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9.1 Workshop Solutions 1

True or False? (i) The answer depends on whether we count roots with multiplicity or not. For example, if p⁢(x)=(x-1)2⁢(x2+1)p(x)=(x-1)^{2}(x^{2}+1) then pp has degree 4 and has one real root with multiplicity two. If we only count the number of distinct roots then n=4n=4, s=1s=1 and n-s=3n-s=3 is odd. If we consider p⁢(x)p(x) to have two real roots (which happen to be equal) then n=4n=4, s=2s=2 and n-s=2n-s=2 is even.

In the general case, p⁢(x)=(x-a1)⁢…⁢(x-as)⁢q1⁢(x)⁢…⁢qj⁢(x)p(x)=(x-a_{1})\ldots(x-a_{s})q_{1}(x)\ldots q_{j}(x) as in slide 1.6 in the notes, and n=s+2⁢jn=s+2j so n-sn-s is even.

(ii) False. For example, (x-1)3(x-1)^{3} has degree 3 but only one root (with multiplicity 3).

(iii) True. We complete the square, but first divide through by (-2)(-2) to obtain x2-3⁢x+72x^{2}-3x+\frac{7}{2}, which equals (x-32)2+54(x-\frac{3}{2})^{2}+\frac{5}{4}.

(iv) False. We have 1-x2=cos2⁡t1-x^{2}=\cos^{2}t so 1-x2=cos2⁡t=|cos⁡t|\sqrt{1-x^{2}}=\sqrt{\cos^{2}t}=|\cos t|. For π2≤t≤π\frac{\pi}{2}\leq t\leq\pi, cos⁡t\cos t is negative so |cos⁡t|=-cos⁡t|\cos t|=-\cos t in that range. Therefore 1-x2={cos⁡t0≤t≤π2,-cos⁡tπ2≤t≤π.\sqrt{1-x^{2}}=\left\{\begin{array}[]{cc}\cos t&0\leq t\leq\frac{\pi}{2},\\ -\cos t&\frac{\pi}{2}\leq t\leq\pi.\end{array}\right.

W1.1 i) x-2x+4=x+4-6x+4=1-6x+4\frac{x-2}{x+4}=\frac{x+4-6}{x+4}=1-\frac{6}{x+4}.

ii) x2+xx-3=x⁢(x-3)+4⁢xx-3=x⁢(x-3)+4⁢(x-3)+12x-3=x+4+12x-3\frac{x^{2}+x}{x-3}=\frac{x(x-3)+4x}{x-3}=\frac{x(x-3)+4(x-3)+12}{x-3}=x+4+% \frac{12}{x-3}.

iii) x2-1x2+x+3=x2+x+3-(x+4)x2+x+3=1-x+4x2+x+3\frac{x^{2}-1}{x^{2}+x+3}=\frac{x^{2}+x+3-(x+4)}{x^{2}+x+3}=1-\frac{x+4}{x^{2}% +x+3}.

iv) x3-2⁢x-1x2+2⁢x+2=x⁢(x2+2⁢x+2)-2⁢x2-4⁢x-1x2+2⁢x+2=x+-2⁢(x2+2⁢x+2)+3x2+2⁢x+2=x-2+3x2+2⁢x+2\frac{x^{3}-2x-1}{x^{2}+2x+2}=\frac{x(x^{2}+2x+2)-2x^{2}-4x-1}{x^{2}+2x+2}=x+% \frac{-2(x^{2}+2x+2)+3}{x^{2}+2x+2}=x-2+\frac{3}{x^{2}+2x+2}.

W1.2 i) Here the degree of the numerator is less than the degree of the denominator, so we don’t require a polynomial term. We have x2-x=x⁢(x-1)x^{2}-x=x(x-1), so the required form of partial fractions is Ax+Bx-1\frac{A}{x}+\frac{B}{x-1}. Then

Ax+Bx-1=5⁢x-3x⁢(x-1)⇔A⁢(x-1)+B⁢x=5⁢x-3.\frac{A}{x}+\frac{B}{x-1}=\frac{5x-3}{x(x-1)}\;\Leftrightarrow\;A(x-1)+Bx=5x-3.

In this case we have the easy trick of setting x=1x=1 to determine BB and x=0x=0 to find AA. When x=1x=1 we have B=2B=2, and when x=0x=0 we have -A=-3-A=-3, so A=3A=3.

ii) Once again we don’t require a polynomial term. We factorize x2-x-2=(x-2)⁢(x+1)x^{2}-x-2=(x-2)(x+1) so the required form of partial fractions is Ax-2+Bx+1\frac{A}{x-2}+\frac{B}{x+1}. Then

6⁢x-9x2-x-2=Ax-2+Bx+1⇔A⁢(x+1)+B⁢(x-2)=6⁢x-9⇔A=1,B=5.\frac{6x-9}{x^{2}-x-2}=\frac{A}{x-2}+\frac{B}{x+1}\;\Leftrightarrow\;A(x+1)+B(% x-2)=6x-9\;\Leftrightarrow A=1,B=5.

iii) Again we don’t require a polynomial term. We factorize g⁢(x)=x3+4⁢x2+5⁢x+2g(x)=x^{3}+4x^{2}+5x+2 by looking for roots. We have g⁢(-1)=-1+4-5+2=0g(-1)=-1+4-5+2=0 so g⁢(x)g(x) is divisible by x+1x+1. Now g⁢(x)=(x+1)⁢(x2+3⁢x2+2⁢x)g(x)=(x+1)(x^{2}+3x^{2}+2x). Finally, x2+3⁢x+2⁢x=(x+1)⁢(x+2)x^{2}+3x+2x=(x+1)(x+2) so g⁢(x)=(x+1)2⁢(x+2)g(x)=(x+1)^{2}(x+2). Hence the required form of partial fractions is Ax+1+B(x+1)2+Cx+2\frac{A}{x+1}+\frac{B}{(x+1)^{2}}+\frac{C}{x+2}. Then

x2+5⁢x+5x3+4⁢x2+5⁢x+2=Ax+1+B(x+1)2+Cx+2⇔x2+5⁢x+5=A⁢(x+1)⁢(x+2)+B⁢(x+2)+C⁢(x+1)2.\frac{x^{2}+5x+5}{x^{3}+4x^{2}+5x+2}=\frac{A}{x+1}+\frac{B}{(x+1)^{2}}+\frac{C% }{x+2}\;\Leftrightarrow\;x^{2}+5x+5=A(x+1)(x+2)+B(x+2)+C(x+1)^{2}.

