Figure 5.13 [left]. Dependence of the coefficient of recovery on . kN/m; cn = 20 kN/m; kn = 600 kN-s/m; b. degrees; c. ks, Ns/m. Figure 5.14 [right]. Deformation of the longitudinal shock absorber with constant (1) and variable (2) damping . X-axis in seconds. 2. The second limit case: there is no lateral shock absorber , and a purely lateral impact is absorbed only by the flexible rod (Soyuz docking mechanism). The equations for the deformation of the rod and the longitudinal This case is equivalent to the impact of mass through a spring and longitudinal shock absorber. The rigidity of the spring and its deformation . The initial conditions are Analysis of the dependences of the parameters shows that the applied mass and rigidity csee Figure 5.12) decrease rapidly when decreases. The decrease in has an especially strong effect on the shock absorption process, since becomes small, which determines the value of the
RkJQdWJsaXNoZXIy MTU5NjU0Mg==