The rotary binding change mechanism of ATP synthases

The F(0)F(1) ATP synthase functions as a rotary motor where subunit rotation driven by a current of protons flowing through F(0) drives the binding changes in F(1) that are required for net ATP synthesis. Recent work that has led to the identification of components of the rotor and stator is reviewed. In addition, a model is proposed to describe the transmission of energy from four proton transport steps to the synthesis of one ATP. Finally, some of the requirements for efficient energy coupling by a rotary binding change mechanism are considered.     

Molecular mechanisms of rotational catalysis in the F(0)F(1) ATP synthase

Rotation of the F(0)F(1) ATP synthase gamma subunit drives each of the three catalytic sites through their reaction pathways. The enzyme completes three cycles and synthesizes or hydrolyzes three ATP for each 360 degrees rotation of the gamma subunit. Mutagenesis studies have yielded considerable information on the roles of interactions between the rotor gamma subunit and the catalytic beta subunits. Amino acid substitutions, such as replacement of the conserved gammaMet-23 by Lys, cause altered interactions between gamma and beta subunits that have dramatic effects on the transition state of the steady state ATP synthesis and hydrolysis reactions. The mutations also perturb transmission of specific conformational information between subunits which is important for efficient conversion of energy between rotation and catalysis, and render the coupling between catalysis and transport inefficient. Amino acid replacements in the transport domain also affect the steady state catalytic transition state indicating that rotation is involved in coupling to transport.     

Coupling of rotation and catalysis in F(1)-ATPase revealed by single-molecule imaging and manipulation

F(1)-ATPase is a rotary molecular motor that proceeds in 120 degrees steps, each driven by ATP hydrolysis. How the chemical reactions that occur in three catalytic sites are coupled to mechanical rotation is the central question. Here, we show by high-speed imaging of rotation in single molecules of F(1) that phosphate release drives the last 40 degrees of the 120 degrees step, and that the 40 degrees rotation accompanies reduction of the affinity for phosphate. We also show, by single-molecule imaging of a fluorescent ATP analog Cy3-ATP while F(1) is forced to rotate slowly, that release of Cy3-ADP occurs at approximately 240 degrees after it is bound as Cy3-ATP at 0 degrees . This and other results suggest that the affinity for ADP also decreases with rotation, and thus ADP release contributes part of energy for rotation. Together with previous results, the coupling scheme is now basically complete.     

Nanoseconds molecular dynamics simulation of primary mechanical energy transfer steps in F1-ATP synthase

The mitochondrial membrane protein FoF1-ATP synthase synthesizes adenosine triphosphate (ATP), the universal currency of energy in the cell. This process involves mechanochemical energy transfer from a rotating asymmetric gamma-'stalk' to the three active sites of the F1 unit, which drives the bound ATP out of the binding pocket. Here, the primary structural changes associated with this energy transfer in F1-ATP synthase were studied with multi-nanosecond molecular dynamics simulations. By forced rotation of the gamma-stalk that mimics the effect of proton motive Fo-rotation during ATP synthesis, a time-resolved atomic model for the structural changes in the F1 part in terms of propagating conformational motions is obtained. For these, different time scales are found, which allows the separation of nanosecond from microsecond conformational motions. In the simulations, rotation of the gamma-stalk lowers the ATP affinity of the betaTP binding pocket and triggers fast, spontaneous closure of the empty betaE subunit. The simulations explain several mutation studies and the reduced hydrolysis rate of gamma-depleted F1-ATPase.     

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.     

Asymmetry in the F1-ATPase and its implications for the rotational cycle

ATP synthase uses a rotary mechanism to carry out its cellular function of manufacturing ATP. The central gamma-shaft rotates inside a hexameric cylinder composed of alternating alpha- and beta-subunits. When operating in the hydrolysis direction under high frictional loads and low ATP concentrations, a coordinated mechanochemical cycle in the three catalytic sites of the beta-subunits rotates the gamma-shaft in three 120 degrees steps. At low frictional loads, the 120 degrees steps alternate with three ATP-independent substeps separated by approximately 30 degrees. We present a quantitative model that accounts for these substeps and show that the observed pauses are due to 1), the asymmetry of the F(1) hexamer that produces a propeller-like motion of the power-stroke and 2), the relatively tight binding of ADP to the catalytic sites.     

