← Back to all lessons
Class 12Trigonometry10:03Published 27 Jun 2025

Inverse Trigonometry Solutions: Exercise 2.2

Worked solutions to the key questions of Class 12 inverse trigonometry Exercise 2.2, using the substitution trick to prove identities and simplify expressions.

This lesson walks through seven important problems from Exercise 2.2 on inverse trigonometric functions. Each one uses the same core idea: substitute the variable as a sine, cosine, secant, or tangent so the expression collapses to a known angle. Along the way we prove the double angle and triple angle identities and simplify several awkward looking inverse expressions down to clean fractions of the original angle.

What you'll learn

  • How to simplify inverse trig expressions by substituting the variable as a sine, cosine, or tangent
  • How to prove the double and triple angle identities for inverse sine and inverse cosine
  • How to reduce expressions with square roots and half angle forms to a simple multiple of the original angle

Lesson chapters

0:00Proving the inverse sine double angle identity
1:36The same expression equals twice inverse cosine
3:09Triple angle identities for inverse sine and cosine
4:50Simplifying a square root over x expression
6:49Simplifying using secant substitution
8:13A half angle simplification
8:47Simplifying cos minus sin over cos plus sin

Lesson notes

This lesson solves the important questions of Exercise 2.2 on inverse trigonometric functions. The common strategy throughout is to substitute the variable as a suitable trig function (a sine, cosine, secant, or tangent) so that each expression reduces to a known angle and the identity falls out.

Proving sin⁡−1 ⁣(2x1−x2)=2sin⁡−1x\sin^{-1}\!\big(2x\sqrt{1-x^2}\big) = 2\sin^{-1}x

This holds for −12≤x≤12-\tfrac{1}{\sqrt 2} \le x \le \tfrac{1}{\sqrt 2}. Start from the left side and put x=sin⁡θx = \sin\theta, so that θ=sin⁡−1x\theta = \sin^{-1}x.

LHS=sin⁡−1 ⁣(2sin⁡θ 1−sin⁡2θ)=sin⁡−1 ⁣(2sin⁡θ cos⁡2θ)\text{LHS} = \sin^{-1}\!\big(2\sin\theta\,\sqrt{1-\sin^2\theta}\big) = \sin^{-1}\!\big(2\sin\theta\,\sqrt{\cos^2\theta}\big)

Since cos⁡2θ=cos⁡θ\sqrt{\cos^2\theta} = \cos\theta on this range,

=sin⁡−1 ⁣(2sin⁡θcos⁡θ)=sin⁡−1 ⁣(sin⁡2θ),= \sin^{-1}\!\big(2\sin\theta\cos\theta\big) = \sin^{-1}\!\big(\sin 2\theta\big),

using 2sin⁡θcos⁡θ=sin⁡2θ2\sin\theta\cos\theta = \sin 2\theta. This simplifies to 2θ=2sin⁡−1x2\theta = 2\sin^{-1}x, which is the right side.

The same expression equals 2cos⁡−1x2\cos^{-1}x

For 12≤x≤1\tfrac{1}{\sqrt 2} \le x \le 1, the same left side equals 2cos⁡−1x2\cos^{-1}x. Here we want the answer in terms of cosine, so put x=cos⁡θx = \cos\theta, giving θ=cos⁡−1x\theta = \cos^{-1}x.

LHS=sin⁡−1 ⁣(2cos⁡θ 1−cos⁡2θ)=sin⁡−1 ⁣(2cos⁡θ sin⁡2θ)\text{LHS} = \sin^{-1}\!\big(2\cos\theta\,\sqrt{1-\cos^2\theta}\big) = \sin^{-1}\!\big(2\cos\theta\,\sqrt{\sin^2\theta}\big)

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

=sin⁡−1 ⁣(2sin⁡θcos⁡θ)=sin⁡−1 ⁣(sin⁡2θ)=2θ=2cos⁡−1x.= \sin^{-1}\!\big(2\sin\theta\cos\theta\big) = \sin^{-1}\!\big(\sin 2\theta\big) = 2\theta = 2\cos^{-1}x.

