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NDA Mathematics · Formula sheet

Differentiation formulas

14 formulas, 1 reference table and 17 common traps for NDA Mathematics Differentiation, grouped by subtopic.

Full notes with worked examples

Core Techniques — Standard Derivatives, Rules, Chain & Logarithmic

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The derivative as a limit (first principles)

First-principles definition

f′(x)=lim⁡h→0f(x+h)−f(x)hf'(x) = \lim_{h\to 0}\frac{f(x+h)-f(x)}{h}

Product and quotient rules

(uv)′=u′v+uv′,(uv)′=u′v−uv′v2(uv)' = u'v + uv', \qquad \left(\frac{u}{v}\right)' = \frac{u'v - uv'}{v^2}

The chain rule (composite functions)

Chain rule

ddx f(g(x))=f′(g(x))⋅g′(x)\frac{d}{dx}\,f(g(x)) = f'(g(x))\cdot g'(x)

Logarithmic differentiation

y=f(x)g(x)  ⇒  1ydydx=g′(x)ln⁡f(x)+g(x)f′(x)f(x)y = f(x)^{g(x)} \;\Rightarrow\; \frac{1}{y}\frac{dy}{dx} = g'(x)\ln f(x) + g(x)\frac{f'(x)}{f(x)}

Derivative of one function with respect to another

Derivative of u w.r.t. v

dudv=du/dxdv/dx\frac{du}{dv} = \frac{du/dx}{dv/dx}

Simplify the inverse-trig first, then differentiate

Standard inverse-trig collapses

tan⁡−12x1−x2=2tan⁡−1xsin⁡−12x1+x2=2tan⁡−1xcos⁡−11−x21+x2=2tan⁡−1xcos⁡−1(sin⁡x)=π2−xtan⁡−1a−b1+ab=tan⁡−1a−tan⁡−1b\tan^{-1}\dfrac{2x}{1-x^2} = 2\tan^{-1}x \qquad \sin^{-1}\dfrac{2x}{1+x^2} = 2\tan^{-1}x \qquad \cos^{-1}\dfrac{1-x^2}{1+x^2} = 2\tan^{-1}x \qquad \cos^{-1}(\sin x) = \dfrac{\pi}{2} - x \qquad \tan^{-1}\dfrac{a-b}{1+ab} = \tan^{-1}a - \tan^{-1}b

Differentiating functional equations

Exponential functional equation

f(x+y)=f(x)f(y)  ⇒  f′(x)=f′(0) f(x)f(x+y)=f(x)f(y) \;\Rightarrow\; f'(x) = f'(0)\,f(x)

Trigonometric Simplification Toolkit

The collapses you reach for most

1+cos⁡x=2cos⁡2x2,1−cos⁡x=2sin⁡2x2,1±sin⁡2x=∣sin⁡x±cos⁡x∣1+\cos x = 2\cos^2\tfrac{x}{2},\quad 1-\cos x = 2\sin^2\tfrac{x}{2},\quad \sqrt{1\pm\sin 2x}=|\sin x\pm\cos x|
  • x2\tfrac{x}{2}half-angle — appears whenever you collapse 1±cos⁡x1\pm\cos x
  • ∣⋯∣|\cdots|the root of a perfect square is a MODULUS; fix the sign on the given interval

Standard derivatives to memorise

Function f(x)Derivative f′(x)
xnx^nn xn−1n\,x^{n-1}
sin⁡x\sin xcos⁡x\cos x
cos⁡x\cos x−sin⁡x-\sin x
tan⁡x\tan xsec⁡2x\sec^2 x
sec⁡x\sec xsec⁡xtan⁡x\sec x\tan x
exe^xexe^x
axa^xaxln⁡aa^x\ln a
The ln⁡a\ln a factor is the most-forgotten part of the table.
ln⁡x\ln x1x\dfrac{1}{x}
log⁡ax\log_a x1xln⁡a\dfrac{1}{x\ln a}
sin⁡−1x\sin^{-1} x11−x2\dfrac{1}{\sqrt{1-x^2}}
tan⁡−1x\tan^{-1} x11+x2\dfrac{1}{1+x^2}
cot⁡x\cot x−csc⁡2x-\csc^2 x
csc⁡x\csc x−csc⁡xcot⁡x-\csc x\cot x
The co-functions (cos, cot, cosec) all carry a MINUS sign.
cos⁡−1x\cos^{-1} x−11−x2-\dfrac{1}{\sqrt{1-x^2}}
cot⁡−1x\cot^{-1} x−11+x2-\dfrac{1}{1+x^2}
sec⁡−1x\sec^{-1} x1∣x∣x2−1\dfrac{1}{|x|\sqrt{x^2-1}}
ln⁡∣x∣\ln|x|1x\dfrac{1}{x} for all x≠0x\neq0
x2x2−a2−a22ln⁡∣x+x2−a2∣\tfrac{x}{2}\sqrt{x^2-a^2}-\tfrac{a^2}{2}\ln\big|x+\sqrt{x^2-a^2}\big|x2−a2\sqrt{x^2-a^2}
The antiderivative of √(x²−a²), read backwards — a 'standard form' the PYQs quote without proof; the +a² sibling differentiates to √(x²+a²).
Radians only. The chain rule extends each of these to a composite argument.

