Derivatives of inverse trigonometric functions

Every time you differentiate sin⁡−1x\sin^{-1}x, cos⁡−1x\cos^{-1}x, or tan⁡−1x\tan^{-1}x, you are using one of six standard results that sit right after the chain rule in the Continuity and Differentiability chapter. These formulas turn up constantly — inside JEE-style composite functions, inside implicit differentiation problems, and inside the trickiest substitution questions where an ugly expression under sin⁡−1\sin^{-1} or tan⁡−1\tan^{-1} collapses to something simple once you spot the right trig identity. Getting comfortable with all six derivatives, their domains, and the chain rule wrapped around them is one of the highest-yield investments you can make in this chapter. This section builds the six formulas from first principles for sin⁡−1x\sin^{-1}x, states the full family, works two representative problems — one plain chain-rule application and one substitution-based simplification — and flags the sign and domain traps that examiners love to test.

The core insight

The derivatives of the six inverse trigonometric functions are fixed algebraic expressions in xx (never containing an inverse trig function themselves), each valid only on a specific domain, and differentiating a composite inverse-trig expression means applying one of these six formulas together with the chain rule — or, better, simplifying the argument with a trigonometric substitution first.

The core idea

Because sin⁡−1x\sin^{-1}x, cos⁡−1x\cos^{-1}x, and so on are defined as the inverses of trig functions restricted to a principal-value branch, their derivatives can be found by implicit differentiation of the corresponding direct trig equation. The result is a short, memorisable table.

ddxsin⁡−1x=11−x2,ddxcos⁡−1x=−11−x2(−1<x<1)\frac{d}{dx}\sin^{-1}x = \frac{1}{\sqrt{1-x^2}}, \qquad \frac{d}{dx}\cos^{-1}x = \frac{-1}{\sqrt{1-x^2}} \qquad (-1<x<1)
ddxtan⁡−1x=11+x2,ddxcot⁡−1x=−11+x2(x∈R)\frac{d}{dx}\tan^{-1}x = \frac{1}{1+x^2}, \qquad \frac{d}{dx}\cot^{-1}x = \frac{-1}{1+x^2} \qquad (x \in \mathbb{R})
ddxsec⁡−1x=1∣x∣x2−1,ddxcsc⁡−1x=−1∣x∣x2−1(∣x∣>1)\frac{d}{dx}\sec^{-1}x = \frac{1}{|x|\sqrt{x^2-1}}, \qquad \frac{d}{dx}\csc^{-1}x = \frac{-1}{|x|\sqrt{x^2-1}} \qquad (|x|>1)

where: xx is the point at which the derivative is evaluated, and the domain restriction next to each formula is where the corresponding inverse function is differentiable — outside it the expression is either undefined or the formula does not apply. Three sub-points are worth holding onto before you touch a single problem.

The co-function pattern. Each "co" function — cos⁡−1\cos^{-1}, cot⁡−1\cot^{-1}, csc⁡−1\csc^{-1} — has exactly the negative of the derivative of its partner (sin⁡−1\sin^{-1}, tan⁡−1\tan^{-1}, sec⁡−1\sec^{-1} respectively). If you remember only the first three formulas, you can write down the other three by flipping the sign.

The chain rule wraps every formula. When the argument is a function g(x)g(x) rather than plain xx, for example y=sin⁡−1(g(x))y = \sin^{-1}(g(x)), the derivative picks up a factor of g′(x)g'(x):

dydx=11−[g(x)]2⋅g′(x)\frac{dy}{dx} = \frac{1}{\sqrt{1-[g(x)]^2}}\cdot g'(x)

This is the single most common source of lost marks: forgetting the g′(x)g'(x) factor entirely.

Simplify before you differentiate. A large class of problems present an intimidating argument inside sin⁡−1\sin^{-1} or tan⁡−1\tan^{-1} that becomes trivial after a trigonometric substitution such as x=sin⁡θx = \sin\theta or x=tan⁡θx = \tan\theta, using identities like the double-angle formulas. Spotting this pattern before reaching for the chain rule saves several lines of algebra and avoids sign errors.

Figure
A number line showing where the derivative formulas for sine inverse and cosine inverse hold between negative one and one, and where the formulas for secant inverse and cosecant inverse hold outside negative one to one
Where each derivative formula is valid -1 1 sin inverse, cos inverse valid here sec inverse, csc inverse sec inverse, csc inverse tan inverse and cot inverse are valid across the whole real line

Why these formulas work

Setting up the goal. The full goal is to derive ddxsin⁡−1x=11−x2\dfrac{d}{dx}\sin^{-1}x = \dfrac{1}{\sqrt{1-x^2}} for −1<x<1-1 < x < 1 starting only from the definition of sin⁡−1x\sin^{-1}x as the inverse of sine restricted to the principal branch [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right], using implicit differentiation and the Pythagorean identity — the same method then reproduces all five remaining formulas by an identical pattern applied to cos⁡y=x\cos y = x, tan⁡y=x\tan y = x, and so on.

