Quick Recap — Indefinite Integrals

  • ∫xn dx=xn+1n+1+C\int x^n\,dx=\dfrac{x^{n+1}}{n+1}+C (n≠−1n\ne-1); ∫1x dx=ln⁡∣x∣+C\int\tfrac1x\,dx=\ln|x|+C.
  • ∫ex dx=ex+C\int e^x\,dx=e^x+C; ∫ax dx=axln⁡a+C\int a^x\,dx=\dfrac{a^x}{\ln a}+C.
  • ∫cos⁡x dx=sin⁡x+C\int\cos x\,dx=\sin x+C, ∫sin⁡x dx=−cos⁡x+C\int\sin x\,dx=-\cos x+C, ∫sec⁡2x dx=tan⁡x+C\int\sec^2x\,dx=\tan x+C.
  • ∫dx1+x2=tan⁡−1x+C\int\tfrac{dx}{1+x^2}=\tan^{-1}x+C, ∫dx1−x2=sin⁡−1x+C\int\tfrac{dx}{\sqrt{1-x^2}}=\sin^{-1}x+C. Integration reverses differentiation.

Beyond-NCERT JEE Formulae

Five results that collapse multi-step JEE integrals into one-liners. NCERT rarely states them, yet JEE Main leans on them every year.

1. The ex[f(x)+f′(x)]e^{x}[f(x)+f'(x)] 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

Because ddx[eaxf(x)]=eax[a f(x)+f′(x)]\dfrac{d}{dx}\big[e^{ax}f(x)\big]=e^{ax}\big[a\,f(x)+f'(x)\big], the scaled version also holds:

∫eax[a f(x)+f′(x)] dx=eaxf(x)+C.\int e^{ax}\big[a\,f(x)+f'(x)\big]\,dx=e^{ax}f(x)+C.

[JEE Tip] When the integrand is exe^{x} times a sum, check whether one part is the derivative of the other. Name ff so that f′f' sits right beside it, and the answer is simply exf(x)e^{x}f(x) with no integration required. Disguised forms such as 1+sin⁡x1+cos⁡x\dfrac{1+\sin x}{1+\cos x} hide an f+f′f+f' pair that surfaces after a half-angle rewrite.

2. Wallis' formula

For powers on the first quadrant, where ∫0π/2sin⁡nx dx=∫0π/2cos⁡nx dx\displaystyle\int_{0}^{\pi/2}\sin^{n}x\,dx=\int_{0}^{\pi/2}\cos^{n}x\,dx:

∫0π/2sin⁡nx dx=(n−1)(n−3)(n−5)⋯n(n−2)(n−4)⋯×{π2,n even1,n odd\int_{0}^{\pi/2}\sin^{n}x\,dx=\dfrac{(n-1)(n-3)(n-5)\cdots}{n(n-2)(n-4)\cdots}\times\begin{cases}\dfrac{\pi}{2}, & n\text{ even}\\[4pt] 1, & n\text{ odd}\end{cases}

Each product descends to 22 for even nn and to 11 for odd nn. The π2\dfrac{\pi}{2} tag appears only when nn is even; odd powers give a pure rational number.

3. The split at ∫02a\displaystyle\int_{0}^{2a}

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

Test the integrand's symmetry about the midpoint x=ax=a: a mirror-symmetric graph doubles the half-integral, while an anti-symmetric one cancels to zero.

4. Integrals of periodic functions

If ff has period TT, meaning f(x+T)=f(x)f(x+T)=f(x), then over any whole number of periods

∫0nTf(x) dx=n∫0Tf(x) dx,n=1,2,3,…\int_{0}^{nT}f(x)\,dx=n\int_{0}^{T}f(x)\,dx,\qquad n=1,2,3,\dots

and more generally ∫aa+nTf(x) dx=n∫0Tf(x) dx\displaystyle\int_{a}^{a+nT}f(x)\,dx=n\int_{0}^{T}f(x)\,dx for every real aa. Always use the true period: both ∣sin⁡x∣|\sin x| and sin⁡2x\sin^{2}x repeat with period π\pi, not 2π2\pi.

5. Weierstrass (half-angle) substitution

Putting t=tan⁡x2t=\tan\dfrac{x}{2} rationalises any integral built from sin⁡x\sin x and cos⁡x\cos x:

sin⁡x=2t1+t2,cos⁡x=1−t21+t2,dx=2 dt1+t2.\sin x=\dfrac{2t}{1+t^{2}},\qquad \cos x=\dfrac{1-t^{2}}{1+t^{2}},\qquad dx=\dfrac{2\,dt}{1+t^{2}}.

