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NCERT Exemplar · Q9

Q.If 2tan⁡−1(cos⁡θ)=tan⁡−1(2csc⁡θ)2\tan^{-1}(\cos\theta)=\tan^{-1}(2\csc\theta), then show that θ=π4\theta=\frac{\pi}{4}.

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Use the identity 2tan⁡−1x=tan⁡−12x1−x22\tan^{-1}x = \tan^{-1}\frac{2x}{1-x^2} to convert the given equation into an algebraic equation in cos⁡θ\cos\theta and csc⁡θ\csc\theta, then simplify to find θ=π4\theta = \frac{\pi}{4}.

The core of this problem is the inverse tangent double-angle identity. When you see 2tan⁡−1(something)2\tan^{-1}(\text{something}), your first instinct should be to rewrite it as a single tan⁡−1\tan^{-1} using:

2tan⁡−1x=tan⁡−12x1−x2,provided ∣x∣<12\tan^{-1}x = \tan^{-1}\frac{2x}{1-x^2}, \quad \text{provided } |x| < 1

Why does this work? Because if tan⁡−1x=α\tan^{-1}x = \alpha, then tan⁡α=x\tan\alpha = x, and tan⁡(2α)=2tan⁡α1−tan⁡2α=2x1−x2\tan(2\alpha) = \frac{2\tan\alpha}{1-\tan^2\alpha} = \frac{2x}{1-x^2}. Taking tan⁡−1\tan^{-1} on both sides gives the identity. The condition ∣x∣<1|x| < 1 ensures the angle stays in the principal range (−π/2,π/2)(-\pi/2, \pi/2), but here we'll check our final answer against the original equation.

Let's apply this to the given equation:

2tan⁡−1(cos⁡θ)=tan⁡−1(2csc⁡θ)2\tan^{-1}(\cos\theta) = \tan^{-1}(2\csc\theta)

  1. Apply the identity to the left-hand side. Let x=cos⁡θx = \cos\theta. Then:

2tan⁡−1(cos⁡θ)=tan⁡−1(2cos⁡θ1−cos⁡2θ)2\tan^{-1}(\cos\theta) = \tan^{-1}\left(\frac{2\cos\theta}{1 - \cos^2\theta}\right)

  1. Simplify the denominator using the Pythagorean identity sin⁡2θ+cos⁡2θ=1\sin^2\theta + \cos^2\theta = 1:

1−cos⁡2θ=sin⁡2θ1 - \cos^2\theta = \sin^2\theta

So the left side becomes:

tan⁡−1(2cos⁡θsin⁡2θ)\tan^{-1}\left(\frac{2\cos\theta}{\sin^2\theta}\right)

  1. Rewrite in terms of cosecant. Since csc⁡θ=1sin⁡θ\csc\theta = \frac{1}{\sin\theta}, we have:

2cos⁡θsin⁡2θ=2cos⁡θ⋅1sin⁡2θ=2cos⁡θ⋅csc⁡2θ\frac{2\cos\theta}{\sin^2\theta} = 2\cos\theta \cdot \frac{1}{\sin^2\theta} = 2\cos\theta \cdot \csc^2\theta

But this isn't yet 2csc⁡θ2\csc\theta. Let's keep it as is for now.

  1. Equate the arguments of tan⁡−1\tan^{-1} on both sides. Since tan⁡−1\tan^{-1} is a one-to-one function on its principal range, if tan⁡−1A=tan⁡−1B\tan^{-1}A = \tan^{-1}B, then A=BA = B. So:

2cos⁡θsin⁡2θ=2csc⁡θ\frac{2\cos\theta}{\sin^2\theta} = 2\csc\theta

  1. Cancel the common factor of 2 (assuming it's non-zero — we'll check later):

cos⁡θsin⁡2θ=csc⁡θ\frac{\cos\theta}{\sin^2\theta} = \csc\theta

  1. Rewrite csc⁡θ\csc\theta as 1/sin⁡θ1/\sin\theta:

cos⁡θsin⁡2θ=1sin⁡θ\frac{\cos\theta}{\sin^2\theta} = \frac{1}{\sin\theta}

  1. Multiply both sides by sin⁡2θ\sin^2\theta (valid as long as sin⁡θ≠0\sin\theta \neq 0; if sin⁡θ=0\sin\theta = 0, the original equation has csc⁡θ\csc\theta undefined, so we can safely assume sin⁡θ≠0\sin\theta \neq 0):

cos⁡θ=sin⁡θ\cos\theta = \sin\theta

  1. Solve the trigonometric equation. cos⁡θ=sin⁡θ\cos\theta = \sin\theta implies:

tan⁡θ=1\tan\theta = 1

The general solution is θ=π4+nπ\theta = \frac{\pi}{4} + n\pi, where nn is an integer.

  1. Check which solution fits the original equation. The original equation involves tan⁡−1(cos⁡θ)\tan^{-1}(\cos\theta) and tan⁡−1(2csc⁡θ)\tan^{-1}(2\csc\theta). For θ=π4\theta = \frac{\pi}{4}:
    • cos⁡π4=12\cos\frac{\pi}{4} = \frac{1}{\sqrt{2}}, so 2tan⁡−1(12)2\tan^{-1}(\frac{1}{\sqrt{2}}) is defined.
    • csc⁡π4=2\csc\frac{\pi}{4} = \sqrt{2}, so tan⁡−1(22)\tan^{-1}(2\sqrt{2}) is defined.
    • Both sides are positive angles less than π/2\pi/2, so the identity holds. …

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