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Class 12Calculus10:21Published 23 Oct 2024

Definite Integrals of Trigonometry by Substitution (Exercise 7.9)

Work through Class XII definite integrals of trigonometric functions using the substitution method, including how to change the limits when you change the variable.

This lesson solves several sure-shot definite integrals from Exercise 7.9 by substitution. Each example shows how to choose the right substitution, convert the limits from x to the new variable, and evaluate cleanly. The problems range from simple powers of sine and cosine to integrals that need an inverse-trig substitution and integration by parts.

What you'll learn

  • How to change the limits of a definite integral when you substitute a new variable
  • Choosing substitutions for integrals built from powers of sine and cosine
  • Simplifying an inverse-tangent integral with an inverse-trig substitution and integration by parts
  • Reading off a derivative directly from an integral using the fundamental theorem

Lesson chapters

0:00Substitution and changing the limits
1:13Inverse tangent over one plus x squared
2:13Root sine times cosine to the fifth
5:41Inverse sine substitution and parts
8:58Sine over one plus cosine squared
10:07Derivative from an integral

Lesson notes

This lesson evaluates a set of definite integrals of trigonometric functions from Exercise 7.9 using the substitution method. The key idea throughout is that when you replace xx with a new variable, you also convert the limits of integration to that variable, so you never have to substitute back.

A simple power of sine

Evaluate

I=∫0π/4sin⁡22x cos⁡2x dx.I = \int_0^{\pi/4} \sin^2 2x \, \cos 2x \, dx.

Put t=sin⁡2xt = \sin 2x. Then dt=2cos⁡2x dxdt = 2\cos 2x \, dx, so cos⁡2x dx=12 dt\cos 2x \, dx = \tfrac{1}{2}\,dt.

Change the limits. When x=0x = 0, t=sin⁡0=0t = \sin 0 = 0. When x=π4x = \tfrac{\pi}{4}, t=sin⁡π2=1t = \sin\tfrac{\pi}{2} = 1.

I=12∫01t2 dt=12[t33]01=16(13−03)=16.I = \frac{1}{2}\int_0^1 t^2 \, dt = \frac{1}{2}\left[\frac{t^3}{3}\right]_0^1 = \frac{1}{6}\big(1^3 - 0^3\big) = \frac{1}{6}.

Inverse tangent over 1+x21 + x^2

Evaluate

I=∫01tan⁡−1x1+x2 dx.I = \int_0^1 \frac{\tan^{-1} x}{1 + x^2}\, dx.

Put t=tan⁡−1xt = \tan^{-1} x, so dt=11+x2 dxdt = \dfrac{1}{1 + x^2}\,dx.

Change the limits. When x=0x = 0, t=tan⁡−10=0t = \tan^{-1} 0 = 0. When x=1x = 1, t=tan⁡−11=π4t = \tan^{-1} 1 = \tfrac{\pi}{4}.

I=∫0π/4t dt=[t22]0π/4=12(π4)2=12⋅π216=π232.I = \int_0^{\pi/4} t \, dt = \left[\frac{t^2}{2}\right]_0^{\pi/4} = \frac{1}{2}\left(\frac{\pi}{4}\right)^2 = \frac{1}{2}\cdot\frac{\pi^2}{16} = \frac{\pi^2}{32}.

Root sine times cosine to the fifth power

Evaluate

I=∫0π/2sin⁡ϕ cos⁡5ϕ dϕ.I = \int_0^{\pi/2} \sqrt{\sin\phi}\,\cos^5\phi \, d\phi.

Split off one cosine and rewrite the rest with cos⁡4ϕ=(1−sin⁡2ϕ)2\cos^4\phi = (1 - \sin^2\phi)^2:

I=∫0π/2sin⁡ϕ (1−sin⁡2ϕ)2cos⁡ϕ dϕ.I = \int_0^{\pi/2} \sqrt{\sin\phi}\,\big(1 - \sin^2\phi\big)^2 \cos\phi \, d\phi.

Put t=sin⁡ϕt = \sin\phi, so dt=cos⁡ϕ dϕdt = \cos\phi \, d\phi. The limits become 00 and 11.

I=∫01t (1−t2)2 dt=∫01t1/2(1−2t2+t4) dt=∫01(t1/2−2t5/2+t9/2) dt.I = \int_0^1 \sqrt{t}\,(1 - t^2)^2 \, dt = \int_0^1 t^{1/2}\big(1 - 2t^2 + t^4\big)\, dt = \int_0^1 \Big(t^{1/2} - 2t^{5/2} + t^{9/2}\Big)\, dt.

