Purine but not pyrimidine nucleotides support rotation of F(1)-ATPase

Rotary Ion-Translocating ATPases/ATP Synthases: Diversity, Similarities, and Differences

Ion-translocating ATPases and ATP synthases (F-, V-, A-type ATPases, and several P-type ATPases and ABC-transporters) catalyze ATP hydrolysis or ATP synthesis coupled with the ion transport across the membrane. F-, V-, and A-ATPases are protein nanomachines that combine transmembrane transport of protons or sodium ions with ATP synthesis/hydrolysis by means of a rotary mechanism. These enzymes are composed of two multisubunit subcomplexes that rotate relative to each other during catalysis. Rotary ATPases phosphorylate/dephosphorylate nucleotides directly, without the generation of phosphorylated protein intermediates. F-type ATPases are found in chloroplasts, mitochondria, most eubacteria, and in few archaea. V-type ATPases are eukaryotic enzymes present in a variety of cellular membranes, including the plasma membrane, vacuoles, late endosomes, and trans-Golgi cisternae. A-type ATPases are found in archaea and some eubacteria. F- and A-ATPases have two main functions: ATP synthesis powered by the proton motive force (pmf) or, in some prokaryotes, sodium-motive force (smf) and generation of the pmf or smf at the expense of ATP hydrolysis. In prokaryotes, both functions may be vitally important, depending on the environment and the presence of other enzymes capable of pmf or smf generation. In eukaryotes, the primary and the most crucial function of F-ATPases is ATP synthesis. Eukaryotic V-ATPases function exclusively as ATP-dependent proton pumps that generate pmf necessary for the transmembrane transport of ions and metabolites and are vitally important for pH regulation. This review describes the diversity of rotary ion-translocating ATPases from different organisms and compares the structural, functional, and regulatory features of these enzymes.

Motile ghosts of the halophilic archaeon, Haloferax volcanii

Archaea swim using the archaellum (archaeal flagellum), a reversible rotary motor consisting of a torque-generating motor and a helical filament, which acts as a propeller. Unlike the bacterial flagellar motor (BFM), ATP (adenosine-5'-triphosphate) hydrolysis probably drives both motor rotation and filamentous assembly in the archaellum. However, direct evidence is still lacking due to the lack of a versatile model system. Here, we present a membrane-permeabilized ghost system that enables the manipulation of intracellular contents, analogous to the triton model in eukaryotic flagella and gliding Mycoplasma We observed high nucleotide selectivity for ATP driving motor rotation, negative cooperativity in ATP hydrolysis, and the energetic requirement for at least 12 ATP molecules to be hydrolyzed per revolution of the motor. The response regulator CheY increased motor switching from counterclockwise (CCW) to clockwise (CW) rotation. Finally, we constructed the torque-speed curve at various [ATP]s and discuss rotary models in which the archaellum has characteristics of both the BFM and F₁-ATPase. Because archaea share similar cell division and chemotaxis machinery with other domains of life, our ghost model will be an important tool for the exploration of the universality, diversity, and evolution of biomolecular machinery.

Tight Chemomechanical Coupling of the F1 Motor Relies on Structural Stability

The F₁ motor is a rotating molecular motor that ensures a tight chemomechanical coupling between ATP hydrolysis/synthesis reactions and rotation steps. However, the mechanism underlying this tight coupling remains to be elucidated. In this study, we used electrorotation in single-molecule experiments using an F₁βE190D mutant to demonstrate that the stall torque was significantly smaller than the wild-type F₁, indicating a loose coupling of this mutant, despite showing similar stepping torque as the wild-type. Experiments on the ATPase activity after heat treatment and gel filtration of the α₃β₃-subcomplex revealed the unstable structure of the βE190D mutant. Our results suggest that the tight chemomechanical coupling of the F₁ motor relies on the structural stability of F₁. We also discuss the difference between the stepping torque and the stall torque.

Application of the fluctuation theorem to motor proteins: from F1-ATPase to axonal cargo transport by kinesin and dynein

The fluctuation theorem is a representative theorem in non-equilibrium statistical physics actively studied in the 1990s. Relating to entropy production in non-equilibrium states, the theorem has been used to estimate the driving power of motor proteins from fluctuation in their motion. In this review, usage of the fluctuation theorem in experiments on motor proteins is illustrated for biologists, especially those who study mechanobiology, in which force measurement is a central issue. We first introduce the application of the fluctuation theorem in measuring the rotary torque of the rotary motor protein F1-ATPase. Next, as an extension of this application, a recent trial estimating the force generated during cargo transport in vivo by the microtubule motors kinesin and dynein is introduced. Elucidation of the physical mechanism of such transport is important, especially for neurons, in which deficits in cargo transport are deeply related to neuronal diseases. Finally, perspectives on the fluctuation theorem as a new technique in the field of neuroscience are discussed.

Catalytic robustness and torque generation of the F1-ATPase

The F₁-ATPase is the catalytic portion of the F_oF₁ ATP synthase and acts as a rotary molecular motor when it hydrolyzes ATP. Two decades have passed since the single-molecule rotation assay of F₁-ATPase was established. Although several fundamental issues remain elusive, basic properties of F-type ATPases as motor proteins have been well characterized, and a large part of the reaction scheme has been revealed by the combination of extensive structural, biochemical, biophysical, and theoretical studies. This review is intended to provide a concise summary of the fundamental features of F₁-ATPases, by use of the well-described model F₁ from the thermophilic Bacillus PS3 (TF₁). In the last part of this review, we focus on the robustness of the rotary catalysis of F₁-ATPase to provide a perspective on the re-designing of novel molecular machines.

