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Indefinite Integration formulas

23 formulas and 26 common traps for NDA Mathematics Indefinite Integration, grouped by subtopic.

Full notes with worked examples

Foundations & Standard Forms

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Antiderivative and the Constant of Integration

Indefinite integral

∫f(x) dx=F(x)+CwhereF′(x)=f(x)\int f(x)\,dx = F(x) + C \quad\text{where}\quad F'(x) = f(x)
  • F(x)F(x)any one antiderivative of ff
  • CCarbitrary constant of integration

The Standard-Formula Table

Power rule (the most-used row)

∫xn dx=xn+1n+1+C(n≠−1)\int x^n\,dx = \dfrac{x^{n+1}}{n+1} + C \quad (n \neq -1)
  • n≠−1n \neq -1the exclusion that makes ∫x−1=ln⁡∣x∣\int x^{-1} = \ln|x| a separate row

Linearity — Integrate Term by Term

Linearity of the integral

∫(a f(x)+b g(x)) dx=a ⁣∫ ⁣f(x) dx+b ⁣∫ ⁣g(x) dx\int\big(a\,f(x)+b\,g(x)\big)\,dx = a\!\int\! f(x)\,dx + b\!\int\! g(x)\,dx

Simplify the Integrand First

The collapse identity

eln⁡u=uekln⁡x=xke^{\ln u} = u \qquad e^{k\ln x} = x^{k}

Exponential Bases — a to the x

Exponential base rule

∫ax dx=axln⁡a+C\int a^x\,dx = \dfrac{a^x}{\ln a} + C
  • aathe constant base, a>0, a≠1a>0,\ a\neq 1
  • ln⁡a\ln anatural log of the base — the divisor

Completing the Square for Quadratic Denominators

Arctan standard form

∫dxx2+k2=1ktan⁡−1 ⁣(xk)+C\int \dfrac{dx}{x^2+k^2} = \dfrac{1}{k}\tan^{-1}\!\Big(\dfrac{x}{k}\Big) + C

The e-to-the-x Times f-plus-f-prime Pattern

Reverse product rule

∫ex(f(x)+f′(x)) dx=exf(x)+C\int e^x\big(f(x)+f'(x)\big)\,dx = e^x f(x) + C

Cyclic and Paired Integrals of e-to-the-x Times Trig

The matched pair

∫excos⁡x dx=ex(cos⁡x+sin⁡x)2+C,∫exsin⁡x dx=ex(sin⁡x−cos⁡x)2+C\int e^x\cos x\,dx = \tfrac{e^x(\cos x+\sin x)}{2}+C,\quad \int e^x\sin x\,dx = \tfrac{e^x(\sin x-\cos x)}{2}+C

Properties of an Antiderivative

Integration and differentiation are inverse

∫F′(x) dx=F(x)+Cddx ⁣∫f(x) dx=f(x)\int F'(x)\,dx = F(x) + C \qquad \dfrac{d}{dx}\!\int f(x)\,dx = f(x)
  • F′(x)F'(x)a derivative; integrating it recovers FF up to a constant

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

Common traps

Never drop the +C on an indefinite integral

An indefinite integral with no +C+C is incomplete. NDA options are written so the 'no constant' version and a wrong-constant version both appear — only the form carrying +C+C (or +k+k) is correct.

The power rule excludes n=−1n=-1

∫x−1 dx\int x^{-1}\,dx is NOT x00\dfrac{x^0}{0} — that is undefined. It is the special row ∫1x dx=ln⁡∣x∣+C\int \dfrac{1}{x}\,dx = \ln|x| + C.

You cannot split a product or a quotient like a sum

∫1x(x2+1) dx≠∫1x dx⋅∫1x2+1 dx\int \dfrac{1}{x(x^2+1)}\,dx \neq \int\dfrac{1}{x}\,dx \cdot \int\dfrac{1}{x^2+1}\,dx. Linearity is for SUMS only — products need substitution or partial fractions.

Resolve the exponent/log BEFORE you integrate

Students who integrate eln⁡(tan⁡x)e^{\ln(\tan x)} as if the exponent were a variable get nonsense. eln⁡(tan⁡x)e^{\ln(\tan x)} is just tan⁡x\tan x — simplify, then integrate.

Divide by ln⁡a\ln a, not by aa

∫ax dx=axln⁡a\int a^x\,dx = \dfrac{a^x}{\ln a}, never axa\dfrac{a^x}{a} and never axln⁡aa^x\ln a (that is the derivative). The ln⁡a\ln a lives in the denominator.

