Integral Calculus 201-SN3-RE • CEGEP, Montreal

Corrected exercises: antiderivatives and the indefinite integral (201-SN3-RE)

This is the corrected exercise set on the indefinite integral and antiderivatives for Integral Calculus, 201-SN3-RE (formerly 201-NYB), the opening chapter of the course. Part A lays the foundations: the definition of an antiderivative and the inverse relation with differentiation, the reason two antiderivatives differ only by a constant, the table of basic formulas and its single gap at n=−1n=-1, the algebraic properties together with the two false rules that almost every student invents at the start of the semester, the antiderivative of ∣x∣|x| and ln⁡∣x∣\ln|x| on two disjoint intervals (exercise 4), and the three forms to recognize, f′f\frac{f'}{f}, f′fnf'f^{n} and f′eff'e^{f} (exercise 5). Part B moves up to exam level with substitution: the direct reflex, the cases where the derivative is missing a constant factor, the substitutions that require back-substitution, and the physics problem where the antiderivative is no longer a formula but a position. It ends with antiderivatives that are not elementary, such as that of e−x2e^{-x^{2}} (exercise 9), and with the method of undetermined coefficients, which guesses the form of the antiderivative and then adjusts it (exercise 10).

Exercises 0.1 and 0.2 open the set with twenty-two antiderivatives to compute directly, as in textbook drill lists. First twelve with the table of basic antiderivatives and linearity: negative and fractional powers such as 1x23\frac{1}{\sqrt[3]{x^{2}}}, a quotient to split, (x2+1)2\left(x^{2}+1\right)^{2} to expand, e2xe^{2x} and 4x4^{x}, cos⁡(3x)\cos(3x), tan⁡2x\tan^{2}x and the inverse sine. Then ten by direct substitution: a linear argument, the forms u′unu'u^{n}, u′u\frac{u'}{u} and u′euu'e^{u}, sin⁡4xcos⁡x\sin^{4}x\cos x, ln⁡xx\frac{\sqrt{\ln x}}{x} and tan⁡(2x)\tan(2x). Each one asks for the value of an antiderivative at a given point, checked as you type it.

Part C goes through the classics: exponentials and logarithms in a base other than ee (exercise 11), a function recovered from its second derivative and a tangent line (exercise 12), five antiderivatives from a test paper to validate by differentiating them (exercise 13), the deflection of a cantilever beam (exercise 14) and the sales of a game launched by word of mouth (exercise 15).

It is written for CEGEP students in the Science program (Sciences de la nature) taking Integral Calculus.

The common thread of the chapter fits in one sentence: integrating is differentiating backwards. Every antiderivative can therefore be checked by differentiating it, in ten seconds, and that check catches most exam mistakes. A student who gets into the habit of differentiating the answer never again loses marks on a forgotten constant or a misplaced chain rule factor.

17 corrected exercises • 170 points • 225 minutes

This chapter is part of 201-SN3-RE, every chapter with its set and sheet Before you start Revision sheet: the traps and the method for this chapter

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Course recap

  • • Definition: FF is an antiderivative of ff on an interval if F′(x)=f(x)F'(x)=f(x) for every xx in that interval. We write ∫f(x)dx=F(x)+C\int f(x)dx=F(x)+C: the indefinite integral is the FAMILY of all antiderivatives.
  • • Two antiderivatives of the same function differ by a constant: if F′=G′F'=G' on an interval, then (F−G)′=0(F-G)'=0, so F−GF-G is constant. This theorem is what justifies the +C+C, and it requires an INTERVAL.
  • • Basic formulas: ∫xndx=xn+1n+1+C\int x^{n}dx=\frac{x^{n+1}}{n+1}+C for n≠−1n\neq -1; ∫dxx=ln⁡∣x∣+C\int\frac{dx}{x}=\ln|x|+C; ∫exdx=ex+C\int e^{x}dx=e^{x}+C; ∫axdx=axln⁡a+C\int a^{x}dx=\frac{a^{x}}{\ln a}+C; ∫cos⁡x dx=sin⁡x+C\int\cos x\,dx=\sin x+C; ∫sin⁡x dx=−cos⁡x+C\int\sin x\,dx=-\cos x+C; ∫sec⁡2x dx=tan⁡x+C\int\sec^{2}x\,dx=\tan x+C.
  • • Inverse trigonometric formulas: ∫dx1+x2=arctan⁡x+C\int\frac{dx}{1+x^{2}}=\arctan x+C and ∫dx1−x2=arcsin⁡x+C\int\frac{dx}{\sqrt{1-x^{2}}}=\arcsin x+C. They are read off the table of derivatives taken backwards.
  • • Linearity (the ONLY algebraic property): ∫(af(x)+bg(x))dx=a∫f(x)dx+b∫g(x)dx\int\left(af(x)+bg(x)\right)dx=a\int f(x)dx+b\int g(x)dx. There is NO product rule and NO quotient rule for integrals.
  • • Substitution: if g′(x)g'(x) appears as a factor, setting u=g(x)u=g(x) gives ∫f(g(x))g′(x)dx=∫f(u)du\int f(g(x))g'(x)dx=\int f(u)du. Always return to the variable xx at the end of an indefinite integral.
  • • The universal check: DIFFERENTIATING the answer must give back the integrand. It costs nothing, it is quick, and it makes the chapter almost foolproof.

Calculations: antiderivatives to compute with the table

Exercise 0.1: Integrate with the table: twelve direct calculations

For each function ff, find the general antiderivative using the table of basic antiderivatives and linearity, then the antiderivative FF that equals zero at the first point given, and give its value at the second point. Exact value, or to three decimal places if it involves ee, π\pi or a logarithm.

One method for all twelve rows: first REWRITE the integrand as a sum of terms from the table, roots as fractional powers, fractions as negative powers, a quotient split term by term over the monomial, a product expanded. Then integrate term by term, dividing by the NEW exponent or by the coefficient kk of the argument. Finally, the condition F(a)=0F(a)=0 fixes the constant, which amounts to computing G(b)−G(a)G(b)-G(a) for any antiderivative GG.

  • a) f(x)=4x3−6x2+2x−5f(x)=4x^{3}-6x^{2}+2x-5, with F(0)=0F(0)=0: give F(2)F(2).
  • b) f(x)=8x3−3x2f(x)=\frac{8}{x^{3}}-\frac{3}{x^{2}}, with F(1)=0F(1)=0: give F(2)F(2).
  • c) f(x)=x3+1x23f(x)=\sqrt[3]{x}+\frac{1}{\sqrt[3]{x^{2}}}, with F(1)=0F(1)=0: give F(8)F(8).
  • d) f(x)=3x4−x+2x3f(x)=\frac{3x^{4}-x+2}{x^{3}}, with F(1)=0F(1)=0: give F(2)F(2).
  • e) f(x)=(x2+1)2f(x)=\left(x^{2}+1\right)^{2}, with F(0)=0F(0)=0: give F(1)F(1).
  • f) f(x)=4e2x−e−x/2f(x)=4e^{2x}-e^{-x/2}, with F(0)=0F(0)=0: give F(ln⁡4)F(\ln 4).
  • g) f(x)=4x+(12)xf(x)=4^{x}+\left(\frac{1}{2}\right)^{x}, with F(0)=0F(0)=0: give F(1)F(1).
  • h) f(x)=cos⁡(3x)−2sin⁡(x2)f(x)=\cos(3x)-2\sin\left(\frac{x}{2}\right), with F(0)=0F(0)=0: give F(π)F(\pi).
  • i) f(x)=tan⁡2x+41+x2f(x)=\tan^{2}x+\frac{4}{1+x^{2}}, with F(0)=0F(0)=0: give F(1)F(1).
  • j) f(x)=1−1−x21−x2f(x)=\frac{1-\sqrt{1-x^{2}}}{\sqrt{1-x^{2}}}, with F(0)=0F(0)=0: give F(12)F\left(\frac{1}{2}\right).
  • k) f(x)=(x+1)2xf(x)=\frac{(x+1)^{2}}{x}, with F(1)=0F(1)=0: give F(e)F(e).
  • l) f(x)=1+xcos⁡x+xexxf(x)=\frac{1+x\cos x+xe^{x}}{x}, with F(1)=0F(1)=0: give F(2)F(2).

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Answers

  • a) F(x)=x4−2x3+x2−5xF(x)=x^{4}-2x^{3}+x^{2}-5x; F(2)=−6F(2)=-6
  • b) F(x)=−4x2+3x+1F(x)=-\frac{4}{x^{2}}+\frac{3}{x}+1; F(2)=32F(2)=\frac{3}{2}
  • c) F(x)=34x43+3x13−154F(x)=\frac{3}{4}x^{\frac{4}{3}}+3x^{\frac{1}{3}}-\frac{15}{4}; F(8)=574=14.25F(8)=\frac{57}{4}=14.25
  • d) F(x)=32x2+1x−1x2−32F(x)=\frac{3}{2}x^{2}+\frac{1}{x}-\frac{1}{x^{2}}-\frac{3}{2}; F(2)=194=4.75F(2)=\frac{19}{4}=4.75
  • e) F(x)=x55+2x33+xF(x)=\frac{x^{5}}{5}+\frac{2x^{3}}{3}+x; F(1)=2815≈1.867F(1)=\frac{28}{15}\approx 1.867
  • f) F(x)=2e2x+2e−x/2−4F(x)=2e^{2x}+2e^{-x/2}-4; F(ln⁡4)=29F(\ln 4)=29
  • g) F(x)=4x2ln⁡2−(1/2)xln⁡2+12ln⁡2F(x)=\frac{4^{x}}{2\ln 2}-\frac{(1/2)^{x}}{\ln 2}+\frac{1}{2\ln 2}; F(1)=2ln⁡2≈2.885F(1)=\frac{2}{\ln 2}\approx 2.885
  • h) F(x)=sin⁡(3x)3+4cos⁡(x2)−4F(x)=\frac{\sin(3x)}{3}+4\cos\left(\frac{x}{2}\right)-4; F(π)=−4F(\pi)=-4
  • i) F(x)=tan⁡x−x+4arctan⁡xF(x)=\tan x-x+4\arctan x; F(1)=tan⁡1−1+π≈3.699F(1)=\tan 1-1+\pi\approx 3.699
  • j) F(x)=arcsin⁡x−xF(x)=\arcsin x-x; F(12)=π6−12≈0.0236F\left(\frac{1}{2}\right)=\frac{\pi}{6}-\frac{1}{2}\approx 0.0236
  • k) F(x)=x22+2x+ln⁡∣x∣−52F(x)=\frac{x^{2}}{2}+2x+\ln|x|-\frac{5}{2}; F(e)=e22+2e−32≈7.631F(e)=\frac{e^{2}}{2}+2e-\frac{3}{2}\approx 7.631
  • l) F(x)=ln⁡∣x∣+sin⁡x+ex−sin⁡1−eF(x)=\ln|x|+\sin x+e^{x}-\sin 1-e; F(2)≈5.432F(2)\approx 5.432

