Inter-subunit rotation and elastic power transmission in F0F1-ATPase

ATP synthase (F-ATPase) produces ATP at the expense of ion-motive force or vice versa. It is composed from two motor/generators, the ATPase (F1) and the ion translocator (F0), which both are rotary steppers. They are mechanically coupled by 360 degrees rotary motion of subunits against each other. The rotor, subunits gamma(epsilon)C10-14, moves against the stator, (alphabeta)3delta(ab2). The enzyme copes with symmetry mismatch (C3 versus C10-14) between its two motors, and it operates robustly in chimeric constructs or with drastically modified subunits. We scrutinized whether an elastic power transmission accounts for these properties. We used the curvature of fluorescent actin filaments, attached to the rotating c ring, as a spring balance (flexural rigidity of 8.10(-26) N x m2) to gauge the angular profile of the output torque at F0 during ATP hydrolysis by F1. The large average output torque (56 pN nm) proved the absence of any slip. Angular variations of the torque were small, so that the output free energy of the loaded enzyme decayed almost linearly over the angular reaction coordinate. Considering the three-fold stepping and high activation barrier (>40 kJ/mol) of the driving motor (F1) itself, the rather constant output torque seen by F0 implied a soft elastic power transmission between F1 and F0. It is considered as essential, not only for the robust operation of this ubiquitous enzyme under symmetry mismatch, but also for a high turnover rate under load of the two counteracting and stepping motors/generators.     

Microsecond time scale rotation measurements of single F1-ATPase molecules

A novel method for detecting F(1)-ATPase rotation in a manner sufficiently sensitive to achieve acquisition rates with a time resolution of 2.5 micros (equivalent to 400,000 fps) is reported. This is sufficient for resolving the rate at which the gamma-subunit travels from one dwell state to another (transition time). Rotation is detected via a gold nanorod attached to the rotating gamma-subunit of an immobilized F(1)-ATPase. Variations in scattered light intensity allow precise measurement of changes in the angular position of the rod below the diffraction limit of light. Using this approach, the transition time of Escherichia coli F(1)-ATPase gamma-subunit rotation was determined to be 7.62 +/- 0.15 (standard deviation) rad/ms. The average rate-limiting dwell time between rotation events observed at the saturating substrate concentration was 8.03 ms, comparable to the observed Mg(2+)-ATPase k(cat) of 130 s(-)(1) (7.7 ms). Histograms of scattered light intensity from ATP-dependent nanorod rotation as a function of polarization angle allowed the determination of the nanorod orientation with respect to the axis of rotation and plane of polarization. This information allowed the drag coefficient to be determined, which implied that the instantaneous torque generated by F(1) was 63.3 +/- 2.9 pN nm. The high temporal resolution of rotation allowed the measurement of the instantaneous torque of F(1), resulting in direct implications for its rotational mechanism.     

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.     

Effect of external torque on the ATP-driven rotation of F1-ATPase

F₁-ATPase is a rotary molecular motor powered by the torque generated by another rotary motor F₀ to synthesize ATP in vivo. Therefore elucidation of the behavior of F₁ under external torque is very important. Here, we applied controlled external torque by electrorotation and investigated the ATP-driven rotation for the first time. The rotation was accelerated by assisting torque and decelerated by hindering torque, but F₁ rarely showed rotations in the ATP synthesis direction. This is consistent with the prediction by models based on the assumption that the rotation is tightly coupled to ATP hydrolysis and synthesis. At low ATP concentrations (2 and 5 μM), 120° stepwise rotation was observed. Due to the temperature rise during experiment, quantitative interpretation of the data is difficult, but we found that the apparent rate constant of ATP binding clearly decreased by hindering torque and increased by assisting torque.     

