ATP Binding Steps Research Articles

Unravelling the intricate cooperativity of subunit gating in P2X2 ion channels

Ionotropic purinergic (P2X) receptors are trimeric channels that are activated by the binding of ATP. They are involved in multiple physiological functions, including synaptic transmission, pain and inflammation. The mechanism of activation is still elusive. Here we kinetically unraveled and quantified subunit activation in P2X2 receptors by an extensive global fit approach with four complex and intimately coupled kinetic schemes to currents obtained from wild type and mutated receptors using ATP and its fluorescent derivative 2-[DY-547P1]-AET-ATP (fATP). We show that the steep concentration-activation relationship in wild type channels is caused by a subunit flip reaction with strong positive cooperativity, overbalancing a pronounced negative cooperativity for the three ATP binding steps, that the net probability fluxes in the model generate a marked hysteresis in the activation-deactivation cycle, and that the predicted fATP binding matches the binding measured by fluorescence. Our results shed light into the intricate activation process of P2X channels.

Tracking the 3D Rotational Dynamics in Nanoscopic Biological Systems.

The rotation of an object cannot be fully tracked without understanding a set of three angles, namely, roll, pitch, and yaw. Tracking these angles as a three-degrees-of-freedom (3-DoF) rotation is a fundamental measurement, facilitating, for example, attitude control of a ship, image stabilization to reduce camera shake, and self-driving cars. Until now, however, there has been no method to track 3-DoF rotation to measure nanometer-scale dynamics in biomolecules and live cells. Here we show that 3-DoF rotation of biomolecules can be visualized via nitrogen-vacancy centers in a fluorescent nanodiamond using a tomographic vector magnetometry technique. We demonstrate application of the method to three different types of biological systems. First, we tracked the rotation of a single molecule of the motor protein F1-ATPase by attaching a nanodiamond to the γ-subunit. We visualized the 3-step rotation of the motor in 3D space and, moreover, a delay of ATP binding or ADP release step in the catalytic reaction. Second, we attached a nanodiamond to a membrane protein in live cells to report on cellular membrane dynamics, showing that 3D rotational motion of the membrane protein correlates with intracellular cytoskeletal density. Last, we used the method to track nonrandom motions in the intestine of Caenorhabditis elegans. Collectively, our findings show that the method can record nanoscale 3-DoF rotation in vitro, in cells, and even in vivo. 3-DoF rotation tracking introduces a new perspective on microscopic biological samples, revealing in greater detail the functional mechanisms due to nanoscale dynamics in molecules and cells.

A RecA protein surface required for activation of DNA polymerase V.

DNA polymerase V (pol V) of Escherichia coli is a translesion DNA polymerase responsible for most of the mutagenesis observed during the SOS response. Pol V is activated by transfer of a RecA subunit from the 3'-proximal end of a RecA nucleoprotein filament to form a functional complex called DNA polymerase V Mutasome (pol V Mut). We identify a RecA surface, defined by residues 112-117, that either directly interacts with or is in very close proximity to amino acid residues on two distinct surfaces of the UmuC subunit of pol V. One of these surfaces is uniquely prominent in the active pol V Mut. Several conformational states are populated in the inactive and active complexes of RecA with pol V. The RecA D112R and RecA D112R N113R double mutant proteins exhibit successively reduced capacity for pol V activation. The double mutant RecA is specifically defective in the ATP binding step of the activation pathway. Unlike the classic non-mutable RecA S117F (recA1730), the RecA D112R N113R variant exhibits no defect in filament formation on DNA and promotes all other RecA activities efficiently. An important pol V activation surface of RecA protein is thus centered in a region encompassing amino acid residues 112, 113, and 117, a surface exposed at the 3'-proximal end of a RecA filament. The same RecA surface is not utilized in the RecA activation of the homologous and highly mutagenic RumA'2B polymerase encoded by the integrating-conjugative element (ICE) R391, indicating a lack of structural conservation between the two systems. The RecA D112R N113R protein represents a new separation of function mutant, proficient in all RecA functions except SOS mutagenesis.

Cardiac myosin binding protein C phosphorylation affects cross-bridge cycle's elementary steps in a site-specific manner.

