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Geometry of Linear Transformations of the Plane

Let V and W be vector spaces. Recall that a function T:V® W is called a linear transformation if it preserves both vector addition and scalar multiplication:

T(v1+ v2)
=
T(v1) + T(v2)
T(rv1)
=
rT(v1)
for all v1, v2 Î V.

If V = R2 and W = R2, then T:R2 ® R2 is a linear transformation if and only if there exists a 2 ×2 matrix A such that T(v) = Av for all v Î R2. Matrix A is called the standard matrix for T. The columns of A are T [ 1 0 ]T and T [ 0 1 ]T, respectively. Since each linear transformation of the plane has a unique standard matrix, we will identify linear transformations of the plane by their standard matrices. It can be shown that if A is invertible, then the linear transformation defined by A maps parallelograms to parallelograms. We will often illustrate the action of a linear transformation T:R2® R2 by looking at the image of a unit square under T.

Rotations

The standard matrix for the linear transformation T:R2 ®R2 that rotates vectors by an angle q is

A = é
ê
ë
cos q
-sin q
sin q
cos q
ù
ú
û
This is easily derived by noting that
T æ
ç
è
é
ê
ë
1
0
ù
ú
û
ö
÷
ø
=
é
ê
ë
cos q
sin q
ù
ú
û
T æ
ç
è
é
ê
ë
0
1
ù
ú
û
ö
÷
ø
=
é
ê
ë
-sin q
cos q
ù
ú
û
.

Reflections

For every line in the plane, there is a linear transformation that reflects vectors about that line. Reflection about the x-axis is given by the standard matrix

A = é
ê
ë
1
0
0
-1
ù
ú
û
which takes the vector [ x y ]T to [ x -y ]T. Reflection about the y-axis is given by the standard matrix
A = é
ê
ë
-1
0
0
1
ù
ú
û
taking [ x y ]T to [ -x y ]T. Finally, reflection about the line y = x is given by
A = é
ê
ë
0
1
1
0
ù
ú
û
and takes the vector [ x y ]T to [ y x ]T.


Expansions and Compressions

The standard matrix
A = é
ê
ë
k
0
0
1
ù
ú
û
``stretches'' the vector [ x y ]T along the x-axis to [ kx y]T for k > 1 and ``compresses'' it along the x-axis for 0 < k < 1.









Similarly,
A = é
ê
ë
1
0
0
k
ù
ú
û
stretches or compresses vectors [ x y ]T to [ x ky ]T along the y-axis.










Shears

The standard matrix

A = é
ê
ë
1
k
0
1
ù
ú
û
taking vectors [ x y ]T to [ (x+ky) y ]T is called a shear in the x-direction.

Similarly,

A = é
ê
ë
1
0
k
1
ù
ú
û
takes vectors [ x y ]T to [ x (y+kx) ]T and is called a shear in the y-direction.








Notes

  • If finitely many linear transformations from R2 to R2 are performed in succession, then there exists a single linear transformation with the same effect.

  • If the standard matrix for a a transformation T: R2® R2 is invertible, then it can be shown that the geometric effect of T is the same as some sequence of reflections, expansions, compressions, and sheers.

In the following Exploration, you can investigate the connection between the entries in a standard matrix and the effect the corresponding linear transformation has geometrically.

Exploration


Key Concept

For every linear transformation T: R2 ® R2 of the plane, there exists a standard matrix A such that

T(v) = Av     for all v Î R2.
Every linear transformation of the plane with an invertible standard matrix has the geometric effect of a sequence of reflections, expansions, compressions, and shears.