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6.4. Transformations of the Euclidean space, ℝ3

So far we have mostly only been considering linear transformations of ℝ2, even though the definitions are stated for ℝn. In this section we will briefly consider linear transformations of ℝ3, and in particular we would like to understand how to think about them as 3×3 matrices.

As usual, we will consider the standard basis vectors

e1=(100) , e2=(010) and e3=(001) in ℝ3. 

Analogous to the 2-dimensional case, we define the scalars ai⁢j for 1≤i,j≤3 by the equations

T⁢(e1) =a11⁢e1+a21⁢e2+a31⁢e3
T⁢(e2) =a12⁢e1+a22⁢e2+a32⁢e3
T⁢(e3) =a13⁢e1+a23⁢e2+a33⁢e3

and write A=(ai⁢j). So A is the matrix associated to the linear transformation T.

Conversely, every matrix A∈M3⁡(ℝ) defines a linear transformation T:ℝ3→ℝ3 by T⁢(v):=A⁢v, via matrix multiplication. In this way, we have a bijective correspondence between linear transformations and matrices, as described in Section 6.2.

Example 6.4.1.

    1. (a)

      Any translation

      T:(xyz)↦(x+ay+bz+c) with (abc)≠(000)

      is not a linear transformation.

    2. (b)

      Let T:ℝ2→ℝ2 be a linear transformation of the plane and A=(ai⁢j) its associated 2×2 matrix. Then the map

      S:(xyz)↦(a11⁢x+a12⁢ya21⁢x+a22⁢yz)=(A⁢(xy)z)

      is a linear transformation. Its associated matrix is

      B=(a11a120a21a220001)=(A00001).

      In particular, we can take T=Rθ or T=Hθ as in Proposition 6.2.8 and 6.2.9. They are given by the matrices

      Rθ=(cos⁡θ-sin⁡θ0sin⁡θcos⁡θ0001) and Hθ=(cos⁡2⁢θsin⁡2⁢θ0sin⁡2⁢θ-cos⁡2⁢θ0001).
    3. (c)

      The reflection in any plane is a linear transformation. For instance, the reflection in the x⁢y-plane, which fixes e1,e2 and sends e3 to -e3 is given by the diagonal matrix (10001000-1).