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Properties of Definite Integrals: The Complete JEE Method

Ritesh Raj · 23 Aug 2026
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23 min read18 sectionsConcept

A definite integral is a number. That single sentence decides most of what follows: a number can be estimated, compared, bounded, split, reflected and paired, and none of those moves need the antiderivative that a beginner reaches for first.

Most JEE questions on this chapter are built on that gap. They hand you an integrand whose antiderivative does not exist in closed form, then reward you for noticing a symmetry. ∫π/245π/24dx1+tan⁡2x3\int_{\pi/24}^{5\pi/24}\frac{dx}{1+\sqrt[3]{\tan 2x}} has no elementary antiderivative. It still takes about forty seconds.

Definite integral as signed area under a curve, with the area above the axis counted positive and below negative

Fundamental concept of the definite integral

Everything in this chapter follows from one distinction. Read this table across, not down.

Indefinite integral ∫f(x) dx\int f(x)\,dxDefinite integral ∫abf(x) dx\int_a^b f(x)\,dx
1. DefinitionThe family of all antiderivatives, ϕ(x)+C\phi(x)+C where ϕ′=f\phi'=fThe single number ϕ(b)−ϕ(a)\phi(b)-\phi(a)
2. What it producesA function of xxA real number, no xx left in it
3. Role of the variablexx survives into the answerxx is a dummy: ∫abf(x) dx=∫abf(t) dt\int_a^b f(x)\,dx=\int_a^b f(t)\,dt
4. Constant of integrationEssential, the answer is wrong without itCancels in the subtraction, never write it
5. Geometrical meaningNone on its ownSigned area between the curve and the xx-axis from aa to bb
6. Effect of swapping limitsNot applicableSign flips: ∫ab=−∫ba\int_a^b=-\int_b^a

The word signed in row 5 is where marks are lost. Area is never negative; a definite integral often is. Where the curve dips below the axis the strip contributes a negative amount, so ∫02πsin⁡x dx=0\int_0^{2\pi}\sin x\,dx=0 even though the curve encloses a total area of 44.

Signed area: the region above the axis counted positive, the region below counted negative, and the two cancelling for sin x over one full period
The first trap of the chapter

"Area under the curve" and "the definite integral" are not synonyms. If a question asks for area, you integrate ∣f(x)∣|f(x)|, which means splitting at every root of ff. If it asks for the integral, you do not split. Reading the wrong one costs the whole question.

The six properties, in one table

PropertyStatementWhat it is really for
IDummy variable∫abf(x) dx=∫abf(t) dt\int_a^b f(x)\,dx=\int_a^b f(t)\,dtLets you rename before pairing two integrals
IIInterchanging limits∫abf(x) dx=−∫baf(x) dx\int_a^b f(x)\,dx=-\int_b^a f(x)\,dxFixes orientation after a substitution
IIISplitting∫abf=∫acf+∫cbf\int_a^b f=\int_a^c f+\int_c^b fHandles modulus, greatest integer, piecewise
IVKing∫abf(x) dx=∫abf(a+b−x) dx\int_a^b f(x)\,dx=\int_a^b f(a+b-x)\,dxThe workhorse of the chapter
VDoubling on [0,2a][0,2a]∫02af=∫0af(x) dx+∫0af(2a−x) dx\int_0^{2a}f=\int_0^a f(x)\,dx+\int_0^a f(2a-x)\,dxCollapses to 00 or 2∫0af2\int_0^a f
VIOdd and even∫−aaf=0\int_{-a}^{a}f=0 if ff odd, =2∫0af=2\int_0^a f if ff evenKills half the integrand on sight

Property III does not require cc to lie between aa and bb. That is worth remembering, because it lets you write ∫−42=∫−4−1+∫−12\int_{-4}^{2}=\int_{-4}^{-1}+\int_{-1}^{2} and also ∫12=∫15+∫52\int_1^2=\int_1^5+\int_5^2 when the second form is the one you can compute.

Property IV, the king property

∫abf(x) dx=∫abf(a+b−x) dx\int_a^b f(x)\,dx=\int_a^b f(a+b-x)\,dx

Why it is true

Put t=a+b−xt=a+b-x, so dt=−dxdt=-dx. When x=ax=a, t=bt=b; when x=bx=b, t=at=a.

∫abf(a+b−x) dx=∫baf(t) (−dt)=∫abf(t) dt\int_a^b f(a+b-x)\,dx=\int_b^a f(t)\,(-dt)=\int_a^b f(t)\,dt

and by Property I that last integral is ∫abf(x) dx\int_a^b f(x)\,dx.

What it means geometrically

x↦a+b−xx\mapsto a+b-x is the reflection of the interval [a,b][a,b] in its own midpoint a+b2\frac{a+b}{2}. So the property says: flip the graph left-to-right about the midpoint of the interval and the area does not change. That is obvious once you see it, and it is the whole content of the property.

Reflection of a curve about the midpoint of the interval of integration, showing the two shaded regions have equal area

The pattern that makes it pay

King is worth using when f(x)+f(a+b−x)f(x)+f(a+b-x) is simpler than either piece. Two shapes account for almost every JEE question:

If f(x)+f(a+b−x)=k, then ∫abf(x) dx=k(b−a)2\text{If }f(x)+f(a+b-x)=k\text{, then }\int_a^b f(x)\,dx=\frac{k(b-a)}{2} If f(x)=g(x)g(x)+g(a+b−x), then ∫abf(x) dx=b−a2\text{If }f(x)=\frac{g(x)}{g(x)+g(a+b-x)}\text{, then }\int_a^b f(x)\,dx=\frac{b-a}{2}

The second is the first in disguise, with k=1k=1.

How to spot it in three seconds

Add the two limits. If a+ba+b is a round number like π2\frac{\pi}{2}, π\pi, 11, 55 or 2π2\pi, and the integrand contains tan⁡\tan, cot⁡\cot, sin⁡\sin, cos⁡\cos or a ratio of the form gg+h\frac{g}{g+h}, try king before anything else.

The one statement that is false

This is the classic two-statement question, and it has been asked in almost exactly this form more than once.

Example 1. (IIT JEE 2013) Statement I: ∫π/6π/3dx1+tan⁡x=π6\int_{\pi/6}^{\pi/3}\frac{dx}{1+\sqrt{\tan x}}=\frac{\pi}{6}. Statement II: ∫abf(x) dx=∫abf(a+b−x) dx\int_a^b f(x)\,dx=\int_a^b f(a+b-x)\,dx. Which is correct?

▸ SHOW SOLUTION

Step 1: Statement II is Property IV, so it is true

Nothing to check.

Step 2: Apply it to Statement I

Here a+b=π6+π3=π2a+b=\frac{\pi}{6}+\frac{\pi}{3}=\frac{\pi}{2}, and tan⁡(π2−x)=cot⁡x\tan\left(\frac{\pi}{2}-x\right)=\cot x.

I=∫π/6π/3dx1+cot⁡x=∫π/6π/3tan⁡x dx1+tan⁡xI=\int_{\pi/6}^{\pi/3}\frac{dx}{1+\sqrt{\cot x}}=\int_{\pi/6}^{\pi/3}\frac{\sqrt{\tan x}\,dx}{1+\sqrt{\tan x}}

Step 3: Add the two forms

2I=∫π/6π/31+tan⁡x1+tan⁡x dx=∫π/6π/3dx=π3−π6=π62I=\int_{\pi/6}^{\pi/3}\frac{1+\sqrt{\tan x}}{1+\sqrt{\tan x}}\,dx=\int_{\pi/6}^{\pi/3}dx=\frac{\pi}{3}-\frac{\pi}{6}=\frac{\pi}{6}

Step 4: Read the last line carefully

2I=π62I=\frac{\pi}{6}, so I=π12I=\frac{\pi}{12}, not π6\frac{\pi}{6}.

Statement I is false, Statement II is true.

The trap is not the mathematics. It is stopping at 2I2I and copying that number down. Every king-property question ends with a division by two, and the wrong option is always waiting there.

Three ways king goes wrong
  1. Forgetting the halving. 2I=k(b−a)2I=k(b-a) is not the answer.
  2. Using the wrong reflection. The map is x↦a+b−xx\mapsto a+b-x, built from the actual limits. On ∫π/6π/3\int_{\pi/6}^{\pi/3} it is x↦π2−xx\mapsto\frac{\pi}{2}-x, not x↦π−xx\mapsto\pi-x.
  3. Applying it across a discontinuity. King is a substitution, and a substitution needs the integrand to be integrable on the whole interval. ∫−11dxx2\int_{-1}^{1}\frac{dx}{x^2} is not 2∫01dxx22\int_0^1\frac{dx}{x^2}; both sides are meaningless, because the integrand blows up at 00.

Odd, even and the two symmetries

Property VI is the special case of Property IV in which the midpoint is the origin. It is worth separating the two symmetries a question can hand you, because students routinely apply the first when only the second is available.

A. Symmetry about zero

On an interval [−a,a][-a,a]:

∫−aaf(x) dx={0if f(−x)=−f(x)2∫0af(x) dxif f(−x)=f(x)\int_{-a}^{a}f(x)\,dx=\begin{cases}0 & \text{if }f(-x)=-f(x)\\[4pt]2\displaystyle\int_0^a f(x)\,dx & \text{if }f(-x)=f(x)\end{cases}

The value of this is not that it saves arithmetic. It is that it lets you delete terms before you integrate anything. In a sum f=fodd+fevenf=f_{\text{odd}}+f_{\text{even}} over a symmetric interval, the odd part contributes nothing at all, so you never compute it.

An odd function on a symmetric interval, with the two shaded regions equal in size and opposite in sign

Example 2. (JEE Main 2026, 21 Jan Shift 1) Find ∫−π/6π/6π+4x111−sin⁡(∣x∣+π6) dx\int_{-\pi/6}^{\pi/6}\frac{\pi+4x^{11}}{1-\sin\left(|x|+\frac{\pi}{6}\right)}\,dx.