Step 1. Let y=sin⁡−1xy = \sin^{-1}x. By definition of the inverse function, this means sin⁡y=x\sin y = x, with yy restricted to the principal branch [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right].

Step 2. Differentiate both sides of sin⁡y=x\sin y = x implicitly with respect to xx, treating yy as a function of xx. The left side needs the chain rule: cos⁡y⋅dydx=1\cos y \cdot \dfrac{dy}{dx} = 1.

Step 3. Solve for dydx\dfrac{dy}{dx}: dydx=1cos⁡y\dfrac{dy}{dx} = \dfrac{1}{\cos y}, valid wherever cos⁡y≠0\cos y \neq 0, i.e. away from y=±π2y = \pm\frac{\pi}{2}, which corresponds to x=±1x = \pm 1.

Step 4. Express cos⁡y\cos y in terms of xx using cos⁡2y+sin⁡2y=1\cos^2 y + \sin^2 y = 1, so cos⁡y=±1−sin⁡2y=±1−x2\cos y = \pm\sqrt{1-\sin^2 y} = \pm\sqrt{1-x^2}. On the principal branch [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right], cosine is never negative, so we take the positive root: cos⁡y=1−x2\cos y = \sqrt{1-x^2}.

Step 5. Substitute back into Step 3 to get dydx=11−x2\dfrac{dy}{dx} = \dfrac{1}{\sqrt{1-x^2}} for −1<x<1-1 < x < 1, exactly the stated formula. The other five formulas follow from the identical three-step pattern (differentiate implicitly, solve for the derivative in terms of the direct trig function, rewrite that function in terms of xx using an identity and the correct sign on the relevant branch) applied to cos⁡y=x\cos y = x, tan⁡y=x\tan y = x, cot⁡y=x\cot y = x, sec⁡y=x\sec y = x, and csc⁡y=x\csc y = x in turn.

Worked example

Differentiate y=tan⁡−1(x2)y = \tan^{-1}(x^2) with respect to xx, then extend the method to y=sin⁡−1(2x1−x2)y = \sin^{-1}(2x\sqrt{1-x^2}) using a substitution.

Step 1. For y=tan⁡−1(x2)y = \tan^{-1}(x^2), identify the composite structure: outer function tan⁡−1(u)\tan^{-1}(u) with inner function u=x2u = x^2.

Step 2. Differentiate the outer function with respect to uu using the standard formula, then substitute u=x2u = x^2: dydu=11+u2=11+x4\dfrac{dy}{du} = \dfrac{1}{1+u^2} = \dfrac{1}{1+x^4}.

Step 3. Differentiate the inner function: dudx=2x\dfrac{du}{dx} = 2x. By the chain rule, dydx=11+x4⋅2x=2x1+x4\dfrac{dy}{dx} = \dfrac{1}{1+x^4}\cdot 2x = \dfrac{2x}{1+x^4}.

Step 4. Now the second, harder function: y=sin⁡−1(2x1−x2)y = \sin^{-1}(2x\sqrt{1-x^2}) for −12≤x≤12-\frac{1}{\sqrt2} \le x \le \frac{1}{\sqrt2}. Substitute x=sin⁡θx = \sin\theta, so θ=sin⁡−1x\theta = \sin^{-1}x and 1−x2=cos⁡θ\sqrt{1-x^2} = \cos\theta for θ∈[−π4,π4]\theta \in \left[-\frac{\pi}{4}, \frac{\pi}{4}\right]. Then 2x1−x2=2sin⁡θcos⁡θ=sin⁡2θ2x\sqrt{1-x^2} = 2\sin\theta\cos\theta = \sin 2\theta by the double-angle identity.

Step 5. Since θ∈[−π4,π4]\theta \in \left[-\frac{\pi}{4}, \frac{\pi}{4}\right], the doubled angle 2θ∈[−π2,π2]2\theta \in \left[-\frac{\pi}{2}, \frac{\pi}{2}\right] lies exactly inside the principal branch, so sin⁡−1(sin⁡2θ)=2θ\sin^{-1}(\sin 2\theta) = 2\theta and y=2θ=2sin⁡−1xy = 2\theta = 2\sin^{-1}x. Differentiating this simplified form directly gives dydx=2⋅11−x2=21−x2\dfrac{dy}{dx} = 2\cdot\dfrac{1}{\sqrt{1-x^2}} = \dfrac{2}{\sqrt{1-x^2}}.

