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)] rule
∫ex[f(x)+f′(x)]dx=exf(x)+C
Because dxd[eaxf(x)]=eax[af(x)+f′(x)], the scaled version also holds:
∫eax[af(x)+f′(x)]dx=eaxf(x)+C.
[JEE Tip] When the integrand is ex times a sum, check whether one part is the derivative of the other. Name f so that f′ sits right beside it, and the answer is simply exf(x) with no integration required. Disguised forms such as 1+cosx1+sinx hide an f+f′ pair that surfaces after a half-angle rewrite.
2. Wallis' formula
For powers on the first quadrant, where ∫0π/2sinnxdx=∫0π/2cosnxdx:
Test the integrand's symmetry about the midpoint x=a: a mirror-symmetric graph doubles the half-integral, while an anti-symmetric one cancels to zero.
4. Integrals of periodic functions
If f has period T, meaning f(x+T)=f(x), then over any whole number of periods
∫0nTf(x)dx=n∫0Tf(x)dx,n=1,2,3,…
and more generally ∫aa+nTf(x)dx=n∫0Tf(x)dx for every real a. Always use the true period: both ∣sinx∣ and sin2x repeat with period π, not 2π.
5. Weierstrass (half-angle) substitution
Putting t=tan2x rationalises any integral built from sinx and cosx:
sinx=1+t22t,cosx=1+t21−t2,dx=1+t22dt.
This turns ∫a+bcosxdx (and likewise the a+bsinx form) into a rational integral in t. For a definite integral with x:0→π, the new limits become t:0→∞.
Solved Examples — Beyond-NCERT Formulae
Example 1 — Spotting f+f′. Evaluate ∫ex(tan−1x+1+x21)dx.
Let f(x)=tan−1x. Then f′(x)=1+x21, so the bracket is exactly f(x)+f′(x). Applying ∫ex[f+f′]dx=exf,
∫ex(tan−1x+1+x21)dx=extan−1x+C.
Example 2 — A disguised f+f′. Evaluate ∫ex1+cosx1+sinxdx.
Rewrite with half-angles, using 1+cosx=2cos22x together with 1+sinx=1+2sin2xcos2x:
1+cosx1+sinx=21sec22x+tan2x.
Take f(x)=tan2x, so that f′(x)=21sec22x and the integrand is ex[f(x)+f′(x)]. Therefore
∫ex1+cosx1+sinxdx=extan2x+C.
Example 3 — The scaled eax version. Evaluate ∫e3x(3sinx+cosx)dx.
Here a=3 with f(x)=sinx, so af(x)+f′(x)=3sinx+cosx fits the pattern eax[af+f′]. Hence
∫e3x(3sinx+cosx)dx=e3xsinx+C.
A quick check confirms it: dxd(e3xsinx)=3e3xsinx+e3xcosx=e3x(3sinx+cosx).
Example 4 — Wallis for an even power. Evaluate ∫0π/2sin6xdx.
With n=6 (even), the descending odd-over-even product carries the 2π factor:
∫0π/2sin6xdx=6⋅4⋅25⋅3⋅1⋅2π=4815⋅2π=325π.
Example 5 — Combining the ∫02a split with Wallis. Evaluate ∫0πsin3xdx.
Here 2a=π, so a=2π. Since sin3(π−x)=sin3x, the integrand is symmetric about x=2π, giving ∫0πsin3xdx=2∫0π/2sin3xdx. Wallis with n=3 (odd) gives ∫0π/2sin3xdx=32, hence
∫0πsin3xdx=2⋅32=34.
Example 6 — The anti-symmetric ∫02a case. Evaluate ∫0πcos3xdx.
Again 2a=π. Now cos3(π−x)=(−cosx)3=−cos3x, so the integrand is anti-symmetric about x=2π and the two halves cancel:
∫0πcos3xdx=0.
Example 7 — A periodic integral. Evaluate ∫0nπ∣sinx∣dx for a positive integer n.
The function ∣sinx∣ has period T=π (not 2π), and over one period ∫0π∣sinx∣dx=∫0πsinxdx=[−cosx]0π=2. Using ∫0nTf=n∫0Tf,
∫0nπ∣sinx∣dx=n∫0π∣sinx∣dx=2n.
For example, ∫05π∣sinx∣dx=10.
Example 8 — Weierstrass substitution. Evaluate ∫0π2+cosxdx.
Put t=tan2x, so cosx=1+t21−t2 and dx=1+t22dt; the range x:0→π corresponds to t:0→∞. The denominator becomes