Visual Tools
Calculators
Tables
Mathematical Keyboard
Converters
Other Tools


Special Derivatives






Derivatives That Require Deeper Techniques


The common derivatives cover polynomials, trigonometric functions, exponentials, and logarithms. Beyond these lie function families whose derivatives are less immediately obvious and harder to rederive on the spot. Inverse trigonometric functions produce algebraic expressions involving square roots. Hyperbolic functions mirror their trigonometric counterparts with subtle sign differences. Piecewise functions demand separate treatment on each interval with careful attention at boundaries.

Most of these derivatives are established through implicit differentiation or the inverse function formula rather than direct computation from the limit definition. Understanding the derivation builds insight; memorizing the result builds speed. Both matter.



Inverse Trigonometric Functions — Arcsine and Arccosine


The derivatives of arcsinx\arcsin x and arccosx\arccos x are:

ddx[arcsinx]=11x2x<1\frac{d}{dx}[\arcsin x] = \frac{1}{\sqrt{1 - x^2}} \qquad |x| < 1


ddx[arccosx]=11x2x<1\frac{d}{dx}[\arccos x] = -\frac{1}{\sqrt{1 - x^2}} \qquad |x| < 1


The two derivatives differ only by sign. This follows from the identity arcsinx+arccosx=π2\arcsin x + \arccos x = \frac{\pi}{2}: differentiating both sides gives (arcsinx)+(arccosx)=0(\arcsin x)' + (\arccos x)' = 0.

To derive the arcsine formula: let y=arcsinxy = \arcsin x, so siny=x\sin y = x with y[π/2,π/2]y \in [-\pi/2, \pi/2]. Differentiating implicitly: cosydydx=1\cos y \cdot \frac{dy}{dx} = 1. Since yy lies in the first or fourth quadrant, cosy0\cos y \geq 0, so cosy=1sin2y=1x2\cos y = \sqrt{1 - \sin^2 y} = \sqrt{1 - x^2}. Solving gives dydx=11x2\frac{dy}{dx} = \frac{1}{\sqrt{1 - x^2}}.

The domain restriction x<1|x| < 1 reflects the range of siny\sin y on [π/2,π/2][-\pi/2, \pi/2]. At x=±1x = \pm 1, the denominator vanishes—the graph of arcsinx\arcsin x has vertical tangents at its endpoints.

Inverse Trigonometric Functions — Arctangent and Arccotangent


ddx[arctanx]=11+x2ddx[arccotx]=11+x2\frac{d}{dx}[\arctan x] = \frac{1}{1 + x^2} \qquad \qquad \frac{d}{dx}[\text{arccot}\, x] = -\frac{1}{1 + x^2}


Again the derivatives are negatives of each other, following from arctanx+arccotx=π2\arctan x + \text{arccot}\, x = \frac{\pi}{2}.

To derive the arctangent formula: let y=arctanxy = \arctan x, so tany=x\tan y = x. Differentiating: sec2ydydx=1\sec^2 y \cdot \frac{dy}{dx} = 1. Using the identity sec2y=1+tan2y=1+x2\sec^2 y = 1 + \tan^2 y = 1 + x^2 gives dydx=11+x2\frac{dy}{dx} = \frac{1}{1 + x^2}.

Unlike arcsine and arccosine, arctangent is defined for all real xx—no domain restriction. The derivative 11+x2\frac{1}{1 + x^2} is always positive, confirming that arctanx\arctan x is strictly increasing. As x±x \to \pm\infty, the derivative approaches zero, reflecting the horizontal asymptotes y=±π2y = \pm\frac{\pi}{2}. The function rises everywhere but flattens out at the extremes.

This derivative appears prominently in integration: 11+x2dx=arctanx+C\int \frac{1}{1 + x^2}\,dx = \arctan x + C.

Inverse Trigonometric Functions — Arcsecant and Arccosecant


ddx[arcsecx]=1xx21x>1\frac{d}{dx}[\text{arcsec}\, x] = \frac{1}{|x|\sqrt{x^2 - 1}} \qquad |x| > 1


ddx[arccscx]=1xx21x>1\frac{d}{dx}[\text{arccsc}\, x] = -\frac{1}{|x|\sqrt{x^2 - 1}} \qquad |x| > 1


The derivation for arcsecant: let y=arcsecxy = \text{arcsec}\, x, so secy=x\sec y = x. Differentiating: secytanydydx=1\sec y \tan y \cdot \frac{dy}{dx} = 1. Since secy=x\sec y = x and tany=±sec2y1=±x21\tan y = \pm\sqrt{\sec^2 y - 1} = \pm\sqrt{x^2 - 1}, the sign depends on the quadrant. The absolute value x|x| in the formula resolves this: secytany=xx21\sec y \tan y = |x|\sqrt{x^2 - 1} across the full domain.

