MATH101 Calculus Workshop Exercise 5 Solutions

W5.1. (i) The indefinite integral is

∫(5⁢x4+2⁢x-1/2+4x-6x4)⁢d⁢x=x5+4⁢x1/2+4⁢log⁡|x|+2⁢x-3+C.\int\bigl(5x^{4}+2x^{-1/2}+{{4}\over{x}}-{{6}\over{x^{4}}}\bigr)dx=x^{5}+4x^{1% /2}+4\log|x|+2x^{-3}+C.

(ii) Likewise we integrate each summand and obtain

∫(e1-3⁢x+5⁢x+7)⁢d⁢x=-13⁢e1-3⁢x+215⁢(5⁢x+7)3/2+C.\int\bigl(e^{1-3x}+\sqrt{5x+7}\bigr)dx={{-1}\over{3}}e^{1-3x}+{{2}\over{15}}(5% x+7)^{3/2}+C.

W5.2. The definite integrals are

(i) ∫01(1-x)5/2⁢d⁢x=[-27⁢(1-x)7/2]01=27;(i)\quad\int_{0}^{1}(1-x)^{5/2}\,dx=\Bigl[-{{2}\over{7}}(1-x)^{7/2}\Bigr]_{0}^% {1}={{2}\over{7}};
(i⁢i) ∫π/4π/3cosec2⁢x⁢d⁢x=[-cot⁡x]π/4π/3=cot⁡π/4-cot⁡π/3=1-1/3,\eqalignno{(ii)\quad\int_{\pi/4}^{\pi/3}{\hbox{cosec}}^{2}x\,dx&=\Bigl[-\cot x% \Bigr]_{\pi/4}^{\pi/3}\cr&=\cot\pi/4-\cot\pi/3\cr&=1-1/\sqrt{3},\cr}

where the integral (ii) is similar to example in lectures.


W5.3. (i) We have

dd⁢x⁢(sec⁡x+tan⁡x)=dd⁢x⁢(1cos⁡x+sin⁡xcos⁡x)=sin⁡xcos2⁡x+1cos2⁡x=sec⁡x⁢tan⁡x+sec2⁡x;\eqalignno{{{d}\over{dx}}\bigl(\sec x+\tan x\bigr)&={{d}\over{dx}}\Bigl({{1}% \over{\cos x}}+{{\sin x}\over{\cos x}}\Bigr)\cr&={{\sin x}\over{\cos^{2}x}}+{{% 1}\over{\cos^{2}x}}\cr&=\sec x\tan x+\sec^{2}x;\cr}

hence we have

dd⁢x⁢log⁡|sec⁡x+tan⁡x|=sec⁡x⁢tan⁡x+sec2⁡xsec⁡x+tan⁡x=sec⁡x.\eqalignno{{{d}\over{dx}}\log\bigl|\sec x+\tan x\bigr|&={{\sec x\tan x+\sec^{2% }x}\over{\sec x+\tan x}}\cr&=\sec x.\cr}

(ii) By the Fundamental Theorem of Calculus and (i), we have

∫sec⁡x⁢d⁢x=log⁡|sec⁡x+tan⁡x|+C.\int\sec x\,dx=\log\bigl|\sec x+\tan x\bigr|+C.

W5.4. (i) We have

∫0πcos2⁡t⁢d⁢t=12⁢∫0π(1+cos⁡2⁢t)⁢d⁢t=12⁢[t+12⁢sin⁡2⁢t]0π=12⁢[π+12⁢sin⁡2⁢π]-12⁢[0]=π2.\eqalignno{\int_{0}^{\pi}\cos^{2}t\,dt&={{1}\over{2}}\int_{0}^{\pi}(1+\cos 2t)% \,dt\cr&={{1}\over{2}}\bigl[t+{{1}\over{2}}\sin 2t\bigr]_{0}^{\pi}\cr&={{1}% \over{2}}\bigl[\pi+{{1}\over{2}}\sin 2\pi\bigr]-{{1}\over{2}}\bigl[0\bigr]\cr&% ={{\pi}\over{2}}.\cr}

