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Mathematics · Ch 5 — Continuity and Differentiability

Derivatives of Inverse Trigonometric Functions

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Derivatives of Inverse Trigonometric Functions

Each inverse trigonometric function is the inverse of a trigonometric function restricted to an

interval on which that function is one-one, and its derivative can be found by writing the

inverse relation as an ordinary (implicit) equation and differentiating both sides -- exactly the

technique Section 5 develops in general, applied here to the six standard inverse functions.

Derivative of sin⁡−1x\sin^{-1}x. Let y=sin⁡−1xy=\sin^{-1}x, for x∈(−1,1)x\in(-1,1) and y∈(−π/2,π/2)y\in(-\pi/2,\pi/2);

this means sin⁡y=x\sin y=x. Differentiating both sides with respect to xx (using the chain rule on

the left, since yy is a function of xx):

cos⁡y⋅dydx=1⟹dydx=1cos⁡y.\cos y\cdot\frac{dy}{dx} = 1 \quad\Longrightarrow\quad \frac{dy}{dx} = \frac{1}{\cos y}.

Since y∈(−π/2,π/2)y\in(-\pi/2,\pi/2), cos⁡y>0\cos y>0, so cos⁡y=1−sin⁡2y=1−x2\cos y=\sqrt{1-\sin^2y}=\sqrt{1-x^2} (taking the

positive root). Hence

ddx(sin⁡−1x)=11−x2,−1<x<1.\frac{d}{dx}\big(\sin^{-1}x\big) = \frac{1}{\sqrt{1-x^2}}, \qquad -1<x<1.

Derivative of cos⁡−1x\cos^{-1}x. By an identical argument with y=cos⁡−1xy=\cos^{-1}x (cos⁡y=x\cos y=x,

y∈(0,π)y\in(0,\pi), so sin⁡y>0\sin y>0 and sin⁡y=1−x2\sin y=\sqrt{1-x^2}): differentiating cos⁡y=x\cos y=x gives

−sin⁡y (dy/dx)=1-\sin y\,(dy/dx)=1, so

ddx(cos⁡−1x)=−11−x2,−1<x<1.\frac{d}{dx}\big(\cos^{-1}x\big) = -\frac{1}{\sqrt{1-x^2}}, \qquad -1<x<1.

(Note sin⁡−1x+cos⁡−1x=π/2\sin^{-1}x+\cos^{-1}x=\pi/2 for all x∈[−1,1]x\in[-1,1] -- a constant -- so their derivatives

must be negatives of each other, exactly as found; this is a useful self-check.)

Derivative of tan⁡−1x\tan^{-1}x. Let y=tan⁡−1xy=\tan^{-1}x, so tan⁡y=x\tan y=x for all real xx, with

y∈(−π/2,π/2)y\in(-\pi/2,\pi/2). Differentiating: sec⁡2y (dy/dx)=1\sec^2y\,(dy/dx)=1, and using sec⁡2y=1+tan⁡2y=1+x2\sec^2y=1+\tan^2y=1+x^2,

ddx(tan⁡−1x)=11+x2,x∈R.\frac{d}{dx}\big(\tan^{-1}x\big) = \frac{1}{1+x^2}, \qquad x\in\mathbb{R}.

Derivative of cot⁡−1x\cot^{-1}x. By the same method with cot⁡y=x\cot y=x: −cosec2y (dy/dx)=1-\text{cosec}^2y\,(dy/dx)=1,

and cosec2y=1+cot⁡2y=1+x2\text{cosec}^2y=1+\cot^2y=1+x^2, so

ddx(cot⁡−1x)=−11+x2,x∈R.\frac{d}{dx}\big(\cot^{-1}x\big) = -\frac{1}{1+x^2}, \qquad x\in\mathbb{R}.

Derivatives of sec⁡−1x\sec^{-1}x and cosec−1x\text{cosec}^{-1}x (for ∣x∣>1|x|>1), obtained the same way from

sec⁡y=x\sec y=x and cosec y=x\text{cosec}\,y=x respectively:

ddx(sec⁡−1x)=1∣x∣x2−1,ddx(cosec−1x)=−1∣x∣x2−1.\frac{d}{dx}\big(\sec^{-1}x\big) = \frac{1}{|x|\sqrt{x^2-1}}, \qquad \frac{d}{dx}\big(\text{cosec}^{-1}x\big) = -\frac{1}{|x|\sqrt{x^2-1}}.

Combined with the chain rule. For a composite argument, e.g. y=sin⁡−1(x2)y=\sin^{-1}(x^2), treat u=x2u=x^2 …