The move that decides everything happens BEFORE you integrate: rewrite. The table knows neither roots, nor fractions, nor products, nor quotients; it knows xnx^{n}, ekxe^{kx}, axa^{x}, sin⁡\sin, cos⁡\cos, sec⁡2\sec^{2}, 1x\frac{1}{x}, 11+x2\frac{1}{1+x^{2}} and 11−x2\frac{1}{\sqrt{1-x^{2}}}. Once the sum is written, linearity does the rest, and there is NO product rule and NO quotient rule for antiderivatives.

a)

F(x)=x4−2x3+x2−5x+CF(x)=x^{4}-2x^{3}+x^{2}-5x+C, and F(0)=0F(0)=0 gives C=0C=0. So F(2)=16−16+4−10=−6F(2)=16-16+4-10=-6. Pitfall: forgetting to divide by the new exponent, 4x3↦4x44x^{3}\mapsto 4x^{4} instead of x4x^{4}.

b)

f(x)=8x−3−3x−2f(x)=8x^{-3}-3x^{-2}, so F(x)=8x−2−2−3x−1−1+C=−4x2+3x+CF(x)=\frac{8x^{-2}}{-2}-\frac{3x^{-1}}{-1}+C=-\frac{4}{x^{2}}+\frac{3}{x}+C. F(1)=−4+3+C=0F(1)=-4+3+C=0 gives C=1C=1, and F(2)=−1+32+1=32F(2)=-1+\frac{3}{2}+1=\frac{3}{2}. Pitfall: the exponent goes UP, x−3x^{-3} becomes x−2−2\frac{x^{-2}}{-2} and not x−4−4\frac{x^{-4}}{-4}.

c)

f(x)=x13+x−23f(x)=x^{\frac{1}{3}}+x^{-\frac{2}{3}}, so F(x)=34x43+3x13+CF(x)=\frac{3}{4}x^{\frac{4}{3}}+3x^{\frac{1}{3}}+C. F(1)=34+3+C=0F(1)=\frac{3}{4}+3+C=0 gives C=−154C=-\frac{15}{4}, and F(8)=34×16+3×2−154=18−154=574=14.25F(8)=\frac{3}{4}\times 16+3\times 2-\frac{15}{4}=18-\frac{15}{4}=\frac{57}{4}=14.25. Pitfall: 1x23=x−23\frac{1}{\sqrt[3]{x^{2}}}=x^{-\frac{2}{3}}, whose antiderivative x1/31/3\frac{x^{1/3}}{1/3} carries a coefficient 33.

d)

Split over the monomial: f(x)=3x−x−2+2x−3f(x)=3x-x^{-2}+2x^{-3}, so F(x)=32x2+1x−1x2+CF(x)=\frac{3}{2}x^{2}+\frac{1}{x}-\frac{1}{x^{2}}+C. F(1)=32+1−1+C=0F(1)=\frac{3}{2}+1-1+C=0 gives C=−32C=-\frac{3}{2}, and F(2)=6+12−14−32=194=4.75F(2)=6+\frac{1}{2}-\frac{1}{4}-\frac{3}{2}=\frac{19}{4}=4.75. Pitfall: integrating the numerator and the denominator separately, a “quotient rule” that does not exist.

e)

Expand: (x2+1)2=x4+2x2+1\left(x^{2}+1\right)^{2}=x^{4}+2x^{2}+1, so F(x)=x55+2x33+x+CF(x)=\frac{x^{5}}{5}+\frac{2x^{3}}{3}+x+C with C=0C=0, and F(1)=15+23+1=2815≈1.867F(1)=\frac{1}{5}+\frac{2}{3}+1=\frac{28}{15}\approx 1.867. Pitfall: answering (x2+1)33\frac{\left(x^{2}+1\right)^{3}}{3}, whose derivative is 2x(x2+1)22x\left(x^{2}+1\right)^{2}: the factor 2x2x is missing, so it is not an antiderivative.

f)

∫ekxdx=ekxk+C\int e^{kx}dx=\frac{e^{kx}}{k}+C, with k=2k=2 then k=−12k=-\frac{1}{2}: F(x)=2e2x+2e−x/2+CF(x)=2e^{2x}+2e^{-x/2}+C. F(0)=2+2+C=0F(0)=2+2+C=0 gives C=−4C=-4. At ln⁡4\ln 4: e2ln⁡4=16e^{2\ln 4}=16 and e−ln⁡42=12e^{-\frac{\ln 4}{2}}=\frac{1}{2}, so F(ln⁡4)=32+1−4=29F(\ln 4)=32+1-4=29. Pitfall: dividing by −12-\frac{1}{2} multiplies by −2-2, and the minus sign in front of e−x/2e^{-x/2} becomes a plus.

g)

∫axdx=axln⁡a+C\int a^{x}dx=\frac{a^{x}}{\ln a}+C, with ln⁡4=2ln⁡2\ln 4=2\ln 2 and ln⁡12=−ln⁡2\ln\frac{1}{2}=-\ln 2: F(x)=4x2ln⁡2−(12)xln⁡2+CF(x)=\frac{4^{x}}{2\ln 2}-\frac{\left(\frac{1}{2}\right)^{x}}{\ln 2}+C. So F(1)=4−12ln⁡2−12−1ln⁡2=32ln⁡2+12ln⁡2=2ln⁡2≈2.885F(1)=\frac{4-1}{2\ln 2}-\frac{\frac{1}{2}-1}{\ln 2}=\frac{3}{2\ln 2}+\frac{1}{2\ln 2}=\frac{2}{\ln 2}\approx 2.885. Pitfall: 4x+1x+1\frac{4^{x+1}}{x+1}, the power rule applied to an exponential.

h)

F(x)=sin⁡(3x)3+4cos⁡(x2)+CF(x)=\frac{\sin(3x)}{3}+4\cos\left(\frac{x}{2}\right)+C, since ∫sin⁡(kx)dx=−cos⁡(kx)k\int\sin(kx)dx=-\frac{\cos(kx)}{k} and dividing by k=12k=\frac{1}{2} multiplies by 22. F(0)=0+4+C=0F(0)=0+4+C=0 gives C=−4C=-4, and F(π)=sin⁡3π3+4cos⁡π2−4=−4F(\pi)=\frac{\sin 3\pi}{3}+4\cos\frac{\pi}{2}-4=-4. Pitfall: the sign, −2sin⁡(x2)-2\sin\left(\frac{x}{2}\right) integrates to +4cos⁡(x2)+4\cos\left(\frac{x}{2}\right).

i)

tan⁡2x\tan^{2}x is not in the table, but tan⁡2x=sec⁡2x−1\tan^{2}x=\sec^{2}x-1 is. So F(x)=tan⁡x−x+4arctan⁡x+CF(x)=\tan x-x+4\arctan x+C with C=0C=0, and F(1)=tan⁡1−1+4×π4=tan⁡1−1+π≈3.699F(1)=\tan 1-1+4\times\frac{\pi}{4}=\tan 1-1+\pi\approx 3.699. Pitfall: tan⁡3x3\frac{\tan^{3}x}{3}, whose derivative is tan⁡2xsec⁡2x\tan^{2}x\sec^{2}x.

j)

Split: f(x)=11−x2−1f(x)=\frac{1}{\sqrt{1-x^{2}}}-1, so F(x)=arcsin⁡x−x+CF(x)=\arcsin x-x+C with C=0C=0, and F(12)=π6−12≈0.0236F\left(\frac{1}{2}\right)=\frac{\pi}{6}-\frac{1}{2}\approx 0.0236. Pitfall: arcsin⁡12=π6\arcsin\frac{1}{2}=\frac{\pi}{6} in radians, not 3030.

k)

Expand, then split: x2+2x+1x=x+2+1x\frac{x^{2}+2x+1}{x}=x+2+\frac{1}{x}, so F(x)=x22+2x+ln⁡∣x∣+CF(x)=\frac{x^{2}}{2}+2x+\ln|x|+C. F(1)=12+2+0+C=0F(1)=\frac{1}{2}+2+0+C=0 gives C=−52C=-\frac{5}{2}, and F(e)=e22+2e+1−52=e22+2e−32≈7.631F(e)=\frac{e^{2}}{2}+2e+1-\frac{5}{2}=\frac{e^{2}}{2}+2e-\frac{3}{2}\approx 7.631. Pitfall: 1x=x−1\frac{1}{x}=x^{-1} is the gap in the power rule, its antiderivative is ln⁡∣x∣\ln|x|.

l)

Split over xx: f(x)=1x+cos⁡x+exf(x)=\frac{1}{x}+\cos x+e^{x}, three families from the table. F(x)=ln⁡∣x∣+sin⁡x+ex+CF(x)=\ln|x|+\sin x+e^{x}+C, F(1)=sin⁡1+e+C=0F(1)=\sin 1+e+C=0, so F(2)=ln⁡2+sin⁡2+e2−sin⁡1−e≈5.432F(2)=\ln 2+\sin 2+e^{2}-\sin 1-e\approx 5.432, calculator in radians.

Check: DIFFERENTIATE each antiderivative you find and you must land back on ff, in ten seconds per row; this check is what catches the forgotten factor 1k\frac{1}{k} and the sign of the sines. For the value, check that F(a)=0F(a)=0 at the starting point, then recompute F(b)F(b) on the calculator.

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Calculations: antiderivatives to compute by substitution

Exercise 0.2: Integrate by direct substitution: ten direct calculations

For each function ff, find an antiderivative by substitution, writing out uu and dudu, then the antiderivative FF that equals zero at the first point given, and give its value at the second point. Exact value, or to three decimal places if it involves ee or a logarithm.

One method for all ten rows: spot the INNER function uu whose derivative is present up to a constant factor; write du=u′(x) dxdu=u'(x)\,dx and adjust the constant; integrate in uu with the table; return to xx. The value asked for is then computed as G(b)−G(a)G(b)-G(a), where GG is the antiderivative found.

  • a) f(x)=(3x−2)4f(x)=(3x-2)^{4}, with F(1)=0F(1)=0: give F(2)F(2).
  • b) f(x)=12x+1f(x)=\frac{1}{\sqrt{2x+1}}, with F(0)=0F(0)=0: give F(4)F(4).
  • c) f(x)=(2x+1)(x2+x+1)3f(x)=(2x+1)\left(x^{2}+x+1\right)^{3}, with F(0)=0F(0)=0: give F(1)F(1).
  • d) f(x)=4x3−2x4−2x+3f(x)=\frac{4x^{3}-2}{x^{4}-2x+3}, with F(0)=0F(0)=0: give F(2)F(2).
  • e) f(x)=(x+1) ex2+2xf(x)=(x+1)\,e^{x^{2}+2x}, with F(0)=0F(0)=0: give F(1)F(1).
  • f) f(x)=sin⁡4xcos⁡xf(x)=\sin^{4}x\cos x, with F(0)=0F(0)=0: give F(π2)F\left(\frac{\pi}{2}\right).
  • g) f(x)=ln⁡xxf(x)=\frac{\sqrt{\ln x}}{x}, with F(1)=0F(1)=0: give F(e4)F(e^{4}).
  • h) f(x)=ex(1+ex)2f(x)=\frac{e^{x}}{\left(1+e^{x}\right)^{2}}, with F(0)=0F(0)=0: give F(ln⁡3)F(\ln 3).
  • i) f(x)=tan⁡(2x)f(x)=\tan(2x), with F(0)=0F(0)=0: give F(π6)F\left(\frac{\pi}{6}\right).
  • j) f(x)=6x(x2+1)3f(x)=\frac{6x}{\left(x^{2}+1\right)^{3}}, with F(0)=0F(0)=0: give F(1)F(1).

