(Downloading may take up to 30 seconds.
If the slide opens in your browser, select File -> Save As to save it.)
Click on image to view larger version.

Fig. 7. Body CoM dynamics following perturbations in relation to spring-mass model
dynamics. (A) Computer simulation of the spring-mass trajectory following a
change from a soft to hard surface, with no change in leg stiffness
(kleg), resulting in an asymmetrical CoM path and a steep
trajectory during take-off at the end of support. (B) Actual CoM vertical
displacement of a human runner encountering an abrupt but expected change from
a soft to hard substrate. The runner maintains similar (symmetrical) CoM
motion by anticipating the change and adjusting kleg
within the first step (Ferris et al.,
1999). (C) Computer simulation of the spring-mass trajectory
following a sudden, unexpected drop in substrate height (40% of leg length).
In the perturbed step, the only model value that differs from the level step
is the limb contact angle (
o), which is steeper due to the
backward motion of the limb before it contacts the ground (see also
Fig. 8B). The angle used in the
simulation was that measured experimentally from guinea fowl. (D) Actual CoM
trajectory and energy changes of running guinea fowl following an unexpected
drop in substrate height equal to 40% of leg length (PEg,
solid blue line; KEv and KEh, solid
green and broken purple lines; Ecom, total center of mass
energy, solid black line). The broken vertical gray line indicates when the
foot contacted the tissue paper `false floor', and the gray box indicates the
duration of stance. The bar graph (right) shows the net energy changes during
the step (between the start and end of the traces on the left). Two response
modes were observed: in most cases the body dynamics of the bird match the
conservative spring-mass model (as shown in C), converting lost
PEg to forward KE (D, top graphs). In some cases,
however, the limb muscles absorb net energy, decreasing the total body
mechanical energy (Ecom; D, bottom graphs). The different
response modes are associated with different limb postures when the foot
contacts the ground (Daley and Biewener,
2006; Daley et al.,
2006).