Based on our recent finding that cardiac myosin binding protein C (cMyBP-C) phosphorylation affects muscle contractility in a site-specific manner, we further studied the force per cross-bridge and the kinetic constants of the elementary steps in the six-state cross-bridge model in cMyBP-C mutated transgenic mice for better understanding of the influence of cMyBP-C phosphorylation on contractile functions. Papillary muscle fibres were dissected from cMyBP-C mutated mice of ADA (Ala273-Asp282-Ala302), DAD (Asp273-Ala282-Asp302), SAS (Ser273-Ala282-Ser302), and t/t (cMyBP-C null) genotypes, and the results were compared to transgenic mice expressing wide-type (WT) cMyBP-C. Sinusoidal analyses were performed with serial concentrations of ATP, phosphate (Pi), and ADP. Both t/t and DAD mutants significantly reduced active tension, force per cross-bridge, apparent rate constant (2πc), and the rate constant of cross-bridge detachment. In contrast to the weakened ATP binding and enhanced Pi and ADP release steps in t/t mice, DAD mice showed a decreased ADP release without affecting the ATP binding and the Pi release. ADA showed decreased ADP release, and slightly increased ATP binding and cross-bridge detachment steps, whereas SAS diminished the ATP binding step and accelerated the ADP release step. t/t has the broadest effects with changes in most elementary steps of the cross-bridge cycle, DAD mimics t/t to a large extent, and ADA and SAS predominantly affect the nucleotide binding steps. We conclude that the reduced tension production in DAD and t/t is the result of reduced force per cross-bridge, instead of the less number of strongly attached cross-bridges. We further conclude that cMyBP-C is an allosteric activator of myosin to increase cross-bridge force, and its phosphorylation status modulates the force, which is regulated by variety of protein kinases.

Role of protons in the pump cycle of KdpFABC investigated by time-resolved kinetic experiments.

The time-resolved kinetics of the KdpFABC complex solubilized in Aminoxide WS-35 was investigated by ATP concentration jump experiments. ATP was photoreleased from its inactive precursor, caged ATP, and charge movements in the membrane domain of the KdpFABC were detected by the electrochromic dye RH421. At low ATP concentrations, the ATP binding step became rate-limiting with an apparent, pH-independent ATP binding affinity of ~70 μM. At saturating ATP concentrations, the rate-limiting step is the conformational transition (E1-P → P-E2) with a rate constant of ~1.7 s(-1) at 20 °C that was independent of K(+) concentration. This observation together with the detected fluorescence decrease indicates that K(+) (or another positive ion) is bound in the membrane domain after enzyme phosphorylation and the conformational transition to the P-E2 state. pH dependence experiments revealed different roles of H(+) in the transport mechanism. Two different functions of protons for the ion pump must be distinguished. On one hand, there are electrogenically bound "functional" protons, which are not transported but prerequisite for the performance of the ATP-driven half-cycle. On the other hand, protons bind to the transport sites, acting as weak congeners of K(+). There possibly are noncompetitively bound protons, affecting the enzyme activity and/or coupling between KdpA and KdpB subunits. Finally, the recently proposed Post-Albers model for the KdpFABC complex was supplemented with stoichiometry factors of 2 for K(+) and 3 for H(+), and additional inhibitory side reactions controlled by H(+) were introduced, which are relevant at pH <6.5 and/or in the absence of K(+).

Structural Basis for the ATP-Induced Isomerization of Kinesin

Kinesin superfamily proteins (KIFs) are microtubule-based molecular motors driven by the energy derived from the hydrolysis of ATP. Previous studies have revealed that the ATP binding step is crucial both for the power stroke to produce motility and for the inter-domain regulation of ATPase activity to guarantee the processive movement of dimeric KIFs. Here, we report the first crystal structure of KIF4 complexed with the non-hydrolyzable ATP analog, AMPPNP (adenylyl imidodiphosphate), at 1.7Å resolution. By combining our structure with previously solved KIF1A structures complexed with two ATP analogs, molecular snapshots during ATP binding reveal that the closure of the nucleotide-binding pocket during ATP binding is achieved by closure of the backdoor. Closure of the backdoor stabilizes two mobile regions, switch I and switch II, to generate the phosphate tube from which hydrolyzed phosphate is released. Through the stabilization of switch II, the local conformational change at the catalytic center is further relayed to the neck-linker element that fully docks to the catalytic core to produce the power stroke. Because the neck linker is a sole element that connects the partner heads in dimeric KIFs, this tight structural coordination between the catalytic center and neck linker enables inter-domain communication between the partner heads. This study also revealed the putative microtubule-binding site of KIF4, thus providing structural insights that describe the specific binding of KIF4 to the microtubule.

