Within the isometry group of the plane, the product of a rotation and a translation can always be expressed as a single rotation (or translation). On the other hand the product of a reflection and a translation is usually not a reflection, but can produce a transformation with no everyday name: a glide reflection.
For example, there is an isometry consisting of the reflection on the x-axis, followed by translation of one unit parallel to it. In co-ordinates, it takes
(x, y) to (x + 1, −y).
It fixes a system of parallel lines, but is a combination of a reflection in a line and a translation parallel to that line. If one considers the effect of a reflection combined with any translation, it is a glide reflection with respect to a line parallel to the line of the reflection, as one sees by resolving the translation into components parallel and orthogonal to that line.
The length of the glide vector is equal to the length of one of the edges parallel to the mirror of reflection.
The length of the glide vector is the length of one of the edges parallel to its mirror.
Let a and b be translations and g1 and g2 be glidereflections, g1 parallel to a with lenght 1/2 a and g2 parallel to b with lenght 1/2 b, and r1, r2, r3, and r4 be rotations of 180 degrees at each vertex of the fundamental region numbered as before.