Torque generation mechanism of F1-ATPase upon NTP binding

Molecular machines fueled by NTP play pivotal roles in a wide range of cellular activities. One common feature among NTP-driven molecular machines is that NTP binding is a major force-generating step among the elementary reaction steps comprising NTP hydrolysis. To understand the mechanism in detail,in this study, we conducted a single-molecule rotation assay of the ATP-driven rotary motor protein F1-ATPase using uridine triphosphate (UTP) and a base-free nucleotide (ribose triphosphate) to investigate the impact of a pyrimidine base or base depletion on kinetics and force generation. Although the binding rates of UTP and ribose triphosphate were 10(3) and 10(6) times, respectively, slower than that of ATP, they supported rotation, generating torque comparable to that generated by ATP. Affinity change of F1 to UTP coupled with rotation was determined, and the results again were comparable to those for ATP, suggesting that F1 exerts torque upon the affinity change to UTP via rotation similar to ATP-driven rotation. Thus, the adenine-ring significantly enhances the binding rate, although it is not directly involved in force generation. Taking into account the findings from another study on F1 with mutated phosphate-binding residues, it was proposed that progressive bond formation between the phosphate region and catalytic residues is responsible for the rotation-coupled change in affinity.

Fo-driven Rotation in the ATP Synthase Direction against the Force of F1 ATPase in the FoF1 ATP Synthase

Living organisms rely on the FoF1 ATP synthase to maintain the non-equilibrium chemical gradient of ATP to ADP and phosphate that provides the primary energy source for cellular processes. How the Fo motor uses a transmembrane electrochemical ion gradient to create clockwise torque that overcomes F1 ATPase-driven counterclockwise torque at high ATP is a major unresolved question. Using single FoF1 molecules embedded in lipid bilayer nanodiscs, we now report the observation of Fo-dependent rotation of the c10 ring in the ATP synthase (clockwise) direction against the counterclockwise force of ATPase-driven rotation that occurs upon formation of a leash with Fo stator subunit a. Mutational studies indicate that the leash is important for ATP synthase activity and support a mechanism in which residues aGlu-196 and cArg-50 participate in the cytoplasmic proton half-channel to promote leash formation.

High-speed angle-resolved imaging of a single gold nanorod with microsecond temporal resolution and one-degree angle precision

We developed two types of high-speed angle-resolved imaging methods for single gold nanorods (SAuNRs) using objective-type vertical illumination dark-field microscopy and a high-speed CMOS camera to achieve microsecond temporal and one-degree angle resolution. These methods are based on: (i) an intensity analysis of focused images of SAuNR split into two orthogonally polarized components and (ii) the analysis of defocused SAuNR images. We determined the angle precision (statistical error) and accuracy (systematic error) of the resultant SAuNR (80 nm × 40 nm) images projected onto a substrate surface (azimuthal angle) in both methods. Although both methods showed a similar precision of ∼1° for the azimuthal angle at a 10 μs temporal resolution, the defocused image analysis showed a superior angle accuracy of ∼5°. In addition, the polar angle was also determined from the defocused SAuNR images with a precision of ∼1°, by fitting with simulated images. By taking advantage of the defocused image method's full revolution measurement range in the azimuthal angle, the rotation of the rotary molecular motor, F1-ATPase, was measured with 3.3 μs temporal resolution. The time constants of the pauses waiting for the elementary steps of the ATP hydrolysis reaction and the torque generated in the mechanical steps have been successfully estimated. The high-speed angle-resolved SAuNR imaging methods will be applicable to the monitoring of the fast conformational changes of many biological molecular machines.

Robustness of the rotary catalysis mechanism of F1-ATPase

F1-ATPase (F1) is the rotary motor protein fueled by ATP hydrolysis. Previous studies have suggested that three charged residues are indispensable for catalysis of F1 as follows: the P-loop lysine in the phosphate-binding loop, GXXXXGK(T/S); a glutamic acid that activates water molecules for nucleophilic attack on the γ-phosphate of ATP (general base); and an arginine directly contacting the γ-phosphate (arginine finger). These residues are well conserved among P-loop NTPases. In this study, we investigated the role of these charged residues in catalysis and torque generation by analyzing alanine-substituted mutants in the single-molecule rotation assay. Surprisingly, all mutants continuously drove rotary motion, even though the rotational velocity was at least 100,000 times slower than that of wild type. Thus, although these charged residues contribute to highly efficient catalysis, they are not indispensable to chemo-mechanical energy coupling, and the rotary catalysis mechanism of F1 is far more robust than previously thought.

Role of the DELSEED loop in torque transmission of F1-ATPase

F(1)-ATPase is an ATP-driven rotary motor that generates torque at the interface between the catalytic β-subunits and the rotor γ-subunit. The β-subunit inwardly rotates the C-terminal domain upon nucleotide binding/dissociation; hence, the region of the C-terminal domain that is in direct contact with γ-termed the DELSEED loop-is thought to play a critical role in torque transmission. We substituted all the DELSEED loop residues with alanine to diminish specific DELSEED loop-γ interactions and with glycine to disrupt the loop structure. All the mutants rotated unidirectionally with kinetic parameters comparable to those of the wild-type F(1), suggesting that the specific interactions between DELSEED loop and γ is not involved in cooperative interplays between the catalytic β-subunits. Glycine substitution mutants generated half the torque of the wild-type F(1), whereas the alanine mutant generated comparable torque. Fluctuation analyses of the glycine/alanine mutants revealed that the γ-subunit was less tightly held in the α(3)β(3)-stator ring of the glycine mutant than in the wild-type F(1) and the alanine mutant. Molecular dynamics simulation showed that the DELSEED loop was disordered by the glycine substitution, whereas it formed an α-helix in the alanine mutant. Our results emphasize the importance of loop rigidity for efficient torque transmissions.