The regulator of the F1 motor: inhibition of rotation of cyanobacterial F1-ATPase by the epsilon subunit

The chloroplast-type F(1) ATPase is the key enzyme of energy conversion in chloroplasts, and is regulated by the endogenous inhibitor epsilon, tightly bound ADP, the membrane potential and the redox state of the gamma subunit. In order to understand the molecular mechanism of epsilon inhibition, we constructed an expression system for the alpha(3)beta(3)gamma subcomplex in thermophilic cyanobacteria allowing thorough investigation of epsilon inhibition. epsilon Inhibition was found to be ATP-independent, and different to that observed for bacterial F(1)-ATPase. The role of the additional region on the gamma subunit of chloroplast-type F(1)-ATPase in epsilon inhibition was also determined. By single molecule rotation analysis, we succeeded in assigning the pausing angular position of gamma in epsilon inhibition, which was found to be identical to that observed for ATP hydrolysis, product release and ADP inhibition, but distinctly different from the waiting position for ATP binding. These results suggest that the epsilon subunit of chloroplast-type ATP synthase plays an important regulator for the rotary motor enzyme, thus preventing wasteful ATP hydrolysis.     

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.     

The kinetic and structural changes of the mitochondrial F1-ATPase with temperature

Mitochondrial F1-ATPase shows a break in the Arrhenius plot with an increase of the activation energy below 17 degrees C, this may imply that the F1-ATPase undergoes a conformational change at this temperature. Further, a structural change of the F1-ATPase is indicated by analysis of the intrinsic fluorescence at 307 nm between 33 and 11 degrees C and also by evaluation of the circular dichroism spectra of the enzyme at temperatures below and above the temperature corresponding to the discontinuity of the Arrhenius plot. It is therefore suggested that F1-ATPase exists in two temperature dependent conformational states to which different catalytic properties may be assigned.     

The F subunit of Thermus thermophilus V1-ATPase promotes ATPase activity but is not necessary for rotation

V(1)-ATPase from the thermophilic bacterium Thermus thermophilus is a molecular rotary motor with a subunit composition of A(3)B(3)DF, and its central rotor is composed of the D and F subunits. To determine the role of the F subunit, we generated an A(3)B(3)D subcomplex and compared it with A(3)B(3)DF. The ATP hydrolyzing activity of A(3)B(3)D (V(max) = 20 s(-1)) was lower than that of A(3)B(3)DF (V(max) = 31 s(-1)) and was more susceptible to MgADP inhibition during ATP hydrolysis. A(3)B(3)D was able to bind the F subunit to form A(3)B(3)DF. The C-terminally truncated F((Delta85-106)) subunit was also bound to A(3)B(3)D, but the F((Delta69-106)) subunit was not, indicating the importance of residues 69-84 of the F subunit for association with A(3)B(3)D. The ATPase activity of A(3)B(3)DF((Delta85-106)) (V(max) = 24 s(-1)) was intermediate between that of A(3)B(3)D and A(3)B(3)DF. A single molecule experiment showed the rotation of the D subunit in A(3)B(3)D, implying that the F subunit is a dispensable component for rotation itself. Thus, the F subunit binds peripherally to the D subunit, but promotes V(1)-ATPase catalysis.     

The role of the DELSEED motif of the beta subunit in rotation of F1-ATPase

F(1)-ATPase is a rotary motor protein, and ATP hydrolysis generates torque at the interface between the gamma subunit, a rotor shaft, and the alpha(3)beta(3) substructure, a stator ring. The region of conserved acidic "DELSEED" motif of the beta subunit has a contact with gamma subunit and has been assumed to be involved in torque generation. Using the thermophilic alpha(3)beta(3)gamma complex in which the corresponding sequence is DELSDED, we replaced each residue and all five acidic residues in this sequence with alanine. In addition, each of two conserved residues at the counterpart contact position of gamma subunit was also replaced. Surprisingly, all of these mutants rotated with as much torque as the wild-type. We conclude that side chains of the DELSEED motif of the beta subunit do not have a direct role in torque generation.     

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

The binding change model for the F(1)-ATPase predicts that its rotation is intimately correlated with the changes in the affinities of the three catalytic sites for nucleotides. If so, subtle differences in the nucleotide structure may have pronounced effects on rotation. Here we show by single-molecule imaging that purine nucleotides ATP, GTP, and ITP support rotation but pyrimidine nucleotides UTP and CTP do not, suggesting that the extra ring in purine is indispensable for proper operation of this molecular motor. Although the three purine nucleotides were bound to the enzyme at different rates, all showed similar rotational characteristics: counterclockwise rotation, 120 degrees steps each driven by hydrolysis of one nucleotide molecule, occasional back steps, rotary torque of approximately 40 piconewtons (pN).nm, and mechanical work done in a step of approximately 80 pN.nm. These latter characteristics are likely to be determined by the rotational mechanism built in the protein structure, which purine nucleotides can energize. With ATP and GTP, rotation was observed even when the free energy of hydrolysis was -80 pN.nm/molecule, indicating approximately 100% efficiency. Reconstituted F(o)F(1)-ATPase actively translocated protons by hydrolyzing ATP, GTP, and ITP, but CTP and UTP were not even hydrolyzed. Isolated F(1) very slowly hydrolyzed UTP (but not CTP), suggesting possible uncoupling from rotation.     