Rotation and structure of FoF1-ATP synthase

F(o)F(1)-ATP synthase is one of the most ubiquitous enzymes; it is found widely in the biological world, including the plasma membrane of bacteria, inner membrane of mitochondria and thylakoid membrane of chloroplasts. However, this enzyme has a unique mechanism of action: it is composed of two mechanical rotary motors, each driven by ATP hydrolysis or proton flux down the membrane potential of protons. The two molecular motors interconvert the chemical energy of ATP hydrolysis and proton electrochemical potential via the mechanical rotation of the rotary shaft. This unique energy transmission mechanism is not found in other biological systems. Although there are other similar man-made systems like hydroelectric generators, F(o)F(1)-ATP synthase operates on the nanometre scale and works with extremely high efficiency. Therefore, this enzyme has attracted significant attention in a wide variety of fields from bioenergetics and biophysics to chemistry, physics and nanoscience. This review summarizes the latest findings about the two motors of F(o)F(1)-ATP synthase as well as a brief historical background.     

Proton-powered subunit rotation in single membrane-bound F0F1-ATP synthase

Synthesis of ATP from ADP and phosphate, catalyzed by F(0)F(1)-ATP synthases, is the most abundant physiological reaction in almost any cell. F(0)F(1)-ATP synthases are membrane-bound enzymes that use the energy derived from an electrochemical proton gradient for ATP formation. We incorporated double-labeled F(0)F(1)-ATP synthases from Escherichia coli into liposomes and measured single-molecule fluorescence resonance energy transfer (FRET) during ATP synthesis and hydrolysis. The gamma subunit rotates stepwise during proton transport-powered ATP synthesis, showing three distinct distances to the b subunits in repeating sequences. The average durations of these steps correspond to catalytic turnover times upon ATP synthesis as well as ATP hydrolysis. The direction of rotation during ATP synthesis is opposite to that of ATP hydrolysis.     

The chemo-mechanical coupled model for F(1)F(0)-motor

F(1)F(0)-motor (ATP synthase) is the universal enzyme in biological energy conversion that is present in the membranes of mitochondria, chloroplasts and bacteria. It uses the energy of the proton gradient across the membrane to synthesize ATP. Previous theory and model about rotation of the ATP synthase is reviewed, then a novel chemo-mechanical coupled model for rotation of the F(1)F(0)-motor is proposed. In the model, more events are considered simultaneously that includes the movement of F(1), the movement of F(0), reactions at F(1) and reactions at F(0). Using the model, the possible substep modes of the rotation for F(1)F(0) are predicted, the dependence of the motor efficiency and its rotation rate on the rigidity of the γ shaft is investigated. We conclude that the γ shaft has a large rotation rate for a limited driving potential because two ends of the γ shaft can rotate alternately for its flexibility. The flexibility also makes the efficiency of F(1)F(0) drop because elastic twisting deformation power is needed during alternate rotation of the γ shaft at two ends.     

Escherichia coli proton-translocating F0F1-ATP synthase and its association with solute secondary transporters and/or enzymes of anaerobic oxidation-reduction under fermentation

The Escherichia coli proton-translocating F0F1-ATP synthase has a priority in H+ circulation through the membrane in maintaining proton-motive force in the context of ATP synthesis and hydrolysis. Recent advances in the study of this complex under fermentative growth have led to hypothesis that, in the absence of oxidative phosphorylation, F0F1 is implicated as an essential part of H+ movement and ATP hydrolysis, associated with solute secondary transporters and/or enzymes of anaerobic oxidation-reduction. These associations can result from a protein-protein interaction by dithiol-disulfide interchange. In such associations F0F1 has novel functions in bacterial cell physiology.     

