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Exercise 3.2 · Q18

Q.If A=[0−tan⁡α2tan⁡α20]A = \begin{bmatrix} 0 & -\tan \frac{\alpha}{2} \\ \tan \frac{\alpha}{2} & 0 \end{bmatrix} and II is the identity matrix of order 2, show that I+A=(I−A)[cos⁡α−sin⁡αsin⁡αcos⁡α]I + A = (I - A) \begin{bmatrix} \cos \alpha & -\sin \alpha \\ \sin \alpha & \cos \alpha \end{bmatrix}.

Puducherry CbseNCERTSubjective· 3mImportance★★★★★est
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This problem uses the Cayley transform to connect a skew-symmetric matrix AA (built from tan⁡(α/2)\tan(\alpha/2)) with a rotation matrix. By computing I+AI+A and I−AI-A, then verifying (I−A)−1(I+A)(I-A)^{-1}(I+A) equals the rotation matrix, we show the given identity holds.

The core idea here is beautiful: any rotation matrix can be expressed as a rational function of a skew-symmetric matrix. This is the Cayley transform for rotations. The matrix AA is skew-symmetric (AT=−AA^T = -A), and the matrix [cos⁡α−sin⁡αsin⁡αcos⁡α]\begin{bmatrix} \cos\alpha & -\sin\alpha \\ \sin\alpha & \cos\alpha \end{bmatrix} is a rotation by angle α\alpha. The identity I+A=(I−A)RI+A = (I-A)R is equivalent to R=(I−A)−1(I+A)R = (I-A)^{-1}(I+A), which is exactly the Cayley transform formula.

Let’s work through it step by step.

  1. Write down the given matrices. We have

A=[0−tan⁡α2tan⁡α20],I=[1001].A = \begin{bmatrix} 0 & -\tan\frac{\alpha}{2} \\ \tan\frac{\alpha}{2} & 0 \end{bmatrix}, \quad I = \begin{bmatrix} 1 & 0 \\ 0 & 1 \end{bmatrix}.

Let t=tan⁡α2t = \tan\frac{\alpha}{2} for brevity. Then A=[0−tt0]A = \begin{bmatrix} 0 & -t \\ t & 0 \end{bmatrix}.

  1. Compute I+AI+A and I−AI-A.

I+A=[1−tt1],I−A=[1t−t1].I+A = \begin{bmatrix} 1 & -t \\ t & 1 \end{bmatrix}, \quad I-A = \begin{bmatrix} 1 & t \\ -t & 1 \end{bmatrix}.

  1. The goal is to show I+A=(I−A)RI+A = (I-A)R, where R=[cos⁡α−sin⁡αsin⁡αcos⁡α]R = \begin{bmatrix} \cos\alpha & -\sin\alpha \\ \sin\alpha & \cos\alpha \end{bmatrix}.

    This is equivalent to showing R=(I−A)−1(I+A)R = (I-A)^{-1}(I+A), provided I−AI-A is invertible. Let’s check: det⁡(I−A)=1⋅1−(t)(−t)=1+t2≠0\det(I-A) = 1\cdot1 - (t)(-t) = 1 + t^2 \neq 0, so it’s invertible.

  2. Find (I−A)−1(I-A)^{-1}.

    For a 2×22\times2 matrix [abcd]\begin{bmatrix} a & b \\ c & d \end{bmatrix}, the inverse is 1ad−bc[d−b−ca]\frac{1}{ad-bc}\begin{bmatrix} d & -b \\ -c & a \end{bmatrix}.

    Here a=1a=1, b=tb=t, c=−tc=-t, d=1d=1, so det⁡=1(1)−t(−t)=1+t2\det = 1(1) - t(-t) = 1+t^2.

    Thus

(I−A)−1=11+t2[1−tt1].(I-A)^{-1} = \frac{1}{1+t^2} \begin{bmatrix} 1 & -t \\ t & 1 \end{bmatrix}.

  1. Compute (I−A)−1(I+A)(I-A)^{-1}(I+A).

(I−A)−1(I+A)=11+t2[1−tt1][1−tt1].(I-A)^{-1}(I+A) = \frac{1}{1+t^2} \begin{bmatrix} 1 & -t \\ t & 1 \end{bmatrix} \begin{bmatrix} 1 & -t \\ t & 1 \end{bmatrix}.

Multiply the matrices:

  • Top-left: 1⋅1+(−t)⋅t=1−t21\cdot1 + (-t)\cdot t = 1 - t^2
  • Top-right: 1⋅(−t)+(−t)⋅1=−t−t=−2t1\cdot(-t) + (-t)\cdot1 = -t - t = -2t
  • Bottom-left: t⋅1+1⋅t=t+t=2tt\cdot1 + 1\cdot t = t + t = 2t
  • Bottom-right: t⋅(−t)+1⋅1=−t2+1=1−t2t\cdot(-t) + 1\cdot1 = -t^2 + 1 = 1 - t^2 So

(I−A)−1(I+A)=11+t2[1−t2−2t2t1−t2].(I-A)^{-1}(I+A) = \frac{1}{1+t^2} \begin{bmatrix} 1-t^2 & -2t \\ 2t & 1-t^2 \end{bmatrix}.

  1. Now use the double-angle formulas. …

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