Controlled rotation of the F₁-ATPase reveals differential and continuous binding changes for ATP synthesis

F₁-ATPase is an ATP-driven rotary molecular motor that synthesizes ATP when rotated in reverse. To elucidate the mechanism of ATP synthesis, we imaged binding and release of fluorescently labelled ADP and ATP while rotating the motor in either direction by magnets. Here we report the binding and release rates for each of the three catalytic sites for 360° of the rotary angle. We show that the rates do not significantly depend on the rotary direction, indicating ATP synthesis by direct reversal of the hydrolysis-driven rotation. ADP and ATP are discriminated in angle-dependent binding, but not in release. Phosphate blocks ATP binding at angles where ADP binding is essential for ATP synthesis. In synthesis rotation, the affinity for ADP increases by >10⁴, followed by a shift to high ATP affinity, and finally the affinity for ATP decreases by >10⁴. All these angular changes are gradual, implicating tight coupling between the rotor angle and site affinities.

Reverse rotation of the F1-ATPase results in the synthesis, rather than hydrolysis of ATP. Adachi et al. show that the molecular mechanism of ATP synthesis is the reverse of hydrolysis-driven rotation of the motor, and that ADP and ATP are discriminated by angle-dependent binding.

Measurements of the driving forces of bio-motors using the fluctuation theorem

The fluctuation theorem (FT), which is a recent achievement in non-equilibrium statistical mechanics, has been suggested to be useful for measuring the driving forces of motor proteins. As an example of this application, we performed single-molecule experiments on F₁-ATPase, which is a rotary motor protein, in which we measured its rotary torque by taking advantage of FT. Because fluctuation is inherent nature in biological small systems and because FT is a non-destructive force measurement method using fluctuation, it will be applied to a wide range of biological small systems in future.

Characteristics of protection by MgADP and MgATP of α3β3γ subcomplex of thermophilic Bacillus PS3 βY341W-mutant F1-ATPase from inhibition by 7-chloro-4-nitrobenz-2-oxa-1,3-diazole support a bi-site mechanism of catalysis

MgADP and MgATP binding to catalytic sites of βY341W-α(3)β(3)γ subcomplex of F(1)-ATPase from thermophilic Bacillus PS3 has been assessed using their effect on the enzyme inhibition by 7-chloro-4-nitrobenz-2-oxa-1,3-diazole (NBD-Cl). It was assumed that NBD-Cl can inhibit only when catalytic sites are empty, and inhibition is prevented if a catalytic site is occupied with a nucleotide. In the absence of an activator, MgADP and MgATP protect βY341W-α(3)β(3)γ subcomplex from inhibition by NBD-Cl by binding to two catalytic sites with an affinity of 37 µM and 12 mM, and 46 µM and 15 mM, respectively. In the presence of an activator lauryldimethylamine-N-oxide (LDAO), MgADP protects βY341W-α(3)β(3)γ subcomplex from inhibition by NBD-Cl by binding to a catalytic site with a K(d) of 12 mM. Nucleotide binding to a catalytic site with affinity in the millimolar range has not been previously revealed in the fluorescence quenching experiments with βY341W-α(3)β(3)γ subcomplex. In the presence of activators LDAO or selenite, MgATP protects βY341W-α(3)β(3)γ subcomplex from inhibition by NBD-Cl only partially, and the enzyme remains sensitive to inhibition by NBD-Cl even at MgATP concentrations that are saturating for ATPase activity. The results support a bi-site mechanism of catalysis by F(1)-ATPases.

Principal role of the arginine finger in rotary catalysis of F1-ATPase

F(1)-ATPase (F(1)) is an ATP-driven rotary motor wherein the γ subunit rotates against the surrounding α(3)β(3) stator ring. The 3 catalytic sites of F(1) reside on the interface of the α and β subunits of the α(3)β(3) ring. While the catalytic residues predominantly reside on the β subunit, the α subunit has 1 catalytically critical arginine, termed the arginine finger, with stereogeometric similarities with the arginine finger of G-protein-activating proteins. However, the principal role of the arginine finger of F(1) remains controversial. We studied the role of the arginine finger by analyzing the rotation of a mutant F(1) with a lysine substitution of the arginine finger. The mutant showed a 350-fold longer catalytic pause than the wild-type; this pause was further lengthened by the slowly hydrolyzed ATP analog ATPγS. On the other hand, the mutant F(1) showed highly unidirectional rotation with a coupling ratio of 3 ATPs/turn, the same as wild-type, suggesting that cooperative torque generation by the 3 β subunits was not impaired. The hybrid F(1) carrying a single copy of the α mutant revealed that the reaction step slowed by the mutation occurs at +200° from the binding angle of the mutant subunit. Thus, the principal role of the arginine finger is not to mediate cooperativity among the catalytic sites, but to enhance the rate of the ATP cleavage by stabilizing the transition state of ATP hydrolysis. Lysine substitution also caused frequent pauses because of severe ADP inhibition, and a slight decrease in ATP-binding rate.

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.

