Abstract Suppose that the ellipsoid of inertia of a rigid body relative to a fixed point O is an ellipsoid of revolution, i.e., A 1 = A 2, whereas the center of gravity of the body lies on the axis of dynamic symmetry of the body. Let us introduce the moving and fixed systems of coordinates Oxyz and Ox 1 y 1 z 1 in the following way (Fig. 3.1):
Lagrange’s Case
01.01.2017
14 pages
Aufsatz/Kapitel (Buch)
Elektronische Ressource
Englisch
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