Conformational change of the chloroplast ATP synthase on the enzyme activation process detected by the trypsin sensitivity of the gamma subunit

Delta mu H(+) is known to stimulate the enzyme activity of chloroplast ATP synthase in addition to its important role as energy supply for ATP synthesis. In the present study, we focused on the relationship between the proton translocation via the membrane sector of ATP synthase, F(o), and the conformational change of the central stalk subunit gamma. The conformational change of CF(1) mainly at the gamma subunit was induced by the proton flow via F(o) in the absence of substrates. The effects of inhibitors on CF(o) or CF(1) for this conformational change were also examined. The observed conformational change was partially suppressed by ADP binding. From these results, we propose the Delta mu H(+)-dependent conformational change of CF(1) on the enzyme activation process, which is affected by both ADP binding to the catalytic sites and proton flow via F(o) portion.     

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.     

Insights into the molecular mechanism of rotation in the Fo sector of ATP synthase

F(1)F(o)-ATP synthase is a ubiquitous membrane protein complex that efficiently converts a cell's transmembrane proton gradient into chemical energy stored as ATP. The protein is made of two molecular motors, F(o) and F(1), which are coupled by a central stalk. The membrane unit, F(o), converts the transmembrane electrochemical potential into mechanical rotation of a rotor in F(o) and the physically connected central stalk. Based on available data of individual components, we have built an all-atom model of F(o) and investigated through molecular dynamics simulations and mathematical modeling the mechanism of torque generation in F(o). The mechanism that emerged generates the torque at the interface of the a- and c-subunits of F(o) through side groups aSer-206, aArg-210, and aAsn-214 of the a-subunit and side groups cAsp-61 of the c-subunits. The mechanism couples protonation/deprotonation of two cAsp-61 side groups, juxtaposed to the a-subunit at any moment in time, to rotations of individual c-subunit helices as well as rotation of the entire c-subunit. The aArg-210 side group orients the cAsp-61 side groups and, thereby, establishes proton transfer via aSer-206 and aAsn-214 to proton half-channels, while preventing direct proton transfer between the half-channels. A mathematical model proves the feasibility of torque generation by the stated mechanism against loads typical during ATP synthesis; the essential model characteristics, e.g., helix and subunit rotation and associated friction constants, have been tested and furnished by steered molecular dynamics simulations.     

An alternative reaction pathway of F1-ATPase suggested by rotation without 80 degrees/40 degrees substeps of a sluggish mutant at low ATP

F(1)-ATPase, a water-soluble portion of F(o)F(1)-ATP synthase, is a rotary motor driven by ATP hydrolysis. The central gamma-subunit rotates in the alpha(3)beta(3) cylinder by repeating four stages of rotation: ATP-binding dwell, rapid 80 degrees substep rotation, catalytic dwell, and rapid 40 degrees substep rotation. In the catalytic dwell, at least two catalytic reactions occur-cleavage of the enzyme-bound ATP and presumably release of the hydrolyzed product(s) from the enzyme-but we found that a slow ATP cleavage mutant of F(1)-ATPase from thermophilic Bacillus PS3 rotates at low ATP concentration without substeps and the catalytic dwell. Analysis indicates that in this alternative reaction pathway the two catalytic reactions occur during the preceding long ATP-binding dwell. Thus, F(1)-ATPase can operate through (at least) two competing reaction pathways, not necessarily through a simple consecutive reaction.     

Rotation of the c subunit oligomer in EF(0)EF(1) mutant cD61N

ATP synthases (F(0)F(1)-ATPases) mechanically couple ion flow through the membrane-intrinsic portion, F(0), to ATP synthesis within the peripheral portion, F(1). The coupling most probably occurs through the rotation of a central rotor (subunits c(10)epsilon gamma) relative to the stator (subunits ab(2)delta(alpha beta)(3)). The translocation of protons is conceived to involve the rotation of the ring of c subunits (the c oligomer) containing the essential acidic residue cD61 against subunits ab(2). In line with this notion, the mutants cD61N and cD61G have been previously reported to lack proton translocation. However, it has been surprising that the membrane-bound mutated holoenzyme hydrolyzed ATP but without translocating protons. Using detergent-solubilized and immobilized EF(0)F(1) and by application of the microvideographic assay for rotation, we found that the c oligomer, which carried a fluorescent actin filament, rotates in the presence of ATP in the mutant cD61N just as in the wild type enzyme. This observation excluded slippage among subunit gamma, the central rotary shaft, and the c oligomer and suggested free rotation without proton pumping between the oligomer and subunit a in the membrane-bound enzyme.     

