Here we report a 2.3-Å crystal structure of scallop myosin S1 complexed with ADP⅐BeF x, as well as three additional structures (at 2.8 -3.8 Å resolution) for this S1 complexed with ATP analogs, some of which are cross-linked by para-phenyl dimaleimide, a short intramolecular cross-linker. In all cases, the complexes are characterized by an unwound SH1 helix first seen in an unusual 2.5-Å scallop myosin-MgADP structure and described as corresponding to a previously unrecognized actin-detached internally uncoupled state. The unwinding of the SH1 helix effectively uncouples the converter͞lever arm module from the motor and allows crosslinking by para-phenyl dimaleimide, which has been shown to occur only in weak actin-binding states of the molecule. Mutations near the metastable SH1 helix that disable the motor can be accounted for by viewing this structural element as a clutch controlling the transmission of torque to the lever arm. We have also determined a 3.2-Å nucleotide-free structure of scallop myosin S1, which suggests that in the near-rigor state there are two conformations in the switch I loop, depending on whether nucleotide is present. Analysis of the subdomain motions in the weak actin-binding states revealed by x-ray crystallography, together with recent electron microscopic results, clarify the mechanical roles of the parts of the motor in the course of the contractile cycle and suggest how strong binding to actin triggers both the power stroke and product release.T he myosin head (subfragment one, or S1) consists of a motor domain (MD) and a lever arm that amplifies small conformational changes of the motor (Fig. 1). The MD comprises four subdomains (the 50-kDa upper and lower subdomains, the N-terminal subdomain, and the converter) linked by three flexible single-stranded joints (switch II, the relay, and the so-called SH1 helix). Motor function results from coupled rigid body rearrangements of the subdomains coordinated with conformational changes in the joints (1, 2). During the acto-myosin contractile cycle (3-5), the MD undergoes a number of conformational changes as the myosin head transduces ATP hydrolysis into mechanical work. The affinity of myosin for actin in the cycle is often described in terms of ''strong'' and ''weak'' actin-binding states. Myosin crystal structures have thus far been obtained only in the absence of actin, and three conformations have been identified, but their place in the contractile cycle has been controversial (6). The first or near-rigor conformation (7), was obtained in the absence of nucleotide, and, because the lever arm orientation was similar to that observed in electron microscopy (EM) images of actomyosin in the rigor state, this conformation was thought to be similar to a true rigor (i.e., strong actin-binding, nucleotide-free) state. More recent studies (8, 9) have shown, however, that this conformation corresponds to a weak actin-binding state occurring shortly after myosin detaches from actin, and that this state can bind to but cannot hydrolyze ATP. I...