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Question

If P is the plane through $(1/2, -1, 0)$ orthogonal to $(0, 1, 0)$ find an isometry F = TC such that F(P) is the plane through $(1, -2, 1)$ orthogonal to $(1, 0, -1)$.

This is an exercise in O'neill's Elementary Differential Geometry.

I found the given plane P: y = -1 and F(P): x-z=$0$

But that's all I did. How should I approach this problem?

  • There is an infinite number of solutions. Try rotating about their line of intersection. – amd May 13 '20 at 05:39

1 Answers1

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First of all, I agree with your plane equations. The first one is affine whereas the second one is linear (RHS=0).

Let us reduce this affine issue into a linear one by bringing affine plane $y=-1$ onto vector plane $y=0$ (using a translation $T$ by vector $V_T=(0,1,0)^T$) according to the following classical pattern :

$$F(X)=S(X+V_T)-V_T\tag{1}$$

to be understood as the composition :

$$\begin{matrix}X&\overset{F}{\longrightarrow}& S(X+V_T)-V_T & \text{affine level}\\\downarrow && \uparrow\\X+V_T &\longrightarrow & S(X+V_T) & \text{linear level} &\end{matrix}.$$

Therefore, let us work on the associated linear subspaces $P_1$ and $P_2$ with resp. normal vectors $N_1=(0,1,0)^T$ and $N_2=(1,0,1)^T/\sqrt{2}$ (please note the second vector has been normalized).

Instead of a rotation, we can look for a symmetry. This symmetry is with respect to one of the two bissector planes $P_3$ or $P'_3$ of $P_1$ and $P_2$, with resp. normals $N_1+N_2$ and $N_1-N_2$.

Let us consider plane $P_3$ with normal $N_1+N_2 =(1/\sqrt{2} , 1, 1/\sqrt{2})^T$ whose unit norm version is $N_3=(1/2,1/\sqrt{2},1/2)^T$.

Now, use the Householder formula of the symmetry matrix with respect to $P_3$:

$$S=I_3-2N_3N_3^T=\begin{pmatrix}1&0&0\\0&1&0\\0&0&1\end{pmatrix}-2\begin{pmatrix} 1/4&a&1/4\\a&1/2&a\\1/4&a&1/4\end{pmatrix}$$ where

$$a:=1/(2\sqrt{2}).$$

Finally :

$$S=\begin{pmatrix}1/2&-1/\sqrt{2}&-1/2\\-1/\sqrt{2}&0&-1/\sqrt{2}\\-1/2&-1/\sqrt{2}&1/2\end{pmatrix}.$$

It remains to apply (1).

Remark : If $N_1-N_2$ had been taken instead of $N_1+N_2$, we would have obtained different symmetry.

Jean Marie
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