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Definite Integration8 min read

Special Definite Integrals: Must-Memorize Results for JEE

Certain definite integrals appear so frequently in competitive exams that memorizing their results can save crucial time and mental effort. This guide presents four fundamental definite integrals with their standard results, along with proofs, related formulas, and problem-solving strategies...

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Special Definite Integrals: Must-Memorize Results for JEE

Introduction

Certain definite integrals appear so frequently in competitive exams that memorizing their results can save crucial time and mental effort. This guide presents four fundamental definite integrals with their standard results, along with proofs, related formulas, and problem-solving strategies tailored for JEE Main and Advanced.


1. The Gaussian Integral

Standard Result

0ex2dx=π2\int_0^\infty e^{-x^2} \, dx = \frac{\sqrt{\pi}}{2} Full version: ex2dx=π\int_{-\infty}^\infty e^{-x^2} \, dx = \sqrt{\pi}

Why it's Important

  • No elementary antiderivative exists.
  • Foundational in probability (normal distribution), physics (heat equation), and statistics.
  • Frequently appears indirectly in JEE problems after a substitution.

Proof (Polar Coordinates)

Let I=0ex2dxI = \int_0^\infty e^{-x^2} dx.
Then: I2=(0ex2dx)(0ey2dy)=00e(x2+y2)dxdy.I^2 = \left( \int_0^\infty e^{-x^2} dx \right) \left( \int_0^\infty e^{-y^2} dy \right) = \int_0^\infty \int_0^\infty e^{-(x^2 + y^2)} dx \, dy. Switch to polar coordinates: x=rcosθ,  y=rsinθx = r \cos\theta,\; y = r \sin\theta, dxdy=rdrdθdx \, dy = r \, dr \, d\theta, with r[0,)r \in [0,\infty), θ[0,π/2]\theta \in [0, \pi/2]: I2=0π/20er2rdrdθ.I^2 = \int_0^{\pi/2} \int_0^\infty e^{-r^2} \, r \, dr \, d\theta. Let u=r2u = r^2, so du=2rdrdu = 2r \, dr. Then: 0rer2dr=120eudu=12.\int_0^\infty r e^{-r^2} dr = \frac12 \int_0^\infty e^{-u} du = \frac12. Thus: I2=0π/212dθ=12π2=π4.I^2 = \int_0^{\pi/2} \frac12 \, d\theta = \frac12 \cdot \frac{\pi}{2} = \frac{\pi}{4}. Hence I=π2I = \frac{\sqrt{\pi}}{2}.

Generalizations to Memorize

IntegralResult (for a>0a>0)
0eax2dx\displaystyle \int_0^\infty e^{-ax^2} dx12πa\displaystyle \frac12 \sqrt{\frac{\pi}{a}}
eax2dx\displaystyle \int_{-\infty}^\infty e^{-ax^2} dxπa\displaystyle \sqrt{\frac{\pi}{a}}
0x2nex2dx\displaystyle \int_0^\infty x^{2n} e^{-x^2} dx(2n1)!!2n+1π\displaystyle \frac{(2n-1)!!}{2^{n+1}} \sqrt{\pi}
0ex2cos(bx)dx\displaystyle \int_0^\infty e^{-x^2} \cos(bx) \, dxπ2eb2/4\displaystyle \frac{\sqrt{\pi}}{2} e^{-b^2/4}

2. Integral of ln(sinx)\ln(\sin x) and ln(cosx)\ln(\cos x)

Standard Result

0π/2ln(sinx)dx=0π/2ln(cosx)dx=π2ln2.\int_0^{\pi/2} \ln(\sin x) \, dx = \int_0^{\pi/2} \ln(\cos x) \, dx = -\frac{\pi}{2} \ln 2.

Proof

Let I=0π/2ln(sinx)dxI = \int_0^{\pi/2} \ln(\sin x) dx.
By the substitution xπ2xx \to \frac{\pi}{2} - x, we get I=0π/2ln(cosx)dxI = \int_0^{\pi/2} \ln(\cos x) dx.

