Structural rearrangements in the active site of smooth-muscle myosin

Exploring NMR methods as a tool to select suitable fluorescent nucleotide analogues

Fluorescent analogues provide important tools for biochemical/biophysical research. However, the analogues contain chemical modifications much larger than those known to affect ligand-binding, such as the inversion of a carbon centre or substitution of an atom. We lack experimental tools and protocols to select the most appropriate fluorescent analogue. Herein, we use several NMR spectroscopy methods, including Saturation Transfer Difference (STD), STD competition and transferred nuclear Overhauser effect spectroscopy (Tr-NOESY), as tools to select appropriate fluorescent probes. Annexin A6 (AnxA6) is a ubiquitous protein that forms in vitro GTP-induced ion channels. We used this protein as a model and screened guanosine triphosphate (GTP) and four fluorescent analogues against AnxA6. STD reported that the GTP moiety of all ligands made similar contacts with the protein, despite additional interactions between the fluorescent tags and AnxA6. Competition STD experiments verified that the analogues and GTP bind to the same site. Tr-NOESY indicated that the bound conformation of the base relative to ribose is altered for some analogues compared to GTP. MANT-GTP or the BODIPY thioester of guanosine 5'-O-(3-thiotriphosphate) are the most suitable fluorescent analogues for AnxA6, according to NMR. These results reveal NMR as a useful technique to select and design proper fluorescent tags for biochemical/biophysical assays.

Loop 1 dynamics in smooth muscle myosin: isoform specific differences modulate ADP release

Isoforms of the smooth muscle (SM) myosin motor domain differ in the presence or absence of a seven amino acid insert in a flexible surface loop spanning the nucleotide-binding pocket known as Loop 1. The presence of this insert leads to a two-fold increase in actin sliding velocity and ADP release rate between these isoforms, although the effect of Loop 1 on the kinetics of ADP release remains unclear. To further investigate the role of the Loop 1 insert in modulating ADP release in SM myosin we have inserted a single tryptophan residue into Loop 1 of both isoforms as a probe of local structural dynamics. By monitoring the dynamics of Loop 1 in relation to the release of ADP we have observed a unique movement of Loop 1 in the inserted isoform, preceding nucleotide release, which is absent in the non-inserted isoform. This movement is sequence dependent as alanine replacement of the insert residues abolishes the transition and slows ADP release. Thus movement of Loop 1 is a critical factor in increasing the ADP release rate in the inserted faster isoform of SM myosin.

EPR spectra and molecular dynamics agree that the nucleotide pocket of myosin V is closed and that it opens on binding actin

We have used EPR spectroscopy and computational modeling of nucleotide-analog spin probes to investigate conformational changes at the nucleotide site of myosin V. We find that, in the absence of actin, the mobility of a spin-labeled diphosphate analog [spin-labeled ADP (SLADP)] bound at the active site is strongly hindered, suggesting a closed nucleotide pocket. The mobility of the analog increases when the MV·SLADP complex (MV=myosin V) binds to actin, implying an opening of the active site in the A·MV·SLADP complex (A=actin). The probe mobilities are similar to those seen with myosin II, despite the fact that myosin V has dramatically altered kinetics. Molecular dynamics (MD) simulation was used to understand the EPR spectra in terms of the X-ray database. The X-ray structure of MV·ADP·BeFx shows a closed nucleotide site and has been proposed to be the detached state. The MV·ADP structure shows an open nucleotide site and has been proposed to be the A·MV·ADP state at the end of the working powerstroke. MD simulation of SLADP docked in the closed conformation gave a probe mobility comparable to that seen in the EPR spectrum of the MV·SLADP complex. The simulation of the open conformation gave a probe mobility that was 35-40° greater than that observed experimentally for the A·MV·SLADP state. Thus, EPR, X-ray diffraction, and computational analysis support the closed conformation as a myosin V state that is detached from actin. The MD results indicate that the MV·ADP crystal structure, which may correspond to the strained actin-bound post-powerstroke conformation resulting from head-head interaction in the dimeric processive motor, is superopened.

