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Exercise 9.3 · Q2

Q.Evaluate the following integrals using properties of integration:

(i) ∫−55xcos⁡ ⁣(ex−1ex+1)dx\displaystyle\int_{-5}^5 x\cos\!\left(\dfrac{e^x-1}{e^x+1}\right)dx
(ii) ∫−π/2π/2(x5+xcos⁡x+tan⁡3x+1) dx\displaystyle\int_{-\pi/2}^{\pi/2} (x^5+x\cos x+\tan^3x+1)\,dx
(iii) ∫−π/4π/4sin⁡2x dx\displaystyle\int_{-\pi/4}^{\pi/4}\sin^2x\,dx
(iv) ∫02πxlog⁡ ⁣(3+cos⁡x3−cos⁡x)dx\displaystyle\int_0^{2\pi} x\log\!\left(\dfrac{3+\cos x}{3-\cos x}\right)dx
(v) ∫02πsin⁡4xcos⁡3x dx\displaystyle\int_0^{2\pi}\sin^4x\cos^3x\,dx
(vi) ∫01∣5x−3∣ dx\displaystyle\int_0^1 |5x-3|\,dx
(vii) ∫0sin⁡2xsin⁡−1t dt+∫0cos⁡2xcos⁡−1t dt\displaystyle\int_0^{\sin^2x}\sin^{-1}\sqrt t\,dt+\int_0^{\cos^2x}\cos^{-1}\sqrt t\,dt
(viii) ∫01log⁡(1+x)1+x2 dx\displaystyle\int_0^1\dfrac{\log(1+x)}{1+x^2}\,dx
(ix) ∫0πxsin⁡x1+sin⁡x dx\displaystyle\int_0^\pi\dfrac{x\sin x}{1+\sin x}\,dx
(x) ∫π/83π/8dx1+tan⁡x\displaystyle\int_{\pi/8}^{3\pi/8}\dfrac{dx}{1+\sqrt{\tan x}}
(xi) ∫0πx[sin⁡2(sin⁡x)+cos⁡2(cos⁡x)]dx\displaystyle\int_0^\pi x\left[\sin^2(\sin x)+\cos^2(\cos x)\right]dx
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We evaluate all eleven integrals purely from the twelve properties of definite integrals (dummy-variable invariance, limit reversal, additivity, linearity, the a+b−xa+b-x reflection, even/odd shortcuts, half-period doubling/cancellation, and the x f(x)x\,f(x) symmetry trick) — never from a raw antiderivative. Several parts collapse instantly to 00 or a multiple of π\pi by checking whether the integrand is even or odd; the rest use the "substitute x→a+b−xx\to a+b-x, add the two copies, solve for II" trick that recurs throughout this section.

Step 1 (i). Determine the parity of g(x)=cos⁡ ⁣(ex−1ex+1)g(x)=\cos\!\left(\dfrac{e^x-1}{e^x+1}\right).

g(−x)=cos⁡ ⁣(e−x−1e−x+1).g(-x)=\cos\!\left(\frac{e^{-x}-1}{e^{-x}+1}\right).

Multiply numerator and denominator by exe^x:

e−x−1e−x+1=1−ex1+ex=−ex−1ex+1.\frac{e^{-x}-1}{e^{-x}+1}=\frac{1-e^x}{1+e^x}=-\frac{e^x-1}{e^x+1}.

So g(−x)=cos⁡ ⁣(−ex−1ex+1)=cos⁡ ⁣(ex−1ex+1)=g(x)g(-x)=\cos\!\left(-\dfrac{e^x-1}{e^x+1}\right)=\cos\!\left(\dfrac{e^x-1}{e^x+1}\right)=g(x) (cosine is even) — gg is even.

Step 2 (i). Determine the parity of the full integrand and apply Property 9.

The integrand is f(x)=x g(x)f(x)=x\,g(x). Since xx is odd and gg is even, f(−x)=(−x)g(−x)=−x g(x)=−f(x)f(-x)=(-x)g(-x)=-x\,g(x)=-f(x), so ff is odd. By Property 9 (odd-function shortcut), ∫−aaf(x) dx=0\displaystyle\int_{-a}^{a}f(x)\,dx=0 for any odd ff. Hence

∫−55xcos⁡ ⁣(ex−1ex+1)dx=0.\int_{-5}^{5}x\cos\!\left(\frac{e^x-1}{e^x+1}\right)dx=0.

Step 3 (ii). Split the integral by linearity (Property 4) and classify each term's parity on [−π/2,π/2][-\pi/2,\pi/2].

