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Indefinite Integration formulas

32 formulas and 35 common traps for MHT-CET Maths Indefinite Integration, grouped by subtopic.

Full notes with worked examples

Foundations — Antiderivatives, the +C, and Standard Formulae

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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=log⁡∣x∣\int x^{-1} = \log|x| a separate row

The Linear-Argument Rule (replace x with ax + b)

Linear-argument rule

∫f(ax+b) dx=1a F(ax+b)+Cwhere∫f(x) dx=F(x)+C\int f(ax+b)\,dx = \dfrac{1}{a}\,F(ax+b) + C \quad\text{where}\quad \int f(x)\,dx = F(x)+C
  • aacoefficient of xx inside — you divide by it
  • ax+bax+bthe argument; must be LINEAR for the shortcut to hold

Linearity and Algebraic Pre-processing

Linearity of integration

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

Finding C from a Boundary Condition

Solving for the constant

f(x)=F(x)+C,C=f(a)−F(a)f(x) = F(x) + C,\qquad C = f(a) - F(a)
  • f(a)=kf(a) = kthe given boundary value
  • F(a)F(a)antiderivative evaluated at the boundary point

Reconstruct the Function, Then Integrate

Composition of a function with itself

(f∘f)(x)=f(f(x))(f\circ f)(x) = f\big(f(x)\big)

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. MHT-CET options are written so that the 'no constant' version and a wrong-constant version both appear — only +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=log⁡∣x∣+C\int \dfrac{1}{x}\,dx = \log|x| + C. This exclusion is tested directly.

Only LINEAR insides get the 1/a shortcut

The rule holds because ddx(ax+b)=a\dfrac{d}{dx}(ax+b) = a is a constant. For a non-linear inside like x2+1x^2+1 or x\sqrt{x}, the derivative is not constant — you must do a full substitution, not just divide by a number.

Divide before you integrate an improper fraction

If the numerator's degree is ≥\geq the denominator's, you cannot jump to a log or arctan form. Polynomial-divide first; the remainder term is what carries the log/arctan.

Solve for C only AFTER integrating

The boundary value applies to ff, not f′f'. Integrate fully first, keep the CC, then substitute the known point. Substituting into f′f' does nothing.

Build f explicitly before integrating

You cannot integrate f(g(x))f(g(x)) until you know ff. Substitute to find the explicit rule first; integrating the composition blind is the most common error on these.

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 — the Workhorse Method

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The Substitution Rule

Substitution rule

∫f(g(x)) g′(x) dx=∫f(u) du,u=g(x)\int f(g(x))\,g'(x)\,dx = \int f(u)\,du,\quad u = g(x)
  • u=g(x)u = g(x)the inner function you rename
  • du=g′(x) dxdu = g'(x)\,dxits differential, which must appear in the integrand

The f'(x)/f(x) → log Pattern

Logarithmic integral

∫f′(x)f(x) dx=log⁡∣f(x)∣+C\int \dfrac{f'(x)}{f(x)}\,dx = \log|f(x)| + C
  • f(x)f(x)the denominator
  • f′(x)f'(x)its derivative — must equal the numerator (up to a constant)

Power of a Function times its Derivative

Power-of-a-function rule

∫[f(x)]n f′(x) dx=[f(x)]n+1n+1+C(n≠−1)\int [f(x)]^n\,f'(x)\,dx = \dfrac{[f(x)]^{n+1}}{n+1} + C \quad (n \neq -1)

Root and Linear-Radical Substitutions

Linear-radical substitution

t=ax+b ⇒ x=t2−ba,dx=2ta dtt = \sqrt{ax+b}\ \Rightarrow\ x = \dfrac{t^2 - b}{a},\quad dx = \dfrac{2t}{a}\,dt

Reciprocal and Take-out-the-Power Substitutions

The reciprocal substitution

t=x±kx  ⇒  dt=(1∓kx2)dxt = x \pm \dfrac{k}{x} \;\Rightarrow\; dt = \left(1 \mp \dfrac{k}{x^2}\right)dx
  • ±k/x\pm k/xsign chosen so dtdt matches the numerator after dividing by x2x^2

Exponential and Special Substitutions

Exponential substitution

t=ex ⇒ dt=ex dxt = e^{x}\ \Rightarrow\ dt = e^{x}\,dx

Common traps

Adjust for the missing constant

If du=g′(x) dxdu = g'(x)\,dx appears up to a numeric factor (e.g. you have x dxx\,dx but du=2x dxdu = 2x\,dx), pull the constant out: x dx=12 dux\,dx = \tfrac12\,du. Forgetting the 12\tfrac12 is the most common slip.

