Skip to content

Mathematics · Ch 10 — Differential Calculus – Differentiability and Methods of Differentiation

Substitution method

10.4.5

Substitution method

Some inverse-trigonometric expressions can in principle be differentiated directly by repeated chain-rule and quotient-rule work, but that route is often extremely laborious. The substitution method replaces the algebra with a well-chosen trigonometric substitution that collapses the expression to something much simpler before any differentiation is attempted.

The idea, illustrated. Consider f(x)=tan⁡−1 ⁣(2x1−x2)f(x)=\tan^{-1}\!\left(\dfrac{2x}{1-x^2}\right). Differentiating this directly via the chain and quotient rules is possible but heavy. Instead, substitute x=tan⁡θx=\tan\theta. Then, recognising the double-angle identity for tangent,

2x1−x2=2tan⁡θ1−tan⁡2θ=tan⁡2θ,\frac{2x}{1-x^2} = \frac{2\tan\theta}{1-\tan^2\theta} = \tan2\theta,

so f(x)=tan⁡−1(tan⁡2θ)=2θ=2tan⁡−1xf(x) = \tan^{-1}(\tan2\theta) = 2\theta = 2\tan^{-1}x (using θ=tan⁡−1x\theta=\tan^{-1}x to undo the substitution). Now differentiating this much simpler form is immediate: f′(x)=2⋅11+x2=21+x2f'(x) = 2\cdot\dfrac{1}{1+x^2} = \dfrac{2}{1+x^2}.

Worked illustration — tan⁡−1 ⁣(1+x1−x)\tan^{-1}\!\left(\dfrac{1+x}{1-x}\right). Substitute x=tan⁡θx=\tan\theta. Then 1+x1−x=1+tan⁡θ1−tan⁡θ=tan⁡ ⁣(π4+θ)\dfrac{1+x}{1-x} = \dfrac{1+\tan\theta}{1-\tan\theta} = \tan\!\left(\dfrac\pi4+\theta\right) (the tangent-addition identity, since tan⁡π4=1\tan\tfrac\pi4=1), so

y=tan⁡−1 ⁣(1+x1−x)=π4+θ=π4+tan⁡−1x,y = \tan^{-1}\!\left(\frac{1+x}{1-x}\right) = \frac{\pi}{4}+\theta = \frac{\pi}{4}+\tan^{-1}x,

and since π/4\pi/4 is a constant, y′=11+x2y' = \dfrac{1}{1+x^2} directly — the substitution converts an intractable-looking quotient inside an inverse tangent into "a constant plus tan⁡−1x\tan^{-1}x", whose derivative is read off instantly.

Worked illustration — a cosine-of-inverse-cosine case. For f(x)=cos⁡−1 ⁣(4x3−3x1)f(x)=\cos^{-1}\!\left(\dfrac{4x^3-3x}{1}\right)-type expressions, substitute x=cos⁡θx=\cos\theta and use the triple-angle identity 4cos⁡3θ−3cos⁡θ=cos⁡3θ4\cos^3\theta-3\cos\theta=\cos3\theta: e.g. for f(x)=cos⁡−1(4x3−3x)f(x)=\cos^{-1}(4x^3-3x), with x=cos⁡θx=\cos\theta, 4x3−3x=cos⁡3θ4x^3-3x=\cos3\theta, so f(x)=cos⁡−1(cos⁡3θ)=3θ=3cos⁡−1xf(x)=\cos^{-1}(\cos3\theta)=3\theta=3\cos^{-1}x, giving f′(x)=−31−x2f'(x) = -\dfrac{3}{\sqrt{1-x^2}} immediately, in place of a direct chain-rule computation through a cubic inside an inverse cosine. …