Modulation of nucleotide specificity of thermophilic F(o)F(1)-ATP Synthase by epsilon-subunit

The C-terminal two α-helices of the ε-subunit of thermophilic Bacillus F(o)F(1)-ATP synthase (TF(o)F(1)) adopt two conformations: an extended long arm ("up-state") and a retracted hairpin ("down-state"). As ATP becomes poor, ε changes the conformation from the down-state to the up-state and suppresses further ATP hydrolysis. Using TF(o)F(1) expressed in Escherichia coli, we compared TF(o)F(1) with up- and down-state ε in the NTP (ATP, GTP, UTP, and CTP) synthesis reactions. TF(o)F(1) with the up-state ε was achieved by inclusion of hexokinase in the assay and TF(o)F(1) with the down-state ε was represented by εΔc-TF(o)F(1), in which ε lacks C-terminal helices and hence cannot adopt the up-state under any conditions. The results indicate that TF(o)F(1) with the down-state ε synthesizes GTP at the same rate of ATP, whereas TF(o)F(1) with the up-state ε synthesizes GTP at a half-rate. Though rates are slow, TF(o)F(1) with the down-state ε even catalyzes UTP and CTP synthesis. Authentic TF(o)F(1) from Bacillus cells also synthesizes ATP and GTP at the same rate in the presence of adenosine 5'-(β,γ-imino)triphosphate (AMP-PNP), an ATP analogue that has been known to stabilize the down-state. NTP hydrolysis and NTP-driven proton pumping activity of εΔc-TF(o)F(1) suggests similar modulation of nucleotide specificity in NTP hydrolysis. Thus, depending on its conformation, ε-subunit modulates substrate specificity of TF(o)F(1).

Fluctuation theorem applied to F1-ATPase

In recent years, theories of nonequilibrium statistical mechanics such as the fluctuation theorem (FT) and the Jarzynski equality have been experimentally applied to micro and nanosized systems. However, so far, these theories are seldom applied to autonomous systems such as motor proteins. In particular, representing the property of entropy production in a small system driven out of equilibrium, FT seems suitable to be applied to them. Hence, for the first time, we employed FT in the single molecule experiments of the motor protein F1-adenosine triphosphatase (F1), in which the rotor γ subunit rotates in the stator α3β3 ring upon adenosine triphosphate hydrolysis. We found that FT provided the better estimation of the rotary torque of F1 than the conventional method.

Simple dark-field microscopy with nanometer spatial precision and microsecond temporal resolution

Molecular motors such as kinesin, myosin, and F(1)-ATPase are responsible for many important cellular processes. These motor proteins exhibit nanometer-scale, stepwise movements on micro- to millisecond timescales. So far, methods developed to measure these small and fast movements with high spatial and temporal resolution require relatively complicated experimental systems. Here, we describe a simple dark-field imaging system that employs objective-type evanescent illumination to selectively illuminate a thin layer on the coverslip and thus yield images with high signal/noise ratios. Only by substituting the dichroic mirror in conventional objective-type total internal reflection fluorescence microscope with a perforated mirror, were nanometer spatial precision and microsecond temporal resolution simultaneously achieved. This system was applied to the study of the rotary mechanism of F(1)-ATPase. The fluctuation of a gold nanoparticle attached to the gamma-subunit during catalytic dwell and the stepping motion during torque generation were successfully visualized with 9.1-mus temporal resolution. Because of the simple optics, this system will be applicable to various biophysical studies requiring high spatial and temporal resolution in vitro and also in vivo.

Activation and stiffness of the inhibited states of F1-ATPase probed by single-molecule manipulation

F(1)-ATPase (F(1)), a soluble portion of F(o)F(1)-ATP synthase (F(o)F(1)), is an ATP-driven motor in which gammaepsilon subunits rotate in the alpha(3)beta(3) cylinder. Activity of F(1) and F(o)F(1) from Bacillus PS3 is attenuated by the epsilon subunit in an inhibitory extended form. In this study we observed ATP-dependent transition of epsilon in single F(1) molecules from extended form to hairpin form by fluorescence resonance energy transfer. The results justify the previous bulk experiments and ensure that fraction of F(1) with hairpin epsilon directly determines the fraction of active F(1) at any ATP concentration. Next, mechanical activation and stiffness of epsilon-inhibited F(1) were examined by the forced rotation of magnetic beads attached to gamma. Compared with ADP inhibition, which is another manner of inhibition, rotation by a larger angle was required for the activation from epsilon inhibition when the beads were forced to rotate to ATP hydrolysis direction, and more torque was required to reach the same rotation angle when beads were forced to rotate to ATP synthesis direction. The results imply that if F(o)F(1) is resting in the epsilon-inhibited state, F(o) motor must transmit to gamma a torque larger than expected from thermodynamic equilibrium to initiate ATP synthesis.

Sequential processing from cell lysis to protein assay on a chip enabling the optimization of an F(1)-ATPase single molecule assay condition

We developed an integrated protein assay device, "Single Molecule MicroTAS (SMM)," which enables cell lysis, protein extraction, purification, and activity assay. The assay was achieved at the single-molecule scale for a genetically engineered protein, F(1)-ATPase, which is the smallest known rotary motor. A cell lysis condition, with a wide range of applied voltages (50-250 V) and other optimized values (pulse width: 50 micros; duty: 0.01%; electrode gap: 25 microm; total flow rate: 5 microL min(-1)) provided a high enough protein concentration for the assay. Successively, the protein was extracted and purified by specific binding in a microfluidic channel. During the assay process, the diffusion effect of lysate between a two-phase laminar flow contributes to optimizing the single-molecule assay condition, because the concentration of the original lysate from the E. coli solution is too high to assay. To achieve the most efficient assay condition, the protein diffusion effect on the assay was experimentally and numerically evaluated. The results reveal that, in our experimental conditions, concentrations of F(1) and other contaminated effluents are optimized for the F(1) rotational assay at a channel position. The adenosine triphosphate (ATP)-driven rotation speed measured in the SMM was compatible with that obtained by conventional purification and assay. Such a sequential process from cell lysis to assay proves that the SMM is an example of a sample-in-answer-out system for F(1) protein evaluation.