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  • a) (3x−2)515\frac{(3x-2)^{5}}{15}; F(2)=102315=68.2F(2)=\frac{1023}{15}=68.2
  • b) 2x+1\sqrt{2x+1}; F(4)=2F(4)=2
  • c) (x2+x+1)44\frac{\left(x^{2}+x+1\right)^{4}}{4}; F(1)=20F(1)=20
  • d) ln⁡∣x4−2x+3∣\ln\left|x^{4}-2x+3\right|; F(2)=ln⁡5≈1.609F(2)=\ln 5\approx 1.609
  • e) 12ex2+2x\frac{1}{2}e^{x^{2}+2x}; F(1)=e3−12≈9.543F(1)=\frac{e^{3}-1}{2}\approx 9.543
  • f) sin⁡5x5\frac{\sin^{5}x}{5}; F(π2)=15F\left(\frac{\pi}{2}\right)=\frac{1}{5}
  • g) 23(ln⁡x)32\frac{2}{3}(\ln x)^{\frac{3}{2}}; F(e4)=163≈5.333F(e^{4})=\frac{16}{3}\approx 5.333
  • h) −11+ex-\frac{1}{1+e^{x}}; F(ln⁡3)=14F(\ln 3)=\frac{1}{4}
  • i) −12ln⁡∣cos⁡(2x)∣-\frac{1}{2}\ln\left|\cos(2x)\right|; F(π6)=ln⁡22≈0.347F\left(\frac{\pi}{6}\right)=\frac{\ln 2}{2}\approx 0.347
  • j) −32(x2+1)2-\frac{3}{2\left(x^{2}+1\right)^{2}}; F(1)=98=1.125F(1)=\frac{9}{8}=1.125

The move that decides everything: find uu by looking for its DERIVATIVE in the integrand. A 2x+12x+1 next to x2+x+1x^{2}+x+1, a 1x\frac{1}{x} next to ln⁡x\ln x, a cos⁡x\cos x next to sin⁡x\sin x: when the derivative is there, up to a constant, the substitution works; when a factor in xx is missing, it does not, and a constant can never be added to make up for an xx.

a)

u=3x−2u=3x-2, du=3 dxdu=3\,dx: ∫(3x−2)4dx=13∫u4du=(3x−2)515+C\int(3x-2)^{4}dx=\frac{1}{3}\int u^{4}du=\frac{(3x-2)^{5}}{15}+C. So F(2)=45−1515=102315=68.2F(2)=\frac{4^{5}-1^{5}}{15}=\frac{1023}{15}=68.2. Pitfall: forgetting the 13\frac{1}{3} and answering (3x−2)55\frac{(3x-2)^{5}}{5}, three times too large.

b)

u=2x+1u=2x+1, du=2 dxdu=2\,dx: ∫(2x+1)−12dx=12⋅u1212=2x+1+C\int(2x+1)^{-\frac{1}{2}}dx=\frac{1}{2}\cdot\frac{u^{\frac{1}{2}}}{\frac{1}{2}}=\sqrt{2x+1}+C. So F(4)=9−1=2F(4)=\sqrt{9}-\sqrt{1}=2. The 12\frac{1}{2} from dudu and the 12\frac{1}{2} from the exponent cancel exactly.

c)

u=x2+x+1u=x^{2}+x+1, du=(2x+1) dxdu=(2x+1)\,dx, present as is: ∫u3du=(x2+x+1)44+C\int u^{3}du=\frac{\left(x^{2}+x+1\right)^{4}}{4}+C. At 00, u=1u=1; at 11, u=3u=3. So F(1)=81−14=20F(1)=\frac{81-1}{4}=20.

d)

The form u′u\frac{u'}{u}: u=x4−2x+3u=x^{4}-2x+3, du=(4x3−2) dxdu=(4x^{3}-2)\,dx, and ∫duu=ln⁡∣u∣+C\int\frac{du}{u}=\ln|u|+C. Here u>0u>0 on [0,2][0, 2] (its minimum, at x=0.53x=\sqrt[3]{0.5}, is about 1.811.81). At 00, u=3u=3; at 22, u=15u=15. So F(2)=ln⁡15−ln⁡3=ln⁡5≈1.609F(2)=\ln 15-\ln 3=\ln 5\approx 1.609. Pitfall: u′u\frac{u'}{u} integrates to ln⁡∣u∣\ln|u|, not to u22\frac{u^{2}}{2} nor to ln⁡∣u′∣\ln|u'|.

e)

The form u′euu'e^{u} with u=x2+2xu=x^{2}+2x, du=(2x+2) dx=2(x+1) dxdu=(2x+2)\,dx=2(x+1)\,dx: a factor 22 is missing, a constant, which we adjust. ∫(x+1)ex2+2xdx=12ex2+2x+C\int(x+1)e^{x^{2}+2x}dx=\frac{1}{2}e^{x^{2}+2x}+C. So F(1)=e3−e02=e3−12≈9.543F(1)=\frac{e^{3}-e^{0}}{2}=\frac{e^{3}-1}{2}\approx 9.543.

f)

u=sin⁡xu=\sin x, du=cos⁡x dxdu=\cos x\,dx: ∫u4du=sin⁡5x5+C\int u^{4}du=\frac{\sin^{5}x}{5}+C. So F(π2)=1−05=15F\left(\frac{\pi}{2}\right)=\frac{1-0}{5}=\frac{1}{5}. Pitfall: taking u=cos⁡xu=\cos x; its derivative −sin⁡x-\sin x only appears to the power 44, not on its own.

g)

u=ln⁡xu=\ln x, du=dxxdu=\frac{dx}{x}: ∫u12du=23(ln⁡x)32+C\int u^{\frac{1}{2}}du=\frac{2}{3}(\ln x)^{\frac{3}{2}}+C. At 11, u=0u=0; at e4e^{4}, u=4u=4. So F(e4)=23×432=23×8=163≈5.333F(e^{4})=\frac{2}{3}\times 4^{\frac{3}{2}}=\frac{2}{3}\times 8=\frac{16}{3}\approx 5.333.

h)

u=1+exu=1+e^{x}, du=exdxdu=e^{x}dx: ∫u−2du=−1u=−11+ex+C\int u^{-2}du=-\frac{1}{u}=-\frac{1}{1+e^{x}}+C. At 00, u=2u=2; at ln⁡3\ln 3, u=4u=4. So F(ln⁡3)=−14+12=14F(\ln 3)=-\frac{1}{4}+\frac{1}{2}=\frac{1}{4}. Pitfall: seeing a u′u\frac{u'}{u} form and writing a logarithm; the square in the denominator makes it a power u−2u^{-2}.

i)

tan⁡(2x)=sin⁡(2x)cos⁡(2x)\tan(2x)=\frac{\sin(2x)}{\cos(2x)}: u=cos⁡(2x)u=\cos(2x), du=−2sin⁡(2x) dxdu=-2\sin(2x)\,dx, so ∫tan⁡(2x) dx=−12ln⁡∣cos⁡(2x)∣+C\int\tan(2x)\,dx=-\frac{1}{2}\ln\left|\cos(2x)\right|+C. At 00, cos⁡0=1\cos 0=1; at π6\frac{\pi}{6}, cos⁡π3=12\cos\frac{\pi}{3}=\frac{1}{2}. So F(π6)=−12ln⁡12=ln⁡22≈0.347F\left(\frac{\pi}{6}\right)=-\frac{1}{2}\ln\frac{1}{2}=\frac{\ln 2}{2}\approx 0.347. Pitfall: two constants at once, the −1-1 from the derivative of cosine and the 22 from the argument.

j)

u=x2+1u=x^{2}+1, du=2x dxdu=2x\,dx, so 6x dx=3 du6x\,dx=3\,du: ∫3u−3du=−32u2=−32(x2+1)2+C\int 3u^{-3}du=-\frac{3}{2u^{2}}=-\frac{3}{2\left(x^{2}+1\right)^{2}}+C. At 00, u=1u=1; at 11, u=2u=2. So F(1)=−38+32=98=1.125F(1)=-\frac{3}{8}+\frac{3}{2}=\frac{9}{8}=1.125.

Check: differentiate the antiderivative you found with the chain rule, and you must get exactly ff back, constant factor included; if a factor 33, 12\frac{1}{2} or −1-1 is missing, the adjustment of dudu is wrong.

Part A: The antiderivative, the table and the forms to recognize (/50)

Exercise 1: What is an antiderivative?

The figure shows three antiderivatives of f(x)=2xf(x)=2x: the parabolas x2x^{2}, x2+2x^{2}+2 and x2−2x^{2}-2. Each one is obtained from another by a vertical translation, and that is exactly what the constant of integration says.

-3-2-1123-4-3-2-11234567x² + 2x²x² − 2
  • a) State the definition of an antiderivative, then check that F(x)=xsin⁡x+cos⁡xF(x)=x\sin x+\cos x is an antiderivative of f(x)=xcos⁡xf(x)=x\cos x.
  • b) Show that F(x)=sin⁡2xF(x)=\sin^{2}x and G(x)=−cos⁡2xG(x)=-\cos^{2}x are both antiderivatives of sin⁡2x\sin 2x. Is this a contradiction? Which theorem settles the question?
  • c) Find the antiderivative FF of f(x)=3x2−4x+1f(x)=3x^{2}-4x+1 that satisfies F(2)=5F(2)=5. How many such antiderivatives are there?
  • d) Using the figure: why do the three curves have the same slope at every xx-value, and why does exactly one antiderivative pass through a given point of the plane?