∫−π/2π/2(x5+xcos⁡x+tan⁡3x+1) dx=∫−π/2π/2x5dx+∫−π/2π/2xcos⁡x dx+∫−π/2π/2tan⁡3x dx+∫−π/2π/21 dx.\int_{-\pi/2}^{\pi/2}(x^5+x\cos x+\tan^3x+1)\,dx=\int_{-\pi/2}^{\pi/2}x^5dx+\int_{-\pi/2}^{\pi/2}x\cos x\,dx+\int_{-\pi/2}^{\pi/2}\tan^3x\,dx+\int_{-\pi/2}^{\pi/2}1\,dx.

  • x5x^5: (−x)5=−x5(-x)^5=-x^5, odd.
  • xcos⁡xx\cos x: xx is odd, cos⁡x\cos x is even, so the product is odd: (−x)cos⁡(−x)=−xcos⁡x(-x)\cos(-x)=-x\cos x.
  • tan⁡3x\tan^3x: tan⁡(−x)=−tan⁡x⇒tan⁡3(−x)=−tan⁡3x\tan(-x)=-\tan x\Rightarrow\tan^3(-x)=-\tan^3x, odd.
  • 11: even (constant).

Step 4 (ii). Apply Property 9 to the three odd terms and evaluate the constant term.

By Property 9 the first three integrals all vanish. For the last, ∫−π/2π/21 dx=π/2−(−π/2)=π\displaystyle\int_{-\pi/2}^{\pi/2}1\,dx=\pi/2-(-\pi/2)=\pi. So

∫−π/2π/2(x5+xcos⁡x+tan⁡3x+1) dx=0+0+0+π=π.\int_{-\pi/2}^{\pi/2}(x^5+x\cos x+\tan^3x+1)\,dx=0+0+0+\pi=\pi.

Step 5 (iii). Use the even-function shortcut (Property 8).

sin⁡2x\sin^2x is even, since sin⁡2(−x)=(−sin⁡x)2=sin⁡2x\sin^2(-x)=(-\sin x)^2=\sin^2x. So

∫−π/4π/4sin⁡2x dx=2∫0π/4sin⁡2x dx.\int_{-\pi/4}^{\pi/4}\sin^2x\,dx=2\int_0^{\pi/4}\sin^2x\,dx.

Step 6 (iii). Evaluate with the half-angle formula.

sin⁡2x=1−cos⁡2x2\sin^2x=\dfrac{1-\cos2x}{2}, so

∫0π/4sin⁡2x dx=12[x−sin⁡2x2]0π/4=12(π4−sin⁡(π/2)2)=12(π4−12)=π8−14.\int_0^{\pi/4}\sin^2x\,dx=\frac12\left[x-\frac{\sin2x}{2}\right]_0^{\pi/4}=\frac12\left(\frac{\pi}{4}-\frac{\sin(\pi/2)}{2}\right)=\frac12\left(\frac{\pi}{4}-\frac12\right)=\frac{\pi}{8}-\frac14.

Doubling: ∫−π/4π/4sin⁡2x dx=2(π8−14)=π4−12.\displaystyle\int_{-\pi/4}^{\pi/4}\sin^2x\,dx=2\left(\frac{\pi}{8}-\frac14\right)=\frac{\pi}{4}-\frac12.

Step 7 (iv). Reflect the original integral I=∫02πxlog⁡ ⁣(3+cos⁡x3−cos⁡x)dxI=\displaystyle\int_0^{2\pi}x\log\!\left(\dfrac{3+\cos x}{3-\cos x}\right)dx using x→2π−xx\to2\pi-x (Property 6).

Write h(x)=log⁡ ⁣(3+cos⁡x3−cos⁡x)h(x)=\log\!\left(\dfrac{3+\cos x}{3-\cos x}\right). Since cos⁡(2π−x)=cos⁡x\cos(2\pi-x)=\cos x (period 2π2\pi), h(2π−x)=h(x)h(2\pi-x)=h(x). By Property 6 (with a=0, b=2πa=0,\ b=2\pi),

I=∫02π(2π−x) h(2π−x) dx=∫02π(2π−x) h(x) dx=2π∫02πh(x) dx−I.I=\int_0^{2\pi}(2\pi-x)\,h(2\pi-x)\,dx=\int_0^{2\pi}(2\pi-x)\,h(x)\,dx=2\pi\int_0^{2\pi}h(x)\,dx-I.

Step 8 (iv). Solve for II in terms of J=∫02πh(x) dxJ=\int_0^{2\pi}h(x)\,dx, then show J=0J=0.