▸ SHOW SOLUTION

Step 1: Split the numerator

The denominator 1−sin⁡(∣x∣+π6)1-\sin\left(|x|+\frac{\pi}{6}\right) contains ∣x∣|x|, so it is an even function of xx.

Step 2: Classify each piece

π1−sin⁡(∣x∣+π6)\dfrac{\pi}{1-\sin\left(|x|+\frac\pi6\right)} is even. 4x111−sin⁡(∣x∣+π6)\dfrac{4x^{11}}{1-\sin\left(|x|+\frac\pi6\right)} is odd over even, so it is odd.

Step 3: Delete the odd part

I=∫−π/6π/6π dx1−sin⁡(∣x∣+π6)=2π∫0π/6dx1−sin⁡(x+π6)I=\int_{-\pi/6}^{\pi/6}\frac{\pi\,dx}{1-\sin\left(|x|+\frac{\pi}{6}\right)}=2\pi\int_0^{\pi/6}\frac{dx}{1-\sin\left(x+\frac{\pi}{6}\right)}

Step 4: Substitute u=x+π6u=x+\frac{\pi}{6}

I=2π∫π/6π/3du1−sin⁡uI=2\pi\int_{\pi/6}^{\pi/3}\frac{du}{1-\sin u}

Step 5: Rationalise

11−sin⁡u=1+sin⁡ucos⁡2u=sec⁡2u+sec⁡utan⁡u\frac{1}{1-\sin u}=\frac{1+\sin u}{\cos^2u}=\sec^2u+\sec u\tan u

Step 6: Integrate

I=2π[tan⁡u+sec⁡u]π/6π/3=2π[(3+2)−(13+23)]I=2\pi\Big[\tan u+\sec u\Big]_{\pi/6}^{\pi/3}=2\pi\left[\left(\sqrt3+2\right)-\left(\frac{1}{\sqrt3}+\frac{2}{\sqrt3}\right)\right]

Step 7: Simplify

13+23=33=3\frac{1}{\sqrt3}+\frac{2}{\sqrt3}=\frac{3}{\sqrt3}=\sqrt3, so the bracket is 3+2−3=2\sqrt3+2-\sqrt3=2.

I=4πI=4\pi

The same idea, with a harder disguise, was IIT JEE 2004: ∫−π/3π/3π+4x32−cos⁡(∣x∣+π3) dx\int_{-\pi/3}^{\pi/3}\frac{\pi+4x^3}{2-\cos\left(|x|+\frac{\pi}{3}\right)}\,dx. Twenty-two years apart, same question.

B. Symmetry about the midpoint

When the interval is not centred at the origin, odd and even are unavailable and king is what you have. On [0,2a][0,2a] Property V splits it cleanly:

∫02af(x) dx={0if f(2a−x)=−f(x)2∫0af(x) dxif f(2a−x)=f(x)\int_0^{2a}f(x)\,dx=\begin{cases}0 & \text{if }f(2a-x)=-f(x)\\[4pt]2\displaystyle\int_0^{a}f(x)\,dx & \text{if }f(2a-x)=f(x)\end{cases}

Read f(2a−x)=f(x)f(2a-x)=f(x) as "the graph is symmetric about the vertical line x=ax=a", and f(2a−x)=−f(x)f(2a-x)=-f(x) as "the graph has a half-turn centre at (a,0)(a,0)".

Why these are the same theorem

Shift by aa. Setting g(u)=f(u+a)g(u)=f(u+a) turns [0,2a][0,2a] into [−a,a][-a,a], and f(2a−x)=f(x)f(2a-x)=f(x) becomes g(−u)=g(u)g(-u)=g(u). Odd and even about the origin, and the two symmetries about x=ax=a, are one statement seen from two positions.

The boundary case: when the integrand breaks

Everything above assumed the integrand is continuous. The interesting questions are the ones where it is not, and the fix is always Property III: split the interval at every point where the formula changes, then integrate each piece with its own formula.

Three kinds of break come up:

BreakWhere to splitTypical integrand
ModulusAt every root of the inside expression∣sin⁡x∣\lvert\sin x\rvert, ∣x2+2x−3∣\lvert x^2+2x-3\rvert
Greatest integerAt every integer value of the inside expression[x][x], [2sin⁡x][2\sin x], [xsin⁡x][x\sin x]
Piecewise definitionAt every changeover point given in the definitionf(x)={⋯f(x)=\begin{cases}\cdots\end{cases}
A step function and a modulus function on the same axes, with the split points marked on the x-axis
The split points are not always the obvious ones

For ∫−22[xsin⁡x] dx\int_{-2}^{2}[x\sin x]\,dx the split is not at the integers −1,0,1-1,0,1. It is where xsin⁡xx\sin x crosses an integer, and on [0,2][0,2] that happens once, at the root of xsin⁡x=1x\sin x=1. Find where the inside changes value, not where xx does.

Type 1, king property

Example 3. (JEE Main 2026, 23 Jan Shift 1) Evaluate ∫π/245π/24dx1+tan⁡2x3\int_{\pi/24}^{5\pi/24}\frac{dx}{1+\sqrt[3]{\tan 2x}}.

▸ SHOW SOLUTION

Step 1: Check the limit sum

a+b=π24+5π24=6π24=π4a+b=\frac{\pi}{24}+\frac{5\pi}{24}=\frac{6\pi}{24}=\frac{\pi}{4}, so the reflection is x↦π4−xx\mapsto\frac{\pi}{4}-x.

Step 2: See what it does to the integrand

2(π4−x)=π2−2x2\left(\frac{\pi}{4}-x\right)=\frac{\pi}{2}-2x, and tan⁡(π2−2x)=cot⁡2x\tan\left(\frac{\pi}{2}-2x\right)=\cot 2x.

I=∫π/245π/24dx1+cot⁡2x3=∫π/245π/24tan⁡2x3 dx1+tan⁡2x3I=\int_{\pi/24}^{5\pi/24}\frac{dx}{1+\sqrt[3]{\cot 2x}}=\int_{\pi/24}^{5\pi/24}\frac{\sqrt[3]{\tan 2x}\,dx}{1+\sqrt[3]{\tan 2x}}

Step 3: Add

2I=∫π/245π/24dx=5π24−π24=π62I=\int_{\pi/24}^{5\pi/24}dx=\frac{5\pi}{24}-\frac{\pi}{24}=\frac{\pi}{6}

Step 4: Halve

I=π12I=\frac{\pi}{12}

Example 4. (JEE Main 2026, 6 Apr Shift 1) Find ∫−π/4π/432cos⁡4x1+esin⁡x dx\int_{-\pi/4}^{\pi/4}\frac{32\cos^4x}{1+e^{\sin x}}\,dx.

▸ SHOW SOLUTION

Step 1: Recognise the 11+eg\frac{1}{1+e^{g}} shape

The reflection here is x↦−xx\mapsto-x, and sin⁡(−x)=−sin⁡x\sin(-x)=-\sin x, so the exponential inverts while cos⁡4x\cos^4x is untouched.

I=∫−π/4π/432cos⁡4x1+e−sin⁡x dx=∫−π/4π/432 esin⁡xcos⁡4x1+esin⁡x dxI=\int_{-\pi/4}^{\pi/4}\frac{32\cos^4x}{1+e^{-\sin x}}\,dx=\int_{-\pi/4}^{\pi/4}\frac{32\,e^{\sin x}\cos^4x}{1+e^{\sin x}}\,dx

Step 2: Add the two forms

2I=∫−π/4π/432cos⁡4x⋅1+esin⁡x1+esin⁡x dx=∫−π/4π/432cos⁡4x dx2I=\int_{-\pi/4}^{\pi/4}32\cos^4x\cdot\frac{1+e^{\sin x}}{1+e^{\sin x}}\,dx=\int_{-\pi/4}^{\pi/4}32\cos^4x\,dx

Step 3: Use evenness

2I=64∫0π/4cos⁡4x dx2I=64\int_0^{\pi/4}\cos^4x\,dx

Step 4: Reduce the power

cos⁡4x=(1+cos⁡2x2)2=14(1+2cos⁡2x+cos⁡22x)=38+cos⁡2x2+cos⁡4x8\cos^4x=\left(\frac{1+\cos2x}{2}\right)^2=\frac{1}{4}\left(1+2\cos2x+\cos^22x\right)=\frac{3}{8}+\frac{\cos2x}{2}+\frac{\cos4x}{8}

Step 5: Integrate

∫0π/4cos⁡4x dx=[3x8+sin⁡2x4+sin⁡4x32]0π/4=3π32+14+0\int_0^{\pi/4}\cos^4x\,dx=\left[\frac{3x}{8}+\frac{\sin2x}{4}+\frac{\sin4x}{32}\right]_0^{\pi/4}=\frac{3\pi}{32}+\frac14+0

Step 6: Finish

2I=64(3π32+14)=6π+162I=64\left(\frac{3\pi}{32}+\frac14\right)=6\pi+16, so I=3π+8I=3\pi+8.

The $1+a^{g(x)}$ family

Whenever the denominator is 1+ag(x)1+a^{g(x)} with gg odd about the midpoint, king turns the integrand into its own complement and the exponential vanishes completely. It works for 1+esin⁡x1+e^{\sin x}, 1+πx1+\pi^x, 1+2tan⁡x1+2^{\tan x}, 1+ax1+a^x alike, and the base never appears in the answer. Seeing that the base is irrelevant is the fastest way to confirm you are on the right track.

Example 5. (JEE Main 2026, 4 Apr Shift 2) Evaluate ∫01cot⁡−1(1+x+x2)dx\int_0^1\cot^{-1}\left(1+x+x^2\right)dx.

