Conformal linear transformation explained

A conformal linear transformation, also called a homogeneous similarity transformation or homogeneous similitude, is a similarity transformation of a Euclidean or pseudo-Euclidean vector space which fixes the origin. It can be written as the composition of an orthogonal transformation (an origin-preserving rigid transformation) with a uniform scaling (dilation). All similarity transformations (which globally preserve the shape but not necessarily the size of geometric figures) are also conformal (locally preserve shape). Similarity transformations which fix the origin also preserve scalar–vector multiplication and vector addition, making them linear transformations.

Every origin-fixing reflection or dilation is a conformal linear transformation, as is any composition of these basic transformations, including rotations and improper rotations and most generally similarity transformations. However, shear transformations and non-uniform scaling are not. Conformal linear transformations come in two types, proper transformations preserve the orientation of the space whereas improper transformations reverse it.

As linear transformations, conformal linear transformations are representable by matrices once the vector space has been given a basis, composing with each-other and transforming vectors by matrix multiplication. The Lie group of these transformations has been called the conformal orthogonal group, the conformal linear transformation group or the homogeneous similtude group.

Alternatively any conformal linear transformation can be represented as a versor (geometric product of vectors);[1] every versor and its negative represent the same transformation, so the versor group (also called the Lipschitz group) is a double cover of the conformal orthogonal group.

Conformal linear transformations are a special type of Möbius transformations (conformal transformations mapping circles to circles); the conformal orthogonal group is a subgroup of the conformal group.

General properties

Across all dimensions, a conformal linear transformation has the following properties:

Two dimensions

In the Euclidean vector plane, an improper conformal linear transformation is a reflection across a line through the origin composed with a positive dilation. Given an orthonormal basis, it can be represented by a matrix of the form

\begin{bmatrix}a&b\\b&-a\end{bmatrix}.

A proper conformal linear transformation is a rotation about the origin composed with a positive dilation. It can be represented by a matrix of the form

\begin{bmatrix}a&-b\\b&a\end{bmatrix}.

Alternately a proper conformal linear transformation can be represented by a complex number of the form

a+bi.

Practical applications

When composing multiple linear transformations, it is possible to create a shear/skew by composing a parent transform with a non-uniform scale, and a child transform with a rotation. Therefore, in situations where shear/skew is not allowed, transformation matrices must also have uniform scale in order to prevent a shear/skew from appearing as the result of composition. This implies conformal linear transformations are required to prevent shear/skew when composing multiple transformations.

In physics simulations, a sphere (or circle, hypersphere, etc.) is often defined by a point and a radius. Checking if a point overlaps the sphere can therefore be performed by using a distance check to the center. With a rotation or flip/reflection, the sphere is symmetric and invariant, therefore the same check works. With a uniform scale, only the radius needs to be changed. However, with a non-uniform scale or shear/skew, the sphere becomes "distorted" into an ellipsoid, therefore the distance check algorithm does not work correctly anymore.

Notes and References

  1. Staples . G.S. . Wylie . D. . 2015 . Clifford algebra decompositions of conformal orthogonal group elements . Clifford Analysis, Clifford Algebras and Their Applications . 4 . 223–240 .
  2. Amir-Moez . Ali R. . Conformal Linear Transformations . Mathematics Magazine . 1967 . 40 . 5 . 268–270 . Taylor & Francis, Ltd. . 10.2307/2688286 . 2688286 . 2023-07-26.