Cardiac Myosin Binding-Protein C (cMyBP-C) Phosphorylation affect Cross-Bridge Function

To understand the functional significance of phosphorylation that takes place in the M domain of cMyBP-C, chemically skinned papillary muscle fibers of transgenic mice were studied by sinusoidal length alterations and concomitant tension transients. Muscle fibers were maximally activated at pCa 4.55 in the solution that mimic physiological conditions (5 mM MgATP, 8 mM Pi, 200 mM total ionic strength with K-acetate) in myocytes. WT mice possess phosphorylation sites S273, S282, and S302. SAS is a single mutant S282A, and ADA and DAD are triple mutants S273A/S282D/S302A and S273D/S282A/S302D, respectively. D models for phosphorylation (phosphomimetic), and A models for non-phosphorylation (phosphor-ablation). Isometric tension and stiffness of DAD were respectively ∼0.5x of those of WT, but tension and stiffness of t/t (cMyBP-C null), ADA, and SAS were respectively similar to WT. The fast rate constant 2πc of DAD and t/t was ∼0.6x of WT, but that of ADA and SAS was similar to WT. The intermediate rate constant 2πb of DAD and SAS was ∼1.3x of WT, but that of ADA and t/t was similar to WT. These results demonstrate that cMyBP-C M domain phosphorylation affects the cross-bridge kinetics at ATP binding and phosphate release steps, indicating that phosphorylation affects myosin structure and its interaction with actin. However, pCa-tension and pCa-stiffness studies demonstrated that pCa50 (Ca2+ sensitivity) and nH (cooperativity) were respectively not different among mutants and WT groups, indicating that phosphorylation of cMyBP-C has a minimal effect on the regulatory system. The decreased amount of isometric tension only in DAD indicates that phosphorylation of S273 and S302 are most significant and they diminish the force generation capability, presumably owing to the extra electrostatic interaction of the M domain of cMyBP-C with actin thin filament, which may serve as a break.

ATP binding and cross‐bridge detachment steps during full Ca2+ activation: comparison of myofibril and muscle fibre mechanics by sinusoidal analysis

Single myofibrils 50–60 μm length and 2–3 μm diameter were isolated from rabbit psoas muscle fibres, and cross-bridge kinetics were studied by small perturbations of the length (∼0.2%) over a range of 15 frequencies (1–250 Hz). The experiments were performed at 15◦C in the presence of 0.05–10 mM MgATP, 8mM phosphate (Pi), 200 mM ionic strength with KAc (acetate), pCa 4.35–4.65, and pH 7.0. Two exponential processes, B and C, were resolved in tension transients. Their apparent rate constants (2πb and 2πc) increased as the [MgATP] was raised from 0.05 mM to 1mM, and then reached saturation at [MgATP] ≥ 1. Given that these rate constants were similar (c/b ∼1.7) at [Pi] ≥ 4 mM, they were combined to achieve an accurate estimate of the kinetic constants: their sum and product were analysed as functions of [MgATP]. These analyses yielded K1 =2.91 ± 0.31 mM −1, k2 =288 ± 36 s−1, and k−2 =10 ± 21 s−1 (±95% confidence limit, n =13 preparations), based on the cross-bridge model: AM+ATP ↔ (step 1) AM.ATP ↔ (step 2) A+M.ATP, where K1 is the ATP association constant (step 1), k2 is the rate constant of the cross-bridge detachment (step 2), and k−2 is the rate constant of its reversal step. These kinetic constants are respectively comparable to those observed in single fibres from rabbit psoas (K1 =2.35 ± 0.31 mM −1, k2 =243 ± 22 s−1, and k−2 =6 ± 14 s−1; n =8 preparations) when analysed by the same methods and under the same experimental conditions. These values are respectively not significantly different from those obtained in myofibrils, indicating that the same kinetic constants can be deduced from myofibril and muscle fibre studies, in terms of ATP binding and cross-bridge detachments steps. The fact that K1 in myofibrils is 1.2 times that in fibres (P≈0.05) may be explained by a small concentration gradient of ATP, ADP and/or Pi in single fibres.