▸ SHOW SOLUTION

Step 1: Turn the cot⁡−1\cot^{-1} into a difference

1+x+x2=1+x(1+x)1+x+x^2=1+x(1+x), and the identity cot⁡−1(1+uv)=tan⁡−1u−tan⁡−1v\cot^{-1}(1+uv)=\tan^{-1}u-\tan^{-1}v holds when uv>−1uv>-1. With u=1+xu=1+x, v=xv=x:

cot⁡−1(1+x+x2)=tan⁡−1(1+x)−tan⁡−1x\cot^{-1}\left(1+x+x^2\right)=\tan^{-1}(1+x)-\tan^{-1}x

Step 2: Split

I=∫01tan⁡−1(1+x) dx−∫01tan⁡−1x dxI=\int_0^1\tan^{-1}(1+x)\,dx-\int_0^1\tan^{-1}x\,dx

Step 3: Shift the first integral

Put u=1+xu=1+x in the first: it becomes ∫12tan⁡−1u du\int_1^2\tan^{-1}u\,du. So

I=∫12tan⁡−1x dx−∫01tan⁡−1x dxI=\int_1^2\tan^{-1}x\,dx-\int_0^1\tan^{-1}x\,dx

Step 4: Use the antiderivative

∫tan⁡−1x dx=xtan⁡−1x−12log⁡e(1+x2)\int\tan^{-1}x\,dx=x\tan^{-1}x-\frac12\log_e\left(1+x^2\right). Call it F(x)F(x).

I=(F(2)−F(1))−(F(1)−F(0))=F(2)−2F(1)+F(0)I=\big(F(2)-F(1)\big)-\big(F(1)-F(0)\big)=F(2)-2F(1)+F(0)

Step 5: Evaluate

F(0)=0F(0)=0, F(1)=π4−12log⁡e2F(1)=\frac{\pi}{4}-\frac12\log_e2, F(2)=2tan⁡−12−12log⁡e5F(2)=2\tan^{-1}2-\frac12\log_e5.

I=2tan⁡−12−12log⁡e5−π2+log⁡e2I=2\tan^{-1}2-\frac12\log_e5-\frac{\pi}{2}+\log_e2

Step 6: Combine the logs

−12log⁡e5+log⁡e2=−12log⁡e5+12log⁡e4=12log⁡e45=−12log⁡e54-\frac12\log_e5+\log_e2=-\frac12\log_e5+\frac12\log_e4=\frac12\log_e\frac45=-\frac12\log_e\frac54.

I=2tan⁡−12−12log⁡e(54)−π2I=2\tan^{-1}2-\frac12\log_e\left(\frac54\right)-\frac{\pi}{2}

Example 6. (IIT JEE 2011) Find ∫log⁡e2log⁡e3xsin⁡x2sin⁡x2+sin⁡(log⁡e6−x2) dx\int_{\sqrt{\log_e2}}^{\sqrt{\log_e3}}\frac{x\sin x^2}{\sin x^2+\sin\left(\log_e6-x^2\right)}\,dx.

▸ SHOW SOLUTION

Step 1: Kill the outer xx first

Put x2=tx^2=t, so 2x dx=dt2x\,dx=dt. The limits become log⁡e2\log_e2 and log⁡e3\log_e3.

I=12∫log⁡e2log⁡e3sin⁡t dtsin⁡t+sin⁡(log⁡e6−t)I=\frac12\int_{\log_e2}^{\log_e3}\frac{\sin t\,dt}{\sin t+\sin\left(\log_e6-t\right)}

Step 2: Check the limit sum

log⁡e2+log⁡e3=log⁡e6\log_e2+\log_e3=\log_e6, which is exactly the constant inside the second sine. That is the signal.

Step 3: Apply king

I=12∫log⁡e2log⁡e3sin⁡(log⁡e6−t)dtsin⁡(log⁡e6−t)+sin⁡tI=\frac12\int_{\log_e2}^{\log_e3}\frac{\sin\left(\log_e6-t\right)dt}{\sin\left(\log_e6-t\right)+\sin t}

Step 4: Add

2I=12∫log⁡e2log⁡e3dt=12(log⁡e3−log⁡e2)=12log⁡e322I=\frac12\int_{\log_e2}^{\log_e3}dt=\frac12\left(\log_e3-\log_e2\right)=\frac12\log_e\frac32

Step 5: Halve

I=14log⁡e(32)I=\frac14\log_e\left(\frac32\right)

Example 7. (IIT JEE 2002) Evaluate ∫0π/2xsin⁡xcos⁡xcos⁡4x+sin⁡4x dx\int_0^{\pi/2}\frac{x\sin x\cos x}{\cos^4x+\sin^4x}\,dx.

▸ SHOW SOLUTION

Step 1: King with a+b=π2a+b=\frac{\pi}{2}

Under x↦π2−xx\mapsto\frac{\pi}{2}-x the fraction sin⁡xcos⁡xcos⁡4x+sin⁡4x\frac{\sin x\cos x}{\cos^4x+\sin^4x} is unchanged, only the leading xx becomes π2−x\frac{\pi}{2}-x.

I=∫0π/2(π2−x)sin⁡xcos⁡xcos⁡4x+sin⁡4x dxI=\int_0^{\pi/2}\frac{\left(\frac{\pi}{2}-x\right)\sin x\cos x}{\cos^4x+\sin^4x}\,dx

Step 2: Add and solve for II

2I=π2∫0π/2sin⁡xcos⁡xcos⁡4x+sin⁡4x dx2I=\frac{\pi}{2}\int_0^{\pi/2}\frac{\sin x\cos x}{\cos^4x+\sin^4x}\,dx

Step 3: Divide top and bottom by cos⁡4x\cos^4x

2I=π2∫0π/2tan⁡xsec⁡2x1+tan⁡4x dx2I=\frac{\pi}{2}\int_0^{\pi/2}\frac{\tan x\sec^2x}{1+\tan^4x}\,dx

Step 4: Substitute u=tan⁡2xu=\tan^2x, du=2tan⁡xsec⁡2x dxdu=2\tan x\sec^2x\,dx

2I=π4∫0∞du1+u2=π4⋅π2=π282I=\frac{\pi}{4}\int_0^{\infty}\frac{du}{1+u^2}=\frac{\pi}{4}\cdot\frac{\pi}{2}=\frac{\pi^2}{8}

Step 5: Halve

I=π216I=\frac{\pi^2}{16}

Example 8. (JEE Main 2026, 8 Apr Shift 2) If ∫π/6π/4(cot⁡(x−π3)cot⁡(x+π3)+1)dx=αlog⁡e(3−1)\int_{\pi/6}^{\pi/4}\left(\cot\left(x-\frac{\pi}{3}\right)\cot\left(x+\frac{\pi}{3}\right)+1\right)dx=\alpha\log_e\left(\sqrt3-1\right), find 9α29\alpha^2.

▸ SHOW SOLUTION

Step 1: Write the product as a single quotient

cot⁡Acot⁡B+1=cos⁡Acos⁡B+sin⁡Asin⁡Bsin⁡Asin⁡B=cos⁡(A−B)sin⁡Asin⁡B\cot A\cot B+1=\frac{\cos A\cos B+\sin A\sin B}{\sin A\sin B}=\frac{\cos(A-B)}{\sin A\sin B}

With A=x−π3A=x-\frac{\pi}{3} and B=x+π3B=x+\frac{\pi}{3}, A−B=−2π3A-B=-\frac{2\pi}{3}, so cos⁡(A−B)=−12\cos(A-B)=-\frac12.

Step 2: Turn the denominator into a difference of cosines

2sin⁡Asin⁡B=cos⁡(A−B)−cos⁡(A+B)=−12−cos⁡2x2\sin A\sin B=\cos(A-B)-\cos(A+B)=-\frac12-\cos2x.

cot⁡Acot⁡B+1=−1212(−12−cos⁡2x)=−1−12−cos⁡2x=21+2cos⁡2x\cot A\cot B+1=\frac{-\frac12}{\frac12\left(-\frac12-\cos2x\right)}=\frac{-1}{-\frac12-\cos2x}=\frac{2}{1+2\cos2x}

Step 3: Integrate with t=tan⁡xt=\tan x

Using cos⁡2x=1−t21+t2\cos 2x=\frac{1-t^2}{1+t^2}, the integrand becomes 2(1+t2)3−t2\frac{2\left(1+t^2\right)}{3-t^2} and dx=dt1+t2dx=\frac{dt}{1+t^2}:

I=∫1/312 dt3−t2=223[log⁡e∣3+t3−t∣]1/31I=\int_{1/\sqrt3}^{1}\frac{2\,dt}{3-t^2}=\frac{2}{2\sqrt3}\left[\log_e\left|\frac{\sqrt3+t}{\sqrt3-t}\right|\right]_{1/\sqrt3}^{1}

Step 4: Put in the limits

At t=1t=1: 3+13−1\frac{\sqrt3+1}{\sqrt3-1}. At t=13t=\frac{1}{\sqrt3}: 3+133−13=4/32/3=2\frac{\sqrt3+\frac1{\sqrt3}}{\sqrt3-\frac1{\sqrt3}}=\frac{4/\sqrt3}{2/\sqrt3}=2.

I=13[log⁡e3+13−1−log⁡e2]I=\frac{1}{\sqrt3}\left[\log_e\frac{\sqrt3+1}{\sqrt3-1}-\log_e2\right]

Step 5: Simplify the bracket

3+13−1=(3+1)22=2+3\frac{\sqrt3+1}{\sqrt3-1}=\frac{\left(\sqrt3+1\right)^2}{2}=2+\sqrt3, so the bracket is log⁡e(2+32)\log_e\left(\frac{2+\sqrt3}{2}\right).

Now rationalise the other way: 1(3−1)2=14−23=4+234=2+32\frac{1}{\left(\sqrt3-1\right)^2}=\frac{1}{4-2\sqrt3}=\frac{4+2\sqrt3}{4}=\frac{2+\sqrt3}{2}. So the bracket is log⁡e(3−1)−2=−2log⁡e(3−1)\log_e\left(\sqrt3-1\right)^{-2}=-2\log_e\left(\sqrt3-1\right).