This turns ∫dxa+bcos⁡x\displaystyle\int\dfrac{dx}{a+b\cos x} (and likewise the a+bsin⁡xa+b\sin x form) into a rational integral in tt. For a definite integral with x:0→πx:0\to\pi, the new limits become t:0→∞t:0\to\infty.

Solved Examples — Beyond-NCERT Formulae

Example 1 — Spotting f+f′f+f'. Evaluate ∫ex(tan⁡−1x+11+x2)dx\displaystyle\int e^{x}\left(\tan^{-1}x+\dfrac{1}{1+x^{2}}\right)dx.

Let f(x)=tan⁡−1xf(x)=\tan^{-1}x. Then f′(x)=11+x2f'(x)=\dfrac{1}{1+x^{2}}, so the bracket is exactly f(x)+f′(x)f(x)+f'(x). Applying ∫ex[f+f′] dx=exf\displaystyle\int e^{x}[f+f']\,dx=e^{x}f,

∫ex(tan⁡−1x+11+x2)dx=extan⁡−1x+C.\int e^{x}\left(\tan^{-1}x+\dfrac{1}{1+x^{2}}\right)dx=e^{x}\tan^{-1}x+C.

Example 2 — A disguised f+f′f+f'. Evaluate ∫ex 1+sin⁡x1+cos⁡x dx\displaystyle\int e^{x}\,\dfrac{1+\sin x}{1+\cos x}\,dx.

Rewrite with half-angles, using 1+cos⁡x=2cos⁡2x21+\cos x=2\cos^{2}\dfrac{x}{2} together with 1+sin⁡x=1+2sin⁡x2cos⁡x21+\sin x=1+2\sin\dfrac{x}{2}\cos\dfrac{x}{2}:

1+sin⁡x1+cos⁡x=12sec⁡2x2+tan⁡x2.\dfrac{1+\sin x}{1+\cos x}=\dfrac{1}{2}\sec^{2}\dfrac{x}{2}+\tan\dfrac{x}{2}.

Take f(x)=tan⁡x2f(x)=\tan\dfrac{x}{2}, so that f′(x)=12sec⁡2x2f'(x)=\dfrac{1}{2}\sec^{2}\dfrac{x}{2} and the integrand is ex[f(x)+f′(x)]e^{x}[f(x)+f'(x)]. Therefore

∫ex 1+sin⁡x1+cos⁡x dx=extan⁡x2+C.\int e^{x}\,\dfrac{1+\sin x}{1+\cos x}\,dx=e^{x}\tan\dfrac{x}{2}+C.

Example 3 — The scaled eaxe^{ax} version. Evaluate ∫e3x(3sin⁡x+cos⁡x) dx\displaystyle\int e^{3x}\big(3\sin x+\cos x\big)\,dx.

Here a=3a=3 with f(x)=sin⁡xf(x)=\sin x, so a f(x)+f′(x)=3sin⁡x+cos⁡xa\,f(x)+f'(x)=3\sin x+\cos x fits the pattern eax[a f+f′]e^{ax}[a\,f+f']. Hence

∫e3x(3sin⁡x+cos⁡x) dx=e3xsin⁡x+C.\int e^{3x}\big(3\sin x+\cos x\big)\,dx=e^{3x}\sin x+C.

A quick check confirms it: ddx(e3xsin⁡x)=3e3xsin⁡x+e3xcos⁡x=e3x(3sin⁡x+cos⁡x).\dfrac{d}{dx}\big(e^{3x}\sin x\big)=3e^{3x}\sin x+e^{3x}\cos x=e^{3x}\big(3\sin x+\cos x\big).

Example 4 — Wallis for an even power. Evaluate ∫0π/2sin⁡6x dx\displaystyle\int_{0}^{\pi/2}\sin^{6}x\,dx.

With n=6n=6 (even), the descending odd-over-even product carries the π2\dfrac{\pi}{2} factor:

∫0π/2sin⁡6x dx=5⋅3⋅16⋅4⋅2⋅π2=1548⋅π2=5π32.\int_{0}^{\pi/2}\sin^{6}x\,dx=\dfrac{5\cdot 3\cdot 1}{6\cdot 4\cdot 2}\cdot\dfrac{\pi}{2}=\dfrac{15}{48}\cdot\dfrac{\pi}{2}=\dfrac{5\pi}{32}.