Final answers: dydx=2x1+x4\dfrac{dy}{dx} = \dfrac{2x}{1+x^4} for y=tan⁡−1(x2)y = \tan^{-1}(x^2), and dydx=21−x2\dfrac{dy}{dx} = \dfrac{2}{\sqrt{1-x^2}} for y=sin⁡−1(2x1−x2)y = \sin^{-1}(2x\sqrt{1-x^2}).

Competitive stretch

If instead the problem gave y=cos⁡−1(1−2x2)y = \cos^{-1}(1-2x^2) with x=sin⁡θx = \sin\theta, the same substitution turns the argument into 1−2sin⁡2θ=cos⁡2θ1 - 2\sin^2\theta = \cos 2\theta, so y=cos⁡−1(cos⁡2θ)y = \cos^{-1}(\cos 2\theta). For θ∈[0,π2]\theta \in \left[0, \frac{\pi}{2}\right] (i.e. x≥0x \ge 0), 2θ∈[0,π]2\theta \in [0, \pi] lies in the principal branch of cos⁡−1\cos^{-1}, giving y=2θ=2sin⁡−1xy = 2\theta = 2\sin^{-1}x, and hence the same derivative dydx=21−x2\dfrac{dy}{dx} = \dfrac{2}{\sqrt{1-x^2}} — a good check that different-looking arguments can collapse to the same simplified answer.

Common traps

  • Mixing up the sign between a function and its co-function derivative, e.g. writing ddxcos⁡−1x=11−x2\frac{d}{dx}\cos^{-1}x = \frac{1}{\sqrt{1-x^2}} instead of the correct negative sign.
  • Forgetting the domain restrictions. The formulas for sin⁡−1x\sin^{-1}x and cos⁡−1x\cos^{-1}x hold only for −1<x<1-1<x<1; for sec⁡−1x\sec^{-1}x and csc⁡−1x\csc^{-1}x, only for ∣x∣>1|x|>1, and the ∣x∣|x| in the denominator must not be dropped.
  • Forgetting to apply the chain rule when the argument is not simply xx, e.g. differentiating sin⁡−1(3x)\sin^{-1}(3x) as 11−x2\frac{1}{\sqrt{1-x^2}} instead of 31−9x2\frac{3}{\sqrt{1-9x^2}}.
  • Choosing the wrong substitution range, so the simplified angle falls outside the principal-value branch, making a cancellation like sin⁡−1(sin⁡2θ)=2θ\sin^{-1}(\sin 2\theta) = 2\theta invalid — always check the branch before dropping the outer and inner inverse functions.

Ask the tutor: Want to practice picking the right substitution for a gnarly inverse-trig argument, with guided hints on tracking the principal-value branch?

Why does the derivative of sin inverse x not contain any inverse trig function itself?

Because after implicit differentiation you get cos⁡y\cos y, not yy itself, and cos⁡y\cos y can always be rewritten purely in terms of xx using the Pythagorean identity cos⁡y=1−x2\cos y = \sqrt{1-x^2} (with the correct sign fixed by the principal branch). This is exactly what makes the six results usable as plain algebraic formulas rather than something you would need to re-derive every time — the inverse function only appears in the original problem, never in the final derivative.

How do I know which trigonometric substitution to try in a simplification problem?

Look at the structure of the argument. An expression like 2x1−x22x\sqrt{1-x^2} or 1−2x21-2x^2 inside sin⁡−1\sin^{-1} or cos⁡−1\cos^{-1} strongly suggests a double-angle identity, so try x=sin⁡θx = \sin\theta. An expression with 2x1−x2\dfrac{2x}{1-x^2} or 1−x21+x2\dfrac{1-x^2}{1+x^2} inside tan⁡−1\tan^{-1} suggests x=tan⁡θx = \tan\theta and the tangent double-angle formula. Matching the algebraic shape of the argument to a known double-angle or triple-angle identity is the fastest way to pick the right substitution.

Do I need to memorise the sec inverse and csc inverse derivatives separately, or can I derive them on the spot?

Either works, but memorising the co-function pattern is faster in an exam: once you know ddxsec⁡−1x=1∣x∣x2−1\frac{d}{dx}\sec^{-1}x = \frac{1}{|x|\sqrt{x^2-1}}, the csc inverse derivative is automatically its negative. If you forget the exact form, you can always re-derive it in under a minute using the same implicit-differentiation method used for sin inverse, starting from sec⁡y=x\sec y = x and using tan⁡y=x2−1\tan y = \sqrt{x^2-1} (with ∣x∣|x| handled via the sign of sec⁡y\sec y on the two branches).

Before this

Where this leads