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  • a) F′(x)=xcos⁡xF'(x)=x\cos x: FF is indeed an antiderivative
  • b) F−G=1F-G=1: two antiderivatives differ by a constant, on an interval
  • c) F(x)=x3−2x2+x+3F(x)=x^{3}-2x^{2}+x+3, and only one
  • d) Vertical translates: parallel tangent lines, one curve through each point
a)

Definition: FF is an antiderivative of ff on an interval II if FF is differentiable on II and F′(x)=f(x)F'(x)=f(x) for every x∈Ix\in I. Check: F′(x)=(xsin⁡x)′+(cos⁡x)′=(sin⁡x+xcos⁡x)−sin⁡x=xcos⁡x=f(x)F'(x)=\left(x\sin x\right)'+\left(\cos x\right)'=(\sin x+x\cos x)-\sin x=x\cos x=f(x) ✓. The two sin⁡x\sin x terms cancel, and that is the whole point of the form given. Note that we are not LOOKING for the antiderivative here, we are CHECKING it: checking is always easier than finding, which is why every integration answer can be verified by differentiation.

b)

F′(x)=2sin⁡xcos⁡x=sin⁡2xF'(x)=2\sin x\cos x=\sin 2x ✓ and G′(x)=−2cos⁡x⋅(−sin⁡x)=2sin⁡xcos⁡x=sin⁡2xG'(x)=-2\cos x\cdot(-\sin x)=2\sin x\cos x=\sin 2x ✓. No contradiction: F(x)−G(x)=sin⁡2x+cos⁡2x=1F(x)-G(x)=\sin^{2}x+\cos^{2}x=1, a CONSTANT. The theorem that settles the question: if two functions have the same derivative on an interval, their difference is constant there (a consequence of the mean value theorem, since (F−G)′=0(F-G)'=0). Two antiderivatives of the same function can therefore differ only by a constant, and that is precisely what the +C+C encodes. Watch the INTERVAL hypothesis: on a domain in two pieces, such as that of 1x\frac{1}{x}, the “constant” can take one value to the left of zero and another to the right.

c)

F(x)=x3−2x2+x+CF(x)=x^{3}-2x^{2}+x+C. The condition F(2)=5F(2)=5 gives 8−8+2+C=58-8+2+C=5, so C=3C=3 and F(x)=x3−2x2+x+3F(x)=x^{3}-2x^{2}+x+3. There is exactly ONE: the initial condition selects a single member of the infinite family. This is the central mechanism of differential equations later in the semester: integration provides the family, the initial condition picks out the solution.

d)

The three curves are vertical translates of one another: going from x2x^{2} to x2+2x^{2}+2 adds the same amount everywhere, which changes no slope. Their common derivative is 2x2x, so at a given xx-value the three tangent lines are parallel. And exactly one antiderivative passes through a point (x0,y0)(x_{0},y_{0}) of the plane, because the equation x02+C=y0x_{0}^{2}+C=y_{0} has the unique solution C=y0−x02C=y_{0}-x_{0}^{2}. Geometrically: the family of antiderivatives fills the plane without any two of them crossing, which gives the right picture of the +C+C as a vertical slider.

Exercise 2: The table of formulas and its single gap

The whole table of basic antiderivatives is the table of derivatives read backwards. Only one formula has a gap, and the exam tests it every semester.

  • a) Compute ∫(x5−3x2+7)dx\int\left(x^{5}-3x^{2}+7\right)dx, ∫dxx4\int\frac{dx}{x^{4}} and ∫x dx\int\sqrt{x}\,dx, first rewriting each integrand as a power of xx.
  • b) Why does the formula ∫xndx=xn+1n+1+C\int x^{n}dx=\frac{x^{n+1}}{n+1}+C fail for n=−1n=-1? What is the integral then, and why the absolute value in the answer?
  • c) Compute ∫(e3x+2x)dx\int\left(e^{3x}+2^{x}\right)dx. Where does the ln⁡2\ln 2 in the denominator come from, and where does the factor 13\frac{1}{3} come from?
  • d) Compute ∫(sec⁡2x−41+x2)dx\int\left(\sec^{2}x-\frac{4}{1+x^{2}}\right)dx and ∫sin⁡(5x)dx\int\sin(5x)dx. What mistake does the student make who answers −cos⁡(5x)+C-\cos(5x)+C to the second one?

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  • a) x66−x3+7x+C\frac{x^{6}}{6}-x^{3}+7x+C; −13x3+C-\frac{1}{3x^{3}}+C; 23x3/2+C\frac{2}{3}x^{3/2}+C
  • b) n+1=0n+1=0; ∫dxx=ln⁡∣x∣+C\int\frac{dx}{x}=\ln|x|+C
  • c) e3x3+2xln⁡2+C\frac{e^{3x}}{3}+\frac{2^{x}}{\ln 2}+C
  • d) tan⁡x−4arctan⁡x+C\tan x-4\arctan x+C; −cos⁡5x5+C-\frac{\cos 5x}{5}+C
a)

Rewrite everything as powers before applying the formula. ∫(x5−3x2+7)dx=x66−x3+7x+C\int\left(x^{5}-3x^{2}+7\right)dx=\frac{x^{6}}{6}-x^{3}+7x+C. Next, ∫dxx4=∫x−4dx=x−3−3+C=−13x3+C\int\frac{dx}{x^{4}}=\int x^{-4}dx=\frac{x^{-3}}{-3}+C=-\frac{1}{3x^{3}}+C: the negative exponent causes no trouble, as long as you remember that −4+1=−3-4+1=-3. Finally, ∫x dx=∫x1/2dx=x3/23/2+C=23x3/2+C\int\sqrt{x}\,dx=\int x^{1/2}dx=\frac{x^{3/2}}{3/2}+C=\frac{2}{3}x^{3/2}+C. Rewriting first is the real technical move: as long as the integrand is not in the form xnx^{n}, no formula applies.

b)

For n=−1n=-1, the denominator n+1n+1 is zero: the formula asks for a division by zero, so it makes no sense. This case is handled separately: ∫dxx=ln⁡∣x∣+C\int\frac{dx}{x}=\ln|x|+C, because (ln⁡∣x∣)′=1x\left(\ln|x|\right)'=\frac{1}{x}. The absolute value is there because 1x\frac{1}{x} also exists for x<0x<0, where ln⁡x\ln x is not defined: for x<0x<0 we have ln⁡∣x∣=ln⁡(−x)\ln|x|=\ln(-x), whose derivative is −1−x=1x\frac{-1}{-x}=\frac{1}{x} ✓. The formula thus covers both sides of the origin. It is the only gap in the table of powers, and it is filled by a function from a completely different family: the power −1-1 integrates to a logarithm, which is far from obvious and deserves to be memorized as an exception.

c)

∫e3xdx=e3x3+C\int e^{3x}dx=\frac{e^{3x}}{3}+C: when you differentiate e3xe^{3x}, the chain rule brings out a factor 3, so you must divide by 3 to compensate. ∫2xdx=2xln⁡2+C\int 2^{x}dx=\frac{2^{x}}{\ln 2}+C: differentiating 2x2^{x} gives 2xln⁡22^{x}\ln 2, hence the division by ln⁡2\ln 2. Total: e3x3+2xln⁡2+C\frac{e^{3x}}{3}+\frac{2^{x}}{\ln 2}+C. In both cases the denominator is exactly the stray factor that differentiation would produce: integrating means cancelling in advance what differentiating would create.

d)

∫sec⁡2x dx=tan⁡x\int\sec^{2}x\,dx=\tan x and ∫dx1+x2=arctan⁡x\int\frac{dx}{1+x^{2}}=\arctan x, so the result is tan⁡x−4arctan⁡x+C\tan x-4\arctan x+C. For the second one: ∫sin⁡(5x)dx=−cos⁡(5x)5+C\int\sin(5x)dx=-\frac{\cos(5x)}{5}+C. The mistake of the student who answers −cos⁡(5x)+C-\cos(5x)+C is forgetting the chain rule: differentiating −cos⁡(5x)-\cos(5x) gives 5sin⁡(5x)5\sin(5x), five times too much. The checking reflex settles it at once, and the general rule to remember is that for a linear argument ax+bax+b, the antiderivative is divided by aa: ∫f(ax+b)dx=F(ax+b)a+C\int f(ax+b)dx=\frac{F(ax+b)}{a}+C. It is the most useful special case of substitution, the one you end up doing in your head.

Exercise 3: Linearity, and the two rules that do not exist

Integration has ONE algebraic property: linearity. Every semester, a majority of students invent two more, by analogy with differentiation.

  • a) State the linearity of the integral, then compute ∫(4cos⁡x−3x+5ex)dx\int\left(4\cos x-\frac{3}{x}+5e^{x}\right)dx.
  • b) A student writes ∫x exdx=x22 ex+C\int x\,e^{x}dx=\frac{x^{2}}{2}\,e^{x}+C. Refute this answer by differentiation, without computing the true antiderivative.
  • c) Another one writes ∫x2+3xxdx=∫(x2+3x)dx∫x dx\int\frac{x^{2}+3x}{x}dx=\frac{\int(x^{2}+3x)dx}{\int x\,dx}. Refute it, then compute the integral correctly.
  • d) Compute ∫x(x2−1)dx\int\sqrt{x}\left(x^{2}-1\right)dx and ∫x3+2x−5x2dx\int\frac{x^{3}+2x-5}{x^{2}}dx. What move do these two calculations have in common, and why is it the only one available at this stage?

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  • a) 4sin⁡x−3ln⁡∣x∣+5ex+C4\sin x-3\ln|x|+5e^{x}+C
  • b) The derivative gives xex+x22exxe^{x}+\frac{x^{2}}{2}e^{x}: wrong
  • c) x22+3x+C\frac{x^{2}}{2}+3x+C
  • d) 27x7/2−23x3/2+C\frac{2}{7}x^{7/2}-\frac{2}{3}x^{3/2}+C; x22+2ln⁡∣x∣+5x+C\frac{x^{2}}{2}+2\ln|x|+\frac{5}{x}+C
a)

Linearity: ∫(af(x)+bg(x))dx=a∫f(x)dx+b∫g(x)dx\int\left(af(x)+bg(x)\right)dx=a\int f(x)dx+b\int g(x)dx for all constants aa and bb. It allows two things, and only two: splitting a SUM, and pulling out a CONSTANT. Application: ∫(4cos⁡x−3x+5ex)dx=4sin⁡x−3ln⁡∣x∣+5ex+C\int\left(4\cos x-\frac{3}{x}+5e^{x}\right)dx=4\sin x-3\ln|x|+5e^{x}+C. A single constant CC is enough for the whole expression, since the sum of three arbitrary constants is still an arbitrary constant.

b)

It is enough to differentiate the proposed answer: (x22ex)′=xex+x22ex\left(\frac{x^{2}}{2}e^{x}\right)'=xe^{x}+\frac{x^{2}}{2}e^{x}, by the product rule. We wanted xexxe^{x} and we get xex+x22exxe^{x}+\frac{x^{2}}{2}e^{x}: the stray term x22ex\frac{x^{2}}{2}e^{x} is nonzero for every x≠0x\neq 0, so the answer is wrong. The lesson goes beyond the exercise: the integral of a product IS NOT the product of the integrals, because differentiating a product produces two terms, not one. There is no product rule for integration; there is integration by parts, which makes up for that absence, and which would give (x−1)ex+C(x-1)e^{x}+C here.

c)

The same method of refutation with a simple case: ∫xxdx=∫1 dx=x+C\int\frac{x}{x}dx=\int 1\,dx=x+C, whereas the proposed formula would give x2/2x2/2=1\frac{x^{2}/2}{x^{2}/2}=1, a constant. A nonconstant function cannot equal a constant, so the rule is false. The correct calculation goes through algebraic SIMPLIFICATION before any integration: x2+3xx=x+3\frac{x^{2}+3x}{x}=x+3 for x≠0x\neq 0, hence ∫x2+3xxdx=x22+3x+C\int\frac{x^{2}+3x}{x}dx=\frac{x^{2}}{2}+3x+C.

d)

First calculation: distribute before integrating, x(x2−1)=x5/2−x1/2\sqrt{x}(x^{2}-1)=x^{5/2}-x^{1/2}, so ∫=27x7/2−23x3/2+C\int=\frac{2}{7}x^{7/2}-\frac{2}{3}x^{3/2}+C. Second calculation: split the fraction term by term, x3+2x−5x2=x+2x−5x2\frac{x^{3}+2x-5}{x^{2}}=x+\frac{2}{x}-\frac{5}{x^{2}}, so ∫=x22+2ln⁡∣x∣+5x+C\int=\frac{x^{2}}{2}+2\ln|x|+\frac{5}{x}+C. The common move is to REWRITE the integrand as a sum of terms from the table before integrating anything. It is the only one available because linearity can only handle sums: as long as a product or a quotient is still standing, no rule of this chapter applies. Hence the opening strategy for every integral in this chapter: distribute, split, simplify, and only then see whether any work is left.

