Some definite integrals defeat direct antidifferentiation but yield easily to clever properties. Mastering these is essential for board exams and JEE alike , every year, a problem appears whose three-line solution depends on the right property.
The eight standard properties
P1 , Reversal.∫abf(x)dx=−∫baf(x)dx.
P2 , Same limits.∫aaf(x)dx=0.
P3 , Variable renaming.∫abf(x)dx=∫abf(t)dt. The variable inside is "dummy" , only the function and the limits matter.
P8 , Periodic functions. If f has period T, then ∫aa+Tf(x)dx=∫0Tf(x)dx for any a. And ∫0nTf(x)dx=n∫0Tf(x)dx.
The king's-rule trick
Property P5 is the workhorse. The technique: if direct integration looks ugly, replace f(x) by f(a−x) and add the two versions. The pieces often combine into a constant or a simpler function.
The classic example. Evaluate I=∫0π/2sinx+cosxsinxdx.
By P5, I=∫0π/2sin(π/2−x)+cos(π/2−x)sin(π/2−x)dx=∫0π/2cosx+sinxcosxdx. Adding the two versions: 2I=∫0π/2sinx+cosxsinx+cosxdx=∫0π/21dx=π/2. So I=π/4.
Even/odd shortcuts
A function is even if f(−x)=f(x), odd if f(−x)=−f(x). On a symmetric interval [−a,a]:
Odd ⇒ integral vanishes by cancellation.
Even ⇒ integral is twice the half-interval integral.
This makes integrals like ∫−11x3cosxdx trivial: x3cosx is odd, so the answer is 0.
Periodicity
For ∫0nπ∣sinx∣dx: ∣sinx∣ has period π, and ∫0πsinxdx=2. So ∫0nπ∣sinx∣dx=2n.
A useful family
A frequent JEE setup. If f(a+b−x)+f(x)= constant or has a known relation to f(x), then P4 with addition yields a closed form.
A special instance: when f(a−x)=f(x) (the function is symmetric about x=a/2), then ∫0axf(x)dx=2a∫0af(x)dx. Proof: let I=∫0axf(x)dx. Substitute x↦a−x: I=∫0a(a−x)f(a−x)dx=∫0a(a−x)f(x)dx=a∫0af(x)dx−I. Solve.
Worked examples
Example 1.∫−π/2π/2sin7xdx.
sin7x is odd on a symmetric interval. Answer: 0.
Example 2.I=∫0π/2log(tanx)dx.
By P5, I=∫0π/2log(tan(π/2−x))dx=∫0π/2log(cotx)dx=−∫0π/2log(tanx)dx=−I. So 2I=0, giving I=0.
Example 3.I=∫0π1+cos2xxsinxdx.
By P5 with a=π: I=∫0π1+cos2(π−x)(π−x)sin(π−x)dx=∫0π1+cos2x(π−x)sinxdx. Add: 2I=∫0π1+cos2xπsinxdx. Substitute u=cosx, du=−sinxdx. Limits: u(0)=1, u(π)=−1. So 2I=π∫−111+u2du=π⋅2tan−11=π⋅2π. Therefore I=π2/4.
Example 4.∫0π/21+tan3xdx.
Let f(x)=1+tan3x1. Then f(π/2−x)=1+cot3x1=1+tan3xtan3x. So f(x)+f(π/2−x)=1. Adding the two versions: 2I=∫0π/21dx=π/2, so I=π/4.
Example 5.∫02πcos2xdx.
cos2x has period π. So the integral is 2∫0πcos2xdx=2⋅π/2=π.
Example 6.∫011+x2ln(1+x)dx (Putnam-style; substitute x=tanθ, θ∈[0,π/4]).
After substitution: ∫0π/4ln(1+tanθ)dθ. By P5 (with a=π/4): replace θ by π/4−θ. We get ln(1+tan(π/4−θ))=ln(1+tanθ2)=ln2−ln(1+tanθ). Adding: 2I=∫0π/4ln2dθ=4πln2. So I=8πln2.
Try it yourself
∫−11(x5−x3+x)dx
∫0π/2cosx+sinxcosxdx
∫0π1+sinxxdx
∫0ax+a−xxdx
∫0π/4ln(1+tanx)dx
∫02π∣cosx∣dx
∫−π/4π/4sin2xdx
∫−π/2π/21+x2x3cosxdx
∫0πxsin3xdx
∫01x(1−x)n , wait, ∫01x(1−x)ndx. (Use x↦1−x.)
∫0π/2sinnx+cosnxsinnxdx
∫−11x2ex2dx (use parity)
∫0nπ∣sinx∣dx where n∈N
∫0π/2log(sinx)dx (a famous one , use P5 and combine with log(cosx) version)
Pitfalls and tricks
Spot symmetry first. Always check if the integrand is odd/even on a symmetric interval , saves time.
King's rule rewards persistence. Apply it, add the two versions, and look for cancellation or simplification.
For periodic functions, integrate over one period and multiply by the number of periods.
Don't forget to substitute the variable after using a property , it's just a rename, but mismatched variables cause confusion.
Absolute values demand splitting.∫ab∣f(x)∣dx requires locating sign changes of f and splitting the interval.