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Fig. 2. Center of mass trajectories (A) and leg kinematics (B,C) for spring-mass running with and without retraction (C, {omega}R=50 deg s-1; B, {omega}R=0 deg s-1). The bars in A indicate the change in centre of mass height between touch-down and take-off. B and C are expanded views of plot A from 0 to 6 m (boxed). For each simulated run, the same initial apex height was used (y0=1.25 m), and for the simulation with retraction, a retraction angle of {alpha}R=60° was assumed (C). Here the model with retraction reached a steady state condition after two steps in contrast to approximately 8 steps for the model without retraction (A,B). The red dotted lines in B and C denote the steady state landing angle {alpha}0*.





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