Modulation of nucleotide binding to the catalytic sites of thermophilic F(1)-ATPase by the epsilon subunit: implication for the role of the epsilon subunit in ATP synthesis

Effect of epsilon subunit on the nucleotide binding to the catalytic sites of F(1)-ATPase from the thermophilic Bacillus PS3 (TF(1)) has been tested by using alpha(3)beta(3)gamma and alpha(3)beta(3)gammaepsilon complexes of TF(1) containing betaTyr341 to Trp substitution. The nucleotide binding was assessed with fluorescence quenching of the introduced Trp. The presence of the epsilon subunit weakened ADP binding to each catalytic site, especially to the highest affinity site. This effect was also observed when GDP or IDP was used. The ratio of the affinity of the lowest to the highest nucleotide binding sites had changed two orders of magnitude by the epsilon subunit. The differences may relate to the energy required for the binding change in the ATP synthesis reaction and contribute to the efficient ATP synthesis.

Temperature dependence of the rotation and hydrolysis activities of F1-ATPase

F₁-ATPase, a water-soluble portion of the enzyme ATP synthase, is a rotary molecular motor driven by ATP hydrolysis. To learn how the kinetics of rotation are regulated, we have investigated the rotational characteristics of a thermophilic F₁-ATPase over the temperature range 4–50°C by attaching a polystyrene bead (or bead duplex) to the rotor subunit and observing its rotation under a microscope. The apparent rate of ATP binding estimated at low ATP concentrations increased from 1.2 × 10⁶ M⁻¹ s⁻¹ at 4°C to 4.3 × 10⁷ M⁻¹ s⁻¹ at 40°C, whereas the torque estimated at 2 mM ATP remained around 40 pN·nm over 4–50°C. The rotation was stepwise at 4°C, even at the saturating ATP concentration of 2 mM, indicating the presence of a hitherto unresolved rate-limiting reaction that occurs at ATP-waiting angles. We also measured the ATP hydrolysis activity in bulk solution at 4–65°C. F₁-ATPase tends to be inactivated by binding ADP tightly. Both the inactivation and reactivation rates were found to rise sharply with temperature, and above 30°C, equilibrium between the active and inactive forms was reached within 2 s, the majority being inactive. Rapid inactivation at high temperatures is consistent with the physiological role of this enzyme, ATP synthesis, in the thermophile.

Identification of the betaTP site in the x-ray structure of F1-ATPase as the high-affinity catalytic site

ATP synthase uses a unique rotary mechanism to couple ATP synthesis and hydrolysis to transmembrane proton translocation. The F(1) subcomplex has three catalytic nucleotide binding sites, one on each beta subunit, with widely differing affinities for MgATP or MgADP. During rotational catalysis, the sites switch their affinities. The affinity of each site is determined by the position of the central gamma subunit. The site with the highest nucleotide binding affinity is catalytically active. From the available x-ray structures, it is not possible to discern the high-affinity site. Using fluorescence resonance energy transfer between tryptophan residues engineered into gamma and trinitrophenyl nucleotide analogs on the catalytic sites, we were able to determine that the high-affinity site is close to the C-terminal helix of gamma, but at considerable distance from its N terminus. Thus, the beta(TP) site in the x-ray structure [Abrahams JP, Leslie AGW, Lutter R, Walker JE (1994) Nature 370:621-628] is the high-affinity site, in agreement with the prediction of Yang et al. [Yang W, Gao YQ, Cui Q, Ma J, Karplus M (2003) Proc Natl Acad Sci USA 100:874-879]. Taking into account the known direction of rotation, the findings establish the sequence of affinities through which each catalytic site cycles during MgATP hydrolysis as low --> high --> medium --> low.

F1-ATPase: a highly coupled reversible rotary motor

F1 (F1-ATPase) is a highly coupled rotary molecular motor and hydrolyses three ATP molecules per turn (3 ATP/turn). Recently, we have developed femtolitre reaction chamber arrays for highly sensitive measurement of biological reactions. By combining this technique with the rotating magnetic tweezers, the coupling ratio of the reverse reaction, ATP synthesis catalysed by single F1 molecules, has been investigated. The low coupling ratio of 10% (0.3 ATP/turn), catalysed by the alpha3beta3gamma subcomplex of F1, was significantly improved to 77% (2.3 ATP/turn) after reconstitution of the epsilon subunit. This result revealed the novel function of the epsilon subunit as a coupling factor of ATP synthesis catalysed by F1. The possible mechanism for highly coupled ATP synthesis supported by the epsilon subunit is discussed.

Single-molecule observation of rotation of F1-ATPase through microbeads

F(o)F(1)-ATP synthase catalyzes the synthesis of ATP using proton-motive force across a membrane. When isolated, the F1 sector, composed of five polypeptide chains with a stoichiometry of alpha(3)beta(3)gammadeltaepsilon, solely hydrolyzes ATP into ADP and phosphate, and is thus called F(1)-ATPase. Rotation of a shaft domain in F(o)F(1)-ATP synthase has been hypothesized by Paul Boyer, and ultimately was confirmed by direct observation as rotation of the gamma-subunit in an isolated alpha(3)beta(3)gamma subcomplex. Unitary turnover of ATP induces 120 degrees steps, consistent with the configuration of three catalytic sites arranged 120 degrees apart around gamma. We have shown the relationships between chemical and mechanical events by imaging individual F(1) molecules under an optical microscope. A new scheme emerges: as soon as a catalytic site binds ATP, the gamma-subunit always turns the same face (interaction surface) to the beta hosting that site; approximately 80 degrees rotation is driven by ATP binding; approximately 40 degrees rotation is induced by completion of hydrolysis [and/or phosphate release] in the site that bound ATP one step earlier.