Now: 2I=0π/2[ln(sinx)+ln(cosx)]dx=0π/2ln ⁣(sin2x2)dx.2I = \int_0^{\pi/2} [\ln(\sin x) + \ln(\cos x)] \, dx = \int_0^{\pi/2} \ln\!\left( \frac{\sin 2x}{2} \right) dx. Thus: 2I=0π/2ln(sin2x)dx0π/2ln2dx.2I = \int_0^{\pi/2} \ln(\sin 2x) \, dx - \int_0^{\pi/2} \ln 2 \, dx. Let t=2xt = 2x in the first integral: 0π/2ln(sin2x)dx=120πln(sint)dt.\int_0^{\pi/2} \ln(\sin 2x) dx = \frac12 \int_0^\pi \ln(\sin t) dt. Using symmetry sin(πt)=sint\sin(\pi - t) = \sin t: 0πln(sint)dt=20π/2ln(sint)dt=2I.\int_0^\pi \ln(\sin t) dt = 2 \int_0^{\pi/2} \ln(\sin t) dt = 2I. Therefore: 2I=12(2I)π2ln2I=π2ln2.2I = \frac12 (2I) - \frac{\pi}{2} \ln 2 \quad\Rightarrow\quad I = -\frac{\pi}{2} \ln 2.

Related Results (Memorize)

IntegralValue
0π/2ln(sinx)dx\displaystyle \int_0^{\pi/2} \ln(\sin x) \, dxπ2ln2-\frac{\pi}{2} \ln 2
0πln(sinx)dx\displaystyle \int_0^{\pi} \ln(\sin x) \, dxπln2-\pi \ln 2
0π/2ln(tanx)dx\displaystyle \int_0^{\pi/2} \ln(\tan x) \, dx00
0π/2ln(secx)dx\displaystyle \int_0^{\pi/2} \ln(\sec x) \, dxπ2ln2\frac{\pi}{2} \ln 2
0π/4ln(tanx)dx\displaystyle \int_0^{\pi/4} \ln(\tan x) \, dxG-G (Catalan’s constant)

3. The xf(sinx)x \cdot f(\sin x) Property

Standard Result

For any function ff such that the integrals exist: 0πxf(sinx)dx=π20πf(sinx)dx.\int_0^\pi x \, f(\sin x) \, dx = \frac{\pi}{2} \int_0^\pi f(\sin x) \, dx.

Proof

Let I=0πxf(sinx)dxI = \int_0^\pi x f(\sin x) dx.
Replace xx by πx\pi - x: I=0π(πx)f(sin(πx))dx=0π(πx)f(sinx)dx.I = \int_0^\pi (\pi - x) f(\sin(\pi - x)) dx = \int_0^\pi (\pi - x) f(\sin x) dx. Hence: I=π0πf(sinx)dxI2I=π0πf(sinx)dx.I = \pi \int_0^\pi f(\sin x) dx - I \quad\Rightarrow\quad 2I = \pi \int_0^\pi f(\sin x) dx. So: I=π20πf(sinx)dx.I = \frac{\pi}{2} \int_0^\pi f(\sin x) dx.

Important Applications

Example 1: Evaluate 0πxsinx1+cos2xdx\int_0^\pi \frac{x \sin x}{1 + \cos^2 x} dx.
Here f(sinx)=sinx1+cos2xf(\sin x) = \frac{\sin x}{1 + \cos^2 x}. Thus: I=π20πsinx1+cos2xdx.I = \frac{\pi}{2} \int_0^\pi \frac{\sin x}{1 + \cos^2 x} dx. Substitute t=cosxt = \cos x, dt=sinxdxdt = -\sin x \, dx: I=π211dt1+t2=π211dt1+t2=π2[tan1t]11=π2π2=π24.I = \frac{\pi}{2} \int_{1}^{-1} \frac{-dt}{1+t^2} = \frac{\pi}{2} \int_{-1}^{1} \frac{dt}{1+t^2} = \frac{\pi}{2} \big[ \tan^{-1}t \big]_{-1}^{1} = \frac{\pi}{2} \cdot \frac{\pi}{2} = \frac{\pi^2}{4}.