Switch I closure simultaneously promotes strong binding to actin and ADP in smooth muscle myosin

The motor protein myosin uses energy derived from ATP hydrolysis to produce force and motion. Important conserved components (P-loop, switch I, and switch II) help propagate small conformational changes at the active site into large scale conformational changes in distal regions of the protein. Structural and biochemical studies have indicated that switch I may be directly responsible for the reciprocal opening and closing of the actin and nucleotide-binding pockets during the ATPase cycle, thereby aiding in the coordination of these important substrate-binding sites. Smooth muscle myosin has displayed the ability to simultaneously bind tightly to both actin and ADP, although it is unclear how both substrate-binding clefts could be closed if they are rigidly coupled to switch I. Here we use single tryptophan mutants of smooth muscle myosin to determine how conformational changes in switch I are correlated with structural changes in the nucleotide and actin-binding clefts in the presence of actin and ADP. Our results suggest that a closed switch I conformation in the strongly bound actomyosin-ADP complex is responsible for maintaining tight nucleotide binding despite an open nucleotide-binding pocket. This unique state is likely to be crucial for prolonged tension maintenance in smooth muscle.

Kinetics and thermodynamics of the rate-limiting conformational change in the actomyosin V mechanochemical cycle

We used FRET to examine the kinetics and thermodynamics of structural changes associated with ADP release in myosin V, which is thought to be a strain-sensitive step in many muscle and non-muscle myosins. We also explored essential dynamics using FIRST/FRODA starting with three different myosin V X-ray crystal structures to examine intrinsic flexibility and correlated motions. Our steady-state and time-resolved FRET analysis demonstrates a temperature-dependent reversible conformational change in the nucleotide-binding pocket (NBP). Our kinetic results demonstrate that the NBP goes from a closed to an open conformation prior to the release of ADP, while the actin-binding cleft remains closed. Interestingly, we find that the temperature dependence of the maximum actin-activated myosin V ATPase rate is similar to the pocket opening step, demonstrating that this is the rate-limiting structural transition in the ATPase cycle. Thermodynamic analysis demonstrates that the transition from the open to closed NBP conformation is unfavorable because of a decrease in entropy. The intrinsic flexibility analysis is consistent with conformational entropy playing a role in this transition as the MV.ADP structure is highly flexible compared to the MV.APO structure. Our experimental and modeling studies support the conclusion of a novel post-power-stroke actomyosin.ADP state in which the NBP and actin-binding cleft are closed. The novel state may be important for strain sensitivity as the transition from the closed to open NBP conformation may be altered by lever arm position.

Multiple conformations of the nucleotide site of Kinesin family motors in the triphosphate state

Identifying conformational changes in kinesin family motors associated with nucleotide and microtubule (MT) binding is essential to determining an atomic-level model for force production and motion by the motors. Using the mobility of nucleotide analog spin probes bound at the active sites of kinesin family motors to monitor conformational changes, we previously demonstrated that, in the ADP state, the open nucleotide site closes upon MT binding [Naber, N., Minehardt, T. J., Rice, S., Chen, X., Grammer, J., Matuska, M., et al. (2003). Closing of the nucleotide pocket of kinesin family motors upon binding to microtubules. Science, 300, 798-801]. We now extend these studies to kinesin-1 (K) and ncd (nonclaret disjunctional protein) motors in ATP and ATP-analog states. Our results reveal structural differences between several triphosphate and transition-state analogs bound to both kinesin and ncd in solution. The spectra of kinesin/ncd in the presence of SLADP•AlFx/BeFx and kinesin, with the mutation E236A (K-E236A; does not hydrolyze ATP) bound to ATP, show an open conformation of the nucleotide pocket similar to that seen in the kinesin/ncd•ADP states. In contrast, the triphosphate analogs K•SLAMPPNP and K-E236A•SLAMPPNP induce a more immobilized component of the electron paramagnetic resonance spectrum, implying closing of the nucleotide site. The MT-bound states of all of the triphosphate analogs reveal two novel spectral components. The equilibrium between these two components is only weakly dependent on temperature. Both components have more restricted mobility than observed in MT-bound diphosphate states. Thus, the closing of the nucleotide pocket when the diphosphate state binds to MTs is amplified in the triphosphate state, perhaps promoting accelerated ATP hydrolysis. Consistent with this idea, molecular dynamics simulations show a good correlation between our spectroscopic data, X-ray crystallography, and the electron microscopy of MT-bound triphosphate-analog states.