These derivatives are less frequently encountered than the arcsine and arctangent versions. They appear primarily in integrals of the form 1xx21dx\int \frac{1}{x\sqrt{x^2 - 1}}\,dx and in problems involving trigonometric substitution.

The domain x>1|x| > 1 reflects the range of secant: secy\sec y never takes values between 1-1 and 11.

Patterns in Inverse Trigonometric Derivatives


The six inverse trigonometric derivatives organize into three pairs, each pair summing to zero:

(arcsinx)+(arccosx)=0(\arcsin x)' + (\arccos x)' = 0, both involving 11x2\frac{1}{\sqrt{1 - x^2}}

(arctanx)+(arccotx)=0(\arctan x)' + (\text{arccot}\, x)' = 0, both involving 11+x2\frac{1}{1 + x^2}

(arcsecx)+(arccscx)=0(\text{arcsec}\, x)' + (\text{arccsc}\, x)' = 0, both involving 1xx21\frac{1}{|x|\sqrt{x^2 - 1}}

Each pair shares the same magnitude because the two functions in each pair sum to a constant (π2\frac{\pi}{2}). The cofunction always carries the negative sign—the same pattern seen in the common trigonometric derivatives where cos\cos, cot\cot, and csc\csc derivatives are negative.

Two distinct algebraic forms appear: 1x2\sqrt{1 - x^2} for the sine/cosine pair, 1+x21 + x^2 for the tangent/cotangent pair, and xx21|x|\sqrt{x^2 - 1} for the secant/cosecant pair. These three expressions reappear in integration, where recognizing them triggers the corresponding inverse trigonometric antiderivative.

Hyperbolic Functions


The hyperbolic functions are defined through exponentials:

sinhx=exex2coshx=ex+ex2tanhx=sinhxcoshx\sinh x = \frac{e^x - e^{-x}}{2} \qquad \cosh x = \frac{e^x + e^{-x}}{2} \qquad \tanh x = \frac{\sinh x}{\cosh x}


Their derivatives parallel the trigonometric pattern:

ddx[sinhx]=coshxddx[coshx]=sinhx\frac{d}{dx}[\sinh x] = \cosh x \qquad \qquad \frac{d}{dx}[\cosh x] = \sinh x


ddx[tanhx]=sech2xddx[cothx]=csch2x\frac{d}{dx}[\tanh x] = \text{sech}^2\, x \qquad \qquad \frac{d}{dx}[\coth x] = -\text{csch}^2\, x


ddx[sechx]=sechxtanhxddx[cschx]=cschxcothx\frac{d}{dx}[\text{sech}\, x] = -\text{sech}\, x \tanh x \qquad \qquad \frac{d}{dx}[\text{csch}\, x] = -\text{csch}\, x \coth x


The critical difference from trigonometric derivatives: (coshx)=sinhx(\cosh x)' = \sinh x carries no negative sign, whereas (cosx)=sinx(\cos x)' = -\sin x does. This single sign difference propagates through all six formulas.

Each derivative is verified directly by differentiating the exponential definitions. For sinhx\sinh x: ddx[exex2]=ex+ex2=coshx\frac{d}{dx}\left[\frac{e^x - e^{-x}}{2}\right] = \frac{e^x + e^{-x}}{2} = \cosh x. No special limits or implicit differentiation are needed—the exponential derivative does all the work.

Inverse Hyperbolic Functions


The inverse hyperbolic functions have derivatives that resemble the inverse trigonometric ones with sign changes under the radical:

ddx[arcsinhx]=1x2+1ddx[arccoshx]=1x21,x>1\frac{d}{dx}[\text{arcsinh}\, x] = \frac{1}{\sqrt{x^2 + 1}} \qquad \qquad \frac{d}{dx}[\text{arccosh}\, x] = \frac{1}{\sqrt{x^2 - 1}}, \quad x > 1


ddx[arctanhx]=11x2,x<1\frac{d}{dx}[\text{arctanh}\, x] = \frac{1}{1 - x^2}, \quad |x| < 1


Compare with inverse trigonometric derivatives: 1x2\sqrt{1 - x^2} becomes x2+1\sqrt{x^2 + 1} or x21\sqrt{x^2 - 1}, and 1+x21 + x^2 becomes 1x21 - x^2. The signs inside the expressions flip.