A Comparison of Single Myofibrils and Single Muscle Fibers from Rabbit Psoas in Terms of MgATP Binding and Cross-Bridge Detachment Steps Studied with Sinusoidal Length Perturbations

Single myofibrils of 40-70 μm in length and 2-4 μm in diameter were isolated from rabbit psoas muscle bundles, and cross-bridge kinetics were studied by small amplitude (0.2%) length perturbations at 15 frequencies (1-250Hz). The experiments were performed at 15°C in the presence of 0.05-10 mM MgATP, 4 mM KH2PO4, 4 mM K2HPO4, 15 mM Na2CP (creatine phosphate), 200 mM ionic strength with KAc (acetate), pCa 4.55, and pH 7.0. Two exponential processes B and C were resolved in tension transients. Their apparent rate constants (2πb and 2πc; b < c) increased ([MgATP]=0.05-1 mM) and saturated (≥1 mM) with an increase in the MgATP concentration. However, they were close together (1.4x) at [Pi]≥4 mM, hence they were combined to deduce the accurate estimate of the kinetic constants: their sum and product were analyzed as functions of [MgATP]. These analyses yielded K1=2.91 ± 0.31 mM−1, k2=288±36 s−1, and k-2=10±21 s−1 (±95% confidence limit, N=13). These results are consistent with the cross-bridge model: AM+ATP <-> (step 1) AM.ATP <-> (step 2) A+M.ATP. These kinetic constants compare to those observed in single fibers (K1=2.35±0.31 mM−1, k2=243±22 s−1, and k-2=6±14 s−1; N=8) under the same experimental conditions and analysis methods. These values are respectively not significantly different from those of myofibrils, indicating that the same kinetic constants can be deduced from myofibril and muscle fiber studies in terms of ATP binding and cross-bridge detachments steps. The fact that in myofibrils K1 is 1.24x of that of fibers, may be explained by a small concentration gradient of ATP, ADP and/or Pi in single fibers.

Mechanical modulation of catalytic power on F1-ATPase

The conformational fluctuation of enzymes has a crucial role in reaction acceleration. However, the contribution to catalysis enhancement of individual substates with conformations far from the average conformation remains unclear. We studied the catalytic power of the rotary molecular motor F(1)-ATPase from thermophilic Bacillus PS3 as it was stalled in transient conformations far from a stable pausing angle. The rate constants of ATP binding and hydrolysis were determined as functions of the rotary angle. Both rates exponentially increase with rotation, revealing the molecular basis of positive cooperativity among three catalytic sites: elementary reaction steps are accelerated via the mechanical rotation driven by other reactions on neighboring catalytic sites. The rate enhancement induced by ATP binding upon rotation was greater than that brought about by hydrolysis, suggesting that the ATP binding step contributes more to torque generation than does the hydrolysis step. Additionally, 9% of the ATP-driven rotary step was supported by thermal diffusion, suggesting that acceleration of the ATP docking process occurs via thermally agitated conformational fluctuations.

Correlation between cross-bridge kinetics obtained from Trp fluorescence of myofibril suspensions and mechanical studies of single muscle fibers in rabbit psoas

Our goal is to correlate kinetic constants obtained from fluorescence studies of myofibril suspension with those from mechanical studies of skinned muscle fibers from rabbit psoas. In myofibril studies, the stopped-flow technique with tryptophan fluorescence was used; in muscle fiber studies, tension transients with small amplitude sinusoidal length perturbations were used. All experiments were performed using the equivalent solution conditions (200mM ionic strength, pH7.00) at 10°C. The concentration of MgATP was varied to characterize kinetic constants of the ATP binding step 1 (K (1): dissociation constant), the binding induced cross-bridge detachment step 2 (k (2), k (-2): rate constants), and the ATP cleavage step 3 (k (3), k (-3)). In myofibrils we found that K (1)=0.52±0.08mM (±95% confidence limits), k (2)=242±24s(-1), and k (-2)≈0; in muscle fibers, K (1)=0.46±0.06mM, k (2)=286±32s(-1), and k (-2)=57±21s(-1). From these results, we conclude that myofibrils and muscle fibers exhibit nearly equal ATP binding step, and nearly equal ATP binding induced cross-bridge detachment step. Consequently, there is a good correlation between process C (phase 2 of step analysis) and the cross-bridge detachment step. The reverse detachment step is finite in fibers, but almost absent in myofibrils. We further studied partially cross-linked myofibrils and found little change in steps 2 and 3, indicating that cross-linking does not affect these steps. However, we found that K (1) is 2.5× of native myofibrils, indicating that MgATP binding is weakened by the presence of the extra load. We further studied the phosphate (Pi) effect in myofibrils, and found that Pi is a competitive inhibitor of MgATP, with the inhibitory dissociation constant of ~9mM. Similar results were also deduced from fiber studies. To characterize the ATP cleavage step in myofibrils, we measured the slow rate constant in fluorescence, and found that k (3)+k (-3)=16±1s(-1).