(ii) We use the addition formulæ and obtain

∫0π/2cos⁡t⁢cos⁡2⁢t⁢d⁢t=12⁢∫0π/2(cos⁡t+cos⁡3⁢t)⁢d⁢t=12⁢[sin⁡t+13⁢sin⁡3⁢t]0π/2=12⁢[sin⁡π2+13⁢sin⁡3⁢π2]-12⁢[0]=12⁢[1-13]=13.\eqalignno{\int_{0}^{\pi/2}\cos t\cos 2t\,dt&={{1}\over{2}}\int_{0}^{\pi/2}(% \cos t+\cos 3t)\,dt\cr&={{1}\over{2}}\bigl[\sin t+{{1}\over{3}}\sin 3t\bigr]_{% 0}^{\pi/2}\cr&={{1}\over{2}}\bigl[\sin{{\pi}\over{2}}+{{1}\over{3}}\sin{{3\pi}% \over{2}}\bigr]-{{1}\over{2}}\bigl[0\bigr]\cr&={{1}\over{2}}\bigl[1-{{1}\over{% 3}}\bigr]\cr&={{1}\over{3}}.\cr}

W5.5 (i) Integrating twice by parts, we have

I=∫x2⁢sin⁡x⁢d⁢x=-x2⁢cos⁡x+∫2⁢x⁢cos⁡x⁢d⁢x=-x2⁢cos⁡x+2⁢x⁢sin⁡x-∫2⁢sin⁡x⁢d⁢x=-x2⁢cos⁡x+2⁢x⁢sin⁡x+2⁢cos⁡x+C.\eqalignno{I&=\int x^{2}\sin x\,dx\cr&=-x^{2}\cos x+\int 2x\cos x\,dx\cr&=-x^{% 2}\cos x+2x\sin x-\int 2\sin x\,dx\cr&=-x^{2}\cos x+2x\sin x+2\cos x+C.\cr}

(ii) Likewise, we have

J=∫x2⁢log⁡x⁢d⁢x=(1/3)⁢x3⁢log⁡x-∫(1/3)⁢x3⁢(1/x)⁢d⁢x=(1/3)⁢x3⁢log⁡x-∫(1/3)⁢x2⁢d⁢x=(1/3)⁢x3⁢log⁡x-(1/9)⁢x3+C.\eqalignno{J&=\int x^{2}\log x\,dx\cr&=(1/3)x^{3}\log x-\int(1/3)x^{3}(1/x)\,% dx\cr&=(1/3)x^{3}\log x-\int(1/3)x^{2}\,dx\cr&=(1/3)x^{3}\log x-(1/9)x^{3}+C.\cr}

W5.6 (i) Integrating twice by parts, we have

I=∫x2⁢cosh⁡x⁢d⁢x=x2⁢sinh⁡x-∫2⁢x⁢sinh⁡x⁢d⁢x=x2⁢sinh⁡x-2⁢x⁢cosh⁡x+∫2⁢cosh⁡x⁢d⁢x=x2⁢sinh⁡x-2⁢x⁢cosh⁡x+2⁢sinh⁡x+C.\eqalignno{I&=\int x^{2}\cosh x\,dx\cr&=x^{2}\sinh x-\int 2x\sinh x\,dx\cr&=x^% {2}\sinh x-2x\cosh x+\int 2\cosh x\,dx\cr&=x^{2}\sinh x-2x\cosh x+2\sinh x+C.\cr}

(ii) Using a hyperbolic identity, we obtain

∫cosh2⁡x⁢d⁢x=12⁢∫(cosh⁡2⁢x+1)⁢d⁢x=14⁢sinh⁡2⁢x+x2+C.\eqalignno{\int\cosh^{2}x\,dx&={{1}\over{2}}\int(\cosh 2x+1)\,dx\cr&={{1}\over% {4}}\sinh 2x+{{x}\over{2}}+C.\cr}

W5.7 Let

In=∫0π/2sinn⁡x⁢d⁢x.I_{n}=\int_{0}^{\pi/2}\sin^{n}xdx.