Integrating term by term:

I=[t3/23/2−2⋅t7/27/2+t11/211/2]01=23−47+211.I = \left[\frac{t^{3/2}}{3/2} - 2\cdot\frac{t^{7/2}}{7/2} + \frac{t^{11/2}}{11/2}\right]_0^1 = \frac{2}{3} - \frac{4}{7} + \frac{2}{11}.

With a common denominator of 231231:

I=154−132+42231=64231.I = \frac{154 - 132 + 42}{231} = \frac{64}{231}.

Inverse sine substitution with integration by parts

Evaluate

I=∫01sin⁡−1 ⁣(2x1+x2)dx.I = \int_0^1 \sin^{-1}\!\left(\frac{2x}{1 + x^2}\right) dx.

Put x=tan⁡θx = \tan\theta, so dx=sec⁡2θ dθdx = \sec^2\theta \, d\theta. Then

2x1+x2=2tan⁡θ1+tan⁡2θ=sin⁡2θ,\frac{2x}{1 + x^2} = \frac{2\tan\theta}{1 + \tan^2\theta} = \sin 2\theta,

so sin⁡−1(sin⁡2θ)=2θ\sin^{-1}(\sin 2\theta) = 2\theta. The limits x=0x = 0 and x=1x = 1 become θ=0\theta = 0 and θ=π4\theta = \tfrac{\pi}{4}.

I=∫0π/42θ sec⁡2θ dθ=2∫0π/4θ sec⁡2θ dθ.I = \int_0^{\pi/4} 2\theta \, \sec^2\theta \, d\theta = 2\int_0^{\pi/4} \theta \, \sec^2\theta \, d\theta.

Integration by parts with first function θ\theta and second function sec⁡2θ\sec^2\theta (whose integral is tan⁡θ\tan\theta):

I=2[θtan⁡θ]0π/4−2∫0π/4tan⁡θ dθ=2[θtan⁡θ]0π/4−2[log⁡∣sec⁡θ∣]0π/4.I = 2\left[\theta \tan\theta\right]_0^{\pi/4} - 2\int_0^{\pi/4} \tan\theta \, d\theta = 2\left[\theta \tan\theta\right]_0^{\pi/4} - 2\Big[\log|\sec\theta|\Big]_0^{\pi/4}.

Evaluating, tan⁡π4=1\tan\tfrac{\pi}{4} = 1 and sec⁡π4=2\sec\tfrac{\pi}{4} = \sqrt{2}:

I=2⋅π4⋅1−2log⁡2=π2−2⋅12log⁡2=π2−log⁡2.I = 2\cdot\frac{\pi}{4}\cdot 1 - 2\log\sqrt{2} = \frac{\pi}{2} - 2\cdot\tfrac{1}{2}\log 2 = \frac{\pi}{2} - \log 2.

Sine over 1+cos⁡2x1 + \cos^2 x

Evaluate

I=∫0π/2sin⁡x1+cos⁡2x dx.I = \int_0^{\pi/2} \frac{\sin x}{1 + \cos^2 x}\, dx.

Put t=cos⁡xt = \cos x, so −sin⁡x dx=dt-\sin x \, dx = dt, that is sin⁡x dx=−dt\sin x \, dx = -dt.

Change the limits. When x=0x = 0, t=cos⁡0=1t = \cos 0 = 1. When x=π2x = \tfrac{\pi}{2}, t=cos⁡π2=0t = \cos\tfrac{\pi}{2} = 0.

I=∫10−dt1+t2=∫01dt1+t2=[tan⁡−1t]01=tan⁡−11−tan⁡−10=π4.I = \int_1^0 \frac{-dt}{1 + t^2} = \int_0^1 \frac{dt}{1 + t^2} = \Big[\tan^{-1} t\Big]_0^1 = \tan^{-1} 1 - \tan^{-1} 0 = \frac{\pi}{4}.

Reading a derivative straight from an integral

If

f(x)=∫0xtsin⁡t dt,f(x) = \int_0^x t \sin t \, dt,

then by the fundamental theorem of calculus, differentiating an integral with respect to its upper limit gives back the integrand:

f′(x)=xsin⁡x.f'(x) = x \sin x.

Key takeaways

  • When you substitute a new variable, convert the limits to that variable so you can evaluate without changing back.
  • For powers of sine and cosine, peel off one factor to match the differential and rewrite the rest with sin⁡2ϕ+cos⁡2ϕ=1\sin^2\phi + \cos^2\phi = 1.
  • An inverse-trig substitution like x=tan⁡θx = \tan\theta can turn an awkward inverse-sine integral into a simple integration by parts.
  • The derivative of ∫0xg(t) dt\int_0^x g(t)\,dt with respect to xx is just g(x)g(x).