In the converse case the problem is solved in several stages or with numerical methods. The equivalent physical model, in which the deformation of the shock 1. Let us examine the first limit case: the initial stage of the longitudinal shock absorber is absent is simplified: Figure 5.11 [left]. Dependence on the coefficient of friction. Figure 5.12 [right]. Dependence of the equivalent masses and applied rigidity for various types of shock absorption systems. X-axes in degrees.
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