Electrostatic interactions in catalytic centers of F1-ATPase

The first part of this paper is a brief review of works concerned with the mechanisms of functioning of F0F1-ATP synthases. F0F1-ATP syntheses operate as rotating molecular machines that provide the synthesis of ATP from ADP and inorganic phosphate (Pi) in mitochondria, chloroplasts, and bacteria at the expense of the energy of electrochemical gradient of hydrogen ions generated across energy-transducing mitochondrial, chloroplast or, bacterial membranes. A distinguishing feature of these enzymes is that they operate as rotary molecular motors. In the second part of the work, we calculated the contribution of electrostatic interactions between charged groups of a substrate (MgATP), reaction products (MgADP and Pi), and charged amino acid residues of the F1-ATPase molecule to energy changes associated with the binding of ATP and its chemical transformations in the catalytic centers located at the interface of the alpha- and beta-subunits of the enzyme (oligomer complex alpha 3 beta 3 gamma of bovine mitochondrial ATPase). The catalytic cycle of ATP hydrolysis considered in the work includes conformational changes of alpha- and beta-subunits caused by unidirectional rotations of the central gamma-subunit. The results of our calculations are consistent with the idea that the energetically favorable process of ATP binding to the "open" catalytic center of F1-ATPase initiates the rotation of the gamma-subunit followed by ATP hydrolysis in another ("closed") catalytic center of the enzyme.     

Observations of rotation within the FoF1-ATP synthase: deciding between rotation of the Foc subunit ring and artifact

F(o)F(1)-ATP synthase mediates coupling of proton flow in F(o) and ATP synthesis/hydrolysis in F(1) through rotation of central rotor subunits. A ring structure of F(o)c subunits is widely believed to be a part of the rotor. Using an attached actin filament as a probe, we have observed the rotation of the F(o)c subunit ring in detergent-solubilized F(o)F(1)-ATP synthase purified from Escherichia coli. Similar studies have been performed and reported recently [Sambongi et al. (1999) Science 286, 1722-1724]. However, in our hands this rotation has been observed only for the preparations which show poor sensitivity to dicyclohexylcarbodiimde, an F(o) inhibitor. We have found that detergents which adequately disperse the enzyme for the rotation assay also tend to transform F(o)F(1)-ATP synthase into an F(o) inhibitor-insensitive state in which F(1) can hydrolyze ATP regardless of the state of the F(o). Our results raise the important issue of whether rotation of the F(o)c ring in isolated F(o)F(1)-ATP synthase can be demonstrated unequivocally with the approach adopted here and also used by Sambongi et al.     

A mathematical model of conformational changes in membrane protein part of F0F1-ATP synthase

The transformation of the electrochemical membrane proton gradient into the energy of chemical bond in adenosinetriphosphate is one of the most important biological processes occurring in the living cell. The main enzyme that directly catalyzes the synthesis of ATP from ADP and Pi in aerobic conditions is F0F1-ATP synthase. In the present study, conformational changes in membrane protein part of ATP synthase during its catalytic cycle were described in terms of dynamic equations of solid state rotation. It was shown that this process should be considered in the framework of classical mechanics. The time dependences of the angle rotation for the protein complex rotates around its central axis were oobtained. Possible types of rotation were analyzed. It was proved that, considering the modern level of knowledge and understanding of ATP synthase structure and function are taken into account, the minimal period of rotor turnover cannot be less than 10(-9) s. With regard for viscous friction and elastic tension in the central axis, the calculated time of whole turnover varies from 10(-6) to 10(-3) and depends on the set of parameters used. These results indicate the essential contribution of friction and elastic tension to the rotation dynamics of the rotor. It is suggested that the proposed model can be used as a part of the entire algorithm for computer simulation of ATP synthase.     

