If D’Alembert principle is used on the particles of a rigid body, the principle would state: When a rigid body that is in equilibrium (either static of dynamic) is subject to virtual compatible displacements, the total virtual work of all external forces is zero; and conversely, if the total virtual work of all external forces acting on a rigid body is zero then the body is in equilibrium. (Lanczos 1970).
CITATION STYLE
Olguín Díaz, E. (2019). Dynamics of a rigid body. In Studies in Systems, Decision and Control (Vol. 191, pp. 231–271). Springer International Publishing. https://doi.org/10.1007/978-3-030-04275-2_5
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