Notations for the moments and principal axes.
The matrix of inertia being a real matrix (whose elements consist
entirely of real numbers) and a symmetric matrix, there exists an
orthonormal basis of vectors in
this matrix of inertia.
The principal axes are defined by vectors and
inertia principal moments are expressed by
.
with and the transpose of .
Note:
is an orthonormal direct basis.
Expression in Any Axis System
I is the matrix of inertia with respect to orthonormal basis
Oxyz.
Huygen's theorem is used to transform the matrix of inertia:
OxyzPxyz (parallel axis theorem).
Let I' be the matrix of inertia with respect to orthonormal
basis Pxyz where , and
M = {u,v,w}: transformation matrix from basis (Pxyz) to basis
(Puvw) TM is the transposed matrix of matrix M.
J is the matrix of inertia with respect to an orthonormal basis
Puvw:
J = TM.I'.M