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Figure 1


Fig. 1. (A) Spring-mass model (or `spring-loaded inverted pendulum', SLIP) for the dynamics of legged terrestrial locomotion. The body is represented by a point mass m, located at the body center of mass (CoM; black circle), and the leg by a linear compression spring with leg stiffness kleg and contact angle {theta}o. (B) Despite its simplicity, the spring-mass model accurately describes the fluctuations in mechanical energy of the body during running (PEg, gravitational potential energy; KEv and KEh, vertical and horizontal kinetic energy, respectively; Ecom, center of mass energy) (Daley and Biewener, 2006; Daley et al., 2006). (C) Furthermore, all terrestrial animals appear to exhibit spring-mass dynamics, whether they run on two, four, six or eight legs. Multiple legs act in concert to produce the effective `leg-spring' dynamics (Holmes et al., 2006). (D) Similarly, a lateral spring-mass model describes well the medio-lateral dynamics of cockroach locomotion, in which three legs operate as a single effective `leg-spring' in the medio-lateral plane (Full et al., 2002).





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