolated from stomates of Vicia faba leaves were studied by application of the whole-cell configuration of the patch-clamp technique. The two types of K+ currents that have recently been identified in guard cells may allow efflux of K+ during stomatal closing, and uptake of K+ during stomatal opening (Schroeder et al., 1987). A detailed characterization of ion transport properties of the inward-rectifying (IK+,in) and the outward-rectifying (IK+,out) K+ conductance is presented here. The permeability ratios of IK+,in and IK+,out currents for K+ over monovalent alkali metal ions were determined. The resulting permeability sequences (PK+ greater than PRb+ greater than PNa+ greater than PLi+ much greater than PCs+) corresponded closely to the ion specificity of guard cell movements in V. faba. Neither K+ currents exhibited significant inactivation when K+ channels were activated for prolonged periods (greater than 10 min). The absence of inactivation may permit long durations of K+ fluxes, which occur during guard cell movements. Activation potentials of inward K+ currents were not shifted when external K+ concentrations were changed. This differs strongly from the behavior of inward-rectifying K+ channels in animal tissue. Blue light and fusicoccin induce hyperpolarization by stimulation of an electrogenic pump. From slow-whole-cell recordings it was concluded that electrogenic pumps require cytoplasmic substrates for full activation and that the magnitude of the pump current is sufficient to drive K+ uptake through IK+,in channels. First, direct evidence was gained for the hypothesis that IK+,in channels are a molecular pathway for K+ accumulation by the finding that IK+,in was blocked by Al3+ ions, which are known to inhibit stomatal opening but not closing. The results presented in this study strongly support a prominent role for IK+,in and IK+,out channels in K+ transport across the plasma membrane of guard cells.     

Observation of a chloride-dependent intermediate during catalysis by angiotensin converting enzyme using radiationless energy transfer

Stopped-flow radiationless energy-transfer kinetics have been used to examine the effects of chloride on the hydrolysis of Dns-Lys-Phe-Ala-Arg by angiotensin converting enzyme. The kinetic constants for hydrolysis at pH 7.5 and 22 degrees C in the presence of 300 mM sodium chloride were KM = 28 microM and kcat = 110 s-1, and in its absence, KM = 240 microM and kcat = 68 s-1. The apparent binding constant for chloride was 4 mM, and the extent of chloride activation in terms of kcat/KM was 14-fold. The effects of chloride on the pre-steady-state were examined at 2 degrees C. In the presence of chloride, two distinct enzyme-substrate complexes were observed, suggesting multiple steps in substrate binding. The initial complex was formed during the mixing period (kobsd greater than 200 s-1) while the second complex was formed much more slowly (kobsd = 40 s-1 when [S] = 5 microM and [NaCl] = 150 mM). Strikingly, in the absence of chloride, only a single, rapidly formed enzyme-substrate complex was observed. These results are consistent with a nonessential activator kinetic mechanism in which the slow step reflects conversion of an initially formed complex, (E X Cl- X S)1, to a more tightly bound complex, (E X Cl- X S)2.     

Rapid charge translocation by the cardiac Na(+)-Ca2+ exchanger after a Ca2+ concentration jump.