Step 6: Read off α\alpha

I=−23log⁡e(3−1) ⇒ α=−23,9α2=9⋅43=12I=-\frac{2}{\sqrt3}\log_e\left(\sqrt3-1\right)\ \Rightarrow\ \alpha=-\frac{2}{\sqrt3},\qquad 9\alpha^2=9\cdot\frac43=12

Type 2, odd and even

Example 9. (JEE Main 2026, 6 Apr Shift 2) Find ∫−11x3+∣x∣+1x2+2∣x∣+1 dx\int_{-1}^{1}\frac{x^3+|x|+1}{x^2+2|x|+1}\,dx.

▸ SHOW SOLUTION

Step 1: Note the denominator is even

x2+2∣x∣+1=(∣x∣+1)2x^2+2|x|+1=\left(|x|+1\right)^2 depends only on ∣x∣|x|, so it is even.

Step 2: Split the numerator into odd and even parts

x3(∣x∣+1)2\frac{x^3}{\left(|x|+1\right)^2} is odd. ∣x∣+1(∣x∣+1)2=1∣x∣+1\frac{|x|+1}{\left(|x|+1\right)^2}=\frac{1}{|x|+1} is even.

Step 3: Delete the odd part and double the even part

I=2∫01dxx+1=2[log⁡e(x+1)]01=2log⁡e2I=2\int_0^1\frac{dx}{x+1}=2\Big[\log_e(x+1)\Big]_0^1=2\log_e2

Example 10. (IIT JEE 2012) Evaluate ∫−π/2π/2[x2+log⁡e(π−xπ+x)]cos⁡x dx\int_{-\pi/2}^{\pi/2}\left[x^2+\log_e\left(\frac{\pi-x}{\pi+x}\right)\right]\cos x\,dx.

▸ SHOW SOLUTION

Step 1: Classify the two terms

x2cos⁡xx^2\cos x is even. For the second, log⁡eπ+xπ−x=−log⁡eπ−xπ+x\log_e\frac{\pi+x}{\pi-x}=-\log_e\frac{\pi-x}{\pi+x}, so log⁡eπ−xπ+x\log_e\frac{\pi-x}{\pi+x} is odd and, multiplied by the even cos⁡x\cos x, stays odd.

Step 2: Delete the odd term

I=2∫0π/2x2cos⁡x dxI=2\int_0^{\pi/2}x^2\cos x\,dx

Step 3: Integrate by parts twice

∫x2cos⁡x dx=x2sin⁡x+2xcos⁡x−2sin⁡x\int x^2\cos x\,dx=x^2\sin x+2x\cos x-2\sin x

Step 4: Substitute the limits

At x=π2x=\frac{\pi}{2} this is π24+0−2\frac{\pi^2}{4}+0-2; at x=0x=0 it is 00.

I=2(π24−2)=π22−4I=2\left(\frac{\pi^2}{4}-2\right)=\frac{\pi^2}{2}-4

Example 11. (IIT JEE 2009) If In=∫−ππsin⁡nx(1+πx)sin⁡x dxI_n=\int_{-\pi}^{\pi}\frac{\sin nx}{\left(1+\pi^x\right)\sin x}\,dx for n=0,1,2,…n=0,1,2,\dots, which of the following hold? (a) In=In+2I_n=I_{n+2} (b) ∑m=110I2m+1=10π\sum_{m=1}^{10}I_{2m+1}=10\pi (c) ∑m=110I2m=0\sum_{m=1}^{10}I_{2m}=0 (d) In=In+1I_n=I_{n+1}

▸ SHOW SOLUTION

Step 1: Kill the 1+πx1+\pi^x with king

The interval is symmetric, so the reflection is x↦−xx\mapsto-x, and sin⁡(−nx)sin⁡(−x)=sin⁡nxsin⁡x\frac{\sin(-nx)}{\sin(-x)}=\frac{\sin nx}{\sin x} is unchanged.

In=∫−πππxsin⁡nx(1+πx)sin⁡x dxI_n=\int_{-\pi}^{\pi}\frac{\pi^x\sin nx}{\left(1+\pi^x\right)\sin x}\,dx

Step 2: Add the two forms

2In=∫−ππsin⁡nxsin⁡x dx=2∫0πsin⁡nxsin⁡x dx2I_n=\int_{-\pi}^{\pi}\frac{\sin nx}{\sin x}\,dx=2\int_0^{\pi}\frac{\sin nx}{\sin x}\,dx

because sin⁡nxsin⁡x\frac{\sin nx}{\sin x} is even. So In=∫0πsin⁡nxsin⁡x dxI_n=\int_0^{\pi}\frac{\sin nx}{\sin x}\,dx.

Step 3: Build a recurrence

In+2−In=∫0πsin⁡(n+2)x−sin⁡nxsin⁡x dx=∫0π2cos⁡(n+1)xsin⁡xsin⁡x dx=2∫0πcos⁡(n+1)x dx=0I_{n+2}-I_n=\int_0^{\pi}\frac{\sin(n+2)x-\sin nx}{\sin x}\,dx=\int_0^{\pi}\frac{2\cos(n+1)x\sin x}{\sin x}\,dx=2\int_0^{\pi}\cos(n+1)x\,dx=0

So In+2=InI_{n+2}=I_n, which is (a).

Step 4: Find the two seed values

I0=0I_0=0 and I1=∫0πdx=πI_1=\int_0^{\pi}dx=\pi.

Step 5: Read off the sums

Odd index gives π\pi every time, so ∑m=110I2m+1=10π\sum_{m=1}^{10}I_{2m+1}=10\pi, which is (b). Even index gives 00 every time, so ∑m=110I2m=0\sum_{m=1}^{10}I_{2m}=0, which is (c). And I1≠I2I_1\ne I_2, so (d) fails.

Correct: (a), (b), (c).

Type 3, greatest integer and fractional part

The rule never changes: find where the inside crosses an integer, split there, and replace [ ⋅ ][\,\cdot\,] by the constant it equals on each piece.

The greatest integer function drawn as a staircase, with the area under it read as a sum of rectangles

Example 12. (IIT JEE 2001) Evaluate ∫π/23π/2[2sin⁡x] dx\int_{\pi/2}^{3\pi/2}[2\sin x]\,dx, where [ ⋅ ][\,\cdot\,] is the greatest integer function.

▸ SHOW SOLUTION

Step 1: Track 2sin⁡x2\sin x across the interval

On [π2,3π2]\left[\frac{\pi}{2},\frac{3\pi}{2}\right], 2sin⁡x2\sin x decreases from 22 down to −2-2.

Step 2: Find the crossing points

2sin⁡x=12\sin x=1 at x=5π6x=\frac{5\pi}{6}; 2sin⁡x=02\sin x=0 at x=πx=\pi; 2sin⁡x=−12\sin x=-1 at x=7π6x=\frac{7\pi}{6}.

Step 3: Read off the constant on each piece

[2sin⁡x]={2,x=π21,π2<x≤5π60,5π6<x<π−1,π≤x<7π6−2,7π6≤x≤3π2[2\sin x]=\begin{cases}2,& x=\frac{\pi}{2}\\[2pt] 1,& \frac{\pi}{2}<x\le\frac{5\pi}{6}\\[2pt] 0,& \frac{5\pi}{6}<x<\pi\\[2pt] -1,& \pi\le x<\frac{7\pi}{6}\\[2pt] -2,& \frac{7\pi}{6}\le x\le\frac{3\pi}{2}\end{cases}

A single point contributes nothing to an integral, so the value 22 can be ignored.

Step 4: Add the rectangles

I=1⋅π3+0⋅π6+(−1)⋅π6+(−2)⋅π3=π3−π6−2π3=−π2I=1\cdot\frac{\pi}{3}+0\cdot\frac{\pi}{6}+(-1)\cdot\frac{\pi}{6}+(-2)\cdot\frac{\pi}{3}=\frac{\pi}{3}-\frac{\pi}{6}-\frac{2\pi}{3}=-\frac{\pi}{2}

Example 13. (JEE Main 2026, 28 Jan Shift 2) Evaluate ∫−π/2π/212(3+[x])3+[sin⁡x]+[cos⁡x] dx\int_{-\pi/2}^{\pi/2}\frac{12\left(3+[x]\right)}{3+[\sin x]+[\cos x]}\,dx.

▸ SHOW SOLUTION

Step 1: Tabulate the three step functions

On [−π2,π2]\left[-\frac{\pi}{2},\frac{\pi}{2}\right] the break points are −1-1, 00 and 11.

Interval[x][x][sin⁡x][\sin x][cos⁡x][\cos x]Integrand
[−π2,−1)\left[-\frac{\pi}{2},-1\right)−2-2−1-10012(1)2=6\frac{12(1)}{2}=6
[−1,0)[-1,0)−1-1−1-10012(2)2=12\frac{12(2)}{2}=12
[0,1)[0,1)00000012(3)3=12\frac{12(3)}{3}=12
[1,π2]\left[1,\frac{\pi}{2}\right]11000012(4)3=16\frac{12(4)}{3}=16

At x=0x=0, cos⁡x=1\cos x=1 so [cos⁡x]=1[\cos x]=1, but that is one point and contributes nothing.

Step 2: Multiply each value by its interval length

I=6(π2−1)+12(1)+12(1)+16(π2−1)I=6\left(\frac{\pi}{2}-1\right)+12(1)+12(1)+16\left(\frac{\pi}{2}-1\right)

Step 3: Collect

I=(6+16)(π2−1)+24=22⋅π2−22+24=11π+2I=\left(6+16\right)\left(\frac{\pi}{2}-1\right)+24=22\cdot\frac{\pi}{2}-22+24=11\pi+2

Example 14. (JEE Main 2026, 22 Jan Shift 1) Evaluate ∫−π/2π/2dx[x]+4\int_{-\pi/2}^{\pi/2}\frac{dx}{[x]+4}.