Exercise 4: Absolute value and disjoint domains

Two situations where the “+C+C” hides a subtlety: when the integrand has a corner, and when the domain is in two pieces.

  • a) Compute ∫∣x∣ dx\int|x|\,dx by treating x≥0x\geq 0 and x<0x<0 separately, then join the two pieces.
  • b) Show that the antiderivative obtained can be written F(x)=x∣x∣2+CF(x)=\frac{x|x|}{2}+C and check that it is differentiable AT 0.
  • c) On R∖{0}\mathbb{R}\setminus\{0\}, is ln⁡∣x∣+C\ln|x|+C the general antiderivative of the function 1x\frac{1}{x}? Justify precisely.
  • d) Which hypothesis of the theorem “two antiderivatives differ by a constant” is at stake in part c)?

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  • a) ±x22+C\pm\frac{x^{2}}{2}+C, a single constant by continuity
  • b) F(x)=x∣x∣2+CF(x)=\frac{x|x|}{2}+C, F′(0)=0F'(0)=0
  • c) No: two independent constants, one per piece
  • d) The interval hypothesis
a)

For x≥0x\geq 0, ∣x∣=x|x|=x, so an antiderivative is x22+C1\frac{x^{2}}{2}+C_{1}. For x<0x<0, ∣x∣=−x|x|=-x, so an antiderivative is −x22+C2-\frac{x^{2}}{2}+C_{2}. These two pieces must JOIN UP: an antiderivative is differentiable, hence continuous, and continuity at 0 forces 02+C1=−02+C2\frac{0}{2}+C_{1}=-\frac{0}{2}+C_{2}, that is, C1=C2C_{1}=C_{2}. So there is only one constant, not two: F(x)=x22+CF(x)=\frac{x^{2}}{2}+C for x≥0x\geq 0, F(x)=−x22+CF(x)=-\frac{x^{2}}{2}+C for x<0x<0.

b)

The two pieces combine into a single formula: if x≥0x\geq 0, x∣x∣2=x⋅x2=x22\frac{x|x|}{2}=\frac{x\cdot x}{2}=\frac{x^{2}}{2} ✓; if x<0x<0, x∣x∣2=x(−x)2=−x22\frac{x|x|}{2}=\frac{x(-x)}{2}=-\frac{x^{2}}{2} ✓. So F(x)=x∣x∣2+CF(x)=\frac{x|x|}{2}+C. Differentiability at 0: the difference quotient is F(h)−F(0)h=h∣h∣/2h=∣h∣2\frac{F(h)-F(0)}{h}=\frac{h|h|/2}{h}=\frac{|h|}{2}, which tends to 0 as h→0h\to 0 from BOTH sides. So F′(0)=0=∣0∣F'(0)=0=|0| ✓. The antiderivative is indeed differentiable everywhere, including at the corner of the integrand: integration SMOOTHS, whereas differentiation breaks. This is a general observation, and it is why a function that is merely continuous still has differentiable antiderivatives.

c)

NO, not as the GENERAL antiderivative. It is true that (ln⁡∣x∣)′=1x\left(\ln|x|\right)'=\frac{1}{x} on all of R∖{0}\mathbb{R}\setminus\{0\}. But the domain is in TWO disjoint pieces, (−∞,0)\left(-\infty, 0\right) and (0,+∞)\left(0, +\infty\right), and nothing forces the constant to be the same on both. The general antiderivative is therefore F(x)=ln⁡∣x∣+C1F(x)=\ln|x|+C_{1} for x>0x>0 and F(x)=ln⁡∣x∣+C2F(x)=\ln|x|+C_{2} for x<0x<0, with C1C_{1} and C2C_{2} INDEPENDENT. For example, the function equal to ln⁡x\ln x for x>0x>0 and to ln⁡(−x)+7\ln(-x)+7 for x<0x<0 does have derivative 1x\frac{1}{x} everywhere, and it cannot be written ln⁡∣x∣+C\ln|x|+C. Unlike part a), no continuity condition links the two constants, since the pieces do not touch.

d)

The hypothesis at stake is that of an INTERVAL. The theorem reads: if F′=G′F'=G' ON AN INTERVAL, then F−GF-G is constant there. Its proof relies on the mean value theorem, which requires being able to connect two points while staying in the domain. On R∖{0}\mathbb{R}\setminus\{0\}, which is not an interval, you cannot go from a negative point to a positive point without crossing 0, where the function does not exist: the argument breaks down, and the conclusion falls with it. In practice in CEGEP, we still write ∫dxx=ln⁡∣x∣+C\int\frac{dx}{x}=\ln|x|+C because we almost always work on only one of the two pieces at a time; but as soon as a definite integral crosses 0, that expression becomes wrong, and the integral is in fact divergent. That is exactly the pitfall of the chapter on improper integrals.

-6-5-4-3-2-1123456-4-3-2-11234ln(−x) + C₁ln(x) + C₂1/x

Exercise 5: Recognize the form: the table of derivatives backwards

Three patterns come back in half of all exam integrals. Spotting them in a few seconds beats any heavy technique.

  • a) State the three forms ∫f′f\int\frac{f'}{f}, ∫f′fn\int f'f^{n} and ∫f′ef\int f'e^{f}, with their antiderivatives.
  • b) Compute ∫2xx2+1dx\int\frac{2x}{x^{2}+1}dx, ∫exex+3dx\int\frac{e^{x}}{e^{x}+3}dx and ∫dxxln⁡x\int\frac{dx}{x\ln x}, identifying ff each time.
  • c) Compute ∫3x2(x3+1)4dx\int 3x^{2}\left(x^{3}+1\right)^{4}dx and ∫cos⁡x esin⁡xdx\int\cos x\,e^{\sin x}dx.
  • d) Compute ∫xx2+1dx\int\frac{x}{x^{2}+1}dx: the form is not exactly the one in a). What adjustment is needed, and why is it allowed?

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  • a) ln⁡∣f∣+C\ln|f|+C; fn+1n+1+C\frac{f^{n+1}}{n+1}+C; ef+Ce^{f}+C
  • b) ln⁡(x2+1)\ln(x^{2}+1); ln⁡(ex+3)\ln(e^{x}+3); ln⁡∣ln⁡x∣\ln|\ln x|, plus CC
  • c) (x3+1)55+C\frac{(x^{3}+1)^{5}}{5}+C; esin⁡x+Ce^{\sin x}+C
  • d) 12ln⁡(x2+1)+C\frac{1}{2}\ln(x^{2}+1)+C: pull out the constant 12\frac{1}{2}
a)

The three forms, all coming from the chain rule read backwards. ∫f′(x)f(x)dx=ln⁡∣f(x)∣+C\int\frac{f'(x)}{f(x)}dx=\ln\left|f(x)\right|+C. ∫f′(x)[f(x)]ndx=[f(x)]n+1n+1+C\int f'(x)\left[f(x)\right]^{n}dx=\frac{\left[f(x)\right]^{n+1}}{n+1}+C for n≠−1n\neq-1. ∫f′(x)ef(x)dx=ef(x)+C\int f'(x)e^{f(x)}dx=e^{f(x)}+C. In all three cases the signature is the same: a composite function MULTIPLIED by the derivative of its inside.

b)

First case: f=x2+1f=x^{2}+1, f′=2xf'=2x, exactly in the numerator, so ∫2xx2+1dx=ln⁡(x2+1)+C\int\frac{2x}{x^{2}+1}dx=\ln\left(x^{2}+1\right)+C (the absolute value is unnecessary, since x2+1x^{2}+1 is always positive). Second: f=ex+3f=e^{x}+3, f′=exf'=e^{x}, present, so ∫exex+3dx=ln⁡(ex+3)+C\int\frac{e^{x}}{e^{x}+3}dx=\ln\left(e^{x}+3\right)+C. Third: rewrite 1xln⁡x=1/xln⁡x\frac{1}{x\ln x}=\frac{1/x}{\ln x}, so f=ln⁡xf=\ln x and f′=1xf'=\frac{1}{x}, hence ∫dxxln⁡x=ln⁡∣ln⁡x∣+C\int\frac{dx}{x\ln x}=\ln\left|\ln x\right|+C. A logarithm of a logarithm, perfectly legitimate.

c)

First: f=x3+1f=x^{3}+1, f′=3x2f'=3x^{2}, exactly as a factor, with n=4n=4: ∫3x2(x3+1)4dx=(x3+1)55+C\int 3x^{2}\left(x^{3}+1\right)^{4}dx=\frac{\left(x^{3}+1\right)^{5}}{5}+C. Second: f=sin⁡xf=\sin x, f′=cos⁡xf'=\cos x, present: ∫cos⁡x esin⁡xdx=esin⁡x+C\int\cos x\,e^{\sin x}dx=e^{\sin x}+C. Systematic check by differentiation: (esin⁡x)′=cos⁡x esin⁡x\left(e^{\sin x}\right)'=\cos x\,e^{\sin x} ✓.

d)

The derivative of f=x2+1f=x^{2}+1 is 2x2x, but the numerator only contains xx: the factor 2 is missing. We ADJUST by writing xx2+1=12⋅2xx2+1\frac{x}{x^{2}+1}=\frac{1}{2}\cdot\frac{2x}{x^{2}+1}, hence ∫xx2+1dx=12ln⁡(x2+1)+C\int\frac{x}{x^{2}+1}dx=\frac{1}{2}\ln\left(x^{2}+1\right)+C. The adjustment is allowed because 12\frac{1}{2} is a CONSTANT, and linearity lets you pull constants out of the integral. It would be forbidden if a factor in xx were missing: you can never write ∫x g(x)dx=x∫g(x)dx\int x\,g(x)dx=x\int g(x)dx. All the flexibility of the method lies in this distinction, and it is what separates a correct substitution from a faulty argument.

Part B: Substitution, the limits of the method and undetermined coefficients (/50)

Exercise 6: Direct substitution: recognizing the hidden derivative

Substitution is the only tool in this chapter that goes beyond the table. Its signature is always the same: a function and its derivative live side by side in the integrand.

  • a) Compute ∫2x(x2+5)7dx\int 2x\left(x^{2}+5\right)^{7}dx, writing out uu, dudu and the return to xx.
  • b) Compute ∫3x2x3+4dx\int\frac{3x^{2}}{x^{3}+4}dx, then ∫ln⁡xxdx\int\frac{\ln x}{x}dx. What structure do these two integrals share?
  • c) Compute ∫x ex2dx\int x\,e^{x^{2}}dx. Compare with ∫ex2dx\int e^{x^{2}}dx: what difference does the factor xx make?
  • d) Compute ∫cos⁡3xsin⁡x dx\int\cos^{3}x\sin x\,dx, then state in one sentence the test that decides whether a substitution will work.

