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Orthogonal Transformation


An orthogonal transformation is a linear transformation T:V->V on a finite-dimensional real vector space that preserves a positive definite inner product. In particular, an orthogonal transformation preserves lengths of vectors and angles between vectors,

 <v,w>=<Tv,Tw>.
(1)

In three dimensions, an orthogonal transformation is either a rigid rotation or an improper rotation (a rotation followed by a flip). If F is the flip and R the rotation, then flipping followed by rotating has the form RF=F(FRF). Thus it can also be realized by a suitable rotation followed by the same flip, though in general this rotation is not R^(-1). Orthogonal transformations may be represented using orthogonal matrices; their set forms the orthogonal group.

Any linear transformation in three dimensions

x_1^'=a_(11)x_1+a_(12)x_2+a_(13)x_3
(2)
x_2^'=a_(21)x_1+a_(22)x_2+a_(23)x_3
(3)
x_3^'=a_(31)x_1+a_(32)x_2+a_(33)x_3
(4)

satisfying the orthogonality condition

 a_(ij)a_(ik)=delta_(jk),
(5)

where Einstein summation has been used and delta_(ij) is the Kronecker delta, is an orthogonal transformation. If A:R^n->R^n is an orthogonal transformation, then det(A)=+/-1.


See also

Improper Rotation, Inner Product, Lie Group, Linear Transformation, Lorentz Transformation, Matrix, Orthogonal Group, Orthogonal Matrix, Orthogonality Condition, Rotation, Unitary Transformation

Portions of this entry contributed by Todd Rowland

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Cite this as:

Weisstein, Eric W., with contributions by Todd Rowland. "Orthogonal Transformation." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/OrthogonalTransformation.html

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