We can carry out the trick of setting x=-1x=-1 and x=-2x=-2 to determine BB and CC, but this won’t be enough to tell us the value of AA. Setting x=-1x=-1 we obtain 1=B1=B, and setting x=-2x=-2 we have -1=C-1=C. Now we can subtract x+2x+2 from the left and right to get x2+4⁢x+3=A⁢(x+1)⁢(x+2)-(x+1)2x^{2}+4x+3=A(x+1)(x+2)-(x+1)^{2}, and then we add (x+1)2(x+1)^{2} to the left and right to get 2⁢x2+6⁢x+4=A⁢(x+1)⁢(x+2)=A⁢(x2+3⁢x+2)2x^{2}+6x+4=A(x+1)(x+2)=A(x^{2}+3x+2), whence A=2A=2. Thus x2+5⁢x+5x3+4⁢x2+5⁢x+2=2x+1+1(x+1)2-1x+2\frac{x^{2}+5x+5}{x^{3}+4x^{2}+5x+2}=\frac{2}{x+1}+\frac{1}{(x+1)^{2}}-\frac{1% }{x+2}.

iv) In this case deg⁡f=1<deg⁡3=3\deg f=1<\deg 3=3, so there is no need to carry out polynomial long division. We first have to factorize the denominator. We observe that g⁢(2)=8-8+8-8=0g(2)=8-8+8-8=0, so g⁢(x)g(x) is divisible by (x-2)(x-2). We have g⁢(x)=(x-2)⁢(x2+4)g(x)=(x-2)(x^{2}+4).

To carry out the partial fractions step, we want to express f⁢(x)/g⁢(x)f(x)/g(x) as Ax-2+B⁢x+Cx2+4\frac{A}{x-2}+\frac{Bx+C}{x^{2}+4}. Multiplying through by g⁢(x)g(x), we have A⁢(x2+4)+(B⁢x+C)⁢(x-2)=2⁢x-20A(x^{2}+4)+(Bx+C)(x-2)=2x-20. We can evaluate at x=2x=2 to obtain 8⁢A=-168A=-16 and hence A=-2A=-2. However, it isn’t a good idea to try to obtain the coefficients B,CB,C by evaluating at ±2⁢i\pm 2{\rm i}. There are two ways of finding B,CB,C. The standard approach is to collect the terms on the left-hand side to obtain: (A+B)⁢x2+(C-2⁢B)⁢x+(4⁢A-2⁢C)=2⁢x-20(A+B)x^{2}+(C-2B)x+(4A-2C)=2x-20. Then A+B=0A+B=0, so B=-A=2B=-A=2, and C-2⁢B=2C-2B=2, so C=2+2⁢B=6C=2+2B=6.

An alternative “trick” method is to substract A⁢(x2+4)A(x^{2}+4) from both sides of the equation to obtain: (B⁢x+C)⁢(x-2)=2⁢x-20+2⁢(x2+4)=2⁢x2+2⁢x-12(Bx+C)(x-2)=2x-20+2(x^{2}+4)=2x^{2}+2x-12. Then 2⁢x2+2⁢x-12=2⁢(x2+x-6)=2⁢(x+3)⁢(x-2)2x^{2}+2x-12=2(x^{2}+x-6)=2(x+3)(x-2) and hence, dividing both sides by (x-2)(x-2), we obtain B⁢x+C=2⁢x+6Bx+C=2x+6.

The answer (by either method) is therefore 2⁢x+6x2+4-2x-2\frac{2x+6}{x^{2}+4}-\frac{2}{x-2}.

v) Here deg⁡f=deg⁡g\deg f=\deg g, so we need to carry out polynomial division before the partial fractions step. We have x3+3⁢x2-x-14=x3+3⁢x2+2⁢x-6-(3⁢x+8)x^{3}+3x^{2}-x-14=x^{3}+3x^{2}+2x-6-(3x+8), so x3+3⁢x2-x-14x3+3⁢x2+2⁢x-6=1-3⁢x+8x3+3⁢x2+2⁢x-6\frac{x^{3}+3x^{2}-x-14}{x^{3}+3x^{2}+2x-6}=1-\frac{3x+8}{x^{3}+3x^{2}+2x-6}. Now we factorize g⁢(x)=x3+3⁢x2+2⁢x-6g(x)=x^{3}+3x^{2}+2x-6. We have g⁢(1)=0g(1)=0 so g⁢(x)g(x) is divisible by (x-1)(x-1). Then g⁢(x)=(x-1)⁢(x2+4⁢x+6)g(x)=(x-1)(x^{2}+4x+6). We now observe that x2+4⁢x+6=(x+2)2+2x^{2}+4x+6=(x+2)^{2}+2 is irreducible. Thus the required form of partial fractions is Ax-1+B⁢x+Cx2+4⁢x+6\frac{A}{x-1}+\frac{Bx+C}{x^{2}+4x+6}. Then

3⁢x+8x3+3⁢x2+2⁢x-6=Ax-1+B⁢x+Cx2+4⁢x+6⇔ 3⁢x+8=A⁢(x2+4⁢x+6)+(B⁢x+C)⁢(x-1).\frac{3x+8}{x^{3}+3x^{2}+2x-6}=\frac{A}{x-1}+\frac{Bx+C}{x^{2}+4x+6}\;% \Leftrightarrow\;3x+8=A(x^{2}+4x+6)+(Bx+C)(x-1).

Now we can carry out the trick of setting x=1x=1 to obtain 11=11⁢A11=11A and hence A=1A=1. Using the standard method (equating coefficients) to find B,CB,C, we have 3⁢x+8=(A+B)⁢x2+(4⁢A+C-B)⁢x+(6⁢A-C)3x+8=(A+B)x^{2}+(4A+C-B)x+(6A-C), and hence A+B=0A+B=0, 4⁢A+C-B=34A+C-B=3 and 6⁢A-C=86A-C=8. Since A=1A=1, we obtain B=-1B=-1 and hence C=3-4⁢A+B=-2C=3-4A+B=-2. With the trick method, we subtract x2+4⁢x+6x^{2}+4x+6 from both sides to obtain -x2-x-2=(B⁢x+C)⁢(x-1)-x^{2}-x-2=(Bx+C)(x-1) and hence, dividing by (x-1)(x-1), we have B⁢x+C=-x-2Bx+C=-x-2.

The answer to the question is therefore 1-1x-1+x+2x2+4⁢x+61-\frac{1}{x-1}+\frac{x+2}{x^{2}+4x+6}.