(i) In particular we have

I0=∫0π/2sin0⁡x⁢d⁢x=∫0π/21⁢d⁢x=π2,I_{0}=\int_{0}^{\pi/2}\sin^{0}x\,dx=\int_{0}^{\pi/2}1dx={{\pi}\over{2}},
I1=∫0π/2sin⁡x⁢d⁢x=[-cos⁡x]0π/2=cos⁡0-cos⁡π/2=1.I_{1}=\int_{0}^{\pi/2}\sin x\,dx=\bigl[-\cos x\bigr]_{0}^{\pi/2}=\cos 0-\cos{% \pi/2}=1.

(ii) We integrate by parts to get, for n>1n>1,

In=∫0π/2sin⁡x⁢sinn-1⁡x⁢d⁢x=[-cos⁡x⁢sinn-1⁡x]0π/2+(n-1)⁢∫0π/2cos2⁡x⁢sinn-2⁡x⁢d⁢x\eqalign{I_{n}&=\int_{0}^{\pi/2}\sin x\sin^{n-1}x\,dx\cr&=\bigl[-\cos x\sin^{n% -1}x\bigr]_{0}^{\pi/2}+(n-1)\int_{0}^{\pi/2}\cos^{2}x\sin^{n-2}x\,dx\cr}

since dd⁢x⁢sinn-1⁡x=(n-1)⁢sinn-2⁡x⁢cos⁡x.{{d}\over{dx}}\sin^{n-1}x=(n-1)\sin^{n-2}x\cos x. We observe that sinn-1⁡0=0\sin^{n-1}0=0 for n>1n>1, and that cos2⁡x=1-sin2⁡x;\cos^{2}x=1-\sin^{2}x; hence

In=(n-1)⁢∫0π/2sinn-2⁡x⁢d⁢x-(n-1)⁢∫0π/2sinn⁡x⁢d⁢x=(n-1)⁢In-2-(n-1)⁢In,\eqalign{I_{n}&=(n-1)\int_{0}^{\pi/2}\sin^{n-2}x\,dx-(n-1)\int_{0}^{\pi/2}\sin% ^{n}x\,dx\cr&=(n-1)I_{n-2}-(n-1)I_{n},\cr}

and we rearrange this to obtain the reduction formula

In=n-1n⁢In.I_{n}={{n-1}\over{n}}I_{n}.

By this reduction formula and the results of (i), we have

I4=34I2=3.14.2I0=3.14.2π2=3⁢π16,I5=45I3=4.25.3I1=815.\eqalign{I_{4}&={{3}\over{4}}I_{2}={{3.1}\over{4.2}}I_{0}={{3.1}\over{4.2}}{{% \pi}\over{2}}={{3\pi}\over{16}},\cr I_{5}&={{4}\over{5}}I_{3}={{4.2}\over{5.3}% }I_{1}={{8}\over{15}}.\cr}

please try to write this nicely


W5.8. (i) Now

dd⁢x⁢sinn⁡x=n⁢sinn-1⁡x⁢cos⁡x,{{d}\over{dx}}\sin^{n}x=n\sin^{n-1}x\cos x,

so

d2d⁢x2⁢sinn⁡x=n⁢(n-1)⁢sinn-2⁡x⁢cos2⁡x-n⁢sinn⁡x=n⁢(n-1)⁢sinn-2⁡x⁢(1-sin2⁡x)-n⁢sinn⁡x=n⁢(n-1)⁢sinn-2⁡x-n2⁢sinn⁡x.\eqalign{{{d^{2}}\over{dx^{2}}}\sin^{n}x&=n(n-1)\sin^{n-2}x\cos^{2}x-n\sin^{n}% x\cr&=n(n-1)\sin^{n-2}x(1-\sin^{2}x)-n\sin^{n}x\cr&=n(n-1)\sin^{n-2}x-n^{2}% \sin^{n}x.\cr}