The gamma subunit in chloroplast F(1)-ATPase can rotate in a unidirectional and counter-clockwise manner

Desethylamiodarone (DEA) acts as a competitive inhibitor of triiodothyronine (T3) binding to the alpha1-thyroid hormone receptor (TR alpha1) but as a non-competitive inhibitor with respect to TR beta1. To gain insight into the position of the binding site of desethylamiodarone on TR beta1 we investigated the naturally occurring mutants Y321C, R429Q, P453A, P453T and the artificial mutants L421R and E457A in the ligand binding domain of human TR beta1. The IC50 values (in microM) of DEA for P453A (50 +/- 11) and P453T (55 +/- 16) mutant TR beta1 are not different from that for the wild type TR beta1 (56 +/- 15), but the IC50 values of R429Q (32 +/- 7; P<0.001) and E457A (17 +/- 3; P<0.001) are significantly lower than of the wild type. Scatchard plots and Langmuir analyses indicate a non-competitive nature of the inhibition by DEA of T3 binding to all four mutant TR beta1s tested. Mutants P453A and P453T do not influence overall electrostatic potential, and also do not influence the affinity for DEA compared to wild type. Mutant E457A causes a change from a negatively charged amino acid to a hydrophobic amino acid, enhancing the affinity for DEA. Mutant R429Q, located in helix 11, causes an electrostatic potential change from positive to uncharged, also resulting in greater affinity for DEA. We therefore postulate that amino acids R429 and E457 are at or close to the binding site for DEA, and that DEA does not bind in the T3 binding pocket itself, in line with the non-competitive nature of the inhibition of T3 binding to TR beta1 by DEA.     

Redox regulation of rotation of the cyanobacterial F1-ATPase containing thiol regulation switch

F(1)-ATP synthase (F(1)-ATPase) is equipped with a special mechanism that prevents the wasteful reverse reaction, ATP hydrolysis, when there is insufficient proton motive force to drive ATP synthesis. Chloroplast F(1)-ATPase is subject to redox regulation, whereby ATP hydrolysis activity is regulated by formation and reduction of the disulfide bond located on the γ subunit. To understand the molecular mechanism of this redox regulation, we constructed a chimeric F(1) complex (α(3)β(3)γ(redox)) using cyanobacterial F(1), which mimics the regulatory properties of the chloroplast F(1)-ATPase, allowing the study of its regulation at the single molecule level. The redox state of the γ subunit did not affect the ATP binding rate to the catalytic site(s) and the torque for rotation. However, the long pauses caused by ADP inhibition were frequently observed in the oxidized state. In addition, the duration of continuous rotation was relatively shorter in the oxidized α(3)β(3)γ(redox) complex. These findings lead us to conclude that redox regulation of CF(1)-ATPase is achieved by controlling the probability of ADP inhibition via the γ subunit inserted region, a sequence feature observed in both cyanobacterial and chloroplast ATPase γ subunits, which is important for ADP inhibition (Sunamura, E., Konno, H., Imashimizu-Kobayashi, M., Sugano, Y., and Hisabori, T. (2010) Plant Cell Physiol. 51, 855-865).     