Single molecule energetics of F1-ATPase motor

Motor proteins are essential in life processes because they convert the free energy of ATP hydrolysis to mechanical work. However, the fundamental question on how they work when different amounts of free energy are released after ATP hydrolysis remains unanswered. To answer this question, it is essential to clarify how the stepping motion of a motor protein reflects the concentrations of ATP, ADP, and P(i) in its individual actions at a single molecule level. The F(1) portion of ATP synthase, also called F(1)-ATPase, is a rotary molecular motor in which the central gamma-subunit rotates against the alpha(3)beta(3) cylinder. The motor exhibits clear step motion at low ATP concentrations. The rotary action of this motor is processive and generates a high torque. These features are ideal for exploring the relationship between free energy input and mechanical work output, but there is a serious problem in that this motor is severely inhibited by ADP. In this study, we overcame this problem of ADP inhibition by introducing several mutations while retaining high enzymatic activity. Using a probe of attached beads, stepping rotation against viscous load was examined at a wide range of free energy values by changing the ADP concentration. The results showed that the apparent work of each individual step motion was not affected by the free energy of ATP hydrolysis, but the frequency of each individual step motion depended on the free energy. This is the first study that examined the stepping motion of a molecular motor at a single molecule level with simultaneous systematic control of DeltaG(ATP). The results imply that microscopically defined work at a single molecule level cannot be directly compared with macroscopically defined free energy input.

Dynamic and coordinating domain motions in the active subunits of the F1-ATPase molecular motor

F1-ATPase is a rotary molecular motor crucial for various cellular functions. In F1-ATPase, the rotation of the gammadeltaepsilon subunits against the hexameric alpha(3)beta(3) subunits is highly coordinative, driven by ATP hydrolysis and structural changes at three beta subunits. However, the dynamical and coordinating structural transitions in the beta subunits are not fully understood at the molecular level. Here we examine structural transitions and domain motions in the active subunits of F1-ATPase via dynamical domain analysis of the alpha(3)beta(3)gammadeltaepsilon complex. The domain movement and hinge axes and bending residues have been identified and determined for various conformational changes of the beta-subunits. P-loop and the ATP-binding pocket are for the first time found to play essential mechanical functions additional to the catalytic roles. The cooperative conformational changes pertaining to the rotary mechanism of F1-ATPase appears to be more complex than Boyer's 'bi-site' activity. These findings provide unique molecular insights into dynamic and cooperative domain motions in F1-ATPase.

The rotor tip inside a bearing of a thermophilic F1-ATPase is dispensable for torque generation

F(1)-ATPase is an ATP-driven rotary molecular motor in which the central gamma-subunit rotates inside a stator cylinder made of alpha(3)beta(3) subunits. To elucidate the role of rotor-stator interactions in torque generation, we truncated the gamma-subunit at its carboxyl terminus, which forms an alpha helix that penetrates deeply into the stator cylinder. We used an alpha(3)beta(3)gamma subcomplex of F(1)-ATPase derived from thermophilic Bacillus PS3 and expressed it in Escherichia coli. We could obtain purified subcomplexes in which 14, 17, or 21 amino-acid residues were deleted. The rotary characteristics of the truncated mutants, monitored by attaching a duplex of 0.49-microm beads to the gamma-subunit, did not differ greatly from those of the wild-type over the ATP concentrations of 20 nM-2 mM, the most conspicuous effect being approximately 50% reduction in torque and approximately 70% reduction in the rate of ATP binding upon deletion of 21 residues. The ATP hydrolysis activity estimated in bulk samples was more seriously affected. The 21-deletion mutant, in particular, was >10-fold less active, but this is likely due to instability of this subcomplex. For torque generation, though not for rapid catalysis, most of the rotor-stator contacts on the deeper half of the penetrating portion of the gamma-subunit are dispensable.

The transmembrane domain provides nucleotide binding specificity to the bacterial conjugation protein TrwB

In order to understand the functional significance of the transmembrane domain of TrwB, an integral membrane protein involved in bacterial conjugation, the protein was purified in the native, and also as a truncated soluble form (TrwBDeltaN70). The intact protein (TrwB) binds preferentially purine over pyrimidine nucleotides, NTPs over NDPs, and ribo- over deoxyribonucleotides. In contrast, TrwBDeltaN70 binds uniformly all tested nucleotides. The transmembrane domain has the general effect of making the nucleotide binding site(s) less accessible, but more selective. This is in contrast to other membrane proteins in which most of the protein mass, including the catalytic domain, is outside the membrane, but whose activity is not modified by the presence or absence of the transmembrane segment.