(ii) We integrate by parts and obtain

In=∫0πex⁢sinn⁡x⁢d⁢x=[ex⁢sinn⁡x]0π-n⁢∫0πex⁢sinn-1⁡x⁢cos⁡x⁢d⁢x.\eqalign{I_{n}&=\int_{0}^{\pi}e^{x}\sin^{n}x\,dx\cr&=\bigl[e^{x}\sin^{n}x\bigr% ]_{0}^{\pi}-n\int_{0}^{\pi}e^{x}\sin^{n-1}x\cos x\,dx.\cr}

so, when we integrate by parts again, we obtain

In=[ex⁢sinn⁡x-n⁢ex⁢sinn-1⁡x⁢cos⁡x]0π+n⁢∫0πex⁢((n-1)⁢sinn-2⁡x-n⁢sinn⁡x)⁢d⁢xIn=n⁢(n-1)⁢In-2-n2⁢In;\eqalign{I_{n}&=\bigl[e^{x}\sin^{n}x-ne^{x}\sin^{n-1}x\cos x\bigr]_{0}^{\pi}+n% \int_{0}^{\pi}e^{x}\bigl((n-1)\sin^{n-2}x-n\sin^{n}x\bigr)dx\cr I_{n}&=n(n-1)I% _{n-2}-n^{2}I_{n};\cr}

hence we have the recurrence relation

In=n⁢(n-1)n2+1In-2  (n>1).I_{n}={{n(n-1)}\over{n^{2}+1}}I_{n-2}\qquad(n>1).

Starting from the result for I1I_{1} in lectures, we deduce

I1=12⁢(eπ+1),I3=3.29+1I1=310(eπ+1),I5=5.425+1I3=313(eπ+1),I7=7.649+1I5=63325(eπ+1).\eqalign{I_{1}&={{1}\over{2}}{(e^{\pi}+1)},\cr I_{3}&={{3.2}\over{9+1}}I_{1}={% {3}\over{10}}({{e^{\pi}+1}}),\cr I_{5}&={{5.4}\over{25+1}}I_{3}={{3}\over{13}}% (e^{\pi}+1),\cr I_{7}&={{7.6}\over{49+1}}I_{5}={{63}\over{325}}(e^{\pi}+1).\cr}

W5.9. (i) Observe that (1+x2)′=2⁢x(1+x^{2})^{\prime}=2x, hence

∫2⁢x1+x2⁢d⁢x=log⁡(1+x2)+C.\int{{2x}\over{1+x^{2}}}dx=\log(1+x^{2})+C.

Alternatively, let u=1+x2u=1+x^{2}, so d⁢ud⁢x=2⁢x{{du}\over{dx}}=2x, and substitute to get

∫2⁢x⁢d⁢x1+x2=∫d⁢uu=log⁡|u|+C=log⁡(1+x2)+C.\eqalign{\int{{2xdx}\over{1+x^{2}}}&=\int{{du}\over{u}}\cr&=\log|u|+C\cr&=\log% (1+x^{2})+C.\cr}

(ii) Observe that dd⁢x⁢(x2+6⁢x+100)=2⁢x+6{{d}\over{dx}}(x^{2}+6x+100)=2x+6, so we let u=x2+6⁢x+100u=x^{2}+6x+100 and then d⁢u/d⁢x=2⁢x+6du/dx=2x+6, so

∫(x+3)⁢d⁢xx2+6⁢x+100=12⁢∫d⁢uu=12⁢log⁡|u|+C=12⁢log⁡(x2+6⁢x+100)+C.\eqalignno{\int{{(x+3)dx}\over{x^{2}+6x+100}}&={{1}\over{2}}\int{{du}\over{u}}% \cr&={{1}\over{2}}\log|u|+C\cr&={{1}\over{2}}\log(x^{2}+6x+100)+C.\cr}

W5.10. (i) By partial fractions, we have

∫2⁢x+3(x+1)⁢(x+2)⁢d⁢x=∫(1x+1+1x+2)⁢d⁢x=log⁡|x+1|+log⁡|x+2|+C.\eqalign{\int{{2x+3}\over{(x+1)(x+2)}}dx&=\int\Bigl({{1}\over{x+1}}+{{1}\over{% x+2}}\Bigr)dx\cr&=\log|x+1|+\log|x+2|+C.\cr}