▸ SHOW SOLUTION

Step 1: List the pieces

π2≈1.5708\frac{\pi}{2}\approx1.5708, so the break points inside the interval are −1-1, 00 and 11.

Interval[x][x]IntegrandLength
[−π2,−1)\left[-\frac{\pi}{2},-1\right)−2-212\frac12π2−1\frac{\pi}{2}-1
[−1,0)[-1,0)−1-113\frac1311
[0,1)[0,1)0014\frac1411
[1,π2]\left[1,\frac{\pi}{2}\right]1115\frac15π2−1\frac{\pi}{2}-1

Step 2: Add

I=(12+15)(π2−1)+13+14=710(π2−1)+712I=\left(\frac12+\frac15\right)\left(\frac{\pi}{2}-1\right)+\frac13+\frac14=\frac{7}{10}\left(\frac{\pi}{2}-1\right)+\frac{7}{12}

Step 3: Simplify

I=7π20−710+712=760(3π−6+5)=760(3π−1)I=\frac{7\pi}{20}-\frac{7}{10}+\frac{7}{12}=\frac{7}{60}\left(3\pi-6+5\right)=\frac{7}{60}\left(3\pi-1\right)

Example 15. (JEE Main 2026, 4 Apr Shift 1) If ∫−22(∣sin⁡x∣+[xsin⁡x])dx=2(3−cos⁡2)+β\int_{-2}^{2}\Big(|\sin x|+[x\sin x]\Big)dx=2\left(3-\cos2\right)+\beta, find βsin⁡(β2)\beta\sin\left(\frac{\beta}{2}\right).

▸ SHOW SOLUTION

Step 1: Do the modulus part

∣sin⁡x∣|\sin x| is even and sin⁡x≥0\sin x\ge0 on [0,2][0,2], so

∫−22∣sin⁡x∣ dx=2∫02sin⁡x dx=2(1−cos⁡2)\int_{-2}^{2}|\sin x|\,dx=2\int_0^2\sin x\,dx=2\left(1-\cos2\right)

Step 2: Deal with the step part

xsin⁡xx\sin x is even, so [xsin⁡x][x\sin x] is even and ∫−22[xsin⁡x] dx=2∫02[xsin⁡x] dx\int_{-2}^{2}[x\sin x]\,dx=2\int_0^2[x\sin x]\,dx.

Step 3: Locate the only crossing

On [0,2][0,2], xsin⁡xx\sin x rises from 00 to 2sin⁡2≈1.8192\sin2\approx1.819, so it crosses the value 11 exactly once. Call that point cc, defined by csin⁡c=1c\sin c=1.

Step 4: Read off the step values

[xsin⁡x]=0[x\sin x]=0 on [0,c)[0,c) and =1=1 on [c,2][c,2], so ∫02[xsin⁡x] dx=2−c\int_0^2[x\sin x]\,dx=2-c.

Step 5: Assemble

∫−22(∣sin⁡x∣+[xsin⁡x])dx=2−2cos⁡2+2(2−c)=6−2cos⁡2−2c=2(3−cos⁡2)−2c\int_{-2}^{2}\Big(|\sin x|+[x\sin x]\Big)dx=2-2\cos2+2(2-c)=6-2\cos2-2c=2\left(3-\cos2\right)-2c

Step 6: Identify β\beta

Comparing, β=−2c\beta=-2c.

Step 7: Use the defining equation of cc

βsin⁡(β2)=−2csin⁡(−c)=2csin⁡c=2⋅1=2\beta\sin\left(\frac{\beta}{2}\right)=-2c\sin(-c)=2c\sin c=2\cdot1=2

The transcendental cc never has to be found. That is the whole point of the question.

Example 16. (JEE Main 2026, 22 Jan Shift 2) If α=∫064(x1/3−[x1/3])dx\alpha=\int_0^{64}\left(x^{1/3}-\left[x^{1/3}\right]\right)dx, find 1π∫0απsin⁡2θsin⁡6θ+cos⁡6θ dθ\frac{1}{\pi}\int_0^{\alpha\pi}\frac{\sin^2\theta}{\sin^6\theta+\cos^6\theta}\,d\theta.

▸ SHOW SOLUTION

Step 1: Substitute to tame the cube root

Put x=t3x=t^3, so dx=3t2 dtdx=3t^2\,dt and tt runs from 00 to 44.

α=∫04(t−[t])3t2 dt=3∫04t2{t} dt\alpha=\int_0^4\left(t-[t]\right)3t^2\,dt=3\int_0^4 t^2\{t\}\,dt

Step 2: Split at the integers

α=3∑n=03∫nn+1t2(t−n) dt=3∑n=03[t44−nt33]nn+1\alpha=3\sum_{n=0}^{3}\int_n^{n+1}t^2(t-n)\,dt=3\sum_{n=0}^{3}\left[\frac{t^4}{4}-\frac{nt^3}{3}\right]_n^{n+1}

Step 3: Evaluate the general term

(n+1)4−n44−n[(n+1)3−n3]3=4n3+6n2+4n+14−n(3n2+3n+1)3\frac{(n+1)^4-n^4}{4}-\frac{n\left[(n+1)^3-n^3\right]}{3}=\frac{4n^3+6n^2+4n+1}{4}-\frac{n\left(3n^2+3n+1\right)}{3}

which simplifies to n22+2n3+14\frac{n^2}{2}+\frac{2n}{3}+\frac14.

Step 4: Sum for n=0,1,2,3n=0,1,2,3

∑n2=14\sum n^2=14, ∑n=6\sum n=6, and there are 44 terms, so the sum is 7+4+1=127+4+1=12.

α=3×12=36\alpha=3\times12=36

Step 5: Recognise the second integrand as periodic

sin⁡6θ+cos⁡6θ=1−3sin⁡2θcos⁡2θ\sin^6\theta+\cos^6\theta=1-3\sin^2\theta\cos^2\theta and sin⁡2θ\sin^2\theta are both unchanged by θ↦θ+π2\theta\mapsto\theta+\frac{\pi}{2}, so the integrand has period π2\frac{\pi}{2}.

Step 6: Count the periods

απ=36π\alpha\pi=36\pi contains 36ππ/2=72\frac{36\pi}{\pi/2}=72 periods, so

∫036π(⋯ ) dθ=72∫0π/2sin⁡2θ dθ1−3sin⁡2θcos⁡2θ\int_0^{36\pi}(\cdots)\,d\theta=72\int_0^{\pi/2}\frac{\sin^2\theta\,d\theta}{1-3\sin^2\theta\cos^2\theta}

Step 7: Evaluate one period

Write the denominator as sin⁡4θ−sin⁡2θcos⁡2θ+cos⁡4θ\sin^4\theta-\sin^2\theta\cos^2\theta+\cos^4\theta, divide top and bottom by cos⁡4θ\cos^4\theta, then put u=tan⁡θu=\tan\theta so that du=sec⁡2θ dθdu=\sec^2\theta\,d\theta:

∫0π/2sin⁡2θ dθ1−3sin⁡2θcos⁡2θ=∫0∞u2 duu4−u2+1=π2\int_0^{\pi/2}\frac{\sin^2\theta\,d\theta}{1-3\sin^2\theta\cos^2\theta}=\int_0^{\infty}\frac{u^2\,du}{u^4-u^2+1}=\frac{\pi}{2}

Step 8: Finish

1π⋅72⋅π2=36\frac{1}{\pi}\cdot72\cdot\frac{\pi}{2}=36

Type 4, modulus: split at the sign changes

Example 17. (JEE Main 2026, 21 Jan Shift 1) Find 6∫0π∣sin⁡3x+sin⁡2x+sin⁡x∣dx6\int_0^{\pi}\left|\sin3x+\sin2x+\sin x\right|dx.

▸ SHOW SOLUTION

Step 1: Factorise the inside

sin⁡3x+sin⁡x=2sin⁡2xcos⁡x\sin3x+\sin x=2\sin2x\cos x, so

sin⁡3x+sin⁡2x+sin⁡x=2sin⁡2xcos⁡x+sin⁡2x=sin⁡2x(2cos⁡x+1)\sin3x+\sin2x+\sin x=2\sin2x\cos x+\sin2x=\sin2x\left(2\cos x+1\right)

Step 2: Factorise further

sin⁡2x=2sin⁡xcos⁡x\sin2x=2\sin x\cos x, so the expression is 2sin⁡xcos⁡x(2cos⁡x+1)2\sin x\cos x\left(2\cos x+1\right).

Step 3: Find the sign changes on (0,π)(0,\pi)

sin⁡x>0\sin x>0 throughout. cos⁡x=0\cos x=0 at x=π2x=\frac{\pi}{2}. 2cos⁡x+1=02\cos x+1=0 at x=2π3x=\frac{2\pi}{3}.

Step 4: Determine the sign on each piece

On (0,π2)\left(0,\frac{\pi}{2}\right): cos⁡x>0\cos x>0, 2cos⁡x+1>02\cos x+1>0, product positive. On (π2,2π3)\left(\frac{\pi}{2},\frac{2\pi}{3}\right): cos⁡x<0\cos x<0, 2cos⁡x+1>02\cos x+1>0, product negative. On (2π3,π)\left(\frac{2\pi}{3},\pi\right): cos⁡x<0\cos x<0, 2cos⁡x+1<02\cos x+1<0, product positive.