Triple angle identities

3sin⁡−1x=sin⁡−1 ⁣(3x−4x3)3\sin^{-1}x = \sin^{-1}\!\big(3x - 4x^3\big)

We use the known identity 3sin⁡θ−4sin⁡3θ=sin⁡3θ3\sin\theta - 4\sin^3\theta = \sin 3\theta. Put x=sin⁡θx = \sin\theta, so θ=sin⁡−1x\theta = \sin^{-1}x, and start from the right side.

RHS=sin⁡−1 ⁣(3sin⁡θ−4sin⁡3θ)=sin⁡−1 ⁣(sin⁡3θ)=3θ=3sin⁡−1x=LHS.\text{RHS} = \sin^{-1}\!\big(3\sin\theta - 4\sin^3\theta\big) = \sin^{-1}\!\big(\sin 3\theta\big) = 3\theta = 3\sin^{-1}x = \text{LHS}.

3cos⁡−1x=cos⁡−1 ⁣(4x3−3x)3\cos^{-1}x = \cos^{-1}\!\big(4x^3 - 3x\big)

For x∈[12,1]x \in \left[\tfrac{1}{2}, 1\right], use 4cos⁡3θ−3cos⁡θ=cos⁡3θ4\cos^3\theta - 3\cos\theta = \cos 3\theta. Put x=cos⁡θx = \cos\theta in the right side.

RHS=cos⁡−1 ⁣(4cos⁡3θ−3cos⁡θ)=cos⁡−1 ⁣(cos⁡3θ)=3θ=3cos⁡−1x=LHS.\text{RHS} = \cos^{-1}\!\big(4\cos^3\theta - 3\cos\theta\big) = \cos^{-1}\!\big(\cos 3\theta\big) = 3\theta = 3\cos^{-1}x = \text{LHS}.

Simplifying tan⁡−1 ⁣1+x2−1x\tan^{-1}\!\dfrac{\sqrt{1+x^2}-1}{x}

For x≠0x \neq 0, put x=tan⁡θx = \tan\theta, so θ=tan⁡−1x\theta = \tan^{-1}x.

tan⁡−11+tan⁡2θ−1tan⁡θ=tan⁡−1sec⁡2θ−1tan⁡θ=tan⁡−1sec⁡θ−1tan⁡θ,\tan^{-1}\frac{\sqrt{1+\tan^2\theta}-1}{\tan\theta} = \tan^{-1}\frac{\sqrt{\sec^2\theta}-1}{\tan\theta} = \tan^{-1}\frac{\sec\theta - 1}{\tan\theta},

using 1+tan⁡2θ=sec⁡2θ1 + \tan^2\theta = \sec^2\theta. Rewriting in sines and cosines,

=tan⁡−11cos⁡θ−1sin⁡θcos⁡θ=tan⁡−11−cos⁡θsin⁡θ.= \tan^{-1}\frac{\tfrac{1}{\cos\theta} - 1}{\tfrac{\sin\theta}{\cos\theta}} = \tan^{-1}\frac{1 - \cos\theta}{\sin\theta}.

Now use the half angle forms 1−cos⁡θ=2sin⁡2θ21 - \cos\theta = 2\sin^2\tfrac{\theta}{2} and sin⁡θ=2sin⁡θ2cos⁡θ2\sin\theta = 2\sin\tfrac{\theta}{2}\cos\tfrac{\theta}{2}:

=tan⁡−12sin⁡2θ22sin⁡θ2cos⁡θ2=tan⁡−1 ⁣(tan⁡θ2)=θ2=12tan⁡−1x.= \tan^{-1}\frac{2\sin^2\tfrac{\theta}{2}}{2\sin\tfrac{\theta}{2}\cos\tfrac{\theta}{2}} = \tan^{-1}\!\big(\tan\tfrac{\theta}{2}\big) = \frac{\theta}{2} = \frac{1}{2}\tan^{-1}x.