W1.3 i) We have x+3(x-1)2=x-1+4(x-1)2=1x-1+4(x-1)2\frac{x+3}{(x-1)^{2}}=\frac{x-1+4}{(x-1)^{2}}=\frac{1}{x-1}+\frac{4}{(x-1)^{2}}. Hence the integral is log⁡|x-1|-4x-1+c\log|x-1|-\frac{4}{x-1}+c.

ii) We make the substitution x=3⁢tan⁡tx=3\tan t, so that d⁢xd⁢t=3⁢sec2⁡t\frac{dx}{dt}=3\sec^{2}t, and x2+9=9⁢(1+tan2⁡t)=9⁢sec2⁡tx^{2}+9=9(1+\tan^{2}t)=9\sec^{2}t. So

∫d⁢xx2+9=∫d⁢xd⁢t⁢d⁢t9⁢sec2⁡t=13⁢∫d⁢t=t3+c=13⁢tan-1⁡x3+c.\int\frac{dx}{x^{2}+9}=\int\frac{\frac{dx}{dt}\,dt}{9\sec^{2}t}=\frac{1}{3}% \int\,dt=\frac{t}{3}+c=\frac{1}{3}\tan^{-1}\frac{x}{3}+c.

(Alternatively, we can just remember the fact that ∫d⁢xx2+a2=1a⁢tan-1⁡xa+c\int\frac{dx}{x^{2}+a^{2}}=\frac{1}{a}\tan^{-1}\frac{x}{a}+c.)

iii) We separate the numerator into the xx term and the constant term, so we have to integrate 4⁢xx2+1\frac{4x}{x^{2}+1} and 9x2+1\frac{9}{x^{2}+1} separately. For the first term we make the substitution u=x2+1u=x^{2}+1, so that d⁢ud⁢x=2⁢x\frac{du}{dx}=2x and so we have ∫4⁢x⁢d⁢xx2+1=∫2⁢d⁢uu=2⁢log⁡|u|+c=2⁢log⁡(x2+1)+c\int\frac{4x\,dx}{x^{2}+1}=\int\frac{2\,du}{u}=2\log|u|+c=2\log(x^{2}+1)+c. The second term is 9⁢tan-1⁡x9\tan^{-1}x. (This is more or less standard, or one can make the substitution x=tan⁡tx=\tan t.)

iv) Once again we separate the numerator, so we have to separately integrate xx2+3\frac{x}{x^{2}+3} and 2x2+3\frac{2}{x^{2}+3}. For the first term, we substitute u=x2+3u=x^{2}+3, to obtain ∫x⁢d⁢xx2+3=12⁢log⁡(x2+3)+c\int\frac{x\,dx}{x^{2}+3}=\frac{1}{2}\log(x^{2}+3)+c. For the second term, we substitute x=3⁢tan⁡tx=\sqrt{3}\tan t, or we remember the integral of 1x2+a2\frac{1}{x^{2}+a^{2}} with a=3a=\sqrt{3}. Then we obtain ∫2x2+3=23⁢tan-1⁡x3+c′\int\frac{2}{x^{2}+3}=\frac{2}{\sqrt{3}}\tan^{-1}\frac{x}{\sqrt{3}}+c^{\prime}. Then

∫x+2x2+3⁢d⁢x=12⁢log⁡(x2+3)+23⁢tan-1⁡x3+c.\int\frac{x+2}{x^{2}+3}\,dx=\frac{1}{2}\log(x^{2}+3)+\frac{2}{\sqrt{3}}\tan^{-% 1}\frac{x}{\sqrt{3}}+c.

W1.4 i) By our answer to W1.2(i), we have ∫5⁢x-3x2-x⁢d⁢x=∫3⁢d⁢xx+∫2⁢d⁢xx-1=3⁢log⁡|x|+2⁢log⁡|x-1|+c=log⁡(|x3⁢(x-1)2|)+c\int\frac{5x-3}{x^{2}-x}\,dx=\int\frac{3\,dx}{x}+\int\frac{2\,dx}{x-1}=3\log|x% |+2\log|x-1|+c=\log(|x^{3}(x-1)^{2}|)+c.

ii) Using our answer above, we have ∫6⁢x-9x2-x-2⁢d⁢x=∫d⁢xx-2+∫5⁢d⁢xx+1=log⁡|x-2|+5⁢log⁡|x+1|+c=log⁡|(x-2)⁢(x+1)5|+c\int\frac{6x-9}{x^{2}-x-2}dx=\int\frac{dx}{x-2}+\int\frac{5\,dx}{x+1}=\log|x-2% |+5\log|x+1|+c=\log|(x-2)(x+1)^{5}|+c

iii) We have ∫x2+5⁢x+5x3+4⁢x2+5⁢x+2⁢d⁢x=∫2⁢d⁢xx+1+∫d⁢x(x+1)2-∫d⁢xx+2=2⁢log⁡|x+1|-1x+1-log⁡|x+2|+c=log⁡|(x+1)2x+2|-1x+1+c\int\frac{x^{2}+5x+5}{x^{3}+4x^{2}+5x+2}\,dx=\int\frac{2\,dx}{x+1}+\int\frac{% dx}{(x+1)^{2}}-\int\frac{dx}{x+2}=2\log|x+1|-\frac{1}{x+1}-\log|x+2|+c=\log% \left|\frac{(x+1)^{2}}{x+2}\right|-\frac{1}{x+1}+c.

iv) By our answer to 1.2(iv), we have ∫2⁢x-20x3-2⁢x2+4⁢x-8⁢d⁢x=∫2⁢x+6x2+4⁢d⁢x-2⁢d⁢xx-2\int\frac{2x-20}{x^{3}-2x^{2}+4x-8}\,dx=\int\frac{2x+6}{x^{2}+4}\,dx-\frac{2\,% dx}{x-2}. To integrate 2⁢xx2+4\frac{2x}{x^{2}+4} we substitute u=x2+4u=x^{2}+4, hence d⁢ud⁢x=2⁢x\frac{du}{dx}=2x and so ∫2⁢x⁢d⁢xx2+4=∫d⁢uu=log⁡|u|+c=log⁡(x2+4)+c\int\frac{2x\,dx}{x^{2}+4}=\int\frac{du}{u}=\log|u|+c=\log(x^{2}+4)+c. To integrate 6x2+4\frac{6}{x^{2}+4}, we substitute x=2⁢tan⁡tx=2\tan t, hence d⁢xd⁢t=2⁢sec2⁡t\frac{dx}{dt}=2\sec^{2}t and x2+4=4⁢(tan2⁡t+1)=4⁢sec2⁡tx^{2}+4=4(\tan^{2}t+1)=4\sec^{2}t. Thus ∫6⁢d⁢xx2+4=∫12⁢sec2⁡t⁢d⁢t4⁢sec2⁡t=3⁢∫d⁢t=3⁢t+c′=3⁢tan-1⁡(x2)+c′\int\frac{6\,dx}{x^{2}+4}=\int\frac{12\sec^{2}t\,dt}{4\sec^{2}t}=3\int\,dt=3t+% c^{\prime}=3\tan^{-1}\left(\frac{x}{2}\right)+c^{\prime}. Finally, we can immediately integrate 2x-2\frac{2}{x-2} to obtain 2⁢log⁡|x-2|+c′′2\log|x-2|+c^{\prime\prime}. Summing all of the terms together, we have:

∫2⁢x-20x3-2⁢x2+4⁢x-8⁢d⁢x=log⁡(x2+4)+3⁢tan-1⁡(x2)-2⁢log⁡|x-2|+C.\int\frac{2x-20}{x^{3}-2x^{2}+4x-8}\,dx=\log(x^{2}+4)+3\tan^{-1}\left(\frac{x}% {2}\right)-2\log|x-2|+C.

v) We have ∫x3+3⁢x2-x-14x3+3⁢x2+2⁢x-6⁢d⁢x=∫1⁢d⁢x-∫d⁢xx-1+∫x+2x2+4⁢x+6⁢d⁢x=x-log⁡|x-1|+∫x+2x2+4⁢x+6⁢d⁢x\int\frac{x^{3}+3x^{2}-x-14}{x^{3}+3x^{2}+2x-6}dx=\int 1\,dx-\int\frac{dx}{x-1% }+\int\frac{x+2}{x^{2}+4x+6}\,dx=x-\log|x-1|+\int\frac{x+2}{x^{2}+4x+6}dx. To obtain the final integral, we substitute u=x2+4⁢x+6u=x^{2}+4x+6. Then d⁢ud⁢x=2⁢x+4\frac{du}{dx}=2x+4 and therefore ∫x+2x2+4⁢x+6⁢d⁢x=12⁢∫d⁢uu=log⁡|u|+c\int\frac{x+2}{x^{2}+4x+6}dx=\frac{1}{2}\int\frac{du}{u}=\log|u|+c. Then

∫x3+3⁢x2-x-14x3+3⁢x2+2⁢x-6⁢d⁢x=x-log⁡|x-1|+12⁢log⁡(x2+4⁢x+6)+c=x+12⁢log⁡(x2+4⁢x+6(x-1)2)+c.\int\frac{x^{3}+3x^{2}-x-14}{x^{3}+3x^{2}+2x-6}dx=x-\log|x-1|+\frac{1}{2}\log(% x^{2}+4x+6)+c=x+\frac{1}{2}\log\left(\frac{x^{2}+4x+6}{(x-1)^{2}}\right)+c.

W1.5. i) First we factorize the denominator x3-x2-8⁢x+12x^{3}-x^{2}-8x+12. By considering factors of 1212, we spot 22 as a root, and then proceed to factorize

x3-x2-8⁢x+12=(x-2)⁢(x2+x-6)=(x-2)⁢(x-2)⁢(x+3)=(x-2)2⁢(x+3);{x^{3}-x^{2}-8x+12=(x-2)(x^{2}+x-6)=(x-2)(x-2)(x+3)=(x-2)^{2}(x+3);}

so the partial fractions have the form

2⁢x2+7(x-2)2⁢(x+3)=Ax-2+B(x-2)2+Cx+3=A⁢(x-2)⁢(x+3)+B⁢(x+3)+C⁢(x-2)2(x-2)2⁢(x+3){{2x^{2}+7}\over{(x-2)^{2}(x+3)}}={A\over{x-2}}+{B\over{(x-2)^{2}}}+{C\over{x+% 3}}={{A(x-2)(x+3)+B(x+3)+C(x-2)^{2}}\over{(x-2)^{2}(x+3)}}

and hence

A⁢(x2+x-6)+B⁢(x+3)+C⁢(x2-4⁢x+4)=2⁢x2+7.A(x^{2}+x-6)+B(x+3)+C(x^{2}-4x+4)=2x^{2}+7.

We can find two of these values by setting x=2x=2 and x=-3x=-3: in the former case we obtain 5⁢B=155B=15 so B=3B=3, and in the latter case we obtain 25⁢C=2525C=25 so C=1C=1. To obtain the value of AA we inspect the constant term: -6⁢A+3⁢B+4⁢C=7-6A+3B+4C=7 so -6⁢A=-6-6A=-6 and hence A=1A=1.

Therefore

2⁢x2+7x3-x2-8⁢x+12=1x-2+3(x-2)2+1x+3{{{2x^{2}+7}\over{x^{3}-x^{2}-8x+12}}={{1}\over{x-2}}+{{3}\over{(x-2)^{2}}}+{{% 1}\over{x+3}}}

and the reqired integral is

∫2⁢x2+7x3-x2-8⁢x+12⁢d⁢x=∫1x-2⁢d⁢x+∫3(x-2)2⁢d⁢x+∫1x+3⁢d⁢x\int{{2x^{2}+7}\over{x^{3}-x^{2}-8x+12}}\,dx=\int{{1}\over{x-2}}dx+\int{{3}% \over{(x-2)^{2}}}dx+\int{{1}\over{x+3}}dx
=log⁡|x-2|-3x-2+log⁡|x+3|+K,=\log|x-2|-{{3}\over{x-2}}+\log|x+3|+K,

for some constant KK.

ii) In this exercise we have to carry out all of the steps (a)-(e) in slide 1.25.

a) We first use division of polynomials to express the rational function x3-2x3-x2+4⁢x-4{{x^{3}-2}\over{x^{3}-x^{2}+4x-4}} as a sum of a polynomial and a rational function f⁢(x)g⁢(x)\frac{f(x)}{g(x)} with deg⁡f<deg⁡g\deg f<\deg g. In this case this step is rather easy, we have:

x3-2x3-x2+4⁢x-4=x3-x2+4⁢x-4+(x2-4⁢x+2)x3-x2+4⁢x-4=1+x2-4⁢x+2x3-x2+4⁢x-4.{{x^{3}-2}\over{x^{3}-x^{2}+4x-4}}={{x^{3}-x^{2}+4x-4+(x^{2}-4x+2)}\over{x^{3}% -x^{2}+4x-4}}=1+\frac{x^{2}-4x+2}{x^{3}-x^{2}+4x-4}.

b) Now we factorize the denominator g⁢(x)=x3-x2+4⁢x-4g(x)=x^{3}-x^{2}+4x-4. We spot that 11 is a root, so (x-1)(x-1) divides g⁢(x)g(x); then g⁢(x)=(x-1)⁢(x2+4)g(x)=(x-1)(x^{2}+4).

c) To proceed, we have to express x2-4⁢x+2(x-1)⁢(x2+4)\frac{x^{2}-4x+2}{(x-1)(x^{2}+4)} in the form Ax-1+B⁢x+Cx2+4\frac{A}{x-1}+\frac{Bx+C}{x^{2}+4}. Then we have

x2-4⁢x+2=A⁢(x2+4)+(B⁢x+C)⁢(x-1)⇒(A+B)⁢x2+(C-B)⁢x+(4⁢A-C)=x2-4⁢x+2.x^{2}-4x+2=A(x^{2}+4)+(Bx+C)(x-1)\;\Rightarrow(A+B)x^{2}+(C-B)x+(4A-C)=x^{2}-4% x+2.