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  • a) (x2+5)88+C\frac{(x^{2}+5)^{8}}{8}+C
  • b) ln⁡∣x3+4∣+C\ln|x^{3}+4|+C; (ln⁡x)22+C\frac{(\ln x)^{2}}{2}+C
  • c) ex22+C\frac{e^{x^{2}}}{2}+C; ∫ex2dx\int e^{x^{2}}dx is not elementary
  • d) −cos⁡4x4+C-\frac{\cos^{4}x}{4}+C; no xx may remain
a)

Set u=x2+5u=x^{2}+5, so du=2x dxdu=2x\,dx: the factor 2x dx2x\,dx in the integral is exactly dudu. The integral becomes ∫u7du=u88+C\int u^{7}du=\frac{u^{8}}{8}+C, and returning to xx gives (x2+5)88+C\frac{(x^{2}+5)^{8}}{8}+C. The return is COMPULSORY for an indefinite integral: an answer left in uu does not answer the question, which was about a function of xx. Check by differentiation: 8(x2+5)7⋅2x8=2x(x2+5)7\frac{8(x^{2}+5)^{7}\cdot 2x}{8}=2x(x^{2}+5)^{7} ✓.

b)

First case: u=x3+4u=x^{3}+4, du=3x2dxdu=3x^{2}dx, the integral becomes ∫duu=ln⁡∣u∣+C=ln⁡∣x3+4∣+C\int\frac{du}{u}=\ln|u|+C=\ln\left|x^{3}+4\right|+C. Second case: u=ln⁡xu=\ln x, du=dxxdu=\frac{dx}{x}, the integral becomes ∫u du=u22+C=(ln⁡x)22+C\int u\,du=\frac{u^{2}}{2}+C=\frac{(\ln x)^{2}}{2}+C. The common structure is ∫f(g(x)) g′(x) dx\int f(g(x))\,g'(x)\,dx: a composite function multiplied by the derivative of its inside. It is the chain rule read backwards, and it is the only thing substitution knows how to undo. Note along the way the form ∫g′gdx=ln⁡∣g∣+C\int\frac{g'}{g}dx=\ln|g|+C, which comes up so often that it deserves to be recognized directly.

c)

With u=x2u=x^{2}, du=2x dxdu=2x\,dx, so x dx=du2x\,dx=\frac{du}{2}: ∫xex2dx=12∫eudu=ex22+C\int xe^{x^{2}}dx=\frac{1}{2}\int e^{u}du=\frac{e^{x^{2}}}{2}+C. On the other hand, ∫ex2dx\int e^{x^{2}}dx has NO elementary antiderivative: no finite combination of the usual functions gives it, and this is not a matter of skill but a theorem. So the factor xx changes everything: it provides the dudu that makes the substitution possible. It is the most instructive comparison in the chapter, because it shows that integration is not a guaranteed procedure the way differentiation is. An elementary function always has an elementary derivative; it does not always have an elementary antiderivative.

d)

Set u=cos⁡xu=\cos x, du=−sin⁡x dxdu=-\sin x\,dx, so sin⁡x dx=−du\sin x\,dx=-du: ∫cos⁡3xsin⁡x dx=−∫u3du=−u44+C=−cos⁡4x4+C\int\cos^{3}x\sin x\,dx=-\int u^{3}du=-\frac{u^{4}}{4}+C=-\frac{\cos^{4}x}{4}+C. The test, in one sentence: the substitution u=g(x)u=g(x) works if, after replacing g(x)g(x) by uu and g′(x)dxg'(x)dx by dudu, there is NO xx LEFT in the integral. That is the complete working criterion, and it can be checked in ten seconds before committing to the calculation. If a lone xx remains, there are two ways out: express it in terms of uu (the back-substitution of the next exercise), or change technique.

Exercise 7: When substitution resists: constants and back-substitution

Two complications separate exam substitution from textbook substitution: the derivative present up to a constant factor, and the leftover xx that has to be re-expressed in terms of uu.

  • a) Compute ∫x2(x3−2)5dx\int x^{2}\left(x^{3}-2\right)^{5}dx: the derivative of the inside is not exactly there, so how do you adjust, and why are you allowed to?
  • b) Compute ∫dx(4x+3)2\int\frac{dx}{\left(4x+3\right)^{2}} and ∫7−2x dx\int\sqrt{7-2x}\,dx (linear arguments).
  • c) Compute ∫xx+1 dx\int x\sqrt{x+1}\,dx. Here the substitution u=x+1u=x+1 leaves an xx standing: what do you do, and why is this move legitimate?
  • d) A student writes ∫x2x3+1 dx=x33⋅23(x3+1)3/2+C\int x^{2}\sqrt{x^{3}+1}\,dx=\frac{x^{3}}{3}\cdot\frac{2}{3}\left(x^{3}+1\right)^{3/2}+C, “pulling out” the x2x^{2} the way you pull out a constant. Diagnose the error precisely.

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  • a) (x3−2)618+C\frac{(x^{3}-2)^{6}}{18}+C
  • b) −14(4x+3)+C-\frac{1}{4(4x+3)}+C; −(7−2x)3/23+C-\frac{(7-2x)^{3/2}}{3}+C
  • c) 25(x+1)5/2−23(x+1)3/2+C\frac{2}{5}(x+1)^{5/2}-\frac{2}{3}(x+1)^{3/2}+C
  • d) A factor in xx does not come out: 29(x3+1)3/2+C\frac{2}{9}(x^{3}+1)^{3/2}+C
a)

Set u=x3−2u=x^{3}-2, so du=3x2dxdu=3x^{2}dx. The integral contains x2dxx^{2}dx, that is, du3\frac{du}{3}: we write ∫x2(x3−2)5dx=13∫u5du=u618+C=(x3−2)618+C\int x^{2}(x^{3}-2)^{5}dx=\frac{1}{3}\int u^{5}du=\frac{u^{6}}{18}+C=\frac{(x^{3}-2)^{6}}{18}+C. We are allowed to because 13\frac{1}{3} is a CONSTANT, and linearity lets you pull constants out. It would be forbidden with a factor in xx: ∫x f(x)dx≠x∫f(x)dx\int x\,f(x)dx\neq x\int f(x)dx, ever. This is the decisive distinction of the chapter, and it separates a correct substitution from the mistake in part d).

b)

Linear arguments, so divide by the coefficient of xx. First case: u=4x+3u=4x+3, du=4dxdu=4dx, ∫dx(4x+3)2=14∫u−2du=−14u+C=−14(4x+3)+C\int\frac{dx}{(4x+3)^{2}}=\frac{1}{4}\int u^{-2}du=-\frac{1}{4u}+C=-\frac{1}{4(4x+3)}+C. Second case: u=7−2xu=7-2x, du=−2dxdu=-2dx, ∫7−2x dx=−12∫u du=−13u3/2+C=−(7−2x)3/23+C\int\sqrt{7-2x}\,dx=-\frac{1}{2}\int\sqrt{u}\,du=-\frac{1}{3}u^{3/2}+C=-\frac{(7-2x)^{3/2}}{3}+C. The negative sign comes from the coefficient −2-2 and is very often forgotten: checking by differentiation catches it every time.

c)

With u=x+1u=x+1 we have du=dxdu=dx and x+1=u\sqrt{x+1}=\sqrt{u}, but the factor xx remains. Express it in terms of uu: since u=x+1u=x+1, x=u−1x=u-1. The integral becomes ∫(u−1)u du=∫(u3/2−u1/2)du=25u5/2−23u3/2+C\int(u-1)\sqrt{u}\,du=\int\left(u^{3/2}-u^{1/2}\right)du=\frac{2}{5}u^{5/2}-\frac{2}{3}u^{3/2}+C, that is, 25(x+1)5/2−23(x+1)3/2+C\frac{2}{5}(x+1)^{5/2}-\frac{2}{3}(x+1)^{3/2}+C. The move is legitimate because a change of variable is a COMPLETE SUBSTITUTION: everything that depends on xx must be rewritten in terms of uu, including the xx's that were not part of the original plan. The relation u=x+1u=x+1 is invertible, so it gives x=u−1x=u-1 for free. This back-substitution is the move the exam rewards most reliably, because it requires understanding the substitution rather than just recognizing it.

d)

The error is treating x2x^{2} as a constant, “integrating it on its own” as x33\frac{x^{3}}{3} while integrating the rest separately. No rule allows that: the integral of a product is not the product of the integrals, and pulling a factor out of the integral is only allowed if it is CONSTANT. The immediate refutation is by differentiation: the proposed answer needs the product rule and gives back 23x2(x3+1)3/2+x5x3+1\frac{2}{3}x^{2}\left(x^{3}+1\right)^{3/2}+x^{5}\sqrt{x^{3}+1}, which is not the integrand x2x3+1x^{2}\sqrt{x^{3}+1}: it is wrong. The correct calculation is an ordinary substitution: u=x3+1u=x^{3}+1, du=3x2dxdu=3x^{2}dx, hence 13∫u du=29(x3+1)3/2+C\frac{1}{3}\int\sqrt{u}\,du=\frac{2}{9}\left(x^{3}+1\right)^{3/2}+C. The irony: the student had the right x2x^{2} right there, and it was exactly the dudu needed.

Exercise 8: Synthesis: from antiderivative to motion

The indefinite integral is not an exercise in symbolic computation: it is the reconstruction of a quantity from its rate of change. Physics makes the most direct use of it.

  • a) A particle has acceleration a(t)=6t−4a(t)=6t-4 (in m/s²), with v(0)=2v(0)=2 m/s and s(0)=3s(0)=3 m. Find v(t)v(t), then s(t)s(t), justifying each constant.
  • b) The rate of change of a population is P′(t)=200e0.1tP'(t)=200e^{0.1t} individuals per year, and P(0)=5000P(0)=5000. Find P(t)P(t), then the population after 10 years.
  • c) Compute ∫2x+3x2+3x+1dx\int\frac{2x+3}{x^{2}+3x+1}dx and ∫dxx(ln⁡x)2\int\frac{dx}{x\left(\ln x\right)^{2}}: what common structure governs these two integrals?
  • d) Faced with an unfamiliar integral from this chapter, in what order should you ask the questions? Illustrate each step with one of the integrals already met.