Simplifying tan⁡−1 ⁣1x2−1\tan^{-1}\!\dfrac{1}{\sqrt{x^2-1}}

For ∣x∣>1|x| > 1, put x=sec⁡θx = \sec\theta, so θ=sec⁡−1x\theta = \sec^{-1}x, and use sec⁡2θ−1=tan⁡2θ\sec^2\theta - 1 = \tan^2\theta.

tan⁡−11sec⁡2θ−1=tan⁡−11tan⁡2θ=tan⁡−11tan⁡θ=tan⁡−1 ⁣(cot⁡θ).\tan^{-1}\frac{1}{\sqrt{\sec^2\theta - 1}} = \tan^{-1}\frac{1}{\sqrt{\tan^2\theta}} = \tan^{-1}\frac{1}{\tan\theta} = \tan^{-1}\!\big(\cot\theta\big).

Writing cot⁡θ=tan⁡ ⁣(π2−θ)\cot\theta = \tan\!\big(\tfrac{\pi}{2} - \theta\big),

=tan⁡−1tan⁡ ⁣(π2−θ)=π2−θ=π2−sec⁡−1x.= \tan^{-1}\tan\!\Big(\frac{\pi}{2} - \theta\Big) = \frac{\pi}{2} - \theta = \frac{\pi}{2} - \sec^{-1}x.

A half angle simplification

Simplify tan⁡−11−cos⁡x1+cos⁡x\tan^{-1}\sqrt{\dfrac{1 - \cos x}{1 + \cos x}}. Use 1−cos⁡x=2sin⁡2x21 - \cos x = 2\sin^2\tfrac{x}{2} and 1+cos⁡x=2cos⁡2x21 + \cos x = 2\cos^2\tfrac{x}{2}:

tan⁡−12sin⁡2x22cos⁡2x2=tan⁡−1tan⁡2x2=tan⁡−1 ⁣(tan⁡x2)=x2.\tan^{-1}\sqrt{\frac{2\sin^2\tfrac{x}{2}}{2\cos^2\tfrac{x}{2}}} = \tan^{-1}\sqrt{\tan^2\tfrac{x}{2}} = \tan^{-1}\!\big(\tan\tfrac{x}{2}\big) = \frac{x}{2}.

Simplifying tan⁡−1 ⁣cos⁡x−sin⁡xcos⁡x+sin⁡x\tan^{-1}\!\dfrac{\cos x - \sin x}{\cos x + \sin x}

This is for −π4<x<π4-\tfrac{\pi}{4} < x < \tfrac{\pi}{4}. Divide the numerator and denominator by cos⁡x\cos x:

tan⁡−1cos⁡x−sin⁡xcos⁡x+sin⁡x=tan⁡−11−tan⁡x1+tan⁡x.\tan^{-1}\frac{\cos x - \sin x}{\cos x + \sin x} = \tan^{-1}\frac{1 - \tan x}{1 + \tan x}.

Using the identity 1−tan⁡x1+tan⁡x=tan⁡ ⁣(π4−x)\dfrac{1 - \tan x}{1 + \tan x} = \tan\!\big(\tfrac{\pi}{4} - x\big),

=tan⁡−1tan⁡ ⁣(π4−x)=π4−x.= \tan^{-1}\tan\!\Big(\frac{\pi}{4} - x\Big) = \frac{\pi}{4} - x.

Key takeaways

  • Substituting x=sin⁡θx = \sin\theta, cos⁡θ\cos\theta, tan⁡θ\tan\theta, or sec⁡θ\sec\theta turns a messy inverse expression into a known angle.
  • The double and triple angle identities (sin⁡2θ\sin 2\theta, 3sin⁡θ−4sin⁡3θ3\sin\theta - 4\sin^3\theta, 4cos⁡3θ−3cos⁡θ4\cos^3\theta - 3\cos\theta) are what let you collapse sin⁡−1(sin⁡kθ)\sin^{-1}(\sin k\theta) to kθk\theta.
  • Half angle forms 1−cos⁡x=2sin⁡2x21 - \cos x = 2\sin^2\tfrac{x}{2} and 1+cos⁡x=2cos⁡2x21 + \cos x = 2\cos^2\tfrac{x}{2} simplify square root expressions to a clean x2\tfrac{x}{2}.