ATP binding and hydrolysis steps of the uni-site catalysis by the mitochondrial F 1-ATPase are affected by inorganic phosphate

The effect of inorganic phosphate (P i) on uni-site ATP binding and hydrolysis by the nucleotide-depleted F 1-ATPase from beef heart mitochondria (ndMF 1) has been investigated. It is shown for the first time that P i decreases the apparent rate constant of uni-site ATP binding by ndMF 1 3-fold with the K d of 0.38 ± 0.14 mM. During uni-site ATP hydrolysis, P i also shifts equilibrium between bound ATP and ADP + P i in the direction of ATP synthesis with the K d of 0.17 ± 0.03 mM. However, 10 mM P i does not significantly affect ATP binding during multi-site catalysis.

Fluorescence Polarization Analysis for Revealing Molecular Mechanism of Nucleotide-Dependent Phospholipid Membrane Binding of MinD Adenosine 5'-Triphosphate, Adenosine Triphosphatase

Membrane binding of Walker type adenosine 5'-triphosphate, adenosine triphosphatase (ATPase), MinD, is a key step in regulating the site of cell division in Escherichia coli. Two lysine residues (K11, K16) in the Walker A motif of MinD have been suggested to be essential for both membrane binding and ATPase activity, but the relationship between the membrane binding of MinD and its ATPase activity is still unclear. To reveal the role of K11 and K16 in MinD membrane interaction and ATP-binding, we compared the functionality of wild-type MinD (WT) and two MinD mutants that lack ATPase activity, where alanine was substituted for lysine at positions 11 and 16 (K11A, K16A), using liposomes and fluorescent-labeled ATP. The ATP dissociation constant (K(d)) of wild-type MinD was 4.9 µM. Unexpectedly, the K(d) values of the two lysine mutants were almost the same as that of wild type, indicating that ATP can bind to MinD mutants, even though these mutants showed no ATPase activity and membrane binding ability. Our results presumed that K11 and K16 residues might play an important role in dimmer formation of MinD, but not ATP binding step, for recruiting to membrane.

Correlation between Myofibrillar Biochemistry and Muscle Fiber Mechanics using Rabbit Psoas Muscle Preparations Indicates that Phase 2 of Step Analysis Represents the Cross-Bridge Detachment Step

Our goal is to correlate results obtained from myofibrillar suspensions and muscle fibers. For myofibrils, tryptophan fluorescence with stopped-flow apparatus was used; for fibers, tension transients with small amplitude sinusoidal length perturbations were used. Experiments were performed in identical solutions with 0.2M ionic strength at pH 7.00. The concentration of MgATP was varied to detect kinetic constants of the ATP binding step 1 (K1: dissociation constant), the cross-bridge detachment step 2 (k2, k-2: rate constants), and the ATP cleavage step 3 (k3, k-3). By following the fast rate constant at 20°C, we found in myofibrils: k2/K1=1.0∈μM−1s−1, K1=0.3mM, k2=300s−1, and k-2≈0; in fibers: k2/K1=0.23∈μM−1s−1, K1=1.58mM, k2=363s−1, k-2=180s−1. From these results we conclude that (1) ATP binding is ∼5X stronger in myofibrils than in fibers, (2) cross-bridge detachment rate is just about the same, and (3) its reversal step is almost absent in myofibrils, but it is finite in fibers. Consequently, we found a good agreement in the results obtained from myofibrils and fibers, indicating that phase 2 of tension transients from step analysis in fibers (Huxley and Simmons, 1971) represents the cross-bridge detachment step. We also studied actin-myosin cross-linked myofibrils and found no difference, indicating that cross-linking does not significantly modify steps 1-3 kinetics. We further studied the Pi effect in myofibrils, and found that Pi is a competitive inhibitor of MgATP with the inhibitory dissociation constant of 7-8mM. To deduce the kinetic constants of the ATP cleavage step, we measured the slower rate constant in fluorescence in myofibrils and found that k3+k-3=10.7s−1 at 4°C. From the Pi burst experiments using radioactive ATP, we found that K3=6.1 at 4°C. From these, k3=9.2s−1 and k-3=1.50s−1 were deduced.