Movements of the epsilon-subunit during catalysis and activation in single membrane-bound H(+)-ATP synthase

F0F1-ATP synthases catalyze proton transport-coupled ATP synthesis in bacteria, chloroplasts, and mitochondria. In these complexes, the epsilon-subunit is involved in the catalytic reaction and the activation of the enzyme. Fluorescence-labeled F0F1 from Escherichia coli was incorporated into liposomes. Single-molecule fluorescence resonance energy transfer (FRET) revealed that the epsilon-subunit rotates stepwise showing three distinct distances to the b-subunits in the peripheral stalk. Rotation occurred in opposite directions during ATP synthesis and hydrolysis. Analysis of the dwell times of each FRET state revealed different reactivities of the three catalytic sites that depended on the relative orientation of epsilon during rotation. Proton transport through the enzyme in the absence of nucleotides led to conformational changes of epsilon. When the enzyme was inactive (i.e. in the absence of substrates or without membrane energization), three distances were found again, which differed from those of the active enzyme. The three states of the inactive enzyme were unequally populated. We conclude that the active-inactive transition was associated with a conformational change of epsilon within the central stalk.     

Luminescence resonance energy transfer measurements in myosin.

Myosin is thought to generate force by a rotation between the relative orientations of two domains. Direct measurements of distances between the domains could potentially confirm and quantify these conformational changes, but efforts have been hampered by the large distances involved. Here we show that luminescence resonance energy transfer (LRET), which uses a luminescent lanthanide as the energy-transfer donor, is capable of measuring these long distances. Specifically, we measure distances between the catalytic domain (Cys707) and regulatory light chain domain (Cys108) of the myosin head. An energy transfer efficiency of 21.2 +/- 1.9% is measured in the myosin complex without nucleotide or actin, corresponding to a distance of 73 A, consistent with the crystal structure of Rayment et al. Upon binding to actin, the energy transfer efficiency decreases by 4.5 +/- 1.0%, indicating a conformational change in myosin that involves a relative rotation and/or translation of Cys707 relative to the light chain domain. Addition of ADP also alters the energy transfer efficiency, likely through a rotation of the probe attached to Cys707. These results demonstrate that LRET is capable of making accurate measurements on the relatively large actomyosin complex, and is capable of detecting conformational changes between the catalytic and light chain domains of myosin.     

Mitochondrial genome integrity mutations uncouple the yeast Saccharomyces cerevisiae ATP synthase

The mitochondrial ATP synthase is a molecular motor, which couples the flow of protons with phosphorylation of ADP. Rotation of the central stalk within the core of ATP synthase effects conformational changes in the active sites driving the synthesis of ATP. Mitochondrial genome integrity (mgi) mutations have been previously identified in the alpha-, beta-, and gamma-subunits of ATP synthase in yeast Kluyveromyces lactis and trypanosome Trypanosoma brucei. These mutations reverse the lethality of the loss of mitochondrial DNA in petite negative strains. Introduction of the homologous mutations in Saccharomyces cerevisiae results in yeast strains that lose mitochondrial DNA at a high rate and accompanied decreases in the coupling of the ATP synthase. The structure of yeast F1-ATPase reveals that the mgi residues cluster around the gamma-subunit and selectively around the collar region of F1. These results indicate that residues within the mgi complementation group are necessary for efficient coupling of ATP synthase, possibly acting as a support to fix the axis of rotation of the central stalk.     

The Mre11:Rad50 structure shows an ATP-dependent molecular clamp in DNA double-strand break repair

The MR (Mre11 nuclease and Rad50 ABC ATPase) complex is an evolutionarily conserved sensor for DNA double-strand breaks, highly genotoxic lesions linked to cancer development. MR can recognize and process DNA ends even if they are blocked and misfolded. To reveal its mechanism, we determined the crystal structure of the catalytic head of Thermotoga maritima MR and analyzed ATP-dependent conformational changes. MR adopts an open form with a central Mre11 nuclease dimer and two peripheral Rad50 molecules, a form suited for sensing obstructed breaks. The Mre11 C-terminal helix-loop-helix domain binds Rad50 and attaches flexibly to the nuclease domain, enabling large conformational changes. ATP binding to the two Rad50 subunits induces a rotation of the Mre11 helix-loop-helix and Rad50 coiled-coil domains, creating a clamp conformation with increased DNA-binding activity. The results suggest that MR is an ATP-controlled transient molecular clamp at DNA double-strand breaks.     

