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Angular velocity tensor
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In physics, the angular velocity tensor is defined as a matrix T such that:
It allows us to express the cross product as a matrix multiplication. It is, by definition, a skew-symmetric matrix with zeros on the main diagonal and plus and minus the components of the angular velocity as the other elements:
Coordinate-free descriptionAt a given time instance , the angular velocity tensor is a linear map between the position vectors and their velocity vectors of a rigid body rotating around the origo:
where we omitted the parameter, and regard and as elements of the same 3-dimensional Euclidean vector space .
The relation between this linear map and the angular velocity pseudovector is the following.
Because of T is the derivative of an orthogonal transformation, the
bilinear form is skew-symmetric. (Here stands for the scalar product). So we can apply the fact of exterior algebra that there is a unique linear form on that
,
where is the wedge product of and .
Taking the dual vector L* of L we get
Introducing , as the Hodge dual of L* , and apply further Hodge dual identities we arrive at
where
by definition.
Because is an arbitrary vector, from nondegeneracy of scalar product follows
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