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Mathematics · Ch 5 — Continuity and Differentiability

Derivatives of Inverse Trigonometric Functions

5.3.3

Derivatives of Inverse Trigonometric Functions

Concept and Approach

Inverse trigonometric functions are continuous on their domains (accepted without proof). To differentiate them we combine the chain rule with implicit differentiation: if y=f−1(x)y = f^{-1}(x) then x=f(y)x = f(y), and differentiating both sides w.r.t. xx gives 1=f′(y)⋅dydx1 = f'(y) \cdot \frac{dy}{dx}, so dydx=1f′(y)\frac{dy}{dx} = \frac{1}{f'(y)}. The work lies in expressing this in terms of xx using trigonometric identities and the domain restrictions of the inverse functions.


Derivative of sin⁡−1x\sin^{-1} x

Let y=sin⁡−1xy = \sin^{-1} x, so x=sin⁡yx = \sin y. Differentiating both sides with respect to xx:

1=cos⁡y⋅dydx⇒dydx=1cos⁡y1 = \cos y \cdot \frac{dy}{dx} \quad\Rightarrow\quad \frac{dy}{dx} = \frac{1}{\cos y}

This is defined only when cos⁡y≠0\cos y \neq 0, i.e. y≠±π2y \neq \pm \frac{\pi}{2}, so x≠±1x \neq \pm 1; the derivative exists for x∈(−1,1)x \in (-1, 1). Since sin⁡y=x\sin y = x,

cos⁡2y=1−sin⁡2y=1−x2\cos^2 y = 1 - \sin^2 y = 1 - x^2

As y=sin⁡−1xy = \sin^{-1} x lies in (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right), cos⁡y\cos y is positive, so cos⁡y=1−x2\cos y = \sqrt{1 - x^2}. Therefore:

dydx=11−x2,x∈(−1,1)\frac{dy}{dx} = \frac{1}{\sqrt{1 - x^2}}, \quad x \in (-1, 1)

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

Watch out

The derivative is not defined at x=±1x = \pm 1 (the denominator is zero); sin⁡−1x\sin^{-1} x has vertical tangents there.


Derivative of cos⁡−1x\cos^{-1} x

Let y=cos⁡−1xy = \cos^{-1} x, so x=cos⁡yx = \cos y. Differentiating with respect to xx:

1=−sin⁡y⋅dydx⇒dydx=−1sin⁡y1 = -\sin y \cdot \frac{dy}{dx} \quad\Rightarrow\quad \frac{dy}{dx} = -\frac{1}{\sin y}

This exists when sin⁡y≠0\sin y \neq 0, i.e. y≠0,πy \neq 0, \pi, so x≠±1x \neq \pm 1 and the domain is x∈(−1,1)x \in (-1, 1). Since cos⁡y=x\cos y = x, sin⁡2y=1−x2\sin^2 y = 1 - x^2; and on the range [0,π][0, \pi], sin⁡y\sin y is non-negative, so sin⁡y=1−x2\sin y = \sqrt{1 - x^2}. Therefore:

dydx=−11−x2,x∈(−1,1)\frac{dy}{dx} = -\frac{1}{\sqrt{1 - x^2}}, \quad x \in (-1, 1)

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

Note

Note ddx(cos⁡−1x)=−ddx(sin⁡−1x)\frac{d}{dx}(\cos^{-1} x) = -\frac{d}{dx}(\sin^{-1} x), consistent with sin⁡−1x+cos⁡−1x=π2\sin^{-1} x + \cos^{-1} x = \frac{\pi}{2}, which gives the same relationship on differentiation.


Derivative of tan⁡−1x\tan^{-1} x

Let y=tan⁡−1xy = \tan^{-1} x, so x=tan⁡yx = \tan y. Differentiating with respect to xx:

1=sec⁡2y⋅dydx⇒dydx=1sec⁡2y1 = \sec^2 y \cdot \frac{dy}{dx} \quad\Rightarrow\quad \frac{dy}{dx} = \frac{1}{\sec^2 y}

Using sec⁡2y=1+tan⁡2y=1+x2\sec^2 y = 1 + \tan^2 y = 1 + x^2:

dydx=11+x2\frac{dy}{dx} = \frac{1}{1 + x^2}

which is defined for all real xx, since 1+x2>01 + x^2 > 0.