Large conformational changes in a kinesin motor catalyzed by interaction with microtubules

Kinesin motor proteins release nucleotide upon interaction with microtubules (MTs), then bind and hydrolyze ATP to move along the MT. Although crystal structures of kinesin motors bound to nucleotides have been solved, nucleotide-free structures have not. Here, using cryomicroscopy and three-dimensional (3D) reconstruction, we report the structure of MTs decorated with a Kinesin-14 motor, Kar3, in the nucleotide-free state, as well as with ADP and AMPPNP, with resolution sufficient to show alpha helices. We find large structural changes in the empty motor, including melting of the switch II helix alpha4, closure of the nucleotide binding pocket, and changes in the central beta sheet reminiscent of those reported for nucleotide-free myosin crystal structures. We propose that the switch II region of the motor controls docking of the Kar3 neck by conformational changes in the central beta sheet, similar to myosin, rather than by rotation of the motor domain, as proposed for the Kif1A kinesin motor.     

Met23Lys mutation in subunit gamma of F(O)F(1)-ATP synthase from Rhodobacter capsulatus impairs the activation of ATP hydrolysis by protonmotive force

H(+)-F(O)F(1)-ATP synthase couples proton flow through its membrane portion, F(O), to the synthesis of ATP in its headpiece, F(1). Upon reversal of the reaction the enzyme functions as a proton pumping ATPase. Even in the simplest bacterial enzyme the ATPase activity is regulated by several mechanisms, involving inhibition by MgADP, conformational transitions of the epsilon subunit, and activation by protonmotive force. Here we report that the Met23Lys mutation in the gamma subunit of the Rhodobacter capsulatus ATP synthase significantly impaired the activation of ATP hydrolysis by protonmotive force. The impairment in the mutant was due to faster enzyme deactivation that was particularly evident at low ATP/ADP ratio. We suggest that the electrostatic interaction of the introduced gammaLys23 with the DELSEED region of subunit beta stabilized the ADP-inhibited state of the enzyme by hindering the rotation of subunit gamma rotation which is necessary for the activation.     

Novel features in the structure of bovine ATP synthase.

The F1F0-ATP synthase from bovine heart mitochondria catalyses the synthesis of ATP from ADP and inorganic phosphate by using the energy of an electrochemical proton gradient derived from electron transport. The enzyme consists of three major domains: the globular F1catalytic domain of known atomic structure lies outside the lipid bilayer and is attached by a central stalk to the intrinsic membrane domain, F0, which transports protons through the membrane. Proton transport through F0evokes structural changes that are probably transmitted by rotation of the stalk to the catalytic sites in F1. In an alpha3beta3gamma1subcomplex, the rotation of the central gamma subunit driven by ATP hydrolysis has been visualised by optical microscopy. In order to prevent the alpha3beta3structure from following the rotation of the central gamma subunit, it has been proposed that the enzyme might have a stator connecting static parts in F0to alpha3beta3,thereby keeping it fixed relative to the rotating parts. Here we present electron microscopy images that reveal three new features in bovine F1F0-ATPase, one of which could be a stator. The second feature is a collar structure above the membrane domain and the third feature is some additional density on top of the F1domain.     