The kinetics of Na(+)-Ca2+ exchange current after a cytoplasmic Ca2+ concentration jump (achieved by photolysis of DM-nitrophen) was measured in excised giant membrane patches from guinea pig or rat heart. Increasing the cytoplasmic Ca2+ concentration from 0.5 microM in the presence of 100 mM extracellular Na+ elicits an inward current that rises with a time constant tau 1 < 50 microseconds and decays to a plateau with a time constant tau 2 = 0.65 +/- 0.18 ms (n = 101) at 21 degrees C. These current signals are suppressed by Ni2+ and dichlorobenzamil. No stationary current, but a transient inward current that rises with tau 1 < 50 microseconds and decays with tau 2 = 0.28 +/- 0.06 ms (n = 53, T = 21 degrees C) is observed if the Ca2+ concentration jump is performed under conditions that promote Ca(2+)-Ca2+ exchange (i.e., no extracellular Na+, 5 mM extracellular Ca2+). The transient and stationary inward current is not observed in the absence of extracellular Ca2+ and Na+. The application of alpha-chymotrypsin reveals the influence of the cytoplasmic regulatory Ca2+ binding site on Ca(2+)-Ca2+ and forward Na(+)-Ca2+ exchange and shows that this site regulates both the transient and stationary current. The temperature dependence of the stationary current exhibits an activation energy of 70 kj/mol for temperatures between 21 degrees C and 38 degrees C, and 138 kj/mol between 10 degrees C and 21 degrees C. For the decay time constant an activation energy of 70 kj/mol is observed in the Na(+)-Ca2+ and the Ca(2+)-Ca2+ exchange mode between 13 degrees C and 35 degrees C. The data indicate that partial reactions of the Na(+)-Ca2+ exchanger associated with Ca2+ binding and translocation are very fast at 35 degrees C, with relaxation time constants of about 6700 s-1 in the forward Na(+)-Ca2+ exchange and about 12,500 s-1 in the Ca(2+)-Ca2+ exchange mode and that net negative charge is moved during Ca2+ translocation. According to model calculations, the turnover number, however, has to be at least 2-4 times smaller than the decay rate of the transient current, and Na+ inward translocation appears to be slower than Ca2+ outward movement.     

Effects of external Rb+ on inward rectifier K+ channels of bovine pulmonary artery endothelial cells

Inward rectifier (IR) K+ channels of bovine pulmonary artery endothelial cells were studied using the whole-cell, cell-attached, and outside-out patch-clamp configurations. The effects of Rb+ on the voltage dependence and kinetics of IR gating were explored, with [Rb+]o + [K+]o = 160 mM. Partial substitution of Rb+ for K+ resulted in voltage-dependent reduction of inward currents, consistent with Rb+ being a weakly permeant blocker of the IR. In cells studied with a K(+)- free pipette solution, external Rb+ reduced inward IR currents to a similar extent at large negative potentials but block at more positive potentials was enhanced. In outside-out patches, the single-channel i-V relationship was approximately linear in symmetrical K+, but rectified strongly outwardly in high [Rb+]o due to a reduced conductance for inward current. The permeability of Rb+ based on reversal potential, Vrev, was 0.45 that of K+, whereas the Rb+ conductance was much lower, 0.034 that of K+, measured at Vrev-80 mV. The steady state voltage- dependence of IR gating was determined in Rb(+)-containing solutions by applying variable prepulses, followed by a test pulse to a potential at which outward current deactivation was observed. As [Rb+]o was increased, the half-activation potential, V1/2, changed less than Vrev. In high [K+]o solutions V1/2 was Vrev-6 mV, while in high [Rb+]o V1/2 was Vrev + 7 mV. This behavior contrasts with the classical parallel shift of V1/2 with Vrev in K+ solutions. Steady state IR gating was less steeply voltage-dependent in high [Rb+]o than in K+ solutions, with Boltzmann slope factors of 6.4 and 4.4 mV, respectively. Rb+ decreased (slowed) both activation and deactivation rate constants defined at V1/2, and decreased the steepness of the voltage dependence of the activation rate constant by 42%. Deactivation of IR channels in outside-out patches was also slowed by Rb+. In summary, Rb+ can replace K+ in setting the voltage-dependence of IR gating, but in doing so alters the kinetics.     

Pre-steady-state and steady-state kinetic analysis of the low molecular weight phosphotyrosyl protein phosphatase from bovine heart.