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


Derivative of cot⁡−1x\cot^{-1} x

Let y=cot⁡−1xy = \cot^{-1} x, so x=cot⁡yx = \cot y. Differentiating with respect to xx:

1=−csc⁡2y⋅dydx⇒dydx=−1csc⁡2y1 = -\csc^2 y \cdot \frac{dy}{dx} \quad\Rightarrow\quad \frac{dy}{dx} = -\frac{1}{\csc^2 y}

Using csc⁡2y=1+cot⁡2y=1+x2\csc^2 y = 1 + \cot^2 y = 1 + x^2:

dydx=−11+x2,x∈R\frac{dy}{dx} = -\frac{1}{1 + x^2}, \quad x \in \mathbb{R}

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

Important

Again ddx(cot⁡−1x)=−ddx(tan⁡−1x)\frac{d}{dx}(\cot^{-1} x) = -\frac{d}{dx}(\tan^{-1} x), consistent with tan⁡−1x+cot⁡−1x=π2\tan^{-1} x + \cot^{-1} x = \frac{\pi}{2}.


Derivative of sec⁡−1x\sec^{-1} x

Let y=sec⁡−1xy = \sec^{-1} x, so x=sec⁡yx = \sec y. Differentiating with respect to xx:

1=sec⁡ytan⁡y⋅dydx⇒dydx=1sec⁡ytan⁡y1 = \sec y \tan y \cdot \frac{dy}{dx} \quad\Rightarrow\quad \frac{dy}{dx} = \frac{1}{\sec y \tan y}

This exists when sec⁡ytan⁡y≠0\sec y \tan y \neq 0; for the range [0,π]∖{π2}[0, \pi] \setminus \{\frac{\pi}{2}\} this holds for ∣x∣>1|x| > 1. Since sec⁡y=x\sec y = x, tan⁡2y=sec⁡2y−1=x2−1\tan^2 y = \sec^2 y - 1 = x^2 - 1, with the sign of tan⁡y\tan y depending on the quadrant:

  • If y∈[0,π2)y \in [0, \frac{\pi}{2}), then tan⁡y≥0\tan y \geq 0, so tan⁡y=x2−1\tan y = \sqrt{x^2 - 1}.
  • If y∈(π2,π]y \in (\frac{\pi}{2}, \pi], then tan⁡y≤0\tan y \leq 0, so tan⁡y=−x2−1\tan y = -\sqrt{x^2 - 1}.

Both cases combine as:

dydx=1∣x∣x2−1,∣x∣>1\frac{dy}{dx} = \frac{1}{|x| \sqrt{x^2 - 1}}, \quad |x| > 1

ddx(sec⁡−1x)=1∣x∣x2−1,∣x∣>1\frac{d}{dx}(\sec^{-1} x) = \frac{1}{|x| \sqrt{x^2 - 1}}, \quad |x| > 1

Tip

An equivalent form is 1xx2−1\frac{1}{x \sqrt{x^2 - 1}} when x>1x > 1 and −1xx2−1-\frac{1}{x \sqrt{x^2 - 1}} when x<−1x < -1; the absolute value combines both.


Derivative of csc⁡−1x\csc^{-1} x

Let y=csc⁡−1xy = \csc^{-1} x, so x=csc⁡yx = \csc y. Differentiating with respect to xx:

1=−csc⁡ycot⁡y⋅dydx⇒dydx=−1csc⁡ycot⁡y1 = -\csc y \cot y \cdot \frac{dy}{dx} \quad\Rightarrow\quad \frac{dy}{dx} = -\frac{1}{\csc y \cot y}

This exists when csc⁡ycot⁡y≠0\csc y \cot y \neq 0; for the range [−π2,π2]∖{0}[-\frac{\pi}{2}, \frac{\pi}{2}] \setminus \{0\} this holds for ∣x∣>1|x| > 1. Since csc⁡y=x\csc y = x, cot⁡2y=csc⁡2y−1=x2−1\cot^2 y = \csc^2 y - 1 = x^2 - 1, with:

  • If y∈(0,π2]y \in (0, \frac{\pi}{2}], then cot⁡y≥0\cot y \geq 0, so cot⁡y=x2−1\cot y = \sqrt{x^2 - 1}.
  • If y∈[−π2,0)y \in [-\frac{\pi}{2}, 0), then cot⁡y≤0\cot y \leq 0, so cot⁡y=−x2−1\cot y = -\sqrt{x^2 - 1}.

Both cases combine as:

dydx=−1∣x∣x2−1,∣x∣>1\frac{dy}{dx} = -\frac{1}{|x| \sqrt{x^2 - 1}}, \quad |x| > 1

ddx(csc⁡−1x)=−1∣x∣x2−1,∣x∣>1\frac{d}{dx}(\csc^{-1} x) = -\frac{1}{|x| \sqrt{x^2 - 1}}, \quad |x| > 1

Note

As expected, ddx(csc⁡−1x)=−ddx(sec⁡−1x)\frac{d}{dx}(\csc^{-1} x) = -\frac{d}{dx}(\sec^{-1} x), consistent with sec⁡−1x+csc⁡−1x=π2\sec^{-1} x + \csc^{-1} x = \frac{\pi}{2}.


Summary Table of Derivatives …