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Mathematics · Ch 10 — Integrals

Integration by Substitution

2

Integration by Substitution

When the integrand is not a standard form directly but can be seen as a composite function multiplied by the derivative of its inner function, the method of substitution converts it

into a standard integral in a new variable.

Derivation from the chain rule. Suppose FF is an antiderivative of ff, so F′=fF'=f, and let

u=g(x)u=g(x) where gg is differentiable. By the chain rule,

ddx[F(g(x))]=F′(g(x))⋅g′(x)=f(g(x))⋅g′(x).\frac{d}{dx}\Big[F\big(g(x)\big)\Big] = F'\big(g(x)\big)\cdot g'(x) = f\big(g(x)\big)\cdot g'(x).

Reading this equation as a statement about antiderivatives (i.e. integrating both sides),

∫f(g(x)) g′(x) dx=F(g(x))+C.\int f\big(g(x)\big)\,g'(x)\,dx = F\big(g(x)\big)+C.

Writing u=g(x)u=g(x) so that du=g′(x) dxdu=g'(x)\,dx, the left side becomes exactly ∫f(u) du=F(u)+C\int f(u)\,du=F(u)+C --

the substitution has turned a composite integral in xx into a (hopefully standard) integral in

uu, to be converted back to xx at the very end by resubstituting u=g(x)u=g(x).

Practical recipe. (i) Identify a part of the integrand, u=g(x)u=g(x), whose derivative g′(x)g'(x)

also appears (up to a constant multiple) elsewhere in the integrand; (ii) compute du=g′(x) dxdu=g'(x)\,dx

and rewrite the ENTIRE integral in terms of uu only, with no xx remaining; (iii) integrate the

resulting standard form in uu; (iv) substitute u=g(x)u=g(x) back to return to xx.

Worked illustration. For ∫2xcos⁡(x2) dx\displaystyle\int 2x\cos(x^2)\,dx: let u=x2u=x^2, so du=2x dxdu=2x\,dx --

exactly the factor 2x dx2x\,dx present in the integral. The integral becomes ∫cos⁡u du=sin⁡u+C=sin⁡(x2)+C\int\cos u\,du=\sin u+C=\sin(x^2)+C, matching Example 2.

Substitution with a trigonometric identity. Sometimes the integrand needs an identity applied

FIRST before a substitution becomes visible. For ∫sin⁡3x dx\int\sin^3x\,dx, write

sin⁡3x=sin⁡x⋅sin⁡2x=sin⁡x (1−cos⁡2x)\sin^3x=\sin x\cdot\sin^2x=\sin x\,(1-\cos^2x) using sin⁡2x+cos⁡2x=1\sin^2x+\cos^2x=1; now u=cos⁡xu=\cos x gives …