rotational invariance of cross product
Theorem
Let R be a rotational matrix, i.e., a real
matrix with and .
Then for all vectors in ,
Proof. Let us first fix some right hand oriented orthonormal basis in . Further, let and be the components of u and v in that basis. Also, in the chosen basis, we denote the entries of R by . Since R is rotational, we have where is the Kronecker delta symbol. Here we use the Einstein summation convention. Thus, in the previous expression, on the left hand side, should be summed over . We shall use the Levi-Civita permutation symbol to write the cross product. Then the :th coordinate of equals . For the th component of we then have
The last line follows since . Since , it follows that
as claimed.
Title | rotational invariance of cross product |
---|---|
Canonical name | RotationalInvarianceOfCrossProduct |
Date of creation | 2013-03-22 13:33:53 |
Last modified on | 2013-03-22 13:33:53 |
Owner | matte (1858) |
Last modified by | matte (1858) |
Numerical id | 6 |
Author | matte (1858) |
Entry type | Theorem |
Classification | msc 15A72 |
Classification | msc 15A90 |