Engineer the numerator into f'(x) + leftover

Rarely is the top exactly f′(x)f'(x). Write it as 'constant ×f′(x)\times f'(x) + remainder', send the first piece to a clean log, and handle the remainder separately. The whole-number coefficient comes from matching.

n = −1 is NOT this rule

If the power is −1-1 (i.e. ∫f′/f\int f'/f), the power rule blows up. That case is the log pattern. Every other integer/fraction power uses un+1n+1\dfrac{u^{n+1}}{n+1}.

Re-express EVERY x, including dx

After t=xt = \sqrt{x}, both the integrand AND dx=2t dtdx = 2t\,dt must be rewritten. Leaving a stray xx or the old dxdx behind is the classic substitution error.

Pick the sign of t = x ± k/x from the numerator

After dividing by x2x^2, if the numerator is 1−kx21 - \dfrac{k}{x^2} use t=x+kxt = x + \dfrac{k}{x}; if it is 1+kx21 + \dfrac{k}{x^2} use t=x−kxt = x - \dfrac{k}{x}. The substitution only works when dtdt reproduces the numerator exactly.

Towers: substitute the INNER exponential

For ∫aaxax dx\int a^{a^x} a^x\,dx, the right substitution is u=axu = a^x, not u=aaxu = a^{a^x}. The stray ax dxa^x\,dx is what becomes dudu (up to log⁡a\log a).

Trigonometric Integrals I — Powers and Identities

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The Standard tan, cot, sec, cosec Integrals

The two that need the conjugate trick

∫sec⁡x dx=log⁡∣sec⁡x+tan⁡x∣+C,∫csc⁡x dx=log⁡∣csc⁡x−cot⁡x∣+C\int \sec x\,dx = \log|\sec x + \tan x| + C,\qquad \int \csc x\,dx = \log|\csc x - \cot x| + C

Power Reduction with Pythagorean Identities

Key reduction identity

tan⁡2x=sec⁡2x−1\tan^2 x = \sec^2 x - 1

Identity Simplification before Integrating

A workhorse collapse

tan⁡x+cot⁡x=sin⁡2x+cos⁡2xsin⁡xcos⁡x=2sin⁡2x=2csc⁡2x\tan x + \cot x = \dfrac{\sin^2 x + \cos^2 x}{\sin x\cos x} = \dfrac{2}{\sin 2x} = 2\csc 2x

Simplify the Inverse-Trig Argument First

Cancel, then integrate

tan⁡−1(tan⁡θ)=θ,sin⁡−1(sin⁡θ)=θ(θ in principal range)\tan^{-1}(\tan\theta) = \theta,\quad \sin^{-1}(\sin\theta)=\theta \quad (\theta\text{ in principal range})

Common traps

∫sec and ∫cosec are NOT plain logs of sec/cosec

∫sec⁡x dx=log⁡∣sec⁡x+tan⁡x∣\int \sec x\,dx = \log|\sec x + \tan x|, not log⁡∣sec⁡x∣\log|\sec x|. The +tan⁡x+\tan x (and −cot⁡x-\cot x for cosec) is exactly what the conjugate trick produces — options drop it to bait you.

Keep one sec²x to pair with the tan-power

The whole method works because sec⁡2x dx=d(tan⁡x)\sec^2 x\,dx = d(\tan x). Each reduction must leave a sec⁡2x\sec^2 x attached to a power of tan⁡x\tan x so the power rule applies — otherwise you stall.

Try an identity before a substitution

Reaching for Weierstrass on ∫(tan⁡x+cot⁡x) dx\int(\tan x + \cot x)\,dx is a long detour — one identity makes it 2csc⁡2x2\csc 2x instantly. Simplify first; substitute only if no identity collapses it.

Reduce the argument BEFORE integrating

Never reach for by-parts on ∫tan⁡−1(⋯ ) dx\int\tan^{-1}(\cdots)\,dx until you've tried to collapse the inside. If the argument is a half/double-angle form, the inverse cancels and the integral is a one-line polynomial — by-parts is a needless detour.

Rational Functions and Partial Fractions

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Standard Quadratic Denominator Forms

The arctan form

∫dxx2+a2=1atan⁡−1xa+C\int \dfrac{dx}{x^2 + a^2} = \dfrac{1}{a}\tan^{-1}\dfrac{x}{a} + C

Completing the square

ax2+bx+c=a(x+b2a)2+(c−b24a)ax^2 + bx + c = a\left(x + \dfrac{b}{2a}\right)^2 + \left(c - \dfrac{b^2}{4a}\right)

Linear Numerator over a Quadratic (Numerator Split)

Numerator as derivative-of-denominator plus constant

px+q=Addx(ax2+bx+c)+Bpx + q = A\dfrac{d}{dx}(ax^2+bx+c) + B
  • AAcoefficient that reproduces the xx-term via (ax2+bx+c)′(ax^2+bx+c)'
  • BBleftover constant — its integral completes the square

Partial-Fraction Decomposition

Distinct-linear decomposition

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

Common traps

x⁴ + bx² + c → try t = x ± k/x

A denominator quadratic in x2x^2 with a matching numerator (1∓k/x2)(1 \mp k/x^2) is the signal for t=x±k/xt = x \pm k/x. It collapses the quartic to a simple t2+1t^2 + 1 arctan — a recurring MHT-CET shape.