Nucleotide pocket thermodynamics measured by EPR reveal how energy partitioning relates myosin speed to efficiency

We have used spin-labeled ADP to investigate the dynamics of the nucleotide-binding pocket in a series of myosins, which have a range of velocities. Electron paramagnetic resonance spectroscopy reveals that the pocket is in equilibrium between open and closed conformations. In the absence of actin, the closed conformation is favored. When myosin binds actin, the open conformation becomes more favored, facilitating nucleotide release. We found that faster myosins favor a more closed pocket in the actomyosin•ADP state, with smaller values of ΔH(0) and ΔS(0), even though these myosins release ADP at a faster rate. A model involving a partitioning of free energy between work-generating steps prior to rate-limiting ADP release explains both the unexpected correlation between velocity and opening of the pocket and the observation that fast myosins are less efficient than slow myosins.

Combining EPR with fluorescence spectroscopy to monitor conformational changes at the myosin nucleotide pocket

We used spin-labeled nucleotide analogs and fluorescence spectroscopy to monitor conformational changes at the nucleotide-binding site of wild-type Dictyostelium discoideum (WT) myosin and a construct containing a single tryptophan at position F239 near the switch 1 loop. Electron paramagnetic resonance (EPR) spectroscopy and tryptophan fluorescence have been used previously to investigate changes at the myosin nucleotide site. A limitation of fluorescence spectroscopy is that it must be done on mutated myosins containing only a single tryptophan. A limitation of EPR spectroscopy is that one infers protein conformational changes from alterations in the mobility of an attached probe. These limitations have led to controversies regarding conclusions reached by the two approaches. For the first time, the data presented here allow direct correlations to be made between the results from the two spectroscopic approaches on the same proteins and extend our previous EPR studies to a nonmuscle myosin. EPR probe mobility indicates that the conformation of the nucleotide pocket of the WTSLADP (spin-labeled ADP) complex is similar to that of skeletal myosin. The pocket is closed in the absence of actin for both diphosphate and triphosphate nucleotide states. In the actin myosin diphosphate state, the pocket is in equilibrium between closed and open conformations, with the open conformation slightly more favorable than that seen for fast skeletal actomyosin. The EPR spectra for the mutant show similar conformations to skeletal myosin, with one exception: in the absence of actin, the nucleotide pocket of the mutant displays an open component that was approximately 4-5 kJ/mol more favorable than in skeletal or WT myosin. These observations resolve the controversies between the two techniques. The data from both techniques confirm that binding of myosin to actin alters the conformation of the myosin nucleotide pocket with similar but not identical energetics in both muscle and nonmuscle myosins.

Nucleotide-dependent conformational states of actin

The influence of the state of the bound nucleotide (ATP, ADP-Pi, or ADP) on the conformational free-energy landscape of actin is investigated. Nucleotide-dependent folding of the DNase-I binding (DB) loop in monomeric actin and the actin trimer is carried out using all-atom molecular dynamics (MD) calculations accelerated with a multiscale implementation of the metadynamics algorithm. Additionally, an investigation of the opening and closing of the actin nucleotide binding cleft is performed. Nucleotide-dependent free-energy profiles for all of these conformational changes are calculated within the framework of metadynamics. We find that in ADP-bound monomer, the folded and unfolded states of the DB loop have similar relative free-energy. This result helps explain the experimental difficulty in obtaining an ordered crystal structure for this region of monomeric actin. However, we find that in the ADP-bound actin trimer, the folded DB loop is stable and in a free-energy minimum. It is also demonstrated that the nucleotide binding cleft favors a closed conformation for the bound nucleotide in the ATP and ADP-Pi states, whereas the ADP state favors an open confirmation, both in the monomer and trimer. These results suggest a mechanism of allosteric interactions between the nucleotide binding cleft and the DB loop. This behavior is confirmed by an additional simulation that shows the folding free-energy as a function of the nucleotide cleft width, which demonstrates that the barrier for folding changes significantly depending on the value of the cleft width.