Step 5: Write down the antiderivative

F(x)=−cos⁡3x3−cos⁡2x2−cos⁡xF(x)=-\frac{\cos3x}{3}-\frac{\cos2x}{2}-\cos x

Step 6: Assemble with the right signs

I=6[(F(π2)−F(0))−(F(2π3)−F(π2))+(F(π)−F(2π3))]I=6\Big[\big(F(\tfrac{\pi}{2})-F(0)\big)-\big(F(\tfrac{2\pi}{3})-F(\tfrac{\pi}{2})\big)+\big(F(\pi)-F(\tfrac{2\pi}{3})\big)\Big]

Step 7: Compute the four values

F(0)=−13−12−1=−116F(0)=-\frac13-\frac12-1=-\frac{11}{6}, F ⁣(π2)=0+12−0=12F\!\left(\frac{\pi}{2}\right)=0+\frac12-0=\frac12, F ⁣(2π3)=−13+14+12=512F\!\left(\frac{2\pi}{3}\right)=-\frac13+\frac14+\frac12=\frac{5}{12}, F(π)=13−12+1=56F(\pi)=\frac13-\frac12+1=\frac56.

Step 8: Substitute

I=6[(12+116)−(512−12)+(56−512)]=6[73+112+512]=6⋅176=17I=6\left[\left(\frac12+\frac{11}{6}\right)-\left(\frac{5}{12}-\frac12\right)+\left(\frac56-\frac{5}{12}\right)\right]=6\left[\frac{7}{3}+\frac{1}{12}+\frac{5}{12}\right]=6\cdot\frac{17}{6}=17

Example 18. (IIT JEE 2014) Evaluate ∫0π1+4sin⁡2x2−4sin⁡x2 dx\int_0^{\pi}\sqrt{1+4\sin^2\frac{x}{2}-4\sin\frac{x}{2}}\,dx.

▸ SHOW SOLUTION

Step 1: Recognise the perfect square

1−4sin⁡x2+4sin⁡2x2=(1−2sin⁡x2)21-4\sin\frac x2+4\sin^2\frac x2=\left(1-2\sin\frac x2\right)^2, so the integrand is ∣1−2sin⁡x2∣\left|1-2\sin\frac x2\right|.

Step 2: Find where the inside changes sign

1−2sin⁡x2=01-2\sin\frac x2=0 gives sin⁡x2=12\sin\frac x2=\frac12, that is x2=π6\frac x2=\frac{\pi}{6}, so x=π3x=\frac{\pi}{3}.

Step 3: Determine the sign

On (0,π3)\left(0,\frac{\pi}{3}\right), sin⁡x2<12\sin\frac x2<\frac12, so the inside is positive. On (π3,π)\left(\frac{\pi}{3},\pi\right) it is negative.

Step 4: Split

I=∫0π/3(1−2sin⁡x2)dx+∫π/3π(2sin⁡x2−1)dxI=\int_0^{\pi/3}\left(1-2\sin\frac x2\right)dx+\int_{\pi/3}^{\pi}\left(2\sin\frac x2-1\right)dx

Step 5: Use the antiderivative x+4cos⁡x2x+4\cos\frac x2

I=[x+4cos⁡x2]0π/3−[x+4cos⁡x2]π/3πI=\left[x+4\cos\frac x2\right]_0^{\pi/3}-\left[x+4\cos\frac x2\right]_{\pi/3}^{\pi}

Step 6: Evaluate

I=(π3+23−4)−(0+4−π3−23)=43−4−π3I=\left(\frac{\pi}{3}+2\sqrt3-4\right)-\left(0+4-\frac{\pi}{3}-2\sqrt3\right)=4\sqrt3-4-\frac{\pi}{3}

Example 19. (JEE Main 2026, 8 Apr Shift 2) Let f(x)=13f(x)=\frac13 for x≤π2x\le\frac{\pi}{2} and f(x)=b(1−sin⁡x)(π−2x)2f(x)=\frac{b\left(1-\sin x\right)}{\left(\pi-2x\right)^2} for x>π2x>\frac{\pi}{2}. If ff is continuous at x=π2x=\frac{\pi}{2}, find ∫03b−6∣x2+2x−3∣dx\int_0^{3b-6}\left|x^2+2x-3\right|dx.

▸ SHOW SOLUTION

Step 1: Take the right-hand limit

Put x=π2+hx=\frac{\pi}{2}+h. Then 1−sin⁡x=1−cos⁡h1-\sin x=1-\cos h and π−2x=−2h\pi-2x=-2h.

lim⁡h→0b(1−cos⁡h)4h2=b4⋅12=b8\lim_{h\to0}\frac{b\left(1-\cos h\right)}{4h^2}=\frac{b}{4}\cdot\frac12=\frac{b}{8}

Step 2: Match it to 13\frac13

b8=13\frac b8=\frac13 gives b=83b=\frac83, so the upper limit is 3b−6=8−6=23b-6=8-6=2.

Step 3: Factorise the modulus

x2+2x−3=(x+3)(x−1)x^2+2x-3=(x+3)(x-1), negative on (−3,1)(-3,1) and positive outside.

Step 4: Split at x=1x=1

I=∫01(3−2x−x2)dx+∫12(x2+2x−3)dxI=\int_0^1\left(3-2x-x^2\right)dx+\int_1^2\left(x^2+2x-3\right)dx

Step 5: Evaluate

First piece: [3x−x2−x33]01=3−1−13=53\left[3x-x^2-\frac{x^3}{3}\right]_0^1=3-1-\frac13=\frac53. Second piece: [x33+x2−3x]12=(83+4−6)−(13+1−3)=23+53=73\left[\frac{x^3}{3}+x^2-3x\right]_1^2=\left(\frac83+4-6\right)-\left(\frac13+1-3\right)=\frac23+\frac53=\frac73.

Step 6: Add

I=53+73=4I=\frac53+\frac73=4

Type 5, periodic integrands

If ff has period TT, an integral over any whole number of periods does not care where it starts.

∫aa+Tf(x) dx=∫0Tf(x) dxand∫0nTf(x) dx=n∫0Tf(x) dx\int_a^{a+T}f(x)\,dx=\int_0^{T}f(x)\,dx\qquad\text{and}\qquad\int_0^{nT}f(x)\,dx=n\int_0^{T}f(x)\,dx A periodic curve with three consecutive period-blocks shaded to show they carry equal area

The three facts worth memorising

∫aa+nTf(x) dx=n∫0Tf(x) dx,∫mTnTf(x) dx=(n−m)∫0Tf(x) dx\int_a^{a+nT}f(x)\,dx=n\int_0^{T}f(x)\,dx,\qquad \int_{mT}^{nT}f(x)\,dx=(n-m)\int_0^{T}f(x)\,dx ∫a+nTb+nTf(x) dx=∫abf(x) dx\int_{a+nT}^{b+nT}f(x)\,dx=\int_a^b f(x)\,dx

Example 20. (JEE Main 2026, 2 Apr Shift 2) Find ∫020π(sin⁡4x+cos⁡4x)dx\int_0^{20\pi}\left(\sin^4x+\cos^4x\right)dx.

▸ SHOW SOLUTION

Step 1: Simplify the integrand

sin⁡4x+cos⁡4x=(sin⁡2x+cos⁡2x)2−2sin⁡2xcos⁡2x=1−sin⁡22x2\sin^4x+\cos^4x=\left(\sin^2x+\cos^2x\right)^2-2\sin^2x\cos^2x=1-\frac{\sin^22x}{2}

Step 2: Find the period

sin⁡22x=1−cos⁡4x2\sin^22x=\frac{1-\cos4x}{2} has period 2π4=π2\frac{2\pi}{4}=\frac{\pi}{2}.

Step 3: Count the periods

20π÷π2=4020\pi\div\frac{\pi}{2}=40.

Step 4: Integrate over one period

∫0π/2(1−1−cos⁡4x4)dx=∫0π/2(34+cos⁡4x4)dx=34⋅π2+0=3π8\int_0^{\pi/2}\left(1-\frac{1-\cos4x}{4}\right)dx=\int_0^{\pi/2}\left(\frac34+\frac{\cos4x}{4}\right)dx=\frac34\cdot\frac{\pi}{2}+0=\frac{3\pi}{8}

Step 5: Multiply

I=40⋅3π8=15πI=40\cdot\frac{3\pi}{8}=15\pi

Example 21. (IIT JEE 2004) Show that ∫0nπ+v∣sin⁡x∣dx=2n+1−cos⁡v\int_0^{n\pi+v}\left|\sin x\right|dx=2n+1-\cos v, where nn is a positive integer and 0≤v<π0\le v<\pi.

▸ SHOW SOLUTION

Step 1: Split off the whole periods

∣sin⁡x∣\left|\sin x\right| has period π\pi, so

∫0nπ+v∣sin⁡x∣dx=∫0nπ∣sin⁡x∣dx+∫nπnπ+v∣sin⁡x∣dx\int_0^{n\pi+v}\left|\sin x\right|dx=\int_0^{n\pi}\left|\sin x\right|dx+\int_{n\pi}^{n\pi+v}\left|\sin x\right|dx

Step 2: Evaluate the whole-period part

∫0π∣sin⁡x∣dx=∫0πsin⁡x dx=2 ⇒ ∫0nπ∣sin⁡x∣dx=2n\int_0^{\pi}\left|\sin x\right|dx=\int_0^{\pi}\sin x\,dx=2\ \Rightarrow\ \int_0^{n\pi}\left|\sin x\right|dx=2n

Step 3: Shift the tail back to the origin

By periodicity ∫nπnπ+v∣sin⁡x∣dx=∫0v∣sin⁡x∣dx\int_{n\pi}^{n\pi+v}\left|\sin x\right|dx=\int_0^{v}\left|\sin x\right|dx, and sin⁡x≥0\sin x\ge0 on [0,v]⊆[0,π)[0,v]\subseteq[0,\pi).

Step 4: Integrate the tail

∫0vsin⁡x dx=1−cos⁡v\int_0^{v}\sin x\,dx=1-\cos v

Step 5: Add

∫0nπ+v∣sin⁡x∣dx=2n+1−cos⁡v\int_0^{n\pi+v}\left|\sin x\right|dx=2n+1-\cos v

Example 22. (JEE Main 2026, 28 Jan Shift 1) Find ∑r=120⌊π(∫0rx∣sin⁡πx∣dx)⌋\displaystyle\sum_{r=1}^{20}\left\lfloor\sqrt{\pi\left(\int_0^r x\left|\sin\pi x\right|dx\right)}\right\rfloor.