Real-time monitoring of conformational dynamics of the epsilon subunit in F1-ATPase

It has been proposed that C-terminal two alpha-helices of the epsilon subunit of F1-ATPase can undergo conformational transition between retracted folded-hairpin form and extended form. Here, using F(1) from thermophilic Bacillus PS3, we monitored this transition in real time by fluorescence resonance energy transfer (FRET) between a donor dye and an acceptor dye attached to N terminus of the gamma subunit and C terminus of the epsilon subunit, respectively. High FRET (extended form) of F1 turned to low FRET (retracted form) by ATP, which then reverted as ATP was hydrolyzed to ADP. 5'-Adenyl-beta,gamma-imidodiphosphate, ADP + AlF4-, ADP + NaN3, and GTP also caused the retracted form, indicating that ATP binding to the catalytic beta subunits induces the transition. The ATP-induced transition from high FRET to low FRET occurred in a similar time scale to the ATP-induced activation of ATPase from inhibition by the epsilon subunit, although detailed kinetics were not the same. The transition became faster as temperature increased, but the extrapolated rate at 65 degrees C (physiological temperature of Bacillus PS3) was still too slow to assign the transition as an obligate step in the catalytic turnover. Furthermore, binding affinity of ATP to the isolated epsilon subunit was weakened as temperature increased, and the dissociation constant extrapolated to 65 degrees C reached to 0.67 mm, a consistent value to assume that the epsilon subunit acts as a sensor of ATP concentration in the cell.

Purification and characterization of the N-terminal domain of ExeA: a novel ATPase involved in the type II secretion pathway of Aeromonas hydrophila

Aeromonas hydrophila secretes a number of degradative enzymes and toxins into the external milieu via the type II secretory pathway or secreton. ExeA is an essential component of this system and is necessary for the localization and/or multimerization of the secretin ExeD. ExeA contains two sequence motifs characteristic of the Walker superfamily of ATPases. Previous examination of substitution derivatives altered in these motifs suggested that ATP binding or hydrolysis is required for ExeAB complex formation and subsequent secretion function. To directly examine ExeA function, the N-terminal cytoplasmic domain of ExeA with the addition of a C-terminal hexahistidine tag (cytExeA) was overproduced in Escherichia coli and purified by metal chelate affinity and anion-exchange chromatographic techniques. Purified preparations of cytExeA exhibited ATPase activity in the presence of several divalent cations, Mg2+ being the preferred cation, with an optimum reaction temperature of approximately 37 to 42 degrees C and an optimum pH of 7 to 8. cytExeA exhibited an apparent K(m) for Mg-ATP of 0.22 mM and a V(max) of 0.72 nmol min(-1) mg(-1) of protein. cytExeA displayed low specificity for nucleoside triphosphate substrates and was significantly inhibited by F-type ATPase inhibitors. Gel filtration analyses of cytExeA, ExeA, and ExeAB indicated that ExeA dimerizes and forms a very large complex with ExeB. These findings support a model whereby ExeAB utilizes energy derived from ATP hydrolysis to facilitate the correct localization and multimerization of the ExeD secretin.

Activation of pausing F1 motor by external force

A rotary motor F(1), a catalytic part of ATP synthase, makes a 120 degrees step rotation driven by hydrolysis of one ATP, which consists of 80 degrees and 40 degrees substeps initiated by ATP binding and probably by ADP and/or P(i) dissociation, respectively. During active rotations, F(1) spontaneously fails in ADP release and pauses after a 80 degrees substep, which is called the ADP-inhibited form. In the present work, we found that, when pushed >+40 degrees with magnetic tweezers, the pausing F(1) resumes its active rotation after releasing inhibitory ADP. The rate constant of the mechanical activation exponentially increased with the pushed angle, implying that F(1) weakens the affinity of its catalytic site for ADP as the angle goes forward. This finding explains not only its unidirectional nature of rotation, but also its physiological function in ATP synthesis; it would readily bind ADP from solution when rotated backward by an F(o) motor in the ATP synthase. Furthermore, the mechanical work for the forced rotation was efficiently converted into work for expelling ADP from the catalytic site, supporting the tight coupling between the rotation and catalytic event.

Highly coupled ATP synthesis by F1-ATPase single molecules

F1-ATPase is the smallest known rotary motor, and it rotates in an anticlockwise direction as it hydrolyses ATP. Single-molecule experiments point towards three catalytic events per turn, in agreement with the molecular structure of the complex. The physiological function of F1 is ATP synthesis. In the ubiquitous F0F1 complex, this energetically uphill reaction is driven by F0, the partner motor of F1, which forces the backward (clockwise) rotation of F1, leading to ATP synthesis. Here, we have devised an experiment combining single-molecule manipulation and microfabrication techniques to measure the yield of this mechanochemical transformation. Single F1 molecules were enclosed in femtolitre-sized hermetic chambers and rotated in a clockwise direction using magnetic tweezers. When the magnetic field was switched off, the F1 molecule underwent anticlockwise rotation at a speed proportional to the amount of synthesized ATP. At 10 Hz, the mechanochemical coupling efficiency was low for the alpha3beta3gamma subcomplex (F1-epsilon)), but reached up to 77% after reconstitution with the epsilon-subunit (F1+epsilon)). We provide here direct evidence that F1 is designed to tightly couple its catalytic reactions with the mechanical rotation. Our results suggest that the epsilon-subunit has an essential function during ATP synthesis.

One rotary mechanism for F1-ATPase over ATP concentrations from millimolar down to nanomolar

F(1)-ATPase is a rotary molecular motor in which the central gamma-subunit rotates inside a cylinder made of alpha(3)beta(3)-subunits. The rotation is driven by ATP hydrolysis in three catalytic sites on the beta-subunits. How many of the three catalytic sites are filled with a nucleotide during the course of rotation is an important yet unsettled question. Here we inquire whether F(1) rotates at extremely low ATP concentrations where the site occupancy is expected to be low. We observed under an optical microscope rotation of individual F(1) molecules that carried a bead duplex on the gamma-subunit. Time-averaged rotation rate was proportional to the ATP concentration down to 200 pM, giving an apparent rate constant for ATP binding of 2 x 10(7) M(-1)s(-1). A similar rate constant characterized bulk ATP hydrolysis in solution, which obeyed a simple Michaelis-Menten scheme between 6 mM and 60 nM ATP. F(1) produced the same torque of approximately 40 pN.nm at 2 mM, 60 nM, and 2 nM ATP. These results point to one rotary mechanism governing the entire range of nanomolar to millimolar ATP, although a switchover between two mechanisms cannot be dismissed. Below 1 nM ATP, we observed less regular rotations, indicative of the appearance of another reaction scheme.