Factor out the leading coefficient first

For ∫dx2x2−2x+1\int\dfrac{dx}{2x^2-2x+1}, pull the 2 out: 2(x2−x+12)2\big(x^2 - x + \tfrac12\big), THEN complete the square inside. Skipping this gives the wrong kk and a wrong coefficient.

The whole bracket must be f+f′f + f'

Identify ff so that the LEFTOVER terms are exactly f′f'. If they are not, the shortcut does not apply and you fall back to substitution or parts. Check by differentiating your proposed exf(x)e^x f(x).

du/dx is the integrand, not the other integral

If u=∫excos⁡x dxu = \int e^x\cos x\,dx, then dudx=excos⁡x\dfrac{du}{dx} = e^x\cos x (you undo the integral), NOT −v-v or any other integral. Differentiation cancels the integral sign directly.

Two true facts can still give a false link

'sin⁡2(x+π)=sin⁡2x\sin^2(x+\pi)=\sin^2 x' is true and 'the integrand is periodic' is true — but neither makes the ANTIDERIVATIVE periodic. Judge the statement about f(x)f(x), not the one about the integrand, on its own.

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 is the most common error on 1±sin⁡2x\sqrt{1\pm\sin 2x} problems.

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.

Integration by Substitution

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Why Substitution Works — the Reverse Chain Rule

Substitution rule

∫f(g(x)) g′(x) dx=∫f(u) du,u=g(x)\int f\big(g(x)\big)\,g'(x)\,dx = \int f(u)\,du,\quad u=g(x)

Algebraic and Composite Substitutions

Power-times-derivative shape

∫(g(x))n g′(x) dx=(g(x))n+1n+1+C\int \big(g(x)\big)^n\,g'(x)\,dx = \dfrac{\big(g(x)\big)^{n+1}}{n+1} + C

The f-prime-over-f to Log Pattern

Log pattern

∫f′(x)f(x) dx=ln⁡∣f(x)∣+C\int \dfrac{f'(x)}{f(x)}\,dx = \ln|f(x)| + C

Trigonometric Substitutions and Identity Reductions

The divide-by-cos-squared move

∫dxa2sin⁡2x+b2cos⁡2x=∫sec⁡2x dxa2tan⁡2x+b2=1abtan⁡−1 ⁣(atan⁡xb)+C\int \dfrac{dx}{a^2\sin^2 x + b^2\cos^2 x} = \int \dfrac{\sec^2 x\,dx}{a^2\tan^2 x + b^2} = \dfrac{1}{ab}\tan^{-1}\!\Big(\dfrac{a\tan x}{b}\Big) + C

Rationalising a Surd Denominator

Conjugate clears the surd

1x+a−x+b=x+a+x+ba−b\dfrac{1}{\sqrt{x+a}-\sqrt{x+b}} = \dfrac{\sqrt{x+a}+\sqrt{x+b}}{a-b}

Spotting a Hidden Derivative

The x-to-the-x derivative

ddx xx=xx(1+ln⁡x)\dfrac{d}{dx}\,x^x = x^x(1+\ln x)

Common traps

Every x must disappear before you integrate in u

After substituting, the integral must be purely in uu and dudu. A leftover xx means uu was chosen badly or a constant factor was mishandled — fix it before integrating.

Carry the sign from du

With u=cos⁡xu=\cos x, du=−sin⁡x dxdu=-\sin x\,dx — the minus sign is part of the substitution. Dropping it flips the answer's sign, and the wrong-sign option is always offered.

Adjust by a constant, never by a variable

If the numerator is kk times f′(x)f'(x) for a constant kk, pull kk out. But if it differs by a FUNCTION of xx, the pattern does not apply — do not force it.

Which of aa, bb goes inside the arctan?

In ∫dta2t2+b2\int \dfrac{dt}{a^2t^2+b^2} the coefficient of t2t^2 ends up multiplying tt inside: tan⁡−1(atb)\tan^{-1}\big(\tfrac{at}{b}\big), not tan⁡−1(bta)\tan^{-1}\big(\tfrac{bt}{a}\big). Check with a=1a=1: ∫dtt2+b2=1btan⁡−1tb\int\frac{dt}{t^2+b^2} = \frac1b\tan^{-1}\frac{t}{b} — tt is divided by the constant term's root. A published key for this exact PYQ had aa and bb swapped; the 1ab\tfrac{1}{ab} outside is the same either way, so only the inside tells the options apart.

A square root forces an absolute value

(sin⁡x−cos⁡x)2=∣sin⁡x−cos⁡x∣\sqrt{(\sin x - \cos x)^2} = |\sin x - \cos x|, and the sign depends on the given range of xx. On 0<x<π40<x<\tfrac{\pi}{4}, cos⁡x>sin⁡x\cos x > \sin x, so it equals cos⁡x−sin⁡x\cos x - \sin x — read the interval before dropping the modulus.