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  • a) v=3t2−4t+2v=3t^{2}-4t+2; s=t3−2t2+2t+3s=t^{3}-2t^{2}+2t+3
  • b) P(t)=2000e0.1t+3000P(t)=2000e^{0.1t}+3000; P(10)≈8437P(10)\approx 8437
  • c) ln⁡∣x2+3x+1∣+C\ln|x^{2}+3x+1|+C; −1ln⁡x+C-\frac{1}{\ln x}+C
  • d) Simplify, table, substitution, back-substitution, then differentiate
a)

Acceleration is the derivative of velocity, so velocity is an antiderivative of acceleration: v(t)=3t2−4t+C1v(t)=3t^{2}-4t+C_{1}. The condition v(0)=2v(0)=2 gives C1=2C_{1}=2, hence v(t)=3t2−4t+2v(t)=3t^{2}-4t+2. Velocity is in turn the derivative of position: s(t)=t3−2t2+2t+C2s(t)=t^{3}-2t^{2}+2t+C_{2}, and s(0)=3s(0)=3 gives C2=3C_{2}=3, hence s(t)=t3−2t2+2t+3s(t)=t^{3}-2t^{2}+2t+3. Each integration produces its own constant, and each constant calls for its own initial condition: two integrations, two conditions, which is exactly why mechanics needs both the initial position AND the initial velocity to predict a motion. Check: s′(t)=3t2−4t+2=v(t)s'(t)=3t^{2}-4t+2=v(t) ✓ and v′(t)=6t−4=a(t)v'(t)=6t-4=a(t) ✓. The figure shows the consequence: the velocity never vanishes (the discriminant of the quadratic is 16 − 24, which is negative) and stays positive, so the position keeps increasing.

b)

P(t)=∫200e0.1tdt=2000.1e0.1t+C=2000e0.1t+CP(t)=\int 200e^{0.1t}dt=\frac{200}{0.1}e^{0.1t}+C=2000e^{0.1t}+C. The condition P(0)=5000P(0)=5000 gives 2000+C=50002000+C=5000, so C=3000C=3000 and P(t)=2000e0.1t+3000P(t)=2000e^{0.1t}+3000. After 10 years: P(10)=2000e1+3000≈2000(2.71828)+3000≈8437P(10)=2000e^{1}+3000\approx 2000(2.71828)+3000\approx 8437 individuals. Note that the constant 30003000 is not a cosmetic detail: it represents the part of the population that does not take part in the exponential growth, and forgetting it would give about 54375437 individuals instead of 84378437, more than a third less.

c)

Both are of the form ∫g′(x)(g(x))ndx\int\frac{g'(x)}{\left(g(x)\right)^{n}}dx. First case: g=x2+3x+1g=x^{2}+3x+1, g′=2x+3g'=2x+3 is exactly in the numerator, so ∫2x+3x2+3x+1dx=ln⁡∣x2+3x+1∣+C\int\frac{2x+3}{x^{2}+3x+1}dx=\ln\left|x^{2}+3x+1\right|+C (the case n=1n=1, which gives the logarithm). Second case: rewrite 1x(ln⁡x)2=1(ln⁡x)2⋅1x\frac{1}{x(\ln x)^{2}}=\frac{1}{(\ln x)^{2}}\cdot\frac{1}{x}, with g=ln⁡xg=\ln x and g′=1xg'=\frac{1}{x} present: ∫u−2du=−1u+C=−1ln⁡x+C\int u^{-2}du=-\frac{1}{u}+C=-\frac{1}{\ln x}+C (the case n=2n=2, which gives a power). The common structure is therefore the same substitution, and only the value of nn decides whether the answer is a logarithm or a power: it is the gap at n=−1n=-1 in the table once again, met in another disguise.

d)

The efficient order: 1) Can I SIMPLIFY the integrand algebraically (distribute, split a fraction, cancel)? Example: ∫x2+3xxdx\int\frac{x^{2}+3x}{x}dx, which becomes ∫(x+3)dx\int(x+3)dx. 2) Is it a DIRECT form from the table, possibly with a linear argument? Example: ∫sin⁡(5x)dx\int\sin(5x)dx, where dividing by 5 is enough. 3) Do I see a function AND its derivative, up to a constant? Then SUBSTITUTION. Example: ∫x2(x3−2)5dx\int x^{2}(x^{3}-2)^{5}dx. 4) Does the substitution leave an xx standing? Then express it in terms of uu. Example: ∫xx+1 dx\int x\sqrt{x+1}\,dx. 5) None of this works? The integral belongs to the next chapter (parts, partial fractions, trigonometry), or has no elementary antiderivative, like ∫ex2dx\int e^{x^{2}}dx. And in every case: DIFFERENTIATE the answer before handing in the paper.

0.511.522.535101520s(t), positionv(t), velocity

Exercise 9: Antiderivatives that do not exist

Every elementary function has an elementary derivative. The converse is FALSE, and that is a theorem, not an admission of ignorance.

  • a) What exactly does “elementary function” mean? Give three common integrands whose antiderivative is not elementary.
  • b) Compare ∫xex2dx\int xe^{x^{2}}dx and ∫ex2dx\int e^{x^{2}}dx: the first can be computed, the second cannot. What changes?
  • c) Does the function e−x2e^{-x^{2}} have antiderivatives? Reconcile your answer with part a).
  • d) What do you actually do when faced with ∫01e−x2dx\int_{0}^{1}e^{-x^{2}}dx? Name the two routes from the course and say which one comes with an error guarantee.

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  • a) Finitely many sums, products, quotients, compositions; e−x2e^{-x^{2}}, sin⁡xx\frac{\sin x}{x}, 1+x3\sqrt{1+x^{3}}
  • b) The factor xx provides the dudu
  • c) Yes: ∫0xe−t2dt\int_{0}^{x}e^{-t^{2}}dt exists, without being elementary
  • d) Series or Simpson, ≈0.7468\approx 0.7468, both with an error bound
a)

An ELEMENTARY function is one obtained from polynomials, exponentials, logarithms, trigonometric functions and their inverses by a FINITE number of sums, products, quotients and compositions. Three common integrands with no elementary antiderivative: e−x2e^{-x^{2}} (the normal distribution in statistics), sin⁡xx\frac{\sin x}{x} (the sinc function, in optics and signal processing), and 1+x3\sqrt{1+x^{3}} (the arc length of certain curves). You can add 1ln⁡x\frac{1}{\ln x} and exx\frac{e^{x}}{x}. Liouville's theorem proves this impossibility: it is not that nobody has found it yet, it is that there is nothing to find.

b)

What changes is the presence of the factor xx. For the first one: u=x2u=x^{2} gives du=2x dxdu=2x\,dx, so the x dxx\,dx present equals du2\frac{du}{2} and the integral becomes 12∫eudu=ex22+C\frac{1}{2}\int e^{u}du=\frac{e^{x^{2}}}{2}+C. The substitution works BECAUSE the derivative of the inside is there, up to a constant. For the second one, that factor is missing: no substitution can absorb the dxdx, and we saw in part a) that no other technique will succeed either. A seemingly harmless factor xx thus makes all the difference between a thirty-second integral and an impossible one: it is the most instructive comparison in the chapter.

c)

YES, it does. There is no contradiction, because these are two DIFFERENT statements. “Having an antiderivative” and “having an ELEMENTARY antiderivative” are not the same thing. The function e−x2e^{-x^{2}} is continuous on R\mathbb{R}, and the fundamental theorem of calculus then guarantees that the function F(x)=∫0xe−t2dtF(x)=\int_{0}^{x}e^{-t^{2}}dt is differentiable with derivative e−x2e^{-x^{2}}: it really is an antiderivative, it EXISTS. It simply cannot be written with the usual symbols. Mathematicians have in fact given it a name, the error function erf⁡\operatorname{erf}, just as ln⁡\ln was once the name given to the antiderivative of 1x\frac{1}{x}. A “new” function is often just an antiderivative that finally got a name.

d)

Two routes. First: SERIES EXPANSION. Replace e−x2e^{-x^{2}} by its Maclaurin series 1−x2+x42!−x63!+⋯1-x^{2}+\frac{x^{4}}{2!}-\frac{x^{6}}{3!}+\cdots, and integrate term by term, which gives 1−13+110−142+⋯≈0.74681-\frac{1}{3}+\frac{1}{10}-\frac{1}{42}+\cdots\approx 0.7468. Since the series is alternating, the error is bounded by the first term left out: the guarantee is explicit. Second: NUMERICAL INTEGRATION, by Simpson's rule for example, which gives 0.7468550.746855 with n=4n=4 against an exact value of 0.7468240.746824; here too an error bound is available, M(b−a)5180n4\frac{M(b-a)^{5}}{180n^{4}}. BOTH routes therefore come with an error guarantee, which is precisely what makes them acceptable in science: an approximation without a bound is worthless. The series is more convenient near its centre of expansion; the numerical method does not care about that, and even applies to data with no formula.

-3-2-1123-1-0.50.511.5e^(−x²)F, zero at 0

Exercise 10: The method of undetermined coefficients

When you GUESS the form of the antiderivative, all that remains is to adjust coefficients by matching. The technique sometimes saves several integrations by parts.

  • a) Find aa and bb so that F(x)=(ax+b)exF(x)=(ax+b)e^{x} is an antiderivative of xexxe^{x}.
  • b) Find aa, bb, cc so that F(x)=(ax2+bx+c)exF(x)=\left(ax^{2}+bx+c\right)e^{x} is an antiderivative of x2exx^{2}e^{x}.
  • c) Guess the form, then find the coefficients of an antiderivative of exsin⁡xe^{x}\sin x.
  • d) What is the advantage of this method over integration by parts, and what is its limitation?

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  • a) a=1a=1, b=−1b=-1: (x−1)ex+C(x-1)e^{x}+C
  • b) (x2−2x+2)ex+C(x^{2}-2x+2)e^{x}+C
  • c) ex(sin⁡x−cos⁡x)2+C\frac{e^{x}(\sin x-\cos x)}{2}+C
  • d) Fast and self-checking; you have to guess the form
a)

Differentiate the assumed form: F′(x)=aex+(ax+b)ex=ex(ax+a+b)F'(x)=ae^{x}+(ax+b)e^{x}=e^{x}\left(ax+a+b\right). We want F′(x)=xex=ex⋅xF'(x)=xe^{x}=e^{x}\cdot x. Dividing by exe^{x}, which is never zero, leaves ax+(a+b)=xax+(a+b)=x. By MATCHING coefficients: the coefficient of xx gives a=1a=1; the constant term gives a+b=0a+b=0, so b=−1b=-1. Hence ∫xexdx=(x−1)ex+C\int xe^{x}dx=(x-1)e^{x}+C. Check: [(x−1)ex]′=ex+(x−1)ex=xex\left[(x-1)e^{x}\right]'=e^{x}+(x-1)e^{x}=xe^{x} ✓.

b)

F′(x)=(2ax+b)ex+(ax2+bx+c)ex=ex[ax2+(2a+b)x+(b+c)]F'(x)=(2ax+b)e^{x}+\left(ax^{2}+bx+c\right)e^{x}=e^{x}\left[ax^{2}+(2a+b)x+(b+c)\right]. We want x2exx^{2}e^{x}, so after dividing by exe^{x}: ax2+(2a+b)x+(b+c)=x2ax^{2}+(2a+b)x+(b+c)=x^{2}. Matching: a=1a=1; then 2a+b=02a+b=0 gives b=−2b=-2; then b+c=0b+c=0 gives c=2c=2. Hence ∫x2exdx=(x2−2x+2)ex+C\int x^{2}e^{x}dx=\left(x^{2}-2x+2\right)e^{x}+C, which agrees with the result of two successive integrations by parts ✓. A single linear system has replaced two rounds of parts.

c)