Example 2: Evaluate 0πx1+sinxdx\int_0^\pi \frac{x}{1 + \sin x} dx.
Here f(sinx)=11+sinxf(\sin x) = \frac{1}{1+\sin x}. Then: I=π20πdx1+sinx.I = \frac{\pi}{2} \int_0^\pi \frac{dx}{1+\sin x}. Multiply numerator and denominator by 1sinx1 - \sin x: I=π20π1sinxcos2xdx=π20π(sec2xsecxtanx)dx=π2[tanxsecx]0π=π.I = \frac{\pi}{2} \int_0^\pi \frac{1 - \sin x}{\cos^2 x} dx = \frac{\pi}{2} \int_0^\pi (\sec^2 x - \sec x \tan x) dx = \frac{\pi}{2} \big[ \tan x - \sec x \big]_0^\pi = \pi.


4. The Dilogarithm Integral

Standard Result

01ln(1+x)xdx=π212.\int_0^1 \frac{\ln(1+x)}{x} \, dx = \frac{\pi^2}{12}.

Proof (Series Expansion)

Recall the Taylor series: ln(1+x)=n=1(1)n1xnn.\ln(1+x) = \sum_{n=1}^\infty \frac{(-1)^{n-1} x^n}{n}. Thus: ln(1+x)x=n=1(1)n1xn1n.\frac{\ln(1+x)}{x} = \sum_{n=1}^\infty \frac{(-1)^{n-1} x^{n-1}}{n}. Integrate term by term from 0 to 1: 01ln(1+x)xdx=n=1(1)n1n01xn1dx=n=1(1)n1n2.\int_0^1 \frac{\ln(1+x)}{x} dx = \sum_{n=1}^\infty \frac{(-1)^{n-1}}{n} \int_0^1 x^{n-1} dx = \sum_{n=1}^\infty \frac{(-1)^{n-1}}{n^2}. This is the alternating sum 1122+132142+1 - \frac{1}{2^2} + \frac{1}{3^2} - \frac{1}{4^2} + \cdots.
We know the Basel sum n=11n2=π26\sum_{n=1}^\infty \frac{1}{n^2} = \frac{\pi^2}{6}.

Separate odd and even terms: n=11n2=k=11(2k1)2+14k=11k2.\sum_{n=1}^\infty \frac{1}{n^2} = \sum_{k=1}^\infty \frac{1}{(2k-1)^2} + \frac14 \sum_{k=1}^\infty \frac{1}{k^2}. Hence: π26=Sodd+π224Sodd=π28.\frac{\pi^2}{6} = S_{\text{odd}} + \frac{\pi^2}{24} \quad\Rightarrow\quad S_{\text{odd}} = \frac{\pi^2}{8}. Now: n=1(1)n1n2=Sodd14k=11k2=π28π224=π212.\sum_{n=1}^\infty \frac{(-1)^{n-1}}{n^2} = S_{\text{odd}} - \frac14 \sum_{k=1}^\infty \frac{1}{k^2} = \frac{\pi^2}{8} - \frac{\pi^2}{24} = \frac{\pi^2}{12}.

Related Logarithmic Integrals

IntegralValue
01ln(1+x)xdx\displaystyle \int_0^1 \frac{\ln(1+x)}{x} dxπ212\frac{\pi^2}{12}
01ln(1x)xdx\displaystyle \int_0^1 \frac{\ln(1-x)}{x} dxπ26-\frac{\pi^2}{6}
01lnx1xdx\displaystyle \int_0^1 \frac{\ln x}{1-x} dxπ26-\frac{\pi^2}{6}
01lnx1+xdx\displaystyle \int_0^1 \frac{\ln x}{1+x} dxπ212-\frac{\pi^2}{12}
01ln(1+x)1+x2dx\displaystyle \int_0^1 \frac{\ln(1+x)}{1+x^2} dxπ8ln2\frac{\pi}{8} \ln 2

5. Application to Previous Year JEE Problems

Problem 1 (JEE Advanced 2012)

Evaluate π/2π/2(x2+ln ⁣(π+xπx))cosxdx\displaystyle \int_{-\pi/2}^{\pi/2} \left( x^2 + \ln\!\left(\frac{\pi+x}{\pi-x}\right) \right) \cos x \, dx.

Solution:
Split the integral: I=π/2π/2x2cosxdxI1  +  π/2π/2ln ⁣(π+xπx)cosxdxI2.I = \underbrace{\int_{-\pi/2}^{\pi/2} x^2 \cos x \, dx}_{I_1} \;+\; \underbrace{\int_{-\pi/2}^{\pi/2} \ln\!\left(\frac{\pi+x}{\pi-x}\right) \cos x \, dx}_{I_2}.