Do not lose the 1 over (a minus b) factor

After conjugating, the constant denominator a−ba-b stays as a multiplier on the whole integral. Forgetting it scales every coefficient wrong — the classic error on x+1−x−1\sqrt{x+1}-\sqrt{x-1} (where a−b=2a-b=2).

x-to-the-x is neither a power nor an exponential

ddxxx≠x⋅xx−1\dfrac{d}{dx}x^x \neq x\cdot x^{x-1} (power rule) and ≠xxln⁡x\neq x^x\ln x (exponential rule). Both the base and the exponent vary, so its derivative is xx(1+ln⁡x)x^x(1+\ln x) — derived via logarithmic differentiation.

Integration by Parts

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The By-Parts Formula and LIATE

Integration by parts

∫u dv=uv−∫v du\int u\,dv = uv - \int v\,du
  • uufactor you differentiate (pick by LIATE)
  • dvdvremaining factor, which you integrate to vv

Integrating a Lone Logarithm

Integral of the logarithm

∫ln⁡x dx=xln⁡x−x+C\int \ln x\,dx = x\ln x - x + C

Products and Telescoping Cancellations

The product-rule trade

∫u dv=uv−∫v du\int u\,dv = uv - \int v\,du

Common traps

Choosing u backwards makes it worse

If ∫v du\int v\,du is harder than where you started, you picked uu and dvdv the wrong way round. LIATE almost always points to the right uu — trust it.

ln x has no naive antiderivative

∫ln⁡x dx\int \ln x\,dx is NOT 1x\dfrac{1}{x} (that is the derivative) and NOT (ln⁡x)22\dfrac{(\ln x)^2}{2}. It is xln⁡x−xx\ln x - x — derive it by parts if you ever forget it.

Simplify disguised factors before applying parts

eln⁡xe^{\ln x} is just xx; eln⁡(tan⁡x)e^{\ln(\tan x)} is just tan⁡x\tan x. Collapse these FIRST — applying by-parts to the disguised form wastes a step and invites errors.

Integration by Partial Fractions

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Decomposition and the Cover-Up Method

Linear-factor decomposition

p(x)(x−a)(x−b)=Ax−a+Bx−b\dfrac{p(x)}{(x-a)(x-b)} = \dfrac{A}{x-a} + \dfrac{B}{x-b}

The Recurring 1 over x times x-to-the-n-plus-1 Family

Closed form for the family

∫dxx(xn+1)=1nln⁡∣xnxn+1∣+C\int \dfrac{dx}{x(x^n+1)} = \dfrac{1}{n}\ln\left|\dfrac{x^n}{x^n+1}\right| + C

Substitute First, Then Decompose

Trig-to-rational substitution

∫sin⁡θ dθf(cos⁡θ)=−∫duf(u),u=cos⁡θ\int \dfrac{\sin\theta\,d\theta}{f(\cos\theta)} = -\int \dfrac{du}{f(u)},\quad u=\cos\theta

Express the Numerator via the Denominator and Its Derivative

Numerator as denom + derivative

N(x)=A D(x)+B D′(x) ⇒ ∫ND dx=Ax+Bln⁡∣D∣+CN(x) = A\,D(x) + B\,D'(x)\ \Rightarrow\ \int \dfrac{N}{D}\,dx = A x + B\ln|D| + C

Common traps

Decompose only a PROPER fraction

If the numerator's degree is ≥\geq the denominator's, do polynomial division FIRST, then decompose the remainder. Skipping this gives a wrong split.

The 1 over n out front is easy to lose

The coefficient is 1n\dfrac{1}{n}, coming from xn−1dx=1nd(xn)x^{n-1}dx = \tfrac1n d(x^n). For n=7n=7 the answer carries 17\tfrac17; the no-coefficient option is the planted distractor.

Carry the minus from du, and the chain factor

u=cos⁡θu=\cos\theta gives du=−sin⁡θ dθdu=-\sin\theta\,d\theta — the leading minus stays. And a factor like 3+4cos⁡θ3+4\cos\theta contributes a 14\tfrac14 to its log coefficient because ddu(3+4u)=4\dfrac{d}{du}(3+4u)=4.

Watch the sign in the denominator's derivative

ddx(2cos⁡x+5sin⁡x)=−2sin⁡x+5cos⁡x\dfrac{d}{dx}(2\cos x + 5\sin x) = -2\sin x + 5\cos x — the cosine term's derivative is −sin⁡-\sin. A sign slip in the 2×22\times2 system swaps AA and BB, the exact distractor the paired items test.

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