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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,
R=50 deg
s-1; B,
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
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
0*.