We can obtain the value of AA by setting x=1x=1, but this method is not helpful for (directly) obtaining the values of BB and CC. Setting x=1x=1 we have 5⁢A=-15A=-1 and so A=-15A=\frac{-1}{5}. Now A+B=1A+B=1, so B=65B=\frac{6}{5}. Finally, C-B=-4C-B=-4 and so C=B-4=-145C=B-4=\frac{-14}{5}. (It is a good idea to check the linear term: we have 4⁢A-C=-45+145=24A-C=\frac{-4}{5}+\frac{14}{5}=2 as required.) Thus ∫x3-2x3-x2+4⁢x-4⁢d⁢x=∫d⁢x-15⁢∫d⁢xx-1+∫65⁢x-145x2+4⁢d⁢x\int{{x^{3}-2}\over{x^{3}-x^{2}+4x-4}}dx=\int dx-\frac{1}{5}\int\frac{dx}{x-1}% +\int\frac{\frac{6}{5}x-\frac{14}{5}}{x^{2}+4}dx.

d) There is one linear factor (x-1)(x-1), and the integral -15⁢∫d⁢xx-1=-15⁢log⁡|x-1|+c\frac{-1}{5}\int\frac{dx}{x-1}=\frac{-1}{5}\log|x-1|+c.

e) The general method for dealing with integrals such as ∫6⁢x-14x2+4⁢d⁢x\int\frac{6x-14}{x^{2}+4}dx is outlined in slides 1.16-17 and demonstrated in slides 1.21-24. We first account for the linear term (6⁢x6x) in the numerator by considering the substitution u=x2+4u=x^{2}+4, whence d⁢ud⁢x=2⁢x\frac{du}{dx}=2x and so

∫6⁢x⁢d⁢xx2+4=3⁢∫d⁢uu=3⁢log⁡|u|+c′=3⁢log⁡(x2+4)+c′.\int\frac{6x\,dx}{x^{2}+4}=3\int\frac{du}{u}=3\log|u|+c^{\prime}=3\log(x^{2}+4% )+c^{\prime}.

For the term -14x2+4\frac{-14}{x^{2}+4} we make the substitution x=2⁢tan⁡tx=2\tan t (or we remember the standard answer as above) to obtain ∫-14⁢d⁢xx2+4=-7⁢tan-1⁡x2+c′′\int\frac{-14\,dx}{x^{2}+4}=-7\tan^{-1}\frac{x}{2}+c^{\prime\prime}. Putting all of the different bits together, we obtain:

∫x3-2x3+3⁢x2+7⁢x+5⁢d⁢x=x-15⁢log⁡|x-1|+35⁢log⁡(x2+4)-75⁢tan-1⁡(x2)+c.\int{{x^{3}-2}\over{x^{3}+3x^{2}+7x+5}}dx=x-\frac{1}{5}\log|x-1|+\frac{3}{5}% \log(x^{2}+4)-\frac{7}{5}\tan^{-1}\left(\frac{x}{2}\right)+c.

W1.6 i) We observe that the coefficients of the the polynomial are real, so 1-3⁢i1-3{\rm i} is also a root by Lemma 1.5 in the notes; hence

(z-1+3⁢i)⁢(z-1-3⁢i)=(z-1)2+9=z2-2⁢z+10(z-1+3{\rm i})(z-1-3{\rm i})=(z-1)^{2}+9=z^{2}-2z+10

is a factor. We write

z4-6⁢z3+26⁢z2-56⁢z+80=(z2-2⁢z+10)⁢(z2+a⁢z+b)z^{4}-6z^{3}+26z^{2}-56z+80=(z^{2}-2z+10)(z^{2}+az+b)

where a,b∈ℝa,b\in{\mathbb{R}}. Since the constant term 10⁢b=8010b=80, we must have b=8b=8. Now the coefficient of zz is 10⁢a-2⁢b=10⁢a-16=-5610a-2b=10a-16=-56, so a=-4a=-4. Now z2-4⁢z+8=0z^{2}-4z+8=0 has roots

z=4±16-322=2±-4;z={{4\pm\sqrt{16-32}}\over{2}}=2\pm\sqrt{-4};

so a complete list of the roots is

1+3⁢i,1-3⁢i,2+2⁢i,2-2⁢i.1+3{\rm i},1-3{\rm i},2+2{\rm i},2-2{\rm i}.

ii) Since the roots of the polynomials x2-2⁢x+10x^{2}-2x+10 and x2-4⁢x+8x^{2}-4x+8 are not real, they are both irreducible real polynomials, so the required factorization is f⁢(x)=(x2-2⁢x+10)⁢(x2-4⁢x+8)f(x)=(x^{2}-2x+10)(x^{2}-4x+8).

iii) We want to write 26f⁢(x)\frac{26}{f(x)} as

26f⁢(x)=α⁢x+βx2-2⁢x+10+γ⁢x+δx2-4⁢x+8.\frac{26}{f(x)}=\frac{\alpha x+\beta}{x^{2}-2x+10}+\frac{\gamma x+\delta}{x^{2% }-4x+8}.

Multiplying through by f⁢(x)f(x), we obtain:

26=(α⁢x+β)⁢(x2-4⁢x+8)+(γ⁢x+δ)⁢(x2-2⁢x+10)26=(\alpha x+\beta)(x^{2}-4x+8)+(\gamma x+\delta)(x^{2}-2x+10)
=(α+γ)⁢x3+(β+δ-4⁢α-2⁢γ)⁢x2+(8⁢α+10⁢γ-4⁢β-2⁢δ)⁢x+(8⁢β+10⁢δ).=(\alpha+\gamma)x^{3}+(\beta+\delta-4\alpha-2\gamma)x^{2}+(8\alpha+10\gamma-4% \beta-2\delta)x+(8\beta+10\delta).