Purification, crystallization, and properties of F1-ATPase complexes from the thermoalkaliphilic Bacillus sp. strain TA2.A1

Recently, we reported the cloning of the atp operon encoding for the F(1)F(0)-ATP synthase from the extremely thermoalkaliphilic bacterium Bacillus sp. strain TA2.A1. In this study, the genes encoding the F(1) moiety of the enzyme complex were cloned from the atp operon into the vector pTrc99A and expressed in Escherichia coli in two variant complexes, F(1)-wt consisting of subunits alpha(3)beta(3)gammadeltaepsilon and F(1)Deltadelta lacking the entire delta-subunit as a prerequisite for overproduction and crystallization trials. Both F(1)-wt and F(1)Deltadelta were successfully overproduced in E. coli and purified in high yield and purity. F(1)Deltadelta was crystallized by micro-batch screening yielding three-dimensional crystals that diffracted to a resolution of 3.1A using a synchrotron radiation source. After establishing cryo and dehydrating conditions, a complete set of diffraction data was collected from a single crystal. No crystals were obtained with F(1)-wt. Data processing of diffraction patterns showed that F(1)Deltadelta crystals belong to the orthorhombic space group P2(1)2(1)2(1) with unit cell parameters of a=121.70, b=174.80, and c=223.50A, alpha, beta, gamma=90.000. The asymmetric unit contained one molecule of bacterial F(1)Deltadelta with a corresponding volume per protein weight (V(M)) of 3.25A(3) Da(-1) and a solvent content of 62.1%. Silver staining of single crystals of F(1)Deltadelta analyzed by SDS-PAGE revealed four bands alpha, beta, gamma, and epsilon with identical M(r)-values as those found in the native F(1)F(0)-ATP synthase isolated from strain TA2.A1 membranes. ATPase assays of F(1)Deltadelta crystals exhibited latent ATP hydrolytic activity that was highly stimulated by lauryldimethylamine oxide, a hallmark of the native enzyme.     

Chaperones of F1-ATPase

Mitochondrial F₁-ATPase contains a hexamer of alternating α and β subunits. The assembly of this structure requires two specialized chaperones, Atp11p and Atp12p, that bind transiently to β and α. In the absence of Atp11p and Atp12p, the hexamer is not formed, and α and β precipitate as large insoluble aggregates. An early model for the mechanism of chaperone-mediated F₁ assembly (Wang, Z. G., Sheluho, D., Gatti, D. L., and Ackerman, S. H. (2000) EMBO J. 19, 1486–1493) hypothesized that the chaperones themselves look very much like the α and β subunits, and proposed an exchange of Atp11p for α and of Atp12p for β; the driving force for the exchange was expected to be a higher affinity of α and β for each other than for the respective chaperone partners. One important feature of this model was the prediction that as long as Atp11p is bound to β and Atp12p is bound to α, the two F₁ subunits cannot interact at either the catalytic site or the noncatalytic site interface. Here we present the structures of Atp11p from Candida glabrata and Atp12p from Paracoccus denitrificans, and we show that some features of the Wang model are correct, namely that binding of the chaperones to α and β prevents further interactions between these F₁ subunits. However, Atp11p and Atp12p do not resemble α or β, and it is instead the F₁ γ subunit that initiates the release of the chaperones from α and β and their further assembly into the mature complex.Mitochondrial F₁-ATPase consists of three α and three β subunits occupying alternate positions in a hexamer that surrounds a rod-like element containing one each of γ, δ, and ϵ subunits (1–3). Three nucleotide-binding catalytic sites (CS)⁴ and three noncatalytic sites (NCS) alternate at the six α/β interfaces. Early work with respiratory-deficient strains of Saccharomyces cerevisiae (4) revealed that two additional mitochondrial proteins, Atp11p and Atp12p, which are not integral subunits of the enzyme, are nonetheless necessary for the assembly of F₁-ATPase. Besides their failure to assemble F₁, a particularly interesting feature of atp11 and atp12 mutants is that they accumulate α and β subunits as high molecular weight aggregates (4) that can be recognized as densely stained inclusion bodies in the mitochondrial matrix (5). Subsequent studies in yeast have shown that Atp12p binds to F₁ α (6) and that Atp11p binds to β (7); these interactions include binding determinants in the nucleotide binding domains (NBD) of the two F₁ subunits. On this basis, it is now recognized that Atp11p and Atp12p are members of two new families of molecular chaperones, pfam06644 and pfam07542 (8), which are required for the assembly of mitochondrial ATP synthase in all eukaryotes. In fact, the first nuclear genetic lesion associated to a defect of mitochondrial ATP synthase in humans was identified in the locus ATPAF2 for Atp12p and was responsible for the death of a 14-month-old infant (9). Atp12p is also present in the α subdivision of Proteobacteria, consistent with the proposed origin of mitochondria from this ancestral line (10).The nature of the interactions between the F₁ subunits and Atp11p and Atp12p has remained elusive because of the lack of structural information for these chaperones. As α and β aggregate in the absence of Atp11p and Atp12p, it is usually assumed that the F₁ subunits are themselves poorly soluble, and that the two chaperones maintain them in a dispersed state until they are incorporated in the mature enzyme. Based on the analysis of the distribution of hydrophilic and hydrophobic areas on the surface of the α and β subunits of F₁, and on the interaction energies between these subunits at the interfaces that provide the CS and NCS sites, Wang et al. (6) have proposed a model of F₁ assembly in which Atp11p binds at the region of the β subunit that contributes to the CS site, and Atp12p binds at the region of the α subunit that contributes to the NCS site. One consequence of this particular binding of Atp11p and Atp12p to the F₁ subunits is that as long as Atp11p is bound to β and Atp12p is bound to α, the two F₁ subunits cannot interact at either the CS or the NCS interface. Since no other modulators of chaperone release are known, the Wang model requires an exchange of Atp11p for α and of Atp12p for β. Implied in this model is that the chaperones must themselves look very much like the α and β subunits, and that the driving force for the exchange must simply be a higher affinity of α and β for each other than for the respective chaperone partners. Here we present the structures of Atp11p from Candida glabrata and Atp12p from Paracoccus denitrificans, and we show that some features of the Wang model are correct, namely that binding of the chaperones to α and β prevents further interactions between these F₁ subunits. However, Atp11p and Atp12p do not resemble α or β, and it is instead the F₁ γ subunit that initiates the release of the chaperones from α and β and their further assembly into mature complex.     