▸ SHOW SOLUTION

Step 1: Integrate over one unit block

On [n,n+1][n,n+1] put x=n+ux=n+u. Then ∣sin⁡πx∣=sin⁡πu\left|\sin\pi x\right|=\sin\pi u for u∈[0,1]u\in[0,1], so

∫nn+1x∣sin⁡πx∣dx=∫01(n+u)sin⁡πu du=n⋅2π+1π=2n+1π\int_n^{n+1}x\left|\sin\pi x\right|dx=\int_0^1(n+u)\sin\pi u\,du=n\cdot\frac{2}{\pi}+\frac{1}{\pi}=\frac{2n+1}{\pi}

Step 2: Sum the blocks

∫0rx∣sin⁡πx∣dx=∑n=0r−12n+1π=r2π\int_0^r x\left|\sin\pi x\right|dx=\sum_{n=0}^{r-1}\frac{2n+1}{\pi}=\frac{r^2}{\pi}

because the odd numbers up to 2r−12r-1 add to r2r^2.

Step 3: Undo the outer operations

π⋅r2π=r2\pi\cdot\frac{r^2}{\pi}=r^2, so  ⋅ =r\sqrt{\ \cdot\ }=r and ⌊r⌋=r\lfloor r\rfloor=r.

Step 4: Add

∑r=120r=20⋅212=210\sum_{r=1}^{20}r=\frac{20\cdot21}{2}=210

Type 6, the integral as an unknown constant

When a definite integral has constant limits, it is a number, so it can be given a name and solved for. This turns a functional equation into ordinary algebra.

Example 23. (JEE Main 2026, 24 Jan Shift 2) If f(x)=ex+∫01(y+xex)f(y) dyf(x)=e^x+\int_0^1\left(y+xe^x\right)f(y)\,dy, find e+f(0)e+f(0).

▸ SHOW SOLUTION

Step 1: Name the two constants

A=∫01y f(y) dy,B=∫01f(y) dyA=\int_0^1 y\,f(y)\,dy,\qquad B=\int_0^1 f(y)\,dy

Both are numbers, so f(x)=ex+A+Bxexf(x)=e^x+A+Bxe^x.

Step 2: Feed the form back into BB

B=∫01(ey+A+Byey)dy=(e−1)+A+B[yey−ey]01=(e−1)+A+BB=\int_0^1\left(e^y+A+Bye^y\right)dy=(e-1)+A+B\Big[ye^y-e^y\Big]_0^1=(e-1)+A+B

Step 3: Read off AA

The BB cancels, leaving 0=(e−1)+A0=(e-1)+A, so A=1−eA=1-e.

Step 4: Evaluate at zero

f(0)=e0+A+0=1+(1−e)=2−ef(0)=e^0+A+0=1+(1-e)=2-e

Step 5: Finish

e+f(0)=e+2−e=2e+f(0)=e+2-e=2

Note that BB was never needed. Whenever one of the named constants cancels, stop chasing it.

Example 24. (JEE Main 2026, 24 Jan Shift 1) A differentiable ff satisfies ∫036f ⁣(tx36)dt=4αf(x)\int_0^{36}f\!\left(\frac{tx}{36}\right)dt=4\alpha f(x). If y=f(x)y=f(x) is a standard parabola through (2,1)(2,1) and (−4,β)(-4,\beta), find βα\beta^{\alpha}.

▸ SHOW SOLUTION

Step 1: Identify the parabola

A standard parabola of the form y=x24ay=\frac{x^2}{4a} through (2,1)(2,1) gives 1=44a1=\frac{4}{4a}, so a=1a=1 and f(x)=x24f(x)=\frac{x^2}{4}.

Step 2: Compute the left side

∫03614(tx36)2dt=x24⋅362∫036t2 dt=x24⋅362⋅3633=36 x212=3x2\int_0^{36}\frac{1}{4}\left(\frac{tx}{36}\right)^2dt=\frac{x^2}{4\cdot36^2}\int_0^{36}t^2\,dt=\frac{x^2}{4\cdot36^2}\cdot\frac{36^3}{3}=\frac{36\,x^2}{12}=3x^2

Step 3: Compare with the right side

3x2=4α⋅x24=αx23x^2=4\alpha\cdot\frac{x^2}{4}=\alpha x^2, so α=3\alpha=3.

Step 4: Find β\beta

β=f(−4)=164=4\beta=f(-4)=\frac{16}{4}=4

Step 5: Finish

βα=43=64\beta^{\alpha}=4^3=64

Type 7, Newton–Leibnitz inside a definite integral

When the unknown function sits inside an integral whose upper limit is xx, differentiate instead of integrating. That is the Newton–Leibnitz rule:

ddx∫u(x)v(x)f(t) dt=f(v(x))v′(x)−f(u(x))u′(x)\frac{d}{dx}\int_{u(x)}^{v(x)}f(t)\,dt=f\big(v(x)\big)v'(x)-f\big(u(x)\big)u'(x)
Constant limits versus variable limits

Constant limits mean the integral is a number: name it and solve algebraically, as in Type 6. A variable upper limit means the integral is a function: differentiate it, as here. Deciding which of the two you are looking at is the entire opening move.

Example 25. (JEE Main 2026, 22 Jan Shift 1) Let f:[1,∞)→Rf:[1,\infty)\to\mathbb{R} be differentiable with 6∫1xf(t) dt=3xf(x)+x3−46\int_1^{x}f(t)\,dt=3xf(x)+x^3-4 for all x≥1x\ge1. Find f(2)−f(3)f(2)-f(3).

▸ SHOW SOLUTION

Step 1: Differentiate both sides

6f(x)=3f(x)+3xf′(x)+3x26f(x)=3f(x)+3xf'(x)+3x^2

Step 2: Rearrange into a linear equation

3f(x)−3xf′(x)=3x2 ⇒ f′(x)−f(x)x=−x3f(x)-3xf'(x)=3x^2\ \Rightarrow\ f'(x)-\frac{f(x)}{x}=-x

Step 3: Recognise the derivative of a quotient

(fx)′=f′x−fx2=1x(f′−fx)=−1\left(\frac{f}{x}\right)'=\frac{f'}{x}-\frac{f}{x^2}=\frac1x\left(f'-\frac fx\right)=-1

Step 4: Integrate

f(x)x=−x+C ⇒ f(x)=−x2+Cx\frac{f(x)}{x}=-x+C\ \Rightarrow\ f(x)=-x^2+Cx

Step 5: Fix CC from the original relation at x=1x=1

The left side is 00, so 0=3f(1)+1−40=3f(1)+1-4, giving f(1)=1f(1)=1, hence −1+C=1-1+C=1 and C=2C=2.

Step 6: Evaluate

f(x)=−x2+2xf(x)=-x^2+2x, so f(2)=0f(2)=0 and f(3)=−3f(3)=-3.

f(2)−f(3)=3f(2)-f(3)=3

Example 26. (JEE Main 2026, 23 Jan Shift 2) Find the number of elements of S={x∈[0,100]:∫0xt2sin⁡(x−t) dt=x2}S=\left\{x\in[0,100]:\int_0^{x}t^2\sin(x-t)\,dt=x^2\right\}.

▸ SHOW SOLUTION

Step 1: Turn the convolution into a plain integral

Put u=x−tu=x-t, so t=x−ut=x-u and dt=−dudt=-du; the limits swap.

∫0xt2sin⁡(x−t) dt=∫0x(x−u)2sin⁡u du\int_0^{x}t^2\sin(x-t)\,dt=\int_0^{x}(x-u)^2\sin u\,du

Step 2: Expand

=x2∫0xsin⁡u du−2x∫0xusin⁡u du+∫0xu2sin⁡u du=x^2\int_0^x\sin u\,du-2x\int_0^x u\sin u\,du+\int_0^x u^2\sin u\,du

Step 3: Use the standard antiderivatives

∫0xsin⁡u du=1−cos⁡x\int_0^x\sin u\,du=1-\cos x; ∫0xusin⁡u du=sin⁡x−xcos⁡x\int_0^x u\sin u\,du=\sin x-x\cos x; ∫0xu2sin⁡u du=2xsin⁡x−(x2−2)cos⁡x−2\int_0^x u^2\sin u\,du=2x\sin x-\left(x^2-2\right)\cos x-2.

Step 4: Collect

x2−x2cos⁡x−2xsin⁡x+2x2cos⁡x+2xsin⁡x−x2cos⁡x+2cos⁡x−2=x2−2+2cos⁡xx^2-x^2\cos x-2x\sin x+2x^2\cos x+2x\sin x-x^2\cos x+2\cos x-2=x^2-2+2\cos x

Step 5: Solve the equation

x2−2+2cos⁡x=x2x^2-2+2\cos x=x^2 gives cos⁡x=1\cos x=1, that is x=2kπx=2k\pi.

Step 6: Count them in [0,100][0,100]

2kπ≤1002k\pi\le100 needs k≤50π≈15.9k\le\frac{50}{\pi}\approx15.9, so k=0,1,…,15k=0,1,\dots,15.

∣S∣=16\left|S\right|=16

Example 27. (JEE Main 2026, 28 Jan Shift 2) Let f(x)=1−2x+∫0xex−tf(t) dtf(x)=1-2x+\int_0^{x}e^{x-t}f(t)\,dt and g(x)=∫0x(f(t)+2)15(t−4)6(t+12)17dtg(x)=\int_0^{x}\left(f(t)+2\right)^{15}(t-4)^6(t+12)^{17}dt. If pp and qq are the points of local minimum and maximum of gg, find ∣p+q∣\left|p+q\right|.