Thus γ=-α\gamma=-\alpha by looking at the coefficient of x3x^{3}. Substituting -α-\alpha for γ\gamma, the coefficient of x2x^{2} becomes β+δ-2⁢α=0\beta+\delta-2\alpha=0, so δ=2⁢α-β\delta=2\alpha-\beta. Now we substitute into the coefficient of xx and obtain 8⁢α-10⁢α-4⁢β-4⁢α+2⁢β=08\alpha-10\alpha-4\beta-4\alpha+2\beta=0, so -6⁢α-2⁢β=0-6\alpha-2\beta=0. Therefore β=-3⁢α\beta=-3\alpha and δ=5⁢α\delta=5\alpha. Now 8⁢β+10⁢δ=-24⁢α+50⁢α=26⁢α8\beta+10\delta=-24\alpha+50\alpha=26\alpha, so α=1\alpha=1. Thus the required expression is

x-3x2-2⁢x+10+5-xx2-4⁢x+8.\frac{x-3}{x^{2}-2x+10}+\frac{5-x}{x^{2}-4x+8}.

iv) Using the partial fractions from the previous part, we have

∫26f⁢(x)⁢d⁢x=∫x-3x2-2⁢x+10⁢d⁢x+∫5-xx2-4⁢x+8⁢d⁢x.\int\!\frac{26}{f(x)}dx=\int\!\frac{x-3}{x^{2}-2x+10}dx+\int\!\frac{5-x}{x^{2}% -4x+8}dx.

For the first of these integrals, Q⁢(x)=x2-2⁢x+10Q(x)=x^{2}-2x+10 and so we substitute s=x-1s=x-1 to get x-3x2-2⁢x+10=s-2s2+9\frac{x-3}{x^{2}-2x+10}=\frac{s-2}{s^{2}+9}. Clearly d⁢xd⁢s=1\frac{dx}{ds}=1 and so the first integral becomes

∫s-2s2+9⁢d⁢s=12⁢∫s⁢d⁢ss2+9-2⁢d⁢ss2+9=12⁢log⁡(s2+9)-23⁢tan-1⁡s3+c\int\frac{s-2}{s^{2}+9}\,ds=\frac{1}{2}\int\frac{s\,ds}{s^{2}+9}-\frac{2\,ds}{% s^{2}+9}=\frac{1}{2}\log(s^{2}+9)-\frac{2}{3}\tan^{-1}\frac{s}{3}+c

where the last equality follows by making two separate substitutions (u=s2+9u=s^{2}+9 and s=3⁢tan⁡ts=3\tan t respectively). We need to express this in terms of xx: hence we have ∫x-3x2-2⁢x+10⁢d⁢x=12⁢log⁡(x2-2⁢x+10)-23⁢tan-1⁡(x-13)+c\int\frac{x-3}{x^{2}-2x+10}\,dx=\frac{1}{2}\log(x^{2}-2x+10)-\frac{2}{3}\tan^{% -1}\left(\frac{x-1}{3}\right)+c.

For the second integral, we have Q⁢(x)=x2-4⁢x+8Q(x)=x^{2}-4x+8 and so we first make the substitution s=x-2s=x-2. Then Q⁢(x)=s2+4Q(x)=s^{2}+4 and so 5-xx2-4⁢x+8=3-ss2+4\frac{5-x}{x^{2}-4x+8}=\frac{3-s}{s^{2}+4}. Hence we have

∫5-xx2-4⁢x+8⁢d⁢x=∫3⁢d⁢ss2+4-s⁢d⁢ss2+4=32⁢tan-1⁡s2-12⁢log⁡(s2+4)+c′\int\frac{5-x}{x^{2}-4x+8}\,dx=\int\frac{3\,ds}{s^{2}+4}-\frac{s\,ds}{s^{2}+4}% =\frac{3}{2}\tan^{-1}\frac{s}{2}-\frac{1}{2}\log(s^{2}+4)+c^{\prime}

Expressing this in terms of xx and putting everything together, we have

∫26f⁢(x)⁢d⁢x=12⁢log⁡(x2-2⁢x+10)-23⁢tan-1⁡(x-13)-12⁢log⁡(x2-4⁢x+8)+32⁢tan-1⁡(x-22)+c\int\!\frac{26}{f(x)}\,dx=\frac{1}{2}\log(x^{2}-2x+10)-\frac{2}{3}\tan^{-1}% \left(\frac{x-1}{3}\right)-\frac{1}{2}\log(x^{2}-4x+8)+\frac{3}{2}\tan^{-1}% \left(\frac{x-2}{2}\right)+c
=12⁢log⁡(x2-2⁢x+10x2-4⁢x+8)+32⁢tan-1⁡(x-22)-23⁢tan-1⁡(x-13)+c.=\frac{1}{2}\log\left(\frac{x^{2}-2x+10}{x^{2}-4x+8}\right)+\frac{3}{2}\tan^{-% 1}\left(\frac{x-2}{2}\right)-\frac{2}{3}\tan^{-1}\left(\frac{x-1}{3}\right)+c.

W1.7. See frame 1.26 for details on this substitution. We have t=tan⁡x2t=\tan\frac{x}{2} so

d⁢td⁢x=12⁢sec2⁡x2=12⁢(1+tan2⁡x2)=1+t22,\frac{dt}{dx}=\frac{1}{2}\sec^{2}\frac{x}{2}=\frac{1}{2}\left(1+\tan^{2}\frac{% x}{2}\right)=\frac{1+t^{2}}{2},

and cos⁡x=1-t21+t2\cos x=\frac{1-t^{2}}{1+t^{2}}, and the limits change as: t=0t=0 when x=0x=0; t=1t=1 when x=π2x=\frac{\pi}{2}. Thus

∫0π2d⁢x5+4⁢cos⁡x=∫012⁢d⁢t5⁢(1+t2)+4⁢(1-t2)=∫012⁢d⁢t9+t2.\int_{0}^{\frac{\pi}{2}}{{dx}\over{5+4\cos x}}=\int_{0}^{1}{{2dt}\over{5(1+t^{% 2})+4(1-t^{2})}}=\int_{0}^{1}{{2dt}\over{9+t^{2}}}.

To determine the last integral we substitute t=3⁢tan⁡ut=3\tan u so that 9+t2=9+9⁢tan2⁡u=9⁢sec2⁡u9+t^{2}=9+9\tan^{2}u=9\sec^{2}u. Then d⁢td⁢u=3⁢sec2⁡u\frac{dt}{du}=3\sec^{2}u and the limits change as: u=0u=0 when t=0t=0 and u=tan-1⁡(13)u=\tan^{-1}\left(\frac{1}{3}\right) when t=1t=1. Thus

∫012⁢d⁢t9+t2=∫0tan-1⁡(13)6⁢sec2⁡u⁢d⁢u9⁢sec2⁡u=23⁢tan-1⁡(13).\int_{0}^{1}{{2\,dt}\over{9+t^{2}}}=\int_{0}^{\tan^{-1}\left(\frac{1}{3}\right% )}{{6\sec^{2}u\,du}\over{9\sec^{2}u}}={{2}\over{3}}\tan^{-1}\left(\frac{1}{3}% \right).