Functional and structural identification of amino acid residues of the P2X2 receptor channel critical for the voltage‐ and [ATP]‐dependent gating

The extracellular ATP-gated cation channel P2X(2) is known to show voltage-dependent gating in spite of the absence of a canonical voltage sensor domain. We previously observed that the hyperpolarization-evoked activation of P2X(2) at the steady state in the presence of ATP varied depending on [ATP]. With increasing [ATP], the conductance-voltage (G-V) relationship shifted to more depolarized potentials and the activation kinetics were accelerated. Using a three-state model consisting of an ATP binding step and a rate limiting gating step, we successfully reproduced the voltage-dependent gating including its [ATP] dependence. In this study, in order to identify the structural basis of voltage and ATP dependence, we analysed various mutants in the Xenopus oocyte expression system under two-electrode voltage clamp. In the ATP binding region mutant K308R, the G-V relationship was shifted towards more hyperpolarized potentials, there was no clear [ATP] dependence, and activation was faster than in wild-type (WT). These results could be simulated by assuming an increase in the off rate of the gating step, in addition to changes in the ATP binding step. With F44C mutation in the 1st transmembrane (TM) region (TM1) or T339S in TM2, activation in low [ATP] was slow and the channel was constitutively active at all membrane potentials in high [ATP]. These results could be simulated by reducing the off rate of the gating step. Phenotypes of the double mutants, K308R/F44C and K308R/T339S, were similar to WT, suggesting that TM and ATP binding region mutants offset the effect of each other. Analysis of the effects on WT of two other agonists, ADP and AP(4)A, revealed that the electrostatic charge is not the sole critical factor. Taking these results together with the recently reported crystal structure, it was suggested that upon binding of ATP, the occupied binding site indirectly interacts with the extracellular end of the TM regions to trigger conformational changes for gating in a voltage-dependent manner.

Dynamic aspects of functional regulation of the ATP receptor channel P2X2

The P2X(2) channel is a ligand-gated channel activated by ATP. Functional features that reflect the dynamic flexibility of the channel include time-dependent pore dilatation following ATP application and direct inhibitory interaction with activated nicotinic acetylcholine receptors on the membrane. We have been studying the mechanisms by which P2X(2) channel functionality is dynamically regulated. Using a Xenopus oocyte expression system, we observed that the pore properties, including ion selectivity and rectification, depend on the open channel density on the membrane. Pore dilatation was apparent when the open channel density was high and inward rectification was modest. We also observed that P2X(2) channels show voltage dependence, despite the absence of a canonical voltage sensor. At a semi-steady state after ATP application, P2X(2) channels were activated upon membrane hyperpolarization. This voltage-dependent activation was also [ATP] dependent. With increases in [ATP], the speed of hyperpolarization-induced activation was increased and the conductance-voltage relationship was shifted towards depolarized potentials. Based on analyses of experimental data and various simulations, we propose that these phenomena can be explained by assuming a fast ATP binding step and a rate-limiting voltage-dependent gating step. Complete elucidation of these regulatory mechanisms awaits dynamic imaging of functioning P2X(2) channels.

Single-molecule Study on the Temperature-sensitive Reaction of F1-ATPase with a Hybrid F1 Carrying a Single β(E190D)

F1-ATPase is a rotary molecular motor in which the γ-subunit rotates against the α3β3 cylinder. The unitary γ-rotation is a 120° step comprising 80 and 40° substeps, each of these initiated by ATP binding and ADP release and by ATP hydrolysis and inorganic phosphate release, respectively. In our previous study on γ-rotation at low temperatures, a highly temperature-sensitive (TS) reaction step of F1-ATPase from thermophilic Bacillus PS3 was found below 9 °C as an intervening pause before the 80° substep at the same angle for ATP binding and ADP release. However, it remains unclear as to which reaction step the TS reaction corresponds. In this study, we found that the mutant F1(βE190D) from thermophilic Bacillus PS3 showed a clear pause of the TS reaction below 18 °C. In an attempt to identify the catalytic state of the TS reaction, the rotation of the hybrid F1, carrying a single copy of βE190D, was observed at 18 °C. The hybrid F1 showed a pause of the TS reaction at the same angle as for the ATP binding of the incorporated βE190D, although kinetic analysis revealed that the TS reaction is not the ATP binding step. These findings suggest that the TS reaction is a structural rearrangement of β before or after ATP binding.