Understanding ATP synthesis: structure and mechanism of the F1-ATPase (Review)

To couple the energy present in the electrochemical proton gradient, established across the mitochondrial membrane by the respiratory chain, to the formation of ATP from ADP and Pi, ATP-synthase goes through a sequence of coordinated conformational changes of its major subunits (alpha, beta). These changes are induced by the rotation of the gamma subunit driven by the translocation of protons through the c subunit of the membrane portion of the enzyme. During this process, the F1-portion of the ATP-synthase adopts at least two major conformations depending on the occupancy of the beta subunits: one with two nucleotides, the other with three. In the two-nucleotide structure, the empty beta subunit adopts an open conformation that is highly different from the other conformations of beta subunits: tight, loose and closed. The three-dimensional structures of the F1-ATPase in each of these two major conformations provide a framework for understanding the mechanism of energy coupling by the enzyme. The energetics associated with two different models of the reaction steps, analysed using molecular dynamics calculations, show that three-nucleotide intermediates do not occur in configurations with an open beta subunit; instead, they are stabilized by completing a jaw-like motion that closes the beta subunit around the nucleotide. Consequently, the energy driven, major conformational change takes place with the beta subunits in the tight, loose and closed conformation.     

Nucleotide binding drives conformational changes in the isolated alpha and beta subunits of the F(1)-ATPase from Escherichia coli

The modeling of the rotatory mechanism performed by the F(1)-ATPase complex during ATP synthesis shows that the beta, but not the alpha subunit, undergoes large conformational changes that depend on the occupancy of the catalytic site. Here we determined by fluorescence spectroscopy the changes in tertiary structure and hydrophobic exposed area of the isolated alpha and beta subunits of the F(1)-ATPase complex from Escherichia coli upon adenine nucleotide binding. The results show that in the absence of intersubunit contacts, the two subunits exhibit markedly similar conformational movements.     

Three myosin V structures delineate essential features of chemo-mechanical transduction

The molecular motor, myosin, undergoes conformational changes in order to convert chemical energy into force production. Based on kinetic and structural considerations, we assert that three crystal forms of the myosin V motor delineate the conformational changes that myosin motors undergo upon detachment from actin. First, a motor domain structure demonstrates that nucleotide-free myosin V adopts a specific state (rigor-like) that is not influenced by crystal packing. A second structure reveals an actomyosin state that favors rapid release of ADP, and differs from the rigor-like state by a P-loop rearrangement. Comparison of these structures with a third structure, a 2.0 angstroms resolution structure of the motor bound to an ATP analog, illuminates the structural features that provide communication between the actin interface and nucleotide-binding site. Paramount among these is a region we name the transducer, which is composed of the seven-stranded beta-sheet and associated loops and linkers. Reminiscent of the beta-sheet distortion of the F1-ATPase, sequential distortion of this transducer region likely controls sequential release of products from the nucleotide pocket during force generation.     

Catalytic control and coupling efficiency of the Escherichia coli FoF1 ATP synthase: influence of the Fo sector and epsilon subunit on the catalytic transition state

The rate-limiting transition state of steady-state ATP hydrolysis and synthesis reactions in the F(o)F(1) ATP synthase involves the rotation of the gamma, epsilon, and c subunits. To probe the role of the transport and coupling mechanisms in controlling catalysis, kinetic and thermodynamic parameters of ATP hydrolysis were determined for enzymes in the presence of the detergent lauryldimethylamine oxide (LDAO), which uncouples active transport and disables the inhibitory effect of the epsilon subunit. At 5 mM LDAO or greater, the inhibitory effects of epsilon subunit are abrogated in both purified F(1) and membranous F(o)F(1). In these conditions, LDAO solubilized F(o)F(1) has a higher k(cat) for ATP hydrolysis than F(1). These results indicate an influence of F(o) on F(1) even though catalysis is uncoupled from transport. The alpha(3)beta(3)gamma complex free of the epsilon subunit is activated at a lower concentration of 0.5 mM LDAO. Significantly, the gammaY205C mutant enzyme is similarly activated at 0.5 mM LDAO, suggesting that the mutant enzyme lacks epsilon inhibition. The gammaY205C F(o)F(1), which has a k(cat) for ATP hydrolysis 2-fold higher than wild type, has an ATP synthesis rate 3-fold lower than wild type, showing that coupling is inefficient. Arrhenius and isokinetic analyses indicate that enzymes that are free of epsilon subunit inhibition have a different transition-state structure from those under the influence of the epsilon subunit. We propose that the epsilon subunit is one of the factors that determines the proper transition-state structure, which is essential for efficient coupling.     

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.