Figure 5.6 [left]. Equivalent schematic in the form of the impact of a single body. Figure 5.7 [right]. Equivalent physical model considering the inertia of the shock absorber. Further, system (5.15) is converted so that the equivalent schematic may be represented as the direct impact of mass (Figure 5.7) through a spring and two sequential inertial shock absorbers (with masses of the moving parts , with characteristics and deformations defined by the expressions In the model, as in the initial model, the inertial forces, are transmitted respectively to masses and . In the approximation to direct impact the intermediate shock absorber becomes infinitely rigid and the system of equations is simplified:
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