Abstract
In Euler’s case, the principal moment of external forces acting on a rigid body relative to a fixed point is equal to zero \( {\mathbf{L}}_0^e=0 \). The dynamic Euler’s equations (1.27) assume the form:
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Chernousko, F.L., Akulenko, L.D., Leshchenko, D.D. (2017). Motion of a Rigid Body by Inertia. Euler’s Case. In: Evolution of Motions of a Rigid Body About its Center of Mass. Springer, Cham. https://doi.org/10.1007/978-3-319-53928-7_2
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DOI: https://doi.org/10.1007/978-3-319-53928-7_2
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