Figure 5.1. Initial schematic of the interaction of two bodies. interaction); are the components of the velocities of the centers of mass along axes The equations of motion around the centers of mass in the projections on the connected axes (Euler equations) where are the main central moments of inertia; are the components of angular velocities and the radius vectors of the point of interaction in projections into theconnected axes; the components of vector F on axes and zare defined by the direction cosines of angles It is assumed that at the point of interaction there is a deformation 6, and it slips from the deformations of three shock absorbers the direction of which, relative to vector F, is defined by the direction cosines of angles , (in this case The forces of the shock absorbers depend on deformations and their first derivatives, that is, the shock absorbers are considered noninertial
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