Site-directed spectroscopic probes of actomyosin structural dynamics

Spectroscopy of myosin and actin has entered a golden age. High-resolution crystal structures of isolated actin and myosin have been used to construct detailed models for the dynamic actomyosin interactions that move muscle. Improved protein mutagenesis and expression technologies have facilitated site-directed labeling with fluorescent and spin probes. Spectroscopic instrumentation has achieved impressive advances in sensitivity and resolution. Here we highlight the contributions of site-directed spectroscopic probes to understanding the structural dynamics of myosin II and its actin complexes in solution and muscle fibers. We emphasize studies that probe directly the movements of structural elements within the myosin catalytic and light-chain domains, and changes in the dynamics of both actin and myosin due to their alternating strong and weak interactions in the ATPase cycle. A moving picture emerges in which single biochemical states produce multiple structural states, and transitions between states of order and dynamic disorder power the actomyosin engine.

Characterization of the pre-force-generation state in the actomyosin cross-bridge cycle

Myosin is an actin-based motor protein that generates force by cycling between actin-attached (strong binding: ADP or rigor) and actin-detached (weak binding: ATP or ADP.P(i)) states during its ATPase cycle. However, it remains unclear what specific conformational changes in the actin binding site take place on binding to actin, and how these structural changes lead to product release and the production of force and motion. We studied the dynamics of the actin binding region of myosin V by using fluorescence resonance energy transfer (FRET) to monitor conformational changes in the upper-50-kDa domain of the actin binding cleft in the weak and strong actin binding states. Steady-state and lifetime data monitoring the FRET signal suggest that the cleft is in a more open conformation in the weak actin binding states. Transient kinetic experiments suggest that a rapid conformational change occurs, which is consistent with cleft closure before actin-activated phosphate release. Our results have identified a pre-force-generation actomyosin ADP.P(i) state, and suggest force generation may occur from a state not yet seen by crystallography in which the actin binding cleft and the nucleotide binding pocket are closed. Computational modeling uncovers dramatic changes in the rigidity of the upper-50-kDa domain in different nucleotide states, which suggests that the intrinsic flexibility of this domain allows myosin motors to accomplish simultaneous tight nucleotide binding (closed nucleotide binding pocket) and high-affinity actin binding (closed actin binding cleft).

Dynamics of the nucleotide pocket of myosin measured by spin-labeled nucleotides

We have used electron paramagnetic probes attached to the ribose of ATP (SL-ATP) to monitor conformational changes in the nucleotide pocket of myosin. Spectra for analogs bound to myosin in the absence of actin showed a high degree of immobilization, indicating a closed nucleotide pocket. In the Actin.Myosin.SL-AMPPNP, Actin.Myosin.SL-ADP.BeF(3), and Actin.Myosin.SL-ADP.AlF(4) complexes, which mimic weakly binding states near the beginning of the power stroke, the nucleotide pocket remained closed. The spectra of the strongly bound Actin.Myosin.SL-ADP complex consisted of two components, one similar to the closed pocket and one with increased probe mobility, indicating a more open pocket, The temperature dependence of the spectra showed that the two conformations of the nucleotide pocket were in equilibrium, with the open conformation more favorable at higher temperatures. These results, which show that opening of the pocket occurs only in the strongly bound states, appear reasonable, as this would tend to keep ADP bound until the end of the power stroke. This conclusion also suggests that force is initially generated by a myosin with a closed nucleotide pocket.