2I=2πJ⇒I=πJ2I=2\pi J\Rightarrow I=\pi J. Split JJ at π\pi (Property 3, additivity) and shift the second piece by x=t+πx=t+\pi:

J=∫0πh(x) dx+∫π2πh(x) dx=∫0πh(x) dx+∫0πh(t+π) dt.J=\int_0^\pi h(x)\,dx+\int_\pi^{2\pi}h(x)\,dx=\int_0^\pi h(x)\,dx+\int_0^\pi h(t+\pi)\,dt.

Since cos⁡(t+π)=−cos⁡t\cos(t+\pi)=-\cos t, h(t+π)=log⁡ ⁣(3−cos⁡t3+cos⁡t)=−log⁡ ⁣(3+cos⁡t3−cos⁡t)=−h(t)h(t+\pi)=\log\!\left(\dfrac{3-\cos t}{3+\cos t}\right)=-\log\!\left(\dfrac{3+\cos t}{3-\cos t}\right)=-h(t). So

J=∫0πh(x) dx−∫0πh(t) dt=0.J=\int_0^\pi h(x)\,dx-\int_0^\pi h(t)\,dt=0.

Hence I=π⋅0=0I=\pi\cdot0=0.

Step 9 (v). Rewrite cos⁡3x\cos^3x using cos⁡2x=1−sin⁡2x\cos^2x=1-\sin^2x, then split by linearity (Property 4).

cos⁡3x=cos⁡x(1−sin⁡2x)=cos⁡x−sin⁡2xcos⁡x,\cos^3x=\cos x(1-\sin^2x)=\cos x-\sin^2x\cos x,

so

∫02πsin⁡4xcos⁡3x dx=∫02πsin⁡4xcos⁡x dx−∫02πsin⁡6xcos⁡x dx.\int_0^{2\pi}\sin^4x\cos^3x\,dx=\int_0^{2\pi}\sin^4x\cos x\,dx-\int_0^{2\pi}\sin^6x\cos x\,dx.

Step 10 (v). Evaluate each piece as a full-period total-derivative integral.

sin⁡4xcos⁡x=ddx ⁣(sin⁡5x5)\sin^4x\cos x=\dfrac{d}{dx}\!\left(\dfrac{\sin^5x}{5}\right), so ∫02πsin⁡4xcos⁡x dx=[sin⁡5x5]02π=sin⁡5(2π)−sin⁡5(0)5=0\displaystyle\int_0^{2\pi}\sin^4x\cos x\,dx=\left[\frac{\sin^5x}{5}\right]_0^{2\pi}=\frac{\sin^5(2\pi)-\sin^5(0)}{5}=0 (since sin⁡0=sin⁡2π=0\sin0=\sin2\pi=0). Likewise sin⁡6xcos⁡x=ddx ⁣(sin⁡7x7)\sin^6x\cos x=\dfrac{d}{dx}\!\left(\dfrac{\sin^7x}{7}\right), giving ∫02πsin⁡6xcos⁡x dx=[sin⁡7x7]02π=0\displaystyle\int_0^{2\pi}\sin^6x\cos x\,dx=\left[\frac{\sin^7x}{7}\right]_0^{2\pi}=0. So

∫02πsin⁡4xcos⁡3x dx=0−0=0.\int_0^{2\pi}\sin^4x\cos^3x\,dx=0-0=0.

Step 11 (vi). Locate the sign-change point of 5x−35x-3 on [0,1][0,1].

5x−3=05x-3=0 at x=35∈[0,1]x=\tfrac35\in[0,1]; 5x−3<05x-3<0 on [0,35)[0,\tfrac35) and 5x−3>05x-3>0 on (35,1](\tfrac35,1]. By additivity (Property 3),

∫01∣5x−3∣ dx=∫03/5(3−5x) dx+∫3/51(5x−3) dx.\int_0^1|5x-3|\,dx=\int_0^{3/5}(3-5x)\,dx+\int_{3/5}^1(5x-3)\,dx.

Step 12 (vi). Evaluate both pieces.

∫03/5(3−5x) dx=[3x−5x22]03/5=95−910=910.\int_0^{3/5}(3-5x)\,dx=\left[3x-\frac{5x^2}{2}\right]_0^{3/5}=\frac95-\frac{9}{10}=\frac{9}{10}.