Common traps

Degrees must be converted to radians first

ddxsin⁡(x∘)=π180cos⁡(x∘)\frac{d}{dx}\sin(x^{\circ}) = \frac{\pi}{180}\cos(x^{\circ}), NOT cos⁡(x∘)\cos(x^{\circ}). The standard table holds only for radian arguments; a degree symbol injects a π/180\pi/180 factor by the chain rule.

Don't power-rule an exponential

ddx(ax)=axln⁡a\frac{d}{dx}(a^x) = a^x\ln a, NOT x ax−1x\,a^{x-1}. The power rule ddx(xn)=nxn−1\frac{d}{dx}(x^n)=nx^{n-1} applies only when the BASE is the variable. When the variable is in the EXPONENT, the derivative carries the base unchanged and picks up a ln⁡a\ln a factor. (And ddxex=ex\frac{d}{dx}e^x = e^x, since ln⁡e=1\ln e = 1.)

Derivative of ln⁡x\ln x is 1/x1/x, not ln⁡x\ln x or xx

ddx(ln⁡x)=1x\frac{d}{dx}(\ln x) = \dfrac{1}{x}. It is neither ln⁡x\ln x (that's its own integral mistake) nor xx. For a general base, ddx(log⁡ax)=1xln⁡a\frac{d}{dx}(\log_a x) = \dfrac{1}{x\ln a} — the extra ln⁡a\ln a lives in the DENOMINATOR here, the opposite of where it sits for axa^x.

The product rule is not the product of derivatives

(uv)′≠u′v′(uv)' \neq u'v'. The correct rule is (uv)′=u′v+uv′(uv)' = u'v + uv' — differentiate one factor at a time and add. For x2sin⁡xx^2\sin x, the answer is 2xsin⁡x+x2cos⁡x2x\sin x + x^2\cos x, not (2x)(cos⁡x)(2x)(\cos x).

Quotient rule — order and sign in the numerator matter

(uv)′=u′v−uv′v2\left(\dfrac{u}{v}\right)' = \dfrac{u'v - uv'}{v^2}, NOT uv′−u′vv2\dfrac{uv' - u'v}{v^2} and NOT u′v+uv′v2\dfrac{u'v + uv'}{v^2}. The derivative-of-the-top term comes first and the two terms are SUBTRACTED. Flipping the order negates the whole answer.

Don't forget the derivative of the inner function

ddxsin⁡(3x2)=cos⁡(3x2)⋅6x\frac{d}{dx}\sin(3x^2) = \cos(3x^2)\cdot 6x, NOT just cos⁡(3x2)\cos(3x^2). The chain rule multiplies by the inner derivative 6x6x; leaving it out is the single most common slip in the chapter. Every layer contributes its own factor.

Don't quotient-rule the raw inverse-trig

Differentiating tan⁡−12x1−x2\tan^{-1}\frac{2x}{1-x^2} directly with the chain + quotient rule is slow and error-prone. The intended path is the x=tan⁡θx=\tan\theta collapse to 2tan⁡−1x2\tan^{-1}x first.

1±cos⁡x1\pm\cos x (half-angle) vs 1±cos⁡2x1\pm\cos 2x (power-reduction)

Different collapses: 1−cos⁡x=2sin⁡2x21-\cos x = 2\sin^2\tfrac{x}{2} but 1−cos⁡2x=2sin⁡2x1-\cos 2x = 2\sin^2 x. Read the angle inside the cosine before choosing the factor — the wrong one halves or doubles the argument.

The root of a perfect square is a MODULUS

(sin⁡x−cos⁡x)2=∣sin⁡x−cos⁡x∣\sqrt{(\sin x-\cos x)^2} = |\sin x-\cos x|, not sin⁡x−cos⁡x\sin x-\cos x. Resolve the sign on the given interval: on (π4,π2)(\tfrac\pi4,\tfrac\pi2) it is +(sin⁡x−cos⁡x)+(\sin x-\cos x); on (0,π4)(0,\tfrac\pi4) it is −(sin⁡x−cos⁡x)-(\sin x-\cos x). Dropping the modulus flips the sign of the whole derivative.

sec⁡±tan⁡\sec\pm\tan — mind which way the half-angle shifts

sec⁡x+tan⁡x=tan⁡ ⁣(π4+x2)\sec x+\tan x=\tan\!\left(\tfrac\pi4+\tfrac x2\right) but sec⁡x−tan⁡x=tan⁡ ⁣(π4−x2)\sec x-\tan x=\tan\!\left(\tfrac\pi4-\tfrac x2\right). Useful check: (sec⁡x+tan⁡x)(sec⁡x−tan⁡x)=sec⁡2x−tan⁡2x=1(\sec x+\tan x)(\sec x-\tan x)=\sec^2x-\tan^2x=1.

