Active and passive transformation

Active and passive transformation

In the physical sciences, an active transformation is one which actually changes the physical state of a system, and makes sense even in the absence of a coordinate system whereas a passive transformation is merely a change in the coordinate system of no physical significance. The distinction between active and passive transformations is one which should always be kept in mind when working with transformations. By default, by "transformation", mathematicians usually mean passive transformations, while physicists could mean either.

As an example, in the vector space R2, let {e1,e2} be a basis, and consider the vector v = "v"1e1 + "v"2e2. Rotation of the plane is given by the matrix:R=egin{pmatrix}cos heta & -sin heta\sin heta & cos hetaend{pmatrix},which can be viewed either as an active transformation or a passive transformation, as described below.

Active transformation

As an active transformation, "R" rotates all vectors, including v and the basis vectors e1 and e2. Thus a new vector v is obtained::mathbf{u}=Rmathbf{v}=v^1Rmathbf{e}_1+v^2Rmathbf{e}_2.

If one views {"R"e1,"R"e2} as a new basis, then the components of the new vector u in the new basis are the same as those of v in the original basis because linear transformations do not act on scalars, and the components of a vector are simply scalars. One may also calculate the components of the new vector in terms of the old basis, in which case the formula:(Rmathbf{v})^b=R_a{}^bv^ais obtained. But note that active transformations make sense even when it is a linear transformation into a different vector space. It only makes sense to write the new vector in the unprimed basis when the transformation is from the space into itself.

Passive transformation

On the other hand, when one views "R" as a passive transformation, the vector v is left unchanged, while the basis vectors get rotated. In order for the vector to remain fixed, the components in terms of the new basis must also change.:mathbf{v}=v^amathbf{e}_a=v'^aRmathbf{e}_aFrom this equation one sees that the new components with respect to the new coordinates are given by :v'^a=(R^{-1})_b{}^av^bso that:mathbf{v}=v'^amathbf{e}'_a=v^b(R^{-1})_b{}^aR_a{}^cmathbf{e}_c=v^bmathbf{e}_b.Thus, in order for the vector to remain unchanged by the passive transformation, the components of the vector "have to" transform, and according to the inverse of the transformation operator.

ee also

* Covariance and contravariance

References


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