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Image Search Results
Journal: PLOS Computational Biology
Article Title: A simulation framework to determine optimal strength training and musculoskeletal geometry for sprinting and distance running
doi: 10.1371/journal.pcbi.1011410
Figure Lengend Snippet: Our differentiable musculoskeletal simulator generates the derivatives of the state variables given the state variables (muscle activations a m , torque actuator activations a T , tendon forces F t , generalized positions q and velocities q ˙ ) and the decision variables (skeleton segment scaling factors p s , muscle volume scaling factors p V m u s c l e , muscle excitations e m , torque actuator excitations e T ). This is achieved by evaluating a set of dynamics equations: activation dynamics, torque actuator dynamics, muscle dynamics, and skeleton dynamics. Evaluating muscle and skeleton dynamics depends on the outputs of musculoskeletal geometry computations (i.e., muscle-tendon lengths l mt and velocities l ˙ m t and muscle moment-arm matrices R ) and on the scaled muscle parameters ( p m , scaled ). Since the scaling of the skeleton and muscle volumes are decision variables, we formulated musculoskeletal geometry computation, muscle parameter scaling and skeleton dynamics as a differentiable function of these decision variables. The dotted boxes indicate the parts of the simulator where we turned non-differentiable computation used in OpenSim and Falisse et al. into differentiable computation. Tendon forces are mapped to joint muscle torques ( τ m ) by the moment-arm matrix ( R ). Torque actuator activations are scaled to torque actuator torques ( τ T ) by a scaling factor of 150 . A contact function ( f contact ) based on the Hunt-Crossley contact model gives the generalized forces resulting from contact ( f c ).
Article Snippet: Our
Techniques: Activation Assay