Rotation of F1-ATPase: how an ATP-driven molecular machine may work

F1-ATPase is a rotary motor made of a single protein molecule. Its rotation is driven by free energy obtained by ATP hydrolysis. In vivo, another motor, Fo, presumably rotates the F1 motor in the reverse direction, reversing also the chemical reaction in F1 to let it synthesize ATP. Here we attempt to answer two related questions, How is free energy obtained by ATP hydrolysis converted to the mechanical work of rotation, and how is mechanical work done on F1 converted to free energy to produce ATP? After summarizing single-molecule observations of F1 rotation, we introduce a toy model and discuss its free-energy diagrams to possibly answer the above questions. We also discuss the efficiency of molecular motors in general.

Chemomechanical coupling in F1-ATPase revealed by simultaneous observation of nucleotide kinetics and rotation

F(1)-ATPase is a rotary molecular motor in which unidirectional rotation of the central gamma subunit is powered by ATP hydrolysis in three catalytic sites arranged 120 degrees apart around gamma. To study how hydrolysis reactions produce mechanical rotation, we observed rotation under an optical microscope to see which of the three sites bound and released a fluorescent ATP analog. Assuming that the analog mimics authentic ATP, the following scheme emerges: (i) in the ATP-waiting state, one site, dictated by the orientation of gamma, is empty, whereas the other two bind a nucleotide; (ii) ATP binding to the empty site drives an approximately 80 degrees rotation of gamma; (iii) this triggers a reaction(s), hydrolysis and/or phosphate release, but not ADP release in the site that bound ATP one step earlier; (iv) completion of this reaction induces further approximately 40 degrees rotation.

ATP synthesis driven by proton transport in F1F0-ATP synthase

Topical questions in ATP synthase research are: (1) how do protons cause subunit rotation and how does rotation generate ATP synthesis from ADP+Pi? (2) How does hydrolysis of ATP generate subunit rotation and how does rotation bring about uphill transport of protons? The finding that ATP synthase is not just an enzyme but rather a unique nanomotor is attracting a diverse group of researchers keen to find answers. Here we review the most recent work on rapidly developing areas within the field and present proposals for enzymatic and mechanoenzymatic mechanisms.

Stepping rotation of F(1)-ATPase with one, two, or three altered catalytic sites that bind ATP only slowly

F(1)-ATPase is an ATP hydrolysis-driven motor in which the gamma subunit rotates in the stator cylinder alpha(3)beta(3). To know the coordination of three catalytic beta subunits during catalysis, hybrid F(1)-ATPases, each containing one, two, or three "slow" mutant beta subunits that bind ATP very slowly, were prepared, and the rotations were observed with a single molecule level. Each hybrid made one, two, or three steps per 360 degrees revolution, respectively, at 5 microm ATP where the wild-type enzyme rotated continuously without step under the same observing conditions. The observed dwell times of the steps are explained by the slow binding rate of ATP. Except for the steps, properties of rotation, such as the torque forces exerted during rotary movement, were not significantly changed from those of the wild-type enzyme. Thus, it appears that the presence of the slow beta subunit(s) does not seriously affect other normal beta subunit(s) in the same F(1)-ATPase molecule and that the order of sequential catalytic events is faithfully maintained even when ATP binding to one or two of the catalytic sites is retarded.

The molecular mechanism of ATP synthesis by F1F0-ATP synthase

ATP synthesis by oxidative phosphorylation and photophosphorylation, catalyzed by F1F0-ATP synthase, is the fundamental means of cell energy production. Earlier mutagenesis studies had gone some way to describing the mechanism. More recently, several X-ray structures at atomic resolution have pictured the catalytic sites, and real-time video recordings of subunit rotation have left no doubt of the nature of energy coupling between the transmembrane proton gradient and the catalytic sites in this extraordinary molecular motor. Nonetheless, the molecular events that are required to accomplish the chemical synthesis of ATP remain undefined. In this review we summarize current state of knowledge and present a hypothesis for the molecular mechanism of ATP synthesis.

Bi-site catalysis in F1-ATPase: does it exist?

The mechanism of action of F(1)F(0)-ATP synthase is controversial. Some favor a tri-site mechanism, where substrate must fill all three catalytic sites for activity, others a bi-site mechanism, where one of the three sites is always unoccupied. New approaches were applied to examine this question. First, ITP was used as hydrolysis substrate; lower binding affinities of ITP versus ATP enable more accurate assessment of sites occupancy. Second, distributions of all eight possible enzyme species (with zero, one, two or three sites filled) as fraction of total enzyme population at each ITP concentration were calculated, and compared with measured ITPase activity. Confirming data were obtained with ATP as substrate. Third, we performed a theoretical analysis of possible bi-site mechanisms. The results argue convincingly that bi-site hydrolysis activity is negligible, and may not even exist. Effectively, tri-site hydrolysis is the only mechanism. We argue that only tri-site hydrolysis drives subunit rotation. Theoretical analyses of possible bi-site mechanisms reveal serious flaws, not previously recognized. One is that, in bi-site catalysis, the predicted direction of subunit rotation is the same for both ATP synthesis and hydrolysis; a second is that infrequently occurring enzyme species are required.