In analytic geometry, spatial transformations in the 3-dimensional Euclidean space are distinguished into **active** or **alibi transformations**, and **passive** or **alias transformations**. An **active transformation**^{[1]} is a transformation which actually changes the physical position (alibi, elsewhere) of a point, or rigid body, which can be defined in the absence of a coordinate system; whereas a **passive transformation**^{[2]} is merely a change in the coordinate system in which the object is described (alias, other name) (change of coordinate map, or change of basis). By *transformation*, mathematicians usually refer to active transformations, while physicists and engineers could mean either. Both types of transformation can be represented by a combination of a translation and a linear transformation.

Put differently, a *passive* transformation refers to description of the *same* object in two different coordinate systems.^{[3]}
On the other hand, an *active transformation* is a transformation of one or more objects with respect to the same coordinate system. For instance, active transformations are useful to describe successive positions of a rigid body. On the other hand, passive transformations may be useful in human motion analysis to observe the motion of the tibia relative to the femur, that is, its motion relative to a (*local*) coordinate system which moves together with the femur, rather than a (*global*) coordinate system which is fixed to the floor.^{[3]}

## Example

As an example, let the vector , be a vector in the plane. A rotation of the vector through an angle θ in counterclockwise direction is given by the rotation matrix:

which can be viewed either as an *active transformation* or a *passive transformation* (where the above matrix will be inverted), as described below.

## Spatial transformations in the Euclidean space

In general a spatial transformation may consist of a translation and a linear transformation. In the following, the translation will be omitted, and the linear transformation will be represented by a 3×3-matrix .

### Active transformation

As an active transformation, transforms the initial vector into a new vector .

If one views as a new basis, then the coordinates of the new vector in the new basis are the same as those of in the original basis. Note that active transformations make sense even as a linear transformation into a different vector space. It makes sense to write the new vector in the unprimed basis (as above) only when the transformation is from the space into itself.

### Passive transformation

On the other hand, when one views as a passive transformation, the initial vector is left unchanged, while the coordinate system and its basis vectors are transformed in the opposite direction, that is, with the inverse transformation .
^{[4]} This gives a new coordinate system XYZ with basis vectors:

The new coordinates of with respect to the new coordinate system XYZ are given by:

- .

From this equation one sees that the new coordinates are given by

- .

As a passive transformation transforms the old coordinates into the new ones.

Note the equivalence between the two kinds of transformations: the coordinates of the new point in the active transformation and the new coordinates of the point in the passive transformation are the same, namely

- .

## See also

## References

**^**Weisstein, Eric W. "Alibi Transformation." From MathWorld--A Wolfram Web Resource.**^**Weisstein, Eric W. "Alias Transformation." From MathWorld--A Wolfram Web Resource.- ^
^{a}^{b}Joseph K. Davidson, Kenneth Henderson Hunt (2004). "§4.4.1 The active interpretation and the active transformation".*Robots and screw theory: applications of kinematics and statics to robotics*. Oxford University Press. p. 74*ff*. ISBN 0-19-856245-4. **^**Amidror, Isaac (2007). "Appendix D: Remark D.12".*The theory of the Moiré phenomenon: Aperiodic layers*. Springer. p. 346. ISBN 978-1-4020-5457-0.

- Dirk Struik (1953)
*Lectures on Analytic and Projective Geometry*, page 84, Addison-Wesley.