Voltage- and [ATP]-dependent Gating of the P2X2 ATP Receptor Channel

P2X receptors are ligand-gated cation channels activated by extracellular adenosine triphosphate (ATP). Nonetheless, P2X2 channel currents observed during the steady-state after ATP application are known to exhibit voltage dependence; there is a gradual increase in the inward current upon hyperpolarization. We used a Xenopus oocyte expression system and two-electrode voltage clamp to analyze this “activation” phase quantitatively. We characterized the conductance–voltage relationship in the presence of various [ATP], and observed that it shifted toward more depolarized potentials with increases in [ATP]. By analyzing the rate constants for the channel's transition between a closed and an open state, we showed that the gating of P2X2 is determined in a complex way that involves both membrane voltage and ATP binding. The activation phase was similarly recorded in HEK293 cells expressing P2X2 even by inside-out patch clamp after intensive perfusion, excluding a possibility that the gating is due to block/unblock by endogenous blocker(s) of oocytes. We investigated its structural basis by substituting a glycine residue (G344) in the second transmembrane (TM) helix, which may provide a kink that could mediate “gating.” We found that, instead of a gradual increase, the inward current through the G344A mutant increased instantaneously upon hyperpolarization, whereas a G344P mutant retained an activation phase that was slower than the wild type (WT). Using glycine-scanning mutagenesis in the background of G344A, we could recover the activation phase by introducing a glycine residue into the middle of second TM. These results demonstrate that the flexibility of G344 contributes to the voltage-dependent gating. Finally, we assumed a three-state model consisting of a fast ATP-binding step and a following gating step and estimated the rate constants for the latter in P2X2-WT. We then executed simulation analyses using the calculated rate constants and successfully reproduced the results observed experimentally, voltage-dependent activation that is accelerated by increases in [ATP].

Motor step size and ATP coupling efficiency of the dsDNA translocase EcoR124I

The Type I restriction-modification enzyme EcoR124I is an archetypical helicase-based dsDNA translocase that moves unidirectionally along the 3′–5′ strand of intact duplex DNA. Using a combination of ensemble and single-molecule measurements, we provide estimates of two physicochemical constants that are fundamental to a full description of motor protein activity—the ATP coupling efficiency (the number of ATP consumed per base pair) and the step size (the number of base pairs transported per motor step). Our data indicate that EcoR124I makes small steps along the DNA of 1 bp in length with 1 ATP consumed per step, but with some uncoupling of the ATPase and translocase cycles occurring so that the average number of ATP consumed per base pair slightly exceeds unity. Our observations form a framework for understanding energy coupling in a great many other motors that translocate along dsDNA rather than ssDNA.

A Pre-Steady State Analysis of Ligand Binding to Human Glucokinase: Evidence for a Preexisting Equilibrium

Cooperativity with glucose is a key feature of human glucokinase (GK), allowing its crucial role as a glucose sensor in hepatic and pancreatic cells. We studied the changes in enzyme intrinsic tryptophan fluorescence induced by binding of different ligands to this monomeric enzyme using stopped-flow and equilibrium binding methods. Glucose binding data under pre-steady state conditions suggest that the free enzyme in solution is in a preexisting equilibrium between at least two conformers (super-open and open) which differ in their affinity for glucose (Kd* = 0.17 +/- 0.02 mM and Kd = 73 +/- 18 mM). Increasing the glucose concentration changes the ratio of the two conformers, thus yielding an apparent Kd of 3 mM (different from a Km of 7-10 mM). The rates of conformational transitions of free and GK complexed with sugar are slow and during catalysis are most likely affected by ATP binding, phosphate transfer, and product release steps to allow the kcat to be 60 s-1. The ATP analogue PNP-AMP binds to free GK (super-open) and GK-glucose (open) complexes with comparable affinities (Kd = 0.23 +/- 0.02 and 0.19 +/- 0.08 mM, respectively). However, cooperativity with PNP-AMP observed under equilibrium binding conditions in the presence of glucose (Hill slope of 1.6) is indicative of further complex tightening to the closed conformation. Another physiological modulator (inhibitor), palmitoyl-CoA, binds to GK with similar characteristics, suggesting that conformational changes induced upon ligand binding are not restricted by an active site ligand. In conclusion, our data support control of GK activity and Km through the ratio of distinct conformers (super-open, open, and closed) through either substrate or other ligand binding and/or dissociation.