∫3/51(5x−3) dx=[5x22−3x]3/51=(52−3)−(910−95)=−12−(−910)=25.\int_{3/5}^1(5x-3)\,dx=\left[\frac{5x^2}{2}-3x\right]_{3/5}^1=\left(\frac52-3\right)-\left(\frac{9}{10}-\frac95\right)=-\frac12-\left(-\frac{9}{10}\right)=\frac{2}{5}.

Adding: ∫01∣5x−3∣ dx=910+25=1310\displaystyle\int_0^1|5x-3|\,dx=\frac{9}{10}+\frac25=\frac{13}{10} (this is exactly the sum of the two triangular areas of the VV-shaped graph — base 35\tfrac35, height 33, plus base 25\tfrac25, height 22).

Step 13 (vii). Differentiate F(x)=∫0sin⁡2xsin⁡−1t dt+∫0cos⁡2xcos⁡−1t dtF(x)=\displaystyle\int_0^{\sin^2x}\sin^{-1}\sqrt t\,dt+\int_0^{\cos^2x}\cos^{-1}\sqrt t\,dt using the First Fundamental Theorem plus the chain rule (on 0≤x≤π/20\le x\le\pi/2, where sin⁡x,cos⁡x≥0\sin x,\cos x\ge0).

F′(x)=sin⁡−1 ⁣sin⁡2x⋅ddx(sin⁡2x)+cos⁡−1 ⁣cos⁡2x⋅ddx(cos⁡2x)=sin⁡−1(sin⁡x)⋅2sin⁡xcos⁡x+cos⁡−1(cos⁡x)⋅(−2sin⁡xcos⁡x).F'(x)=\sin^{-1}\!\sqrt{\sin^2x}\cdot\frac{d}{dx}(\sin^2x)+\cos^{-1}\!\sqrt{\cos^2x}\cdot\frac{d}{dx}(\cos^2x)=\sin^{-1}(\sin x)\cdot2\sin x\cos x+\cos^{-1}(\cos x)\cdot(-2\sin x\cos x).

On [0,π/2][0,\pi/2], sin⁡−1(sin⁡x)=x\sin^{-1}(\sin x)=x and cos⁡−1(cos⁡x)=x\cos^{-1}(\cos x)=x, so

F′(x)=x⋅2sin⁡xcos⁡x−x⋅2sin⁡xcos⁡x=0.F'(x)=x\cdot2\sin x\cos x-x\cdot2\sin x\cos x=0.

Step 14 (vii). FF is constant — evaluate it at the convenient point x=0x=0.

Since F′(x)≡0F'(x)\equiv0 on [0,π/2][0,\pi/2], F(x)=F(0)F(x)=F(0) for every xx in this interval. At x=0x=0: sin⁡2(0)=0\sin^2(0)=0 and cos⁡2(0)=1\cos^2(0)=1, so

F(0)=∫00sin⁡−1t dt+∫01cos⁡−1t dt=0+∫01cos⁡−1t dt.F(0)=\int_0^0\sin^{-1}\sqrt t\,dt+\int_0^1\cos^{-1}\sqrt t\,dt=0+\int_0^1\cos^{-1}\sqrt t\,dt.

Step 15 (vii). Evaluate ∫01cos⁡−1t dt\displaystyle\int_0^1\cos^{-1}\sqrt t\,dt by the substitution t=u2t=u^2.

dt=2u dudt=2u\,du, u:0→1u:0\to1:

∫01cos⁡−1t dt=2∫01ucos⁡−1u du.\int_0^1\cos^{-1}\sqrt t\,dt=2\int_0^1u\cos^{-1}u\,du.

Integrate by parts (p=cos⁡−1u, dq=u dup=\cos^{-1}u,\ dq=u\,du): ∫01ucos⁡−1u du=[u22cos⁡−1u]01+12∫01u21−u2 du=0+12∫01u21−u2 du\displaystyle\int_0^1u\cos^{-1}u\,du=\left[\frac{u^2}{2}\cos^{-1}u\right]_0^1+\frac12\int_0^1\frac{u^2}{\sqrt{1-u^2}}\,du=0+\frac12\int_0^1\frac{u^2}{\sqrt{1-u^2}}\,du (the boundary term vanishes since cos⁡−11=0\cos^{-1}1=0 and the u=0u=0 term is 00). Substituting u=sin⁡θu=\sin\theta: ∫01u21−u2 du=∫0π/2sin⁡2θ dθ=π4\displaystyle\int_0^1\frac{u^2}{\sqrt{1-u^2}}\,du=\int_0^{\pi/2}\sin^2\theta\,d\theta=\frac{\pi}{4}. So ∫01ucos⁡−1u du=π8\displaystyle\int_0^1u\cos^{-1}u\,du=\frac{\pi}{8}, and ∫01cos⁡−1t dt=2⋅π8=π4\displaystyle\int_0^1\cos^{-1}\sqrt t\,dt=2\cdot\frac{\pi}{8}=\frac{\pi}{4}. Hence F(x)≡π4F(x)\equiv\dfrac{\pi}{4} for every x∈[0,π/2]x\in[0,\pi/2] (self-check: repeating the identical computation for ∫01sin⁡−1t dt\int_0^1\sin^{-1}\sqrt t\,dt gives π/4\pi/4 too, so F(π/2)=π/4F(\pi/2)=\pi/4 as well, confirming the constant is consistent at both ends).

