Part of the International Centre for Mechanical Sciences book series (CISM, volume 53)
The tensor of inertia of a rigid body can be represented in the formBoth the moments of inertia A, B, C and the products of inertia D, E, F here appear as the constitutent elements of the tensor of inertia. They are subject to the frequently used inequalities.
Unable to display preview. Download preview PDF.
© Springer-Verlag Wien 1974