A typical vector (i.e., a vector such as the radius vector )
is transformed to its negative under inversion of its
coordinate axes. Such "proper" vectors are known as polar
vectors. A vector-like object which is invariant under inversion is called a
pseudovector, also called an axial vector (as a result of such vectors frequently
arising as vectors describing rotation; Arfken 1985, p. 128; Morse and Feshbach
1953). The cross product
(1)
|
is a pseudovector, whereas the vector triple product
(2)
|
is a polar vector. (Polar) vectors and pseudovectors are interrelated in the following ways under application of the cross product,
(3)
|
(4)
|
Examples of pseudovectors therefore include the angular velocity vector , angular momentum
, torque
, auxiliary magnetic field
, and magnetic dipole moment
.
Given a transformation matrix ,
(5)
|
where Einstein summation has been used.