Step 16 (viii). Convert to a trig integral via x=tan⁡θx=\tan\theta.

dx=sec⁡2θ dθdx=\sec^2\theta\,d\theta, 1+x2=sec⁡2θ1+x^2=\sec^2\theta; x:0→1⇒θ:0→π/4x:0\to1\Rightarrow\theta:0\to\pi/4. So

I=∫01log⁡(1+x)1+x2 dx=∫0π/4log⁡(1+tan⁡θ) dθ.I=\int_0^1\frac{\log(1+x)}{1+x^2}\,dx=\int_0^{\pi/4}\log(1+\tan\theta)\,d\theta.

Step 17 (viii). Reflect with θ→π/4−θ\theta\to\pi/4-\theta (Property 6) and add.

tan⁡ ⁣(π4−θ)=1−tan⁡θ1+tan⁡θ\tan\!\left(\dfrac{\pi}{4}-\theta\right)=\dfrac{1-\tan\theta}{1+\tan\theta}, so 1+tan⁡ ⁣(π4−θ)=(1+tan⁡θ)+(1−tan⁡θ)1+tan⁡θ=21+tan⁡θ1+\tan\!\left(\dfrac{\pi}{4}-\theta\right)=\dfrac{(1+\tan\theta)+(1-\tan\theta)}{1+\tan\theta}=\dfrac{2}{1+\tan\theta}. Hence

I=∫0π/4log⁡ ⁣(21+tan⁡θ)dθ=∫0π/4log⁡2 dθ−∫0π/4log⁡(1+tan⁡θ) dθ=π4log⁡2−I.I=\int_0^{\pi/4}\log\!\left(\frac{2}{1+\tan\theta}\right)d\theta=\int_0^{\pi/4}\log2\,d\theta-\int_0^{\pi/4}\log(1+\tan\theta)\,d\theta=\frac{\pi}{4}\log2-I.

So 2I=π4log⁡2⇒I=πlog⁡282I=\dfrac{\pi}{4}\log2\Rightarrow I=\dfrac{\pi\log2}{8}.

Step 18 (ix). Reflect I=∫0πxsin⁡x1+sin⁡x dxI=\displaystyle\int_0^\pi\frac{x\sin x}{1+\sin x}\,dx with x→π−xx\to\pi-x (Property 6) and add.

sin⁡(π−x)=sin⁡x\sin(\pi-x)=\sin x, so

I=∫0π(π−x)sin⁡x1+sin⁡x dx=π∫0πsin⁡x1+sin⁡x dx−I  ⟹  2I=π∫0πsin⁡x1+sin⁡x dx.I=\int_0^\pi\frac{(\pi-x)\sin x}{1+\sin x}\,dx=\pi\int_0^\pi\frac{\sin x}{1+\sin x}\,dx-I \implies 2I=\pi\int_0^\pi\frac{\sin x}{1+\sin x}\,dx.

Step 19 (ix). Evaluate K=∫0πsin⁡x1+sin⁡x dx=∫0π[1−11+sin⁡x]dx=π−LK=\displaystyle\int_0^\pi\frac{\sin x}{1+\sin x}\,dx=\int_0^\pi\left[1-\frac{1}{1+\sin x}\right]dx=\pi-L, where L=∫0πdx1+sin⁡xL=\displaystyle\int_0^\pi\frac{dx}{1+\sin x}.

Use the Weierstrass substitution t=tan⁡(x/2)t=\tan(x/2): sin⁡x=2t1+t2\sin x=\dfrac{2t}{1+t^2}, dx=2 dt1+t2dx=\dfrac{2\,dt}{1+t^2}, x:0→π⇒t:0→∞x:0\to\pi\Rightarrow t:0\to\infty (an improper integral, per the Improper Integrals topic). …

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