(ii) The partial fractions here give

∫x(x-1)2=∫x-1+1(x-1)2⁢d⁢x=∫d⁢xx-1⁢d⁢x+∫d⁢x(x-1)2=log⁡|x-1|-1x-1+C.\eqalign{\int{{x}\over{(x-1)^{2}}}&=\int{{x-1+1}\over{(x-1)^{2}}}dx\cr&=\int{{% dx}\over{x-1}}dx+\int{{dx}\over{(x-1)^{2}}}\cr&=\log|x-1|-{{1}\over{x-1}}+C.\cr}

W5.11. Let u=sin2⁡tu=\sin^{2}t so that d⁢ud⁢t=2⁢cos⁡t⁢sin⁡t{{du}\over{dt}}=2\cos t\sin t and 1-u=1-sin2⁡t=cos2⁡t.1-u=1-\sin^{2}t=\cos^{2}t. Then

u|01t|0π/2\matrix{u&|&0&1\cr t&|&0&\pi/2\cr}

and so we obtain by substituting

Jk=∫01(1-u)k/2⁢u-1/2⁢d⁢u=2⁢∫0π/2cosk⁡t⁢(sin⁡t)-1⁢cos⁡t⁢sin⁡t⁢d⁢t=2∫0π/2cosk+1tdt=2Ik+1,\eqalign{J_{k}&=\int_{0}^{1}(1-u)^{k/2}u^{-1/2}\,du\cr&=2\int_{0}^{\pi/2}\cos^% {k}t(\sin t)^{-1}\cos t\sin t\,dt\cr&=2\int_{0}^{\pi/2}\cos^{k+1}t\,dt=2I_{k+1% },\cr}

where we recall the notation of lectures. In particular,

J3=2⁢I4=3⁢π8.J_{3}=2I_{4}={{3\pi}\over{8}}.

W5.12. (i) Let x=3⁢tan⁡ux=3\tan u, so that d⁢xd⁢u=3⁢sec2⁡u{{dx}\over{du}}=3\sec^{2}u and 9+x2=9⁢(1+tan2⁡u)=9⁢sec2⁡u9+x^{2}=9(1+\tan^{2}u)=9\sec^{2}u. The limits of integration change as

x| 3  →∞u| π/6  (π/2)-,\eqalign{x&|\quad\sqrt{3}\qquad\rightarrow\infty\cr u&|\quad\pi/6\qquad(\pi/2)% -,\cr}

Hence

∫3∞d⁢x9+x2=∫π/6π/2-3⁢sec2⁡u32⁢sec2⁡u⁢d⁢u=13⁢∫π/6π/2-d⁢u=π/9.\eqalign{\int_{\sqrt{3}}^{\infty}{{dx}\over{9+x^{2}}}&=\int_{\pi/6}^{\pi/2-}{{% 3\sec^{2}u}\over{3^{2}\sec^{2}u}}du\cr&={{1}\over{3}}\int_{\pi/6}^{\pi/2-}du% \cr&=\pi/9.\cr}

(ii) In this integral we let x=3⁢tan⁡ux=3\tan u, so that d⁢xd⁢u=3⁢sec2⁡u{{dx}\over{du}}=3\sec^{2}u and 9+x2=9⁢(1+tan2⁡u)=9⁢sec2⁡u9+x^{2}=9(1+\tan^{2}u)=9\sec^{2}u as before. The limits of integration change as

x| 0  →∞u| 0  (π/2)-,\eqalign{x&|\quad 0\qquad\rightarrow\infty\cr u&|\quad 0\qquad(\pi/2)-,\cr}

