We have measured the conventional electron paramagnetic resonance (EPR) spectrum of spin-labeled myosin filaments as a function of the nucleotide occupancy of the active site of the enzyme. The probe used was 4-(2-iodoacetamido)-2,2,6,6-tetramethylpiperidine-1-oxyl (IASL), which reacts specifically with sulfhydryl 1 of the myosin head. In the absence of nucleotide, the probe remains strongly immobilized (rigidly attached to the myosin head) so that no nanosecond rotational motions are detectable. When MgADP is added to IASL-labeled myosin filaments (T = 20 degrees C), the probe mobility increases slightly. During steady-state MgADP hydrolysis (T = 20 degrees C), the probe undergoes large-amplitude nanosecond rotational motion. These results are consistent with previous studies of myosin monomers, heavy meromyosin, and myosin subfragment 1. Isoclinic points observed in overlays of sequential EPR spectra recorded during ATP hydrolysis strongly suggest that the probes fall into two motional classes, separated by approximately an order of magnitude in effective rotational correlation time. Both of the observed states are distinct from the conformation of myosin in the absence of nucleotides, and the spectrum of the less mobile population is indistinguishable from that observed in the presence of MgADP. The addition of ADP and vanadate to IASL-myosin gives rise to two motional classes virtually identical with those observed in the presence of ATP, but the relative concentrations of the spin populations are significantly different. We have quantitated the percentage of myosin in each motional state during ATP hydrolysis. The result agrees well with the predicted percentages in the two predominant chemical states in the myosin ATPase cycle. Spectra obtained in the presence of nucleotide analogues permit us to assign the conformational states to specific chemical states. We propose that the two motional classes represent two distinct local conformations of myosin that are in exchange with one another during the ATP hydrolysis reaction cycle.

We have used electron paramagnetic resonance (EPR) spectroscopy to detect ATP- and calcium-induced changes in the structure of spin-labeled myosin heads in glycerinated rabbit psoas muscle fibers in key physiological states. The probe was a nitroxide iodoacetamide derivative attached selectively to myosin SH1 (Cys 707), the conventional EPR spectra of which have been shown to resolve several conformational states of the myosin ATPase cycle, on the basis of nanosecond rotational motion within the protein. Spectra were acquired in rigor and during the steady-state phases of relaxation and isometric contraction. Spectral components corresponding to specific conformational states and biochemical intermediates were detected and assigned by reference to EPR spectra of trapped kinetic intermediates. In the absence of ATP, all of the myosin heads were rigidly attached to the thin filament, and only a single conformation was detected, in which there was no sub-microsecond probe motion. In relaxation, the EPR spectrum resolved two conformations of the myosin head that are distinct from rigor. These structural states were virtually identical to those observed previously for isolated myosin and were assigned to the populations of the M*.ATP and M**.ADP.Pi states. During isometric contraction, the EPR spectrum resolves the same two conformations observed in relaxation, plus a small fraction (20-30%) of heads in the oriented actin-bound conformation that is observed in rigor. This rigor-like component is a calcium-dependent, actin-bound state that may represent force-generating cross-bridges. As the spin label is located near the nucleotide-binding pocket in a region proposed to be pivotal for large-scale force-generating structural changes in myosin, we propose that the observed spectroscopic changes indicate directly the key steps in energy transduction in the molecular motor of contracting muscle.

Skeletal muscle fibers consist of hexagonally packed actin and myosin filaments. According to x-ray diffraction and electron microscopy (EM), the structure is highly ordered both in hexagonal packing and along the filament axis. Globular actin monomers are organized in a doublestranded helix, while myosin molecules are stacked so that

We have used saturation transfer electron paramagnetic resonance (ST-EPR) to detect the microsecond rotational motions of spin-labeled myosin heads in bundles of skinned muscle fibers, under conditions of rigor, relaxation, and isometric contraction. Experiments were performed on fiber bundles perfused continuously with an ATP-regenerating system. Conditions were identical to those we have used in previous studies of myosin head orientation, except that the fibers were perpendicular to the magnetic field, making the spectra primarily sensitive to rotational motion rather than to the orientational distribution. In rigor, the high intensity of the ST-EPR signal indicates the absence of microsecond rotational motion, showing that heads are all rigidly bound to actin. However, in both relaxation and contraction, considerable microsecond rotational motion is observed, implying that the previously reported orientational disorder under these conditions is dynamic, not static, on the microsecond time scale. The behavior in relaxation is essentially the same as that observed when myosin heads are detached from actin in the absence of ATP (Barnett and Thomas, 1984), corresponding to an effective rotational correlation time of approximately 10 microseconds. Slightly less mobility is observed during contraction. One possible interpretation is that in contraction all heads have the same mobility, corresponding to a correlation time of approximately 25 microseconds. Alternatively, more than one motional population may be present. For example, assuming that the spectrum in contraction is a linear combination of those in relaxation (mobile) and rigor (immobile), we obtained a good fit with a mole fraction of 78-88% of the heads in the mobile state. These results are consistent with previous STEPR studies on contracting myofibrils(Thomas et al., 1980). Thus most myosin heads undergo microsecond rotational motions most of the time during isometric contraction, at least in the probed region of the myosin head.These motions could arise primarily from the free rotations of heads detached from actin. However, if most of these heads are attached to actin during contraction, as suggested by stiffness measurements, this result provides support for the hypothesis that sub-millisecond rotational motions of actin-attached myosin heads play an important role in force generation.

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