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... In Chap. ... sign cos : By the theorem on the motion of the center of masses in the space in projections to the related axes .x ; y ; z/ and the theorem on the change of the kinematic moment with respect to these axes, we obtain the following complete system of differential equations in the dynamical quasi-velocity space R1 fvg S2 f; g C R3 fx ;y ;z g: v cos P v sin C y v sin sin P 2 2 z v sin cos C .y C z / D Fx =m; v sin cos C v cos ... I2 n0 d cos with variable coefficient....

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