Hence

∫0∞d⁢x(9+x2)2=∫0π/2-3⁢sec2⁡u92⁢sec4⁡u⁢d⁢u=127⁢∫0π/2-cos2⁡u⁢d⁢u=12×27⁢∫0π/2-(1+cos⁡2⁢u)⁢d⁢u=12×27⁢[u+12⁢sin⁡2⁢u]0π/2-=12×27⁢[π2+12⁢sin⁡π]-12×27⁢[0]=π108.\eqalign{\int_{0}^{\infty}{{dx}\over{(9+x^{2})^{2}}}&=\int_{0}^{\pi/2-}{{3\sec% ^{2}u}\over{9^{2}\sec^{4}u}}du\cr&={{1}\over{27}}\int_{0}^{\pi/2-}\cos^{2}u\,% du\cr&={{1}\over{2\times 27}}\int_{0}^{\pi/2-}(1+\cos 2u)du\cr&={{1}\over{2% \times 27}}\Bigl[u+{{1}\over{2}}\sin 2u\Bigr]_{0}^{\pi/2-}\cr&={{1}\over{2% \times 27}}\Bigl[{{\pi}\over{2}}+{{1}\over{2}}\sin\pi\Bigr]-{{1}\over{2\times 2% 7}}\Bigl[0\Bigr]\cr&={{\pi}\over{108}}.}

W5.13. (i) We make the substitution u=x2+4⁢x+5u=x^{2}+4x+5, so d⁢u/d⁢x=2⁢x+4du/dx=2x+4 and find the integral

J1=∫2⁢x+4x2+4⁢x+5⁢d⁢x=∫d⁢uu=log⁡|u|+C=log⁡(x2+4⁢x+5)+C.\eqalignno{J_{1}&=\int{{2x+4}\over{x^{2}+4x+5}}dx\cr&=\int{{du}\over{u}}\cr&=% \log|u|+C\cr&=\log(x^{2}+4x+5)+C.\cr}

(ii) In the integral

J2=∫d⁢x(x+2)2+1J_{2}=\int{{dx}\over{(x+2)^{2}+1}}

we substitute x+2=tan⁡tx+2=\tan t, so d⁢x/d⁢t=sec2⁡tdx/dt=\sec^{2}t and (x+2)2+1=tan2⁡t+1=sec2⁡t(x+2)^{2}+1=\tan^{2}t+1=\sec^{2}t; hence

J2=∫d⁢x(x+2)2+1=∫sec2⁡t⁢d⁢tsec2⁡t=∫d⁢t=t+C=tan-1⁡(x+2)+C.\eqalignno{J_{2}&=\int{{dx}\over{(x+2)^{2}+1}}\cr&=\int{{\sec^{2}tdt}\over{% \sec^{2}t}}\cr&=\int dt\cr&=t+C\cr&=\tan^{-1}(x+2)+C.\cr}

(iii) Now we look for constants AA and BB such that

∫x⁢d⁢xx2+4⁢x+5=A⁢∫2⁢x+4x2+4⁢x+5+B⁢∫d⁢xx2+4⁢x+5\int{{xdx}\over{x^{2}+4x+5}}=A\int{{2x+4}\over{x^{2}+4x+5}}+B\int{{dx}\over{x^% {2}+4x+5}}

and then

x=A⁢(2⁢x+4)+Bx=A(2x+4)+B

so A=1/2A=1/2 and B=-2B=-2; hence

∫x⁢d⁢xx2+4⁢x+5=12⁢log⁡(x2+4⁢x+5)-2⁢tan-1⁡(x+2)+C.\int{{xdx}\over{x^{2}+4x+5}}={{1}\over{2}}\log(x^{2}+4x+5)-2\tan^{-1}(x+2)+C.

W5.14. The difference of squares identity gives (1-x)⁢(1+x)=1-x2(1-x)(1+x)=1-x^{2}, so

∫1+x1-x⁢d⁢x=∫1+x1-x2⁢d⁢x=∫d⁢x1-x2+∫x⁢d⁢x1-x2=sin-1⁡x-1-x2+C,\eqalignno{\int{{\sqrt{1+x}}\over{\sqrt{1-x}}}dx&=\int{{1+x}\over{\sqrt{1-x^{2% }}}}dx\cr&=\int{{dx}\over{\sqrt{1-x^{2}}}}+\int{{xdx}\over{\sqrt{1-x^{2}}}}\cr% &=\sin^{-1}x-\sqrt{1-x^{2}}+C,\cr}

where the final integral is given by guesswork or by using the substitution u=1-x2u=1-x^{2}.