ATP synthase motor components: proposal and animation of two dynamic models for stator function

Recent research indicates that ATP synthases (F(0)F(1)) contain two distinct nanomotors, one an electrochemically driven proton motor contained within F(0) that drives an ATP hydrolysis-driven motor (F(1)) in reverse during ATP synthesis. This is depicted in recent models as involving a series of events in which each of the three alphabeta pairs comprising F(1) is induced via a centrally rotating subunit (gamma) to undergo the sequential binding changes necessary to synthesize ATP (binding change mechanism). Stabilization of this rotary process (i.e., to minimize "wobble" of F(1)) is provided in current models by a peripheral stalk or "stator" that has recently been shown to extend from near the bottom of the ATP synthase molecule to the very top of F(1). Although quite elegant, these models envision the stator as fixed during ATP synthesis, i.e., bound to only a single alphabeta pair. This is despite the fact that the binding change mechanism views each alphabeta pair as going through the same sequential order of conformational changes which demonstrate a chemical equivalency among them. For this reason, we propose here two different dynamic models for stator function during ATP synthesis. Both models have been designed to maintain chemical equivalency among the three alphabeta pairs during ATP synthesis and both have been animated.     

Catalytic site forms and controls in ATP synthase catalysis

A suggested minimal scheme for substrate binding by and interconversion of three forms of the catalytic sites of the ATP synthase is presented. Each binding change, that drives simultaneous interchange of the three catalytic site forms, requires a 120 degrees rotation of the gamma with respect to the beta subunits. The binding of substrate(s) at two catalytic sites is regarded as sufficing for near maximal catalytic rates to be attained. Although three sites do not need to be filled for rapid catalysis, during rapid bisite catalysis some enzyme may be transiently present with three sites filled. Forms with preferential binding for ADP and P(i) or for ATP are considered to arise from the transition state and participate in other steps of the catalysis. Intermediate forms and steps that may be involved are evaluated. Experimental evidence for energy-dependent steps and for control of coupling to proton translocation and transition state forms are reviewed. Impact of relevant past data on present understanding of catalytic events is considered. In synthesis a key step is suggested in which proton translocation begins to deform an open site so as to increase the affinity for ADP and P(i), that then bind and pass through the transition state, and yield tightly bound ATP in one binding change. ADP binding appears to be a key parameter controlling rotation during synthesis. In hydrolysis ATP binding to a loose site likely precedes any proton translocation, with proton movement occurring as the tight site form develops. Aspects needing further study are noted. Characteristics of the related MgADP inhibition of the F(1) ATPases that have undermined many observations are summarized, and relations of three-site filling to catalysis are assessed.     

Kinetic model of ATP synthase: pH dependence of the rate of ATP synthesis

Recently, a novel molecular mechanism of torque generation in the F(0) portion of ATP synthase was proposed [Rohatgi, Saha and Nath (1998) Curr. Sci. 75, 716-718]. In this mechanism, rotation of the c-subunit was conceived to take place in 12 discrete steps of 30 degrees each due to the binding and unbinding of protons to/from the leading and trailing Asp-61 residues of the c-subunit, respectively. Based on this molecular mechanism, a kinetic scheme has been developed in this work. The scheme considers proton transport driven by a concentration gradient of protons across the proton half-channels, and the rotation of the c-subunit by changes in the electrical potential only. This kinetic scheme has been analyzed mathematically and an expression has been obtained to explain the pH dependence of the rate of ATP synthesis by ATP synthase under steady state operating conditions. For a single set of three enzymological kinetic parameters, this expression predicts the rates of ATP synthesis which agree well with the experimental data over a wide range of pH(in) and pH(out). A logical consequence of our analysis is that DeltapH and Deltapsi are kinetically inequivalent driving forces for ATP synthesis.     