W1.8. i) (See 1.32 in the notes for this substitution.) We substitute u=2⁢x+3u=2x+3, so that d⁢ud⁢x=2\frac{du}{dx}=2 and hence ∫(2⁢x+3)3/2⁢d⁢x=12⁢∫u3/2⁢d⁢u=12⋅25⁢u5/2+c=15⁢(2⁢x+3)5/2+c\int(2x+3)^{3/2}\,dx=\frac{1}{2}\int u^{3/2}\,du=\frac{1}{2}\cdot\frac{2}{5}u^% {5/2}+c=\frac{1}{5}(2x+3)^{5/2}+c.

ii) (See 1.37 and 1.40 in the notes.) For this case we can either substitute x=2⁢tan⁡tx=2\tan t or x=2⁢sinh⁡tx=2\sinh t. We choose the latter, so we have d⁢xd⁢t=2⁢cosh⁡t\frac{dx}{dt}=2\cosh t and x2+4=4⁢sinh2⁡t+4=4⁢cosh2⁡t=2⁢cosh⁡t\sqrt{x^{2}+4}=\sqrt{4\sinh^{2}t+4}=\sqrt{4\cosh^{2}t}=2\cosh t. (This is true since cosh⁡t\cosh t is always positive.) Now ∫d⁢xx2+4=∫2⁢cosh⁡t⁢d⁢t2⁢cosh⁡t=t+c=sinh-1⁡(x2)+c\int\frac{dx}{\sqrt{x^{2}+4}}=\int\frac{2\cosh t\,dt}{2\cosh t}=t+c=\sinh^{-1}% \left(\frac{x}{2}\right)+c.

iii) (This is a bit of a trick question: we notice that the numerator is of the form f′⁢(x)⁢d⁢xf^{\prime}(x)\,dx, where the denominator is f⁢(x)\sqrt{f(x)}. You should keep your eyes peeled for integrals of this form.) We set u=x2-4u=x^{2}-4, then d⁢ud⁢x=2⁢x\frac{du}{dx}=2x and hence ∫2⁢x⁢d⁢xx2-4=∫u-1/2⁢d⁢u=2⁢u1/2+c=2⁢x2-4+c\int\frac{2x\,dx}{\sqrt{x^{2}-4}}=\int u^{-1/2}{du}=2u^{1/2}+c=2\sqrt{x^{2}-4}+c.

W1.9. (i) Let x=tan⁡ux=\tan u, so that d⁢xd⁢u=sec2⁡u{{dx}\over{du}}=\sec^{2}u and 1+x2=1+tan2⁡u=sec2⁡u1+x^{2}=1+\tan^{2}u=\sec^{2}u. The limits of integration change as

x| 03u| 0π/3\begin{matrix}x&|\quad 0&\sqrt{3}\cr u&|\quad 0&\pi/3\end{matrix}

Hence

∫03d⁢x1+x2=∫0π/3sec2⁡usec2⁡u⁢d⁢u=∫0π/3d⁢u=π/3.{\int_{0}^{\sqrt{3}}{{dx}\over{1+x^{2}}}=\int_{0}^{\pi/3}{{\sec^{2}u}\over{% \sec^{2}u}}du=\int_{0}^{\pi/3}du=\pi/3.}

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

x|1/31u|π/6π/4\begin{matrix}x&|&1/\sqrt{3}&1\cr u&|&\pi/6&\pi/4\end{matrix}

Hence

∫1/31d⁢x(1+x2)2=∫π/6π/4sec2⁡usec4⁡u⁢d⁢u=∫π/6π/4d⁢usec2⁡u=∫π/6π/4cos2⁡u⁢d⁢u\int^{1}_{1/\sqrt{3}}{{dx}\over{(1+x^{2})^{2}}}=\int^{\pi/4}_{\pi/6}{{\sec^{2}% u}\over{\sec^{4}u}}du=\int_{\pi/6}^{\pi/4}{{du}\over{\sec^{2}u}}=\int_{\pi/6}^% {\pi/4}\cos^{2}u\,du
=12∫π/6π/4(cos2u+1)du=12[12sin2u+u]π/6π/4=12(12sinπ2+π4-12sinπ3-π6)={{1}\over{2}}\int_{\pi/6}^{\pi/4}(\cos 2u+1)\,du={{1}\over{2}}\Bigl[{{1}\over% {2}}\sin 2u+u\Bigr]_{\pi/6}^{\pi/4}=\frac{1}{2}\left(\frac{1}{2}\sin\frac{\pi}% {2}+\frac{\pi}{4}-\frac{1}{2}\sin\frac{\pi}{3}-\frac{\pi}{6}\right)
=12(12-34+π12)=2-38+π24.=\frac{1}{2}\left(\frac{1}{2}-\frac{\sqrt{3}}{4}+\frac{\pi}{12}\right)=\frac{2% -\sqrt{3}}{8}+\frac{\pi}{24}.

(iii) In this integral we get rid of x1/2x^{1/2} by making the substitution u=x1/2u=x^{1/2}; that is, x=u2x=u^{2}, so d⁢xd⁢u=2⁢u{{dx}\over{du}}=2u and change the limits to

x|13u|13.\begin{matrix}x&|&1&3\cr u&|&1&\sqrt{3}.\end{matrix}

Then the integral to consider is

∫13d⁢x(1+x)⁢x1/2=∫132⁢u⁢d⁢u(1+u2)⁢u=2⁢∫13d⁢u1+u2=[2⁢tan-1⁡u]13\int_{1}^{3}{{dx}\over{(1+x)x^{1/2}}}=\int_{1}^{\sqrt{3}}{{2u\,du}\over{(1+u^{% 2})u}}=2\int_{1}^{\sqrt{3}}{{du}\over{1+u^{2}}}=\bigl[2\tan^{-1}u\Bigr]_{1}^{% \sqrt{3}}

=2tan-13-2tan-11=2π3-2π4=π6=2\tan^{-1}\sqrt{3}-2\tan^{-1}1=2\frac{\pi}{3}-2\frac{\pi}{4}=\frac{\pi}{6}. Hence

∫13d⁢x(1+x)⁢x1/2=π6.\int_{1}^{3}{{dx}\over{(1+x)x^{1/2}}}={{\pi}\over{6}}.