  • I1I_1: The integrand x2cosxx^2 \cos x is even, so I1=20π/2x2cosxdx.I_1 = 2 \int_0^{\pi/2} x^2 \cos x \, dx. Use integration by parts twice (or known result) to get I1=π224I_1 = \frac{\pi^2}{2} - 4.
  • I2I_2: The function ln ⁣(π+xπx)\ln\!\left(\frac{\pi+x}{\pi-x}\right) is odd, and cosx\cos x is even, so their product is odd. Hence I2=0I_2 = 0.

Thus I=π224I = \frac{\pi^2}{2} - 4.

Problem 2 (JEE Main Pattern)

Evaluate 0πxsinx1+cos2xdx\displaystyle \int_0^\pi \frac{x \sin x}{1 + \cos^2 x} \, dx.

Solution:
Use the xf(sinx)x f(\sin x) property: I=π20πsinx1+cos2xdx.I = \frac{\pi}{2} \int_0^\pi \frac{\sin x}{1 + \cos^2 x} dx. Substitute t=cosxt = \cos x: I=π211dt1+t2=π211dt1+t2=π2π2=π24.I = \frac{\pi}{2} \int_{1}^{-1} \frac{-dt}{1+t^2} = \frac{\pi}{2} \int_{-1}^{1} \frac{dt}{1+t^2} = \frac{\pi}{2} \cdot \frac{\pi}{2} = \frac{\pi^2}{4}.

Problem 3 (JEE Advanced Pattern)

Prove 0π/4ln(1+tanx)dx=π8ln2\displaystyle \int_0^{\pi/4} \ln(1+\tan x) \, dx = \frac{\pi}{8} \ln 2.

Solution:
Let I=0π/4ln(1+tanx)dxI = \int_0^{\pi/4} \ln(1+\tan x) dx.
Substitute xπ4xx \to \frac{\pi}{4} - x: I=0π/4ln ⁣(1+tan ⁣(π4x))dx=0π/4ln ⁣(1+1tanx1+tanx)dx=0π/4ln ⁣(21+tanx)dx.I = \int_0^{\pi/4} \ln\!\left(1 + \tan\!\left(\frac{\pi}{4} - x\right)\right) dx = \int_0^{\pi/4} \ln\!\left(1 + \frac{1 - \tan x}{1 + \tan x}\right) dx = \int_0^{\pi/4} \ln\!\left(\frac{2}{1+\tan x}\right) dx. Thus: I=0π/4ln2dxI2I=π4ln2I=π8ln2.I = \int_0^{\pi/4} \ln 2 \, dx - I \quad\Rightarrow\quad 2I = \frac{\pi}{4} \ln 2 \quad\Rightarrow\quad I = \frac{\pi}{8} \ln 2.


6. Quick Reference Table (Memorize!)

IntegralResultKey Property
0ex2dx\int_0^\infty e^{-x^2} dxπ2\frac{\sqrt{\pi}}{2}Gaussian, polar coordinates
0π/2ln(sinx)dx\int_0^{\pi/2} \ln(\sin x) dxπ2ln2-\frac{\pi}{2} \ln 2Symmetry & double‑angle
0πxf(sinx)dx\int_0^\pi x f(\sin x) dxπ20πf(sinx)dx\frac{\pi}{2} \int_0^\pi f(\sin x) dxKing’s property
01ln(1+x)xdx\int_0^1 \frac{\ln(1+x)}{x} dxπ212\frac{\pi^2}{12}Series expansion

7. Tips for JEE Aspirants

  1. Commit these results to memory – they are often required as intermediate steps in time‑sensitive exams.
  2. Recognize disguised forms – many integrals can be transformed into one of these four by a simple substitution.
  3. Combine with other properties – use symmetry, periodicity, and substitution to reduce an unfamiliar integral to a standard form.
  4. Practice derivations – understanding the proofs helps you adapt the results to variations that may appear in the exam.
  5. Use the quick‑reference table during revision to reinforce recall.

Master these four special definite integrals thoroughly. They are not just formulas but powerful tools that, when recognized, can turn a lengthy problem into a one‑line solution.

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Practice with real JEE Main questions and see these methods in action.

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