Factor the sign on x² before completing the square

With −x2-x^2 terms, pull out the −1-1 first: 7−6x−x2=−(x2+6x−7)7 - 6x - x^2 = -(x^2 + 6x - 7). Forgetting the sign flip turns an arcsin into a (wrong) log or vice versa.

Split the numerator BEFORE completing the square

The derivative-piece must come out first (it gives the \sqrt{} or log term). Only the leftover constant goes through completing the square. Completing the square first leaves the xx in the numerator with nowhere to go.

Improper fraction? Divide before decomposing

Partial fractions require the numerator degree to be LESS than the denominator's. If not, polynomial-divide first, then decompose the proper remainder.

Repeated factor needs every power

For (x−a)2(x-a)^2 you must include BOTH Ax−a\dfrac{A}{x-a} and B(x−a)2\dfrac{B}{(x-a)^2}. Dropping the first-power term gives an unsolvable system.

Trigonometric Integrals II — Rational Forms and Substitutions

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The Half-Angle (Weierstrass) Substitution

Weierstrass substitution

t=tan⁡x2:sin⁡x=2t1+t2, cos⁡x=1−t21+t2, dx=2 dt1+t2t = \tan\dfrac{x}{2}:\quad \sin x = \dfrac{2t}{1+t^2},\ \cos x = \dfrac{1-t^2}{1+t^2},\ dx = \dfrac{2\,dt}{1+t^2}

Divide by cos²x for a + b·sin²x Forms

After dividing by cos²x

∫sec⁡2x dxA+Btan⁡2x→ t=tan⁡x ∫dtA+Bt2\int \dfrac{\sec^2 x\,dx}{A + B\tan^2 x} \xrightarrow{\,t=\tan x\,} \int \dfrac{dt}{A + Bt^2}

Product of Two Shifted Sines (or Cosines)

Shifted-angle split

1sin⁡(x−a)sin⁡(x−b)=1sin⁡(b−a)[cot⁡(x−b)−cot⁡(x−a)]\dfrac{1}{\sin(x-a)\sin(x-b)} = \dfrac{1}{\sin(b-a)}\big[\cot(x-b) - \cot(x-a)\big]
  • sin⁡(b−a)\sin(b-a)constant divisor — the sine of the difference of the two shifts

Trig to Partial Fractions (substitute, then decompose)

The bridge

∫R(sin⁡x) cos⁡x dx  → t=sin⁡x   ∫R(t) dt    (now rational — decompose)\int R(\sin x)\,\cos x\,dx \;\xrightarrow{\,t=\sin x\,}\; \int R(t)\,dt \;\;(\text{now rational — decompose})

The Fractional-Power tan Trick

The reduction (m + n even)

∫sin⁡mx cos⁡nx dx→ t=tan⁡x ∫tm (1+t2)m+n2−1 dt\int \sin^m x\,\cos^n x\,dx \xrightarrow{\,t=\tan x\,} \int t^{m}\,(1+t^2)^{\frac{m+n}{2}-1}\,dt

Numerator as Denominator + its Derivative

Decomposition of the numerator

num=A⋅den+B⋅(den)′  ⇒  ∫numden dx=Ax+Blog⁡∣den∣+C\text{num} = A\cdot\text{den} + B\cdot(\text{den})' \;\Rightarrow\; \int\dfrac{\text{num}}{\text{den}}\,dx = Ax + B\log|\text{den}| + C

Common traps

Weierstrass is for a + b·sin/cos, not a + b·sin²

If the denominator has sin⁡2x\sin^2 x or cos⁡2x\cos^2 x (an even power), the half-angle substitution gives a messy quartic. Use divide-by-cos⁡2x\cos^2 x instead — the next concept.

Three sin/cos denominators, three substitutions

Denominator has sin⁡2/cos⁡2\sin^2/\cos^2 (even, plain angle): divide by cos⁡2x\cos^2 x, use t=tan⁡xt=\tan x. Denominator has sin⁡2x/cos⁡2x\sin 2x/\cos 2x (double angle): use t=tan⁡xt=\tan x with the 2x2x formulae. Denominator has plain sin⁡x/cos⁡x\sin x/\cos x (odd, single power): use Weierstrass t=tan⁡(x/2)t=\tan(x/2). Picking the wrong one makes the algebra explode.