▸ SHOW SOLUTION

Step 1: Pull the exe^x out

f(x)=1−2x+ex∫0xe−tf(t) dtf(x)=1-2x+e^{x}\int_0^{x}e^{-t}f(t)\,dt

Step 2: Differentiate

f′(x)=−2+ex∫0xe−tf(t) dt+ex⋅e−xf(x)=−2+(f(x)−1+2x)+f(x)f'(x)=-2+e^{x}\int_0^{x}e^{-t}f(t)\,dt+e^x\cdot e^{-x}f(x)=-2+\big(f(x)-1+2x\big)+f(x)

Step 3: Simplify and solve

f′=2f+2x−3f'=2f+2x-3 with f(0)=1f(0)=1. Trying f=αx+βf=\alpha x+\beta gives α=2β−3\alpha=2\beta-3 and 0=2α+20=2\alpha+2, so α=−1\alpha=-1, β=1\beta=1.

f(x)=1−xf(x)=1-x

Step 4: Write down g′g'

g′(x)=(3−x)15(x−4)6(x+12)17g'(x)=\left(3-x\right)^{15}(x-4)^6(x+12)^{17}

Step 5: Read the sign changes off the exponents

(x−4)6(x-4)^6 has an even exponent, so it never changes sign. (3−x)15(3-x)^{15} flips at x=3x=3, and (x+12)17(x+12)^{17} flips at x=−12x=-12.

Step 6: Tabulate

For x<−12x<-12: positive times negative, so g′<0g'<0. For −12<x<3-12<x<3: positive times positive, so g′>0g'>0. For x>3x>3: negative times positive, so g′<0g'<0.

Step 7: Classify

g′g' goes negative to positive at x=−12x=-12, a local minimum, so p=−12p=-12. It goes positive to negative at x=3x=3, a local maximum, so q=3q=3.

∣p+q∣=∣−9∣=9\left|p+q\right|=\left|-9\right|=9

Type 8, estimating without evaluating

Some questions never want the value. They want a bound, and the tool is the comparison property:

m≤f(x)≤M on [a,b] ⟹ m(b−a)≤∫abf(x) dx≤M(b−a)m\le f(x)\le M\text{ on }[a,b]\ \Longrightarrow\ m(b-a)\le\int_a^b f(x)\,dx\le M(b-a) A curve trapped between its minimum and maximum on an interval, with the two bounding rectangles drawn

Two companions are worth knowing: g≤f≤hg\le f\le h on [a,b][a,b] gives ∫abg≤∫abf≤∫abh\int_a^b g\le\int_a^b f\le\int_a^b h, and ∣∫abf∣≤∫ab∣f∣\left|\int_a^b f\right|\le\int_a^b\left|f\right|.

Example 28. (JEE Advanced 2012) Let f′(x)=192x32+sin⁡4(πx)f'(x)=\frac{192x^3}{2+\sin^4(\pi x)} for all x∈Rx\in\mathbb{R}, with f ⁣(12)=0f\!\left(\frac12\right)=0. If m≤∫1/21f(x) dx≤Mm\le\int_{1/2}^{1}f(x)\,dx\le M, find the possible mm and MM.

▸ SHOW SOLUTION

Step 1: Bound the derivative

sin⁡4(πx)∈[0,1]\sin^4(\pi x)\in[0,1], so 2+sin⁡4(πx)∈[2,3]2+\sin^4(\pi x)\in[2,3] and, for x>0x>0,

192x33≤f′(x)≤192x32,that is64x3≤f′(x)≤96x3\frac{192x^3}{3}\le f'(x)\le\frac{192x^3}{2},\qquad\text{that is}\qquad 64x^3\le f'(x)\le96x^3

Step 2: Integrate the bounds from 12\frac12 to xx

∫1/2x64t3 dt≤f(x)−f ⁣(12)≤∫1/2x96t3 dt\int_{1/2}^{x}64t^3\,dt\le f(x)-f\!\left(\tfrac12\right)\le\int_{1/2}^{x}96t^3\,dt

Step 3: Use f ⁣(12)=0f\!\left(\frac12\right)=0

16x4−1≤f(x)≤24x4−3216x^4-1\le f(x)\le24x^4-\frac32

Step 4: Integrate again from 12\frac12 to 11

∫1/21(16x4−1)dx≤∫1/21f(x) dx≤∫1/21(24x4−32)dx\int_{1/2}^{1}\left(16x^4-1\right)dx\le\int_{1/2}^{1}f(x)\,dx\le\int_{1/2}^{1}\left(24x^4-\frac32\right)dx

Step 5: Evaluate both sides

Left: 165(1−132)−12=165⋅3132−12=3110−12=2610=2.6\frac{16}{5}\left(1-\frac1{32}\right)-\frac12=\frac{16}{5}\cdot\frac{31}{32}-\frac12=\frac{31}{10}-\frac12=\frac{26}{10}=2.6. Right: 245⋅3132−34=9320−34=7820=3.9\frac{24}{5}\cdot\frac{31}{32}-\frac34=\frac{93}{20}-\frac34=\frac{78}{20}=3.9.

Step 6: Match against the options

2.6≤∫1/21f≤3.92.6\le\int_{1/2}^{1}f\le3.9, so any valid pair must satisfy m≤2.6m\le2.6 and M≥3.9M\ge3.9. Of the offered pairs only m=1, M=12m=1,\ M=12 works.

Example 29. (IIT JEE 2000) Let g(x)=∫0xf(t) dtg(x)=\int_0^{x}f(t)\,dt where 12≤f(t)≤1\frac12\le f(t)\le1 for t∈[0,1]t\in[0,1] and 0≤f(t)≤120\le f(t)\le\frac12 for t∈[1,2]t\in[1,2]. Bound g(2)g(2).

▸ SHOW SOLUTION

Step 1: Split at the changeover

g(2)=∫01f(t) dt+∫12f(t) dtg(2)=\int_0^1 f(t)\,dt+\int_1^2 f(t)\,dt

Step 2: Bound each piece with its own constants

12≤∫01f≤1,0≤∫12f≤12\frac12\le\int_0^1 f\le1,\qquad 0\le\int_1^2 f\le\frac12

Step 3: Add the inequalities

12≤g(2)≤32\frac12\le g(2)\le\frac32

Decision chart

Decision chart for choosing the right definite-integral property from the shape of the integrand
What you seeFirst move
a+ba+b is round, integrand has tan⁡\tan, cot⁡\cot or gg+h\frac{g}{g+h}King, then add and halve
Denominator 1+ag(x)1+a^{g(x)} with gg odd about the midpointKing, the base cancels
Limits −a-a to aaSplit into odd and even parts, delete the odd one
Limits 00 to 2a2aTest f(2a−x)f(2a-x) against f(x)f(x)
[ ⋅ ][\,\cdot\,] or { ⋅ }\{\,\cdot\,\} anywhereFind where the inside crosses an integer, then split
∣ ⋅ ∣\lvert\ \cdot\ \rvert anywhereFind the roots of the inside, then split
Limits are a large multiple of a periodCount periods, integrate one
Integral with constant limits inside the definition of ffName it, solve algebraically
Integral with variable upper limitDifferentiate, Newton–Leibnitz
Question asks for a range, not a valueBound the integrand, then integrate the bounds

Quick recall

SituationResult
Swap the limits∫abf=−∫baf\int_a^b f=-\int_b^a f
King∫abf(x) dx=∫abf(a+b−x) dx\int_a^b f(x)\,dx=\int_a^b f(a+b-x)\,dx
f(x)+f(a+b−x)=kf(x)+f(a+b-x)=k∫abf=k(b−a)2\int_a^b f=\frac{k(b-a)}{2}
f(x)=g(x)g(x)+g(a+b−x)f(x)=\frac{g(x)}{g(x)+g(a+b-x)}∫abf=b−a2\int_a^b f=\frac{b-a}{2}
ff odd on [−a,a][-a,a]∫−aaf=0\int_{-a}^{a}f=0
ff even on [−a,a][-a,a]∫−aaf=2∫0af\int_{-a}^{a}f=2\int_0^a f
f(2a−x)=−f(x)f(2a-x)=-f(x)∫02af=0\int_0^{2a}f=0
f(2a−x)=f(x)f(2a-x)=f(x)∫02af=2∫0af\int_0^{2a}f=2\int_0^a f
ff has period TT∫aa+nTf=n∫0Tf\int_a^{a+nT}f=n\int_0^{T}f
∫0nπ+v∣sin⁡x∣ dx\int_0^{n\pi+v}\lvert\sin x\rvert\,dx2n+1−cos⁡v2n+1-\cos v
∫0rx∣sin⁡πx∣ dx\int_0^r x\lvert\sin\pi x\rvert\,dxr2π\frac{r^2}{\pi}
m≤f≤Mm\le f\le M on [a,b][a,b]m(b−a)≤∫abf≤M(b−a)m(b-a)\le\int_a^b f\le M(b-a)
Newton–Leibnitzddx∫uvf(t) dt=f(v)v′−f(u)u′\frac{d}{dx}\int_{u}^{v}f(t)\,dt=f(v)v'-f(u)u'
The habit that makes this chapter fast

Before writing a single line, do three checks in this order. One: add the limits and see whether a+ba+b is round. Two: look for ∣ ⋅ ∣\lvert\ \cdot\ \rvert, [ ⋅ ][\,\cdot\,] or a piecewise definition, and if one is there, find the split points first. Three: ask whether the limits are constants or contain xx. Those three checks classify nearly every question in this chapter, and each takes about five seconds.

What a wrong start costs you

Reaching for the antiderivative on a king-property question is not a slower route to the same answer. On ∫π/245π/24dx1+tan⁡2x3\int_{\pi/24}^{5\pi/24}\frac{dx}{1+\sqrt[3]{\tan 2x}} there is no antiderivative to find, so the attempt goes nowhere and takes four minutes to establish that. In an exam where a question is worth about ninety seconds, the cost of the wrong opening move is the question plus two more.

Work through the full chapter with proofs, the complete problem bank and worked solutions in the IITianForum lecture notes PDF, then come back and try the ten shifts you have not seen yet.

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