A clear prediction of the helix-coil model for force generation in muscle is that force should be produced when the equilibrium (helix-coil) of a rigor (or activated) fiber is perturbed by a temperature jump near the melting temperature of the light meromyosin/heavy meromyosin hinge. An infrared, iodine-photodissociation laser was used to heat the fibers by ==50C in under 1 ps. Under ionic conditions where rigor bridges are predominantly associated with the thick filament backbone, an abrupt drop in tension typical of normal thermoelastic expansion was seen. A similar response was observed below 41'C for thick rilament-released rigor bridges. Above this temperature, a rubber-like thermoelastic response was obtained typical of a helix-coil transition. At temperatures near 50TC, the amount of force generated by a rigor fiber was large and comparable to that seen for an activated fiber at 50C. The relaxation spectra of force generation obtained for both systems (rigor *and activated) show a step change followed by a biexponential kinetic process. The reciprocal relaxation times and amplitudes for these individual processes in activated and rigor fibers differ only by factors of 24. Force generation in the rigor muscle appears to arise from melting in the subfragment 2 hinge region of the myosin molecule since binding of subfragment 2 to the thick filament backbone inhibits force production. No significant force generation was observed following temperature jumps of relaxed fibers.It is likely that force generation in skeletal muscle results from a structural change in myosin crossbridge [the heavy meromyosin (HMM) region of myosin] while it is attached to actin in an active bridge cycle. One suggested mechanism (1, 2) is that the structural transition is confined to the myosin head [subfragment 1 (S-1) subunit], resulting in a change in the effective angle of this moiety while it is bound to actin. Another proposal (3, 4) is that a part of the a-helical subfragment 2 (S-2) segment of the crossbridge [the light meromyosin (LMM)/HMM hinge domain] undergoes melting to random-coil when the actin-attached bridge swings away from the stabilizing environment of the thick filament surface. This process induces shortening in S-2 and produces the force required to slide the thin filaments relative to the thick filaments during active contraction.Force generation by polymers, like the a-helical coiled-coil of the hinge, that undergo a transition from an extended semirigid form (helical in structure) to a highly flexible random-coil form, buffeted by thermal (Brownian) motion, is a well-documented phenomenon. The heating of a rubber-like thermoelastic polymer (as the above is described) results in contraction; expansion results when a substance with normal thermoelasticity is heated. To date, only normal thermoelasticity has been observed in muscle and not the rubber-like