Parametric, Implicit & Higher-Order Derivatives

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Implicit differentiation

Implicit rule of thumb

ddx[ y-term ]=(its derivative)⋅dydx\frac{d}{dx}\big[\,y\text{-term}\,\big] = (\text{its derivative})\cdot\frac{dy}{dx}

Parametric differentiation

Parametric first derivative

dydx=dy/dtdx/dt\frac{dy}{dx} = \frac{dy/dt}{dx/dt}

Higher-order derivatives

Second derivative

d2ydx2=ddx ⁣(dydx)\frac{d^2y}{dx^2} = \frac{d}{dx}\!\left(\frac{dy}{dx}\right)

Second derivative of an inverse — the d²x/dy² identity

Second derivative of the inverse

d2xdy2=−d2y/dx2(dy/dx)3\frac{d^2x}{dy^2} = -\frac{d^2y/dx^2}{\left(dy/dx\right)^{3}}

Common traps

Every yy-term needs a dydx\frac{dy}{dx} factor

Differentiating y2y^2 w.r.t. xx gives 2ydydx2y\dfrac{dy}{dx}, NOT 2y2y. Because yy is a function of xx, the chain rule attaches a dydx\frac{dy}{dx} to every yy-term. Forgetting it is the defining error of implicit differentiation — you'd never recover dydx\frac{dy}{dx} to solve for.

Don't invert the parametric ratio

dydx=dy/dtdx/dt\dfrac{dy}{dx} = \dfrac{dy/dt}{dx/dt} — the yy-rate is on TOP, the xx-rate on the bottom (it cancels like a fraction: dydt÷dxdt\frac{dy}{dt}\div\frac{dx}{dt}). Writing dx/dtdy/dt\frac{dx/dt}{dy/dt} gives the reciprocal dxdy\frac{dx}{dy} instead. For x=t2,y=t3x=t^2, y=t^3 the slope is 3t22t=3t2\frac{3t^2}{2t}=\frac{3t}{2}, not 23t\frac{2}{3t}.

d2ydx2\frac{d^2y}{dx^2} is not (dydx)2\left(\frac{dy}{dx}\right)^2

The second derivative means 'differentiate the first derivative AGAIN', not 'square the first derivative'. For y=x3y=x^3: dydx=3x2\frac{dy}{dx}=3x^2, so d2ydx2=6x\frac{d^2y}{dx^2}=6x — whereas (dydx)2=9x4\left(\frac{dy}{dx}\right)^2 = 9x^4, a completely different (and wrong) object.

Second derivatives don't invert like first derivatives

dxdy=1/dydx\frac{dx}{dy}=1/\frac{dy}{dx} is fine, but d2xdy2≠1/d2ydx2\frac{d^2x}{dy^2}\neq 1/\frac{d^2y}{dx^2}. The right formula has (dy/dx)3(dy/dx)^3 in the denominator and a minus sign.

Differentiability — When the Derivative Exists

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The left-hand = right-hand derivative test

One-sided derivative test

f′(c−)=f′(c+)  ⟺  f differentiable at cf'(c^-) = f'(c^+) \iff f \text{ differentiable at } c

Derivative at an awkward point via the limit definition

Derivative from first principles

f′(c)=lim⁡h→0f(c+h)−f(c)hf'(c) = \lim_{h \to 0} \dfrac{f(c+h) - f(c)}{h}

Common traps

The implication only runs one way

'Differentiable ⇒\Rightarrow continuous' is true; 'continuous ⇒\Rightarrow differentiable' is FALSE. NDA statement-questions plant the reversed (false) version to catch you.

Continuity first, then slopes

If the pieces don't even meet (discontinuous at the join), stop — it cannot be differentiable. Only when continuous do you compare LHD and RHD.

Not every |·| means non-differentiable

∣x∣|x| has a corner, but x∣x∣x|x|, x2∣x∣x^2|x|, and e∣x∣⋅(smoothing)e^{|x|}\cdot(\text{smoothing}) can be differentiable at the split. Always rewrite piecewise and compare one-sided derivatives — don't assume the modulus kills differentiability.

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