Spectral shift in heavy-meromyosin induced by substrate

The dynamics of the relay loop tryptophan residue in the Dictyostelium myosin motor domain and the origin of spectroscopic signals

Steady-state and time-resolved fluorescence measurements were performed on a Dictyostelium discoideum myosin II motor domain construct retaining a single tryptophan residue at position 501, located on the relay loop. Other tryptophan residues were mutated to phenylalanine. The Trp-501 residue showed a large enhancement in fluorescence in the presence of ATP and a small quench in the presence of ADP as a result of perturbing both the ground and excited state processes. Fluorescence lifetime and quantum yield measurements indicated that at least three microstates of Trp-501 were present in all nucleotide states examined, and these could not be assigned to a particular gross conformation of the motor domain. Enhancement in emission intensity was associated with a reduction of the contribution from a statically quenched component and an increase in a component with a 5-ns lifetime, with little change in the contribution from a 1-ns lifetime component. Anisotropy measurements indicated that the Trp-501 side chain was relatively immobile in all nucleotide states, and the fluorescence was effectively depolarized by rotation of the whole motor domain with a correlation time on 50-70 ns. Overall these data suggest that the backbone of the relay loop remains structured throughout the myosin ATPase cycle but that the Trp-501 side chain experiences a different weighting in local environments provided by surrounding residues as the adjacent converter domain rolls around the relay loop.

Chemomechanical transduction in the actomyosin molecular motor by 2',3'-dideoxydidehydro-ATP and characterization of its interaction with myosin subfragment 1 in the presence and absence of actin

The effect of torsional freedom about the N-glycoside bond of ATP in the ability of the nucleoside triphosphate to support chemomechanical transduction (Takenaka et al., 1978) has been investigated by examining the ability of the nucleotide analogue 2',3'-dideoxy-2',3'-didehydro-ATP (1b, enf-ATP) to act as a substrate for myosin subfragment 1 in the presence and absence of actin and to support actin sliding in the standard in vitro motility assay. By converting the ribosyl ring of the natural substrate to the rigid and almost planar enofuranosyl ring, effects on torsional freedom about the N-glycoside bond due to changes in ribosyl ring pucker and/or by steric interferences of the protons attached to the 2' and 3' carbons are eliminated allowing for increased torsional freedom about the N-glycoside bond. The data indicate that this enofuranosyl analogue is an excellent substrate for subfragment 1 and actosubfragment 1 and produces actin sliding velocities which are twice as fast as those observed with ATP in the standard in vitro motility assay. The analogue diphosphate is trapped in S1 by the common P(i) analogues, but the rate of formation of the ternary complex formed with Vi is very slow compared to that observed with MgADP. Similar conformations of S1 are formed with Mg.enf-ATP and MgATP under steady-state conditions, but S1 with bound Mg.enf-ADP differs significantly from that observed with MgADP.

The mechanism of muscle contraction

Knowledge of the mechanism of contraction has been obtained from studies of the interaction of actin and myosin in solution, from an elucidation of the structure of muscle fibers, and from measurements of the mechanics and energetics of fiber contraction. Many of the states and the transition rates between them have been established for the hydrolysis of ATP by actin and myosin subfragments in solution. A major goal is to now understand how the kinetics of this interaction are altered when it occurs in the organized array of the myofibril. Early work on the structure of muscle suggested that changes in the orientation of myosin cross-bridges were responsible for the generation of force. More recently, fluorescent and paramagnetic probes attached to the cross-bridges have suggested that at least some domains of the cross-bridges do not change orientation during force generation. A number of properties of active cross-bridges have been defined by measurements of steady state contractions of fibers and by the transients which follow step changes in fiber length or tension. Taken together these studies have provided firm evidence that force is generated by a cyclic interaction in which a myosin cross-bridge attaches to actin, exerts force through a "powerstroke" of 12 nm, and is then released by the binding of ATP. The mechanism of this interaction at the molecular level remains unknown.

The process in which nucleotide is buried into the active site of heavy meromyosin

The process in which nucleotide is buried into the active site of heavy meromyosin was studied with stopped-flow apparatus by monitoring the time-course of the large fluorescence increase of 1,N6-ethenoadenosine triphosphate (epsilon-ATP) when it binds from acrylamide-containing solutions. We have recently reported that free epsilon-ATP fluorescence is effectively quenched by acrylamide while bound epsilon-ATP is resistant to quenching by acrylamide. In the present study it was found that in the first step the phosphate moiety binds at a high rate, while the adenine moiety is still on the rim of the active site; the adenine moiety is then pulled into a crevice, and finally epsilon-ATP hydrolysis occurs.

The effects of solvent viscosity on the kinetic parameters of myosin and heavy meromyosin ATPase

The effects of different solvent viscosities on the kinetic parameters of ATP hydrolysis by myosin and heavy meromyosin (HMM) were investigated at high and low ionic strength (i.e., 0.53 and 0.08 M KCl where myosin is polymerized into thick filament). The solvent viscosity was adjusted by the addition of appropriate amounts of sucrose. The maximum rate constants (Vm) for both myosin and HMM decreased monotonically with increasing solvent viscosity at either ionic strength. The Michaelis constants (Km) for soluble myosin and HMM became minima at a viscosity nearly twice that of the solvent without sucrose, then increased abruptly with increasing solvent viscosity. On the other hand, Km of polymerized myosin at the low ionic strength decreased monotonically with increasing solvent viscosity. These experimental results are discussed with special reference to Kramers' kinetic theory of a chemically reacting system in viscous media.

Thermal transitions of myosin and its helical fragments. II. Solvent-induced variations in conformational stability

The melting behavior of myosin and myosin rod has been studied over the pH range 5.4-7.0, in 0.5 M KCl. Both proteins exhibit almost identical T-m values, which increase from about 37 to 43 degrees as the pH is elevated through the range of study, T-m follows a sigmoidal dependence upon pH, and the inflection point occurs near pH 6.5. The influence of salt concentration on T-m was studied, by the variation of KCl from 0.15 to 2.92 M. With an increasing KCl concentration, both proteins exhibit similar, sigmoidal declines in T-m from about 44 to 34 degrees. Under all conditions of pH and ionic strength studied, melting is accompanied by an absorption of H+ by the protein. The concentration of the protein, the age of the preparation, and the presence of divalent metal ions fail to exert a significant effect on the T-m values obtained by our methods. The effects of salt concentration and pH on the thermal stability of myosin and myosin rod are discussed in terms of the location of the melting process within the myosin molecule. Myosin is shown to possess several of the requisite features for energy transduction via a proton-coupling mechanism. These features provide a framework for investigating some aspects of the molecular basis of muscle contraction within the context of the sliding filament model.