Thermal inactivation of electron-transport functions and F0F1-ATPase activities

Bovine heart submitochondrial particles in suspension were heated at a designated temperature for 3 min, then cooled for biochemical assays at 30 degrees C. By enzyme activity measurements and polarographic assay of oxygen consumption, it is shown that the thermal denaturation of the respiratory chain takes place in at least four stages and each stage is irreversible. The first stage occurs at 51.0 +/- 1.0 degrees C, with the inactivation of NADH-linked respiration, ATP-driven reverse electron transport, F0F1 catalyzed ATP/Pi exchange, NADH and succinate-driven ATP synthesis. The second stage occurs at 56.0 +/- 1.0 degrees C, with the inactivation of succinate-linked proton pumping and respiration. The third stage occurs at 59.0 +/- 1.0 degrees C, with the inactivation of electron transfer from cytochrome c to cytochrome oxidase and ATP-dependent proton pumping. The ATP hydrolysis activity of F0F1 persists to 61.0 +/- 1.0 degrees C. An additional transition, detectable by differential scanning calorimetry, occurring around 70.0 +/- 2.0 degrees C, is probably associated with thermal denaturation of cytochrome c and other stable membrane proteins. In the presence of either mitochondrial matrix fluid or 2 mM mercaptoethanol, all five stages give rise to endothermic effects, with the absorption of approx. 25 J/g protein. Under aerobic conditions, however, the first four transitions become strongly exothermic, and release a total of approx. 105 J/g protein. Solubilized and reconstituted F0F1 vesicles also exhibit different inactivation temperatures for the ATP/Pi exchange, proton pumping and ATP hydrolysis activities. The first two activities are abolished at 49.0 +/- 1.0 degrees C, but the latter at 58.0 +/- 2.0 degrees C. Differential scanning calorimetry also detects biphasic transitions of F0F1, with similar temperatures of denaturation (49.0 and 54.0 degrees C). From these and other results presented in this communication, the following is concluded. (1) A selective inactivation, by the temperature treatment, of various functions of the electron-transport chain and of the F0F1 complex can be done. (2) The ATP synthesis activity of the F0F1 complex involves either a catalytic or a regulation subunit(s) which is not essential for ATP hydrolysis and the proton translocation. This subunit is 10 degrees C less stable than the hydrolytic site. Micromolar ADP stabilizes it from thermal denaturation by 4-5 degrees C, although ADP up to millimolar concentration does not protect the hydrolytic site and the proton-translocation site.(ABSTRACT TRUNCATED AT 400 WORDS)     

F1-ATPase rotates by an asymmetric, sequential mechanism using all three catalytic subunits

F1-ATPase, the catalytic part of FoF1-ATP synthase, rotates the central gamma subunit within the alpha3beta3 cylinder in 120 degrees steps, each step consuming a single ATP molecule. However, how the catalytic activity of each beta subunit is coordinated with the other two beta subunits to drive rotation remains unknown. Here we show that hybrid F1 containing one or two mutant beta subunits with altered catalytic kinetics rotates in an asymmetric stepwise fashion. Analysis of the rotations reveals that for any given beta subunit, the subunit binds ATP at 0 degrees, cleaves ATP at approximately 200 degrees and carries out a third catalytic event at approximately 320 degrees. This demonstrates the concerted nature of the F1 complex activity, where all three beta subunits participate to drive each 120 degrees rotation of the gamma subunit with a 120 degrees phase difference, a process we describe as a 'sequential three-site mechanism'.     

Differential effects of triphenyltin and 8-azido-ATP on the ATP synthesis, ATP-Pi exchange, and ATP hydrolysis in liposomes containing ATP synthase and bacteriorhodopsin

The ATP hydrolysis activity of purified ATP synthase reconstituted in liposomes was inhibited by triphenyltin in a manner different from that of other thiol-specific reagents. In liposomes containing ATP synthase and bacteriorhodopsin, ATP hydrolysis and ATP-Pi exchange were inhibited by triphenyltin to a greater extent than the ATP synthesis, in contrast to what was found with an F1-specific inhibitor, 8-azido-ATP. The possibility is discussed that ATP hydrolysis and ATP synthesis are differently coupled to proton conduction through F0.     

Observation of calcium-dependent unidirectional rotational motion in recombinant photosynthetic F1-ATPase molecules

ATP hydrolysis and synthesis by the F(0)F(1)-ATP synthase are coupled to proton translocation across the membrane in the presence of magnesium. Calcium is known, however, to disrupt this coupling in the photosynthetic enzyme in a unique way: it does not support ATP synthesis, and CaATP hydrolysis is decoupled from any proton translocation, but the membrane does not become leaky to protons. Understanding the molecular basis of these calcium-dependent effects can shed light on the as yet unclear mechanism of coupling between proton transport and rotational catalysis. We show here, using an actin filament gamma-rotation assay, that CaATP is capable of sustaining rotational motion in a highly active hybrid photosynthetic F(1)-ATPase consisting of alpha and beta subunits from Rhodospirillum rubrum and gamma subunit from spinach chloroplasts (alpha(R)(3)beta(R)(3)gamma(C)). The rotation was found to be similar to that induced by MgATP in Escherichia coli F(1)-ATPase molecules. Our results suggest a possible long range pathway that enables the bound CaATP to induce full rotational motion of gamma but might block transmission of this rotational motion into proton translocation by the F(0) part of the ATP synthase.     