Split it — don't reach for Weierstrass

Weierstrass on a product of two shifted sines produces a quartic in tt and stalls. The shifted-angle split is one identity and one line. Keep the constant sin⁡(b−a)\sin(b-a) out front — it is NOT a function of xx.

No spare cos/sin → no bridge

The substitution only works if exactly one cos⁡x dx\cos x\,dx (or sin⁡x dx\sin x\,dx) is available to become dtdt and everything else turns rational in tt. If both sin⁡x\sin x and cos⁡x\cos x appear in odd/mixed ways with nothing spare, fall back to Weierstrass.

Check m + n is an even integer first

The trick only collapses cleanly when m+nm + n is an even integer (so cos⁡m+nx\cos^{m+n}x becomes an integer power of sec⁡2x\sec^2 x). If it is odd, this route leaves a stray sec⁡x\sec x or cos⁡x\cos x and you need a different method.

Convert tan-fractions to sin/cos first

A ratio in tan⁡x\tan x is easiest after multiplying through by cos⁡x\cos x to get a sin/cos ratio — then the 'denominator + its derivative' decomposition is clean.

Integration by Parts

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Integration by Parts and the LIATE Rule

Integration by parts

∫u dv=uv−∫v du\int u\,dv = uv - \int v\,du
  • uufactor to differentiate (earliest in LIATE)
  • dvdvfactor to integrate (the rest, including dxdx)

Cyclic Integrals (Return-to-Self)

The cyclic result

∫eaxsin⁡bx dx=eax(asin⁡bx−bcos⁡bx)a2+b2+C\int e^{ax}\sin bx\,dx = \dfrac{e^{ax}(a\sin bx - b\cos bx)}{a^2 + b^2} + C

The eˣ[f(x) + f'(x)] Family

The eˣ[f + f'] shortcut

∫ex[f(x)+f′(x)] dx=exf(x)+C\int e^x\big[f(x) + f'(x)\big]\,dx = e^x f(x) + C
  • f(x)f(x)the function whose value lands in the answer
  • f′(x)f'(x)its derivative — must be the other half of the bracket

Integrals of √(quadratic) — Standard Results (syllabus reference)

Square root of a quadratic — the three results

∫a2−x2 dx=x2a2−x2+a22sin⁡−1xa+C\int \sqrt{a^2 - x^2}\,dx = \dfrac{x}{2}\sqrt{a^2 - x^2} + \dfrac{a^2}{2}\sin^{-1}\dfrac{x}{a} + C
  • a2−x2a^2 - x^2arcsin result
  • a2+x2, x2−a2a^2 + x^2,\ x^2 - a^2log results (signs differ)

Generalised (Tabular) By-Parts — a shortcut

Tabular by-parts series

∫u v dx=u v1−u′ v2+u′′ v3−u′′′ v4+⋯\int u\,v\,dx = u\,v_1 - u'\,v_2 + u''\,v_3 - u'''\,v_4 + \cdots
  • u′,u′′,…u', u'', \ldotssuccessive derivatives of the polynomial uu
  • v1,v2,…v_1, v_2, \ldotssuccessive integrals of vv

Common traps

A lone log or inverse-trig still uses parts

∫log⁡x dx\int \log x\,dx and ∫tan⁡−1x dx\int \tan^{-1}x\,dx look like single functions, but they are integrated by parts with dv=dx, v=xdv = dx,\ v = x. There is no direct formula.

Stop after two rounds — don't loop forever

The point of a cyclic integral is that the original II reappears after two rounds. Recognise it and solve algebraically; a third by-parts just sends you in circles.

Use identities to expose f + f'

The bracket rarely arrives as a clean f+f′f + f'. Apply identities first — e.g. 1+cot⁡2=csc⁡21 + \cot^2 = \csc^2 — so that one term is a function and the other is its exact derivative. Then the answer is immediate.

Syllabus result, not a current bank pattern

This bank's recent CET questions keep the square root in a DENOMINATOR (handled by the numerator-split + completing-the-square concepts). The ∫quadratic dx\int\sqrt{\text{quadratic}}\,dx form here is on the syllabus and could appear — but don't expect it among the tagged drills, because the live bank has none yet.

Only for a polynomial first function

The shortcut relies on the polynomial's derivatives reaching zero. If neither factor is a polynomial (e.g. ∫exsin⁡x dx\int e^x\sin x\,dx), the table never terminates — use ordinary or cyclic by-parts instead.

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