F1-ATPase, the C-terminal end of subunit gamma is not required for ATP hydrolysis-driven rotation

ATP hydrolysis by the isolated F(1)-ATPase drives the rotation of the central shaft, subunit gamma, which is located within a hexagon formed by subunits (alphabeta)(3). The C-terminal end of gamma forms an alpha-helix which properly fits into the "hydrophobic bearing" provided by loops of subunits alpha and beta. This "bearing" is expected to be essential for the rotary function. We checked the importance of this contact region by successive C-terminal deletions of 3, 6, 9, 12, 15, and 18 amino acid residues (Escherichia coli F(1)-ATPase). The ATP hydrolysis activity of a load-free ensemble of F(1) with 12 residues deleted decreased to 24% of the control. EF(1) with deletions of 15 or 18 residues was inactive, probably because it failed to assemble. The average torque generated by a single molecule of EF(1) when loaded by a fluorescent actin filament was, however, unaffected by deletions of up to 12 residues, as was their rotational behavior (all samples rotated during 60 +/- 19% of the observation time). Activation energy analysis with the ensemble revealed a moderate decrease from 54 kJ/mol for EF(1) (full-length gamma) to 34 kJ/mol for EF(1)(gamma-12). These observations imply that the intactness of the C terminus of subunit gamma provides structural stability and/or routing during assembly of the enzyme, but that it is not required for the rotary action under load, proper.     

The unbinding of ATP from F1-ATPase

Using molecular dynamics, we study the unbinding of ATP in F(1)-ATPase from its tight binding state to its weak binding state. The calculations are made feasible through use of interpolated atomic structures from Wang and Oster [Nature 1998, 396: 279-282]. These structures are applied to atoms distant from the catalytic site. The forces from these distant atoms gradually drive a large primary region through a series of sixteen equilibrated steps that trace the hinge bending conformational change in the beta-subunit that drives rotation of gamma-subunit. As the rotation progresses, we find a sequential weakening and breaking of the hydrogen bonds between the ATP molecule and the alpha- and beta-subunits of the ATPase. This finding agrees with the "binding-zipper" model [Oster and Wang, BIOCHIM: Biophys. Acta 2000, 1458: 482-510.] In this model, the progressive formation of the hydrogen bonds is the energy source driving the rotation of the gamma-shaft during hydrolysis. Conversely, the corresponding sequential breaking of these bonds is driven by rotation of the shaft during ATP synthesis. Our results for the energetics during rotation suggest that the nucleotide's coordination with Mg(2+) during binding and release is necessary to account for the observed high efficiency of the motor.