The structural basis for unidirectional rotation of thermoalkaliphilic F1-ATPase

The ATP synthase of the thermoalkaliphilic Bacillus sp. TA2.A1 operates exclusively in ATP synthesis direction. In the crystal structure of the nucleotide-free alpha(3)beta(3)gamma epsilon subcomplex (TA2F(1)) at 3.1 A resolution, all three beta subunits adopt the open beta(E) conformation. The structure shows salt bridges between the helix-turn-helix motif of the C-terminal domain of the beta(E) subunit (residues Asp372 and Asp375) and the N-terminal helix of the gamma subunit (residues Arg9 and Arg10). These electrostatic forces pull the gamma shaft out of the rotational center and impede rotation through steric interference with the beta(E) subunit. Replacement of Arg9 and Arg10 with glutamines eliminates the salt bridges and results in an activation of ATP hydrolysis activity, suggesting that these salt bridges prevent the native enzyme from rotating in ATP hydrolysis direction. A similar bending of the gamma shaft as in the TA2F(1) structure was observed by single-particle analysis of the TA2F(1)F(o) holoenzyme.     

Structure of dimeric ATP synthase from mitochondria: an angular association of monomers induces the strong curvature of the inner membrane

Respiration in all cells depends upon synthesis of ATP by the ATP synthase complex, a rotary motor enzyme. The structure of the catalytic moiety of ATP synthase, the so-called F(1) headpiece, is well established. F(1) is connected to the membrane-bound and ion translocating F(0) subcomplex by a central stalk. A peripheral stalk, or stator, prevents futile rotation of the headpiece during catalysis. Although the enzyme functions as a monomer, several lines of evidence have recently suggested that monomeric ATP synthase complexes might interact to form a dimeric supercomplex in mitochondria. However, due to its fragility, the structure of ATP synthase dimers has so far not been precisely defined for any organism. Here we report the purification of a stable dimeric ATP synthase supercomplex, using mitochondria of the alga Polytomella. Structural analysis by electron microscopy and single particle analysis revealed that dimer formation is based on specific interaction of the F(0) parts, not the F(1) headpieces which are not at all in close proximity. Remarkably, the angle between the two F(0) part is about 70 degrees, which induces a strong local bending of the membrane. Hence, the function of ATP synthase dimerisation is to control the unique architecture of the mitochondrial inner membrane.     

The Na(+)-translocating F(1)F(0) ATP synthase of Propionigenium modestum: mechanochemical insights into the F(0) motor that drives ATP synthesis

The ATP synthase of Propionigenium modestum encloses a rotary motor involved in the production of ATP from ADP and inorganic phosphate utilizing the free energy of an electrochemical Na(+) ion gradient. This enzyme clearly belongs to the family of F(1)F(0) ATP synthases and uses exclusively Na(+) ions as the physiological coupling ion. The motor domain, F(0), comprises subunit a and the b subunit dimer which are part of the stator and the subunit c oligomer acting as part of the rotor. During ATP synthesis, Na(+) translocation through F(0) proceeds from the periplasm via the stator channel (subunit a) onto a Na(+) binding site of the rotor (subunit c). Upon rotation of the subunit c oligomer versus subunit a, the occupied rotor site leaves the interface with the stator and the Na(+) ion can freely dissociate into the cytoplasm. Recent experiments demonstrate that the membrane potential is crucial for ATP synthesis under physiological conditions. These findings support the view that voltage generates torque in F(0), which drives the rotation of the gamma subunit thus liberating tightly bound ATP from the catalytic sites in F(1). We suggest a mechanochemical model for the transduction of transmembrane Na(+)-motive force into rotary torque by the F(0) motor that can account quantitatively for the experimental data.