The complete time course of the hydrolysis of p-nitrophenyl phosphate catalyzed by the low molecular weight (acid) phosphotyrosyl protein phosphatase from bovine heart was elucidated and analyzed in detail. Burst titration kinetics were demonstrated for the first time with this class of enzyme. At pH 7.0, 4.5 degrees C, a transient pre-steady-state "burst" of p-nitrophenol was formed with a rate constant of 48 s-1. The burst was effectively stoichiometric and corresponded to a single enzyme active site/molecule. The burst was followed by a slow steady-state turnover of the phosphoenzyme intermediate with a rate constant of 1.2 s-1. Product inhibition studies indicated an ordered uni-bi kinetic scheme for the hydrolysis. Partition experiments conducted for several substrates revealed a constant product ratio. Vmax was constant for these substrates, and the overall rate of hydrolysis was increased greatly in the presence of alcohol acceptors. An enzyme-catalyzed 18O exchange between inorganic phosphate and water was detected and occurred with kcat = 4.47 x 10(-3) s-1 at pH 5.0, 37 degrees C. These results were all consistent with the existence of a phosphoenzyme intermediate in the catalytic pathway and with the breakdown of the intermediate being the rate-limiting step. The true Michaelis binding constant Ks = 6.0 mM, the apparent Km = 0.38 mM, and the rate constants for phosphorylation (k2 = 540 s-1) and dephosphorylation (k3 = 36.5 s-1) were determined under steady-state conditions with p-nitrophenyl phosphate at pH 5.0 and 37 degrees C in the presence of phosphate acceptors. The energies of activation for the enzyme-catalyzed hydrolysis at pH 5.0 and 7.0 were 13.6 and 14.1 kcal/mol, respectively. The activation energy for the enzyme-catalyzed medium 18O exchange between phosphate and water was 20.2 kcal/mol. Using the available equilibrium and rate constants, an energetic diagram was constructed for the enzyme-catalyzed reaction.     

Viscosity dependence of ethidium-DNA intercalation kinetics

The kinetics of ethidium intercalation into double-stranded poly[d(G-C)] were investigated by use of repetitive pressure-jump chemical relaxation at 20 degrees C in low ionic strength (0.1 M NaCl) aqueous buffers containing either glycerol or methanol. The viscosity of the various solvents differed by more than an order of magnitude while other physical properties (e.g., dielectric constant) remained approximately constant. The single-reciprocal kinetic relaxation time (tau -1) increases linearly with DNA concentration. The observed association rate constant is lower in all organic-aqueous mixtures than in water and is inversely proportional to the viscosity. These results provide evidence for an additional step in the intercalation mechanism which is identified as an obligatory DNA conformational change preceding ethidium intercalation. From the data presented, the equilibrium constant of this local conformational change is approximately 10(-3), i.e., greatly favoring the structure incapable of intercalation. The corresponding kinetics were not directly determined; however, in order to be consistent with all of the data the forward and/or reverse rate constants of the conformational change must be larger than the rate of the intercalation reaction. Thus, it is proposed that the rate of the conformational change back to the nonintercalating B-DNA structure is greater than approximately 500 s-1, implying a rate of opening greater than approximately 0.5 s-1, in agreement with other hydrogen exchange and NMR data. The observed overall rate constant for the dissociation of ethidium is inversely proportional to the solvent density, possibly reflecting a dependence on the solvent free volume. The overall volume change of intercalation is less negative in the organic-aqueous solvent mixtures than in water.     

Cadmium block of calcium current in frog sympathetic neurons.

Cd2+ blocks whole-cell calcium currents in frog sympathetic neurons by 50% at approximately 300 nM. Strong depolarizations rapidly reverse that blockade (tau = 1.3 ms at +120 mV). Reblocking follows bimolecular kinetics (rate = 1.2 x 10(8) M-1 s-1) at voltages where channels are mostly open (0 to +30 mV). The unblocking rate is approximately 50 s-1, so the dissociation constant calculated from the rate constants is approximately 400 nM. Steady-state block is strong at -80 mV, so closed channels can also be blocked. However, reblocking is extremely slow (tau = 1-2 s) at voltages where the channels are mostly closed. The rates for Cd2+ entry and exit are greater than 100-fold lower for closed channels than for open channels, and closed channels appear to be closed at both ends.