Example 5 — Combining the ∫02a\displaystyle\int_{0}^{2a} split with Wallis. Evaluate ∫0πsin⁡3x dx\displaystyle\int_{0}^{\pi}\sin^{3}x\,dx.

Here 2a=π2a=\pi, so a=π2a=\dfrac{\pi}{2}. Since sin⁡3(π−x)=sin⁡3x\sin^{3}(\pi-x)=\sin^{3}x, the integrand is symmetric about x=π2x=\dfrac{\pi}{2}, giving ∫0πsin⁡3x dx=2∫0π/2sin⁡3x dx\displaystyle\int_{0}^{\pi}\sin^{3}x\,dx=2\int_{0}^{\pi/2}\sin^{3}x\,dx. Wallis with n=3n=3 (odd) gives ∫0π/2sin⁡3x dx=23\displaystyle\int_{0}^{\pi/2}\sin^{3}x\,dx=\dfrac{2}{3}, hence

∫0πsin⁡3x dx=2⋅23=43.\int_{0}^{\pi}\sin^{3}x\,dx=2\cdot\dfrac{2}{3}=\dfrac{4}{3}.

Example 6 — The anti-symmetric ∫02a\displaystyle\int_{0}^{2a} case. Evaluate ∫0πcos⁡3x dx\displaystyle\int_{0}^{\pi}\cos^{3}x\,dx.

Again 2a=π2a=\pi. Now cos⁡3(π−x)=(−cos⁡x)3=−cos⁡3x\cos^{3}(\pi-x)=(-\cos x)^{3}=-\cos^{3}x, so the integrand is anti-symmetric about x=π2x=\dfrac{\pi}{2} and the two halves cancel:

∫0πcos⁡3x dx=0.\int_{0}^{\pi}\cos^{3}x\,dx=0.

Example 7 — A periodic integral. Evaluate ∫0nπ∣sin⁡x∣ dx\displaystyle\int_{0}^{n\pi}|\sin x|\,dx for a positive integer nn.

The function ∣sin⁡x∣|\sin x| has period T=πT=\pi (not 2π2\pi), and over one period ∫0π∣sin⁡x∣ dx=∫0πsin⁡x dx=[−cos⁡x]0π=2\displaystyle\int_{0}^{\pi}|\sin x|\,dx=\int_{0}^{\pi}\sin x\,dx=\big[-\cos x\big]_{0}^{\pi}=2. Using ∫0nTf=n∫0Tf\displaystyle\int_{0}^{nT}f=n\int_{0}^{T}f,

∫0nπ∣sin⁡x∣ dx=n∫0π∣sin⁡x∣ dx=2n.\int_{0}^{n\pi}|\sin x|\,dx=n\int_{0}^{\pi}|\sin x|\,dx=2n.

For example, ∫05π∣sin⁡x∣ dx=10\displaystyle\int_{0}^{5\pi}|\sin x|\,dx=10.

Example 8 — Weierstrass substitution. Evaluate ∫0πdx2+cos⁡x\displaystyle\int_{0}^{\pi}\dfrac{dx}{2+\cos x}.

Put t=tan⁡x2t=\tan\dfrac{x}{2}, so cos⁡x=1−t21+t2\cos x=\dfrac{1-t^{2}}{1+t^{2}} and dx=2 dt1+t2dx=\dfrac{2\,dt}{1+t^{2}}; the range x:0→πx:0\to\pi corresponds to t:0→∞t:0\to\infty. The denominator becomes

2+cos⁡x=2(1+t2)+(1−t2)1+t2=3+t21+t2,2+\cos x=\dfrac{2(1+t^{2})+(1-t^{2})}{1+t^{2}}=\dfrac{3+t^{2}}{1+t^{2}},

so the integrand collapses to 2 dt3+t2\dfrac{2\,dt}{3+t^{2}}. Therefore

\int_{0}^{\pi}\dfrac{dx}{2+\cos x}=\int_{0}^{\infty}\dfrac{2\,dt}{3+t^{2}}=\dfrac{2}{\sqrt{3}}\left[\tan^{-1}\dfrac{t}{\sqrt{3}}\right]_{0}^{\infty}=\dfrac{2}{\sqrt{3}}\cdot\dfrac{\pi}{2}=\dfrac{\pi}{\sqrt{3}}.