(iv) To determine this integral we substitute x=2⁢sin⁡tx=2\sin t or x=2⁢cos⁡tx=2\cos t. (Note that either choice gives a useful simplification of the term 4-x2\sqrt{4-x^{2}}.) If we set x=2⁢sin⁡tx=2\sin t then we have d⁢xd⁢t=2⁢cos⁡t\frac{dx}{dt}=2\cos t and 4-x2=4-4⁢sin2⁡t=4⁢cos2⁡t=|2⁢cos⁡t|\sqrt{4-x^{2}}=\sqrt{4-4\sin^{2}t}=\sqrt{4\cos^{2}t}=|2\cos t|. The range of integration is 0≤x≤10\leq x\leq 1, hence 0≤sin⁡t≤120\leq\sin t\leq\frac{1}{2} which corresponds to 0≤t≤π60\leq t\leq\frac{\pi}{6}. Thus ∫01d⁢x4-x2=∫0π/62⁢cos⁡t⁢d⁢t|2⁢cos⁡t|\int_{0}^{1}\frac{dx}{\sqrt{4-x^{2}}}=\int_{0}^{\pi/6}\frac{2\cos t\,dt}{|2% \cos t|}. In this range of values of tt we have 1≥cos⁡t≥321\geq\cos t\geq\frac{\sqrt{3}}{2} and so in particular cos⁡t>0\cos t>0, so |cos⁡t|=cos⁡t|\cos t|=\cos t. Therefore ∫0π/62⁢cos⁡t⁢d⁢t|2⁢cos⁡t|=∫0π/6d⁢t=π/6\int_{0}^{\pi/6}\frac{2\cos t\,dt}{|2\cos t|}=\int_{0}^{\pi/6}dt=\pi/6.

(v) For this part we set x=cosh⁡tx=\cosh t. Then x2-1=cosh2⁡t-1=sinh2⁡tx^{2}-1=\cosh^{2}t-1=\sinh^{2}t. Also, since 1<a<b1<a<b then the region a<x<ba<x<b corresponds to α=cosh-1⁡a<t<cosh-1⁡b=β\alpha=\cosh^{-1}a<t<\cosh^{-1}b=\beta. Now tt is positive throughout this interval, so sinh⁡t\sinh t is positive too and hence x2-1=sinh2⁡t=sinh⁡t\sqrt{x^{2}-1}=\sqrt{\sinh^{2}t}=\sinh t. Finally, d⁢xd⁢t=sinh⁡t\frac{dx}{dt}=\sinh t, so the integral is ∫αβsinh⁡t.sinh⁡t⁢d⁢t=∫αβsinh2⁡t⁢d⁢t\int_{\alpha}^{\beta}\sinh t.\sinh t\,dt=\int_{\alpha}^{\beta}\sinh^{2}t\,dt. To find this integral we use the equality sinh2⁡t=12⁢(cosh⁡2⁢t-1)\sinh^{2}t=\frac{1}{2}(\cosh 2t-1). Thus

∫abx2-1⁢d⁢x=12⁢∫αβ(cosh⁡2⁢t-1)⁢d⁢t=12⁢[12⁢sinh⁡2⁢t-t]αβ=12⁢[sinh⁡t⁢cosh⁡t-t]αβ.\int_{a}^{b}\sqrt{x^{2}-1}\,dx=\frac{1}{2}\int_{\alpha}^{\beta}(\cosh 2t-1)\,% dt=\frac{1}{2}\left[\frac{1}{2}\sinh 2t-t\right]_{\alpha}^{\beta}=\frac{1}{2}% \left[\sinh t\cosh t-t\right]_{\alpha}^{\beta}.

We have cosh⁡α=a\cosh\alpha=a and sinh⁡α=cosh2⁡α-1=a2-1\sinh\alpha=\sqrt{\cosh^{2}\alpha-1}=\sqrt{a^{2}-1}. Similarly, sinh⁡β=b2-1\sinh\beta=\sqrt{b^{2}-1}. Therefore ∫abx2-1⁢d⁢x=12⁢(b⁢b2-1-a⁢a2-1-cosh-1⁡b+cosh-1⁡a)\int_{a}^{b}\sqrt{x^{2}-1}\,dx=\frac{1}{2}(b\sqrt{b^{2}-1}-a\sqrt{a^{2}-1}-% \cosh^{-1}b+\cosh^{-1}a). We can further simplify using the formula cosh-1⁡x=log⁡(x+x2-1)\cosh^{-1}x=\log(x+\sqrt{x^{2}-1}) for x≥1x\geq 1. Therefore

∫abx2-1⁢d⁢x=12⁢(b⁢b2-1-a⁢a2-1-log⁡(b+b2-1a+a2-1)).\int_{a}^{b}\sqrt{x^{2}-1}\,dx=\frac{1}{2}\left(b\sqrt{b^{2}-1}-a\sqrt{a^{2}-1% }-\log\left(\frac{b+\sqrt{b^{2}-1}}{a+\sqrt{a^{2}-1}}\right)\right).

W1.10. We start with the quadratic

x2-4⁢x+8=(x-2)2+4x^{2}-4x+8=(x-2)^{2}+4

and let x-2=2⁢sinh⁡ux-2=2\sinh u so that d⁢xd⁢u=2⁢cosh⁡u{{dx}\over{du}}=2\cosh u and

x2-4⁢x+8=4⁢(1+sinh2⁡u)=4⁢cosh2⁡u;x^{2}-4x+8=4(1+\sinh^{2}u)=4\cosh^{2}u;

further, the limits change

x|02u|log⁡(2-1)0,\begin{matrix}x&|&0&2\cr u&|&\log(\sqrt{2}-1)&0,\cr\end{matrix}

since -2=2⁢sinh⁡u-2=2\sinh u implies that -2=eu-e-u-2=e^{u}-e^{-u} or e2⁢u+2⁢eu=1e^{2u}+2e^{u}=1, hence that eu+1=2,e^{u}+1=\sqrt{2}, so u=log⁡(2-1)u=\log(\sqrt{2}-1).

This we substitute into the integral and obtain

∫02d⁢x(x2-4⁢x+8)1/2=∫log⁡(2-1)02⁢cosh⁡u2⁢cosh⁡u⁢d⁢u=∫log⁡(2-1)0d⁢u=-log⁡(2-1)=log⁡(1+2){\int_{0}^{2}{{dx}\over{(x^{2}-4x+8)^{1/2}}}=\int_{\log(\sqrt{2}-1)}^{0}{{2% \cosh u}\over{2\cosh u}}du=\int_{\log(\sqrt{2}-1)}^{0}du=-\log(\sqrt{2}-1)=% \log(1+\sqrt{2})}

where the last equality holds because 12-1=2+12-1=2+1\frac{1}{\sqrt{2}-1}=\frac{\sqrt{2}+1}{2-1}=\sqrt{2}+1.