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An orthogonal matrix is a square matrix that has rows and columns equal to orthogonal unit vectors.

The classification of these matrices is more complicated in higher dimensions, but for 2×22\times 2 matrices, there are only two types of orthogonal matrices, as we will now show.

Suppose that we have a 2×22\times 2 orthogonal matrix AA: A=[abcd]A=\left[ \begin{array}{ccc} a & b \\ c & d \end{array} \right] Then the following conditions hold: a2+b2=1a^2+b^2=1 c2+d2=1c^2+d^2=1 ac+bd=0ac+bd=0 Without loss of generality, let a=cos⁡θa=\cos\theta and b=sin⁡θb=\sin\theta. Then we have the following: c2+d2=1c^2+d^2=1 ccos⁡θ+dsin⁡θ=0c\cos\theta+d\sin\theta=0 Solving for cc, we find that c=−dtan⁡θc=-d\tan\theta. Plugging into the first equation, d2+(−dtan⁡θ)2=1d^2+(-d\tan\theta)^2=1 d2sec⁡2θ=1d^2\sec^2\theta=1 d=cos⁡θ,−cos⁡θd=\cos\theta, -\cos\theta c=−sin⁡θ,sin⁡θc=-\sin\theta, \sin\theta Thus, any 2×22\times 2 orthogonal matrix has one of the following two forms: A=[cos⁡θsin⁡θ−sin⁡θcos⁡θ]A=\left[ \begin{array}{ccc} \cos\theta & \sin\theta \\ -\sin\theta & \cos\theta \end{array} \right] A=[cos⁡θsin⁡θsin⁡θ−cos⁡θ]A=\left[ \begin{array}{ccc} \cos\theta & \sin\theta \\ \sin\theta & -\cos\theta \end{array} \right] These are more than just simple expressions for orthogonal matrices; these forms both have distinct meanings in the language of linear transformations.

The first form is a rotation. This matrix will rotate every vector by an angle −θ-\theta (Whoops!). The second form is a reflection. This matrix will reflect every vector across the line defined by polar angle θ2\frac{\theta}{2} (Again, watch out!).

Type a concept, like “slope” or “photosynthesis”.

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