These derivatives can be established through implicit differentiation or through the logarithmic representations. For instance, arcsinhx=ln(x+x2+1)\text{arcsinh}\, x = \ln(x + \sqrt{x^2 + 1}). Differentiating this logarithmic form directly using the chain rule confirms 1x2+1\frac{1}{\sqrt{x^2 + 1}}.

Inverse hyperbolic derivatives appear in integration: 1x2+1dx=arcsinhx+C\int \frac{1}{\sqrt{x^2 + 1}}\,dx = \text{arcsinh}\, x + C and 1x21dx=arccoshx+C\int \frac{1}{\sqrt{x^2 - 1}}\,dx = \text{arccosh}\, x + C provide alternatives to trigonometric substitution for certain radical integrals.

Piecewise Functions


A piecewise function uses different formulas on different intervals. On each interval's interior, standard differentiation rules apply to the governing formula. The derivative of the piecewise function is itself piecewise—computed piece by piece.

The challenge lies at the boundaries. At a point x=cx = c where the formula changes, the derivative exists only if three conditions hold: the function is continuous at cc (the pieces connect), the left-hand derivative exists, and the right-hand derivative exists and equals the left-hand derivative.

Consider f(x)=x2f(x) = x^2 for x1x \leq 1 and f(x)=2x1f(x) = 2x - 1 for x>1x > 1. Continuity at x=1x = 1: f(1)=1f(1) = 1 from the left, 2(1)1=12(1) - 1 = 1 from the right—they match. Left derivative at 11: ddx[x2]x=1=2\frac{d}{dx}[x^2]\big|_{x=1} = 2. Right derivative at 11: ddx[2x1]x=1=2\frac{d}{dx}[2x - 1]\big|_{x=1} = 2. Both derivatives match, so f(1)=2f'(1) = 2.

If either continuity fails or the one-sided derivatives disagree, the function is not differentiable at that boundary. The absolute value function x|x| is the canonical example: continuous at x=0x = 0, but left derivative 1-1 and right derivative +1+1 do not match.

Summary of Special Derivatives


The complete set of special derivative formulas:

ddx[arcsinx]=11x2ddx[arccosx]=11x2\frac{d}{dx}[\arcsin x] = \frac{1}{\sqrt{1-x^2}} \qquad \frac{d}{dx}[\arccos x] = -\frac{1}{\sqrt{1-x^2}}


ddx[arctanx]=11+x2ddx[arccotx]=11+x2\frac{d}{dx}[\arctan x] = \frac{1}{1+x^2} \qquad \frac{d}{dx}[\text{arccot}\, x] = -\frac{1}{1+x^2}


ddx[arcsecx]=1xx21ddx[arccscx]=1xx21\frac{d}{dx}[\text{arcsec}\, x] = \frac{1}{|x|\sqrt{x^2-1}} \qquad \frac{d}{dx}[\text{arccsc}\, x] = -\frac{1}{|x|\sqrt{x^2-1}}


ddx[sinhx]=coshxddx[coshx]=sinhx\frac{d}{dx}[\sinh x] = \cosh x \qquad \frac{d}{dx}[\cosh x] = \sinh x


ddx[tanhx]=sech2xddx[cothx]=csch2x\frac{d}{dx}[\tanh x] = \text{sech}^2\, x \qquad \frac{d}{dx}[\coth x] = -\text{csch}^2\, x


ddx[sechx]=sechxtanhxddx[cschx]=cschxcothx\frac{d}{dx}[\text{sech}\, x] = -\text{sech}\, x\tanh x \qquad \frac{d}{dx}[\text{csch}\, x] = -\text{csch}\, x\coth x


ddx[arcsinhx]=1x2+1ddx[arccoshx]=1x21\frac{d}{dx}[\text{arcsinh}\, x] = \frac{1}{\sqrt{x^2+1}} \qquad \frac{d}{dx}[\text{arccosh}\, x] = \frac{1}{\sqrt{x^2-1}}


ddx[arctanhx]=11x2\frac{d}{dx}[\text{arctanh}\, x] = \frac{1}{1-x^2}


Together with the common derivatives, these formulas cover every standard function encountered in calculus. Recognizing the algebraic forms—1x2\sqrt{1-x^2}, 1+x21+x^2, x2±1\sqrt{x^2 \pm 1}, 1x21-x^2—is equally important for integration, where these expressions signal inverse trigonometric or inverse hyperbolic antiderivatives.