Differentiating a product ex×e^{x}\times trigonometric function always regenerates both functions sin⁡\sin and cos⁡\cos: so we guess the form F(x)=ex(asin⁡x+bcos⁡x)F(x)=e^{x}\left(a\sin x+b\cos x\right). Differentiate: F′(x)=ex(asin⁡x+bcos⁡x)+ex(acos⁡x−bsin⁡x)=ex[(a−b)sin⁡x+(a+b)cos⁡x]F'(x)=e^{x}\left(a\sin x+b\cos x\right)+e^{x}\left(a\cos x-b\sin x\right)=e^{x}\left[(a-b)\sin x+(a+b)\cos x\right]. We want exsin⁡xe^{x}\sin x, so a−b=1a-b=1 and a+b=0a+b=0. The second gives b=−ab=-a, and substituting: 2a=12a=1, so a=12a=\frac{1}{2} and b=−12b=-\frac{1}{2}. Conclusion: ∫exsin⁡x dx=ex(sin⁡x−cos⁡x)2+C\int e^{x}\sin x\,dx=\frac{e^{x}\left(\sin x-\cos x\right)}{2}+C. This is the so-called CYCLIC case, which parts solve in two rounds plus an equation in II; here a single matching is enough.

d)

ADVANTAGE: the method replaces several successive integrations with a single differentiation followed by a linear system, which is faster and above all less exposed to sign errors, very common in repeated parts. It also makes checking immediate, since the answer has been differentiated along the way. LIMITATION: you have to GUESS the right form at the start, which is only possible for well-identified families, essentially polynomial times exponential, polynomial times sine or cosine, and exponential times trigonometric function. Faced with ∫ln⁡x dx\int\ln x\,dx or ∫dxx2+1\int\frac{dx}{x^{2}+1}, no obvious form comes to mind and the method cannot get started. It therefore complements integration by parts without replacing it, just as the method of undetermined coefficients will complement variation of parameters in the chapter on differential equations.

Part C: the classics (/50)

Exercise 11: Other bases: 10 to the x, the common log and the three e's

The table gives ∫exdx=ex+C\int e^{x}dx=e^{x}+C and ∫dxx=ln⁡∣x∣+C\int\frac{dx}{x}=\ln|x|+C. As soon as the base is no longer ee, a natural logarithm appears in the denominator, and that is the one people forget.

  • a) Compute ∫10xdx\int 10^{x}dx and give the decimal value of the coefficient obtained in front of 10x10^{x}.
  • b) Compute ∫32xdx\int 3^{2x}dx in two ways: by the substitution u=2xu=2x, then by writing 32x=9x3^{2x}=9^{x}. Show that the two answers agree.
  • c) Compute ∫x 5x2dx\int x\,5^{x^{2}}dx.
  • d) Compute ∫log⁡10xxdx\int\frac{\log_{10}x}{x}dx, starting by writing log⁡10x=ln⁡xln⁡10\log_{10}x=\frac{\ln x}{\ln 10}.
  • e) Compute ∫xedx\int x^{e}dx, ∫exdx\int e^{x}dx and ∫eedx\int e^{e}dx. Why do these three integrals, which look alike, fall under three different rules?

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  • a) 10xln⁡10+C\frac{10^{x}}{\ln 10}+C, coefficient ≈0.4343\approx 0.4343
  • b) 32x2ln⁡3+C=9xln⁡9+C\frac{3^{2x}}{2\ln 3}+C=\frac{9^{x}}{\ln 9}+C
  • c) 5x22ln⁡5+C\frac{5^{x^{2}}}{2\ln 5}+C
  • d) (ln⁡x)22ln⁡10+C\frac{(\ln x)^{2}}{2\ln 10}+C
  • e) xe+1e+1\frac{x^{e+1}}{e+1}, exe^{x}, eexe^{e}x: power, exponential, constant
a)

Since (10x)′=10xln⁡10\left(10^{x}\right)'=10^{x}\ln 10, we compensate: ∫10xdx=10xln⁡10+C\int 10^{x}dx=\frac{10^{x}}{\ln 10}+C. The coefficient is 1ln⁡10≈0.4343\frac{1}{\ln 10}\approx 0.4343. Check: (10xln⁡10)′=10xln⁡10ln⁡10=10x\left(\frac{10^{x}}{\ln 10}\right)'=\frac{10^{x}\ln 10}{\ln 10}=10^{x} ✓.

b)

Substitution: u=2xu=2x, du=2 dxdu=2\,dx, so ∫32xdx=12∫3udu=32x2ln⁡3+C\int 3^{2x}dx=\frac{1}{2}\int 3^{u}du=\frac{3^{2x}}{2\ln 3}+C. Rewriting: 32x=(32)x=9x3^{2x}=\left(3^{2}\right)^{x}=9^{x}, so ∫9xdx=9xln⁡9+C\int 9^{x}dx=\frac{9^{x}}{\ln 9}+C. Now ln⁡9=ln⁡32=2ln⁡3\ln 9=\ln 3^{2}=2\ln 3 and 9x=32x9^{x}=3^{2x}: the two answers are identical, with coefficient 12ln⁡3≈0.4551\frac{1}{2\ln 3}\approx 0.4551.

c)

u=x2u=x^{2}, du=2x dxdu=2x\,dx, so x dx=du2x\,dx=\frac{du}{2}: ∫x 5x2dx=12∫5udu=5x22ln⁡5+C\int x\,5^{x^{2}}dx=\frac{1}{2}\int 5^{u}du=\frac{5^{x^{2}}}{2\ln 5}+C. The coefficient is 12ln⁡5≈0.3107\frac{1}{2\ln 5}\approx 0.3107. Two factors pile up in the denominator: the 22 from the substitution and the ln⁡5\ln 5 from the base.

d)

∫log⁡10xxdx=1ln⁡10∫ln⁡xxdx\int\frac{\log_{10}x}{x}dx=\frac{1}{\ln 10}\int\frac{\ln x}{x}dx. With u=ln⁡xu=\ln x, du=dxxdu=\frac{dx}{x}: 1ln⁡10⋅(ln⁡x)22+C=(ln⁡x)22ln⁡10+C\frac{1}{\ln 10}\cdot\frac{(\ln x)^{2}}{2}+C=\frac{(\ln x)^{2}}{2\ln 10}+C, with coefficient 12ln⁡10≈0.2171\frac{1}{2\ln 10}\approx 0.2171. Without the change of base, it is tempting to write (log⁡10x)22\frac{(\log_{10}x)^{2}}{2}, which is wrong: its derivative is log⁡10xxln⁡10\frac{\log_{10}x}{x\ln 10}, a factor ln⁡10\ln 10 is missing.

e)

∫xedx=xe+1e+1+C\int x^{e}dx=\frac{x^{e+1}}{e+1}+C: it is a POWER of xx with a constant exponent, so the power rule applies. ∫exdx=ex+C\int e^{x}dx=e^{x}+C: it is an EXPONENTIAL, the variable is in the exponent. ∫eedx=eex+C\int e^{e}dx=e^{e}x+C: it is a CONSTANT, about 15.1515.15, which integrates to eexe^{e}x. The rule depends on where the variable sits, never on what the symbols look like.

Exercise 12: Recovering a function from its second derivative and a tangent line

A function ff satisfies f′′(x)=6x−12f''(x)=6x-12 for every real xx, and the line with equation y=3x−2y=3x-2 is tangent to its graph at the point with xx-coordinate 11.

  • a) Write f′(x)f'(x) with a constant C1C_{1}. Which piece of information in the statement fixes C1C_{1}? Compute it.
  • b) Write f(x)f(x) with a constant C2C_{2}. Which second piece of information fixes C2C_{2}? Compute it.
  • c) Compute f(2)f(2), then check that f(x)=(x−2)3+2f(x)=(x-2)^{3}+2.
  • d) At what other point is the tangent line to the graph parallel to the line y=3x−2y=3x-2? Give its coordinates and the equation of this tangent line.
  • e) A student writes “f′(1)=3x−2f'(1)=3x-2 evaluated at 11, so f′(1)=1f'(1)=1”. What is the student confusing?

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  • a) f′(x)=3x2−12x+12f'(x)=3x^{2}-12x+12
  • b) f(x)=x3−6x2+12x−6f(x)=x^{3}-6x^{2}+12x-6
  • c) f(2)=2f(2)=2; f(x)=(x−2)3+2f(x)=(x-2)^{3}+2
  • d) (3,3)(3, 3), tangent line y=3x−6y=3x-6
  • e) The yy-value 11 is not the slope 33
a)

f′(x)=3x2−12x+C1f'(x)=3x^{2}-12x+C_{1}. The tangent line at x=1x=1 has slope 33, so f′(1)=3f'(1)=3: 3−12+C1=33-12+C_{1}=3, hence C1=12C_{1}=12 and f′(x)=3x2−12x+12f'(x)=3x^{2}-12x+12. The SLOPE of the tangent line fixes the constant of the derivative.

b)

f(x)=x3−6x2+12x+C2f(x)=x^{3}-6x^{2}+12x+C_{2}. The point of tangency lies both on the graph and on the tangent line: f(1)=3×1−2=1f(1)=3\times 1-2=1. So 1−6+12+C2=11-6+12+C_{2}=1, hence C2=−6C_{2}=-6 and f(x)=x3−6x2+12x−6f(x)=x^{3}-6x^{2}+12x-6. A tangent line provides TWO conditions, a slope and a point, exactly what two integrations need.

c)

f(2)=8−24+24−6=2f(2)=8-24+24-6=2. And (x−2)3+2=x3−6x2+12x−8+2=x3−6x2+12x−6(x-2)^{3}+2=x^{3}-6x^{2}+12x-8+2=x^{3}-6x^{2}+12x-6 ✓. The graph is that of x3x^{3} shifted 22 to the right and 22 up: (2,2)(2, 2) is its centre of symmetry and its inflection point, where f′′(x)=6x−12f''(x)=6x-12 is zero.

d)

We want f′(x)=3f'(x)=3: 3x2−12x+12=33x^{2}-12x+12=3, that is, x2−4x+3=0x^{2}-4x+3=0, with roots x=1x=1 and x=3x=3. The other point is (3,f(3))=(3,3)(3, f(3))=(3, 3), since f(3)=1+2=3f(3)=1+2=3. The tangent line there has equation y=3(x−3)+3=3x−6y=3(x-3)+3=3x-6, parallel to y=3x−2y=3x-2 without being the same line. The two points of tangency are symmetric about the centre (2,2)(2, 2), as the symmetry of the graph suggested.

e)

The student confuses the yy-VALUE of the line at x=1x=1, which is 11 and gives f(1)f(1), with its SLOPE, which is 33 and gives f′(1)f'(1). With f′(1)=1f'(1)=1, the student would find C1=10C_{1}=10 and everything after it would be wrong. The figure in the solution shows the graph and its two tangent lines of slope 33.

1234-6-4-2246810two tangent lines of slope 3(1, 1)(3, 3)

Exercise 13: Five antiderivatives taken from a test paper

Here are five answers taken from the same exam paper. For each one, say whether it is true or false by DIFFERENTIATING the proposed answer, and correct it if it is false.

  • a) ∫ln⁡x dx=1x+C\int\ln x\,dx=\frac{1}{x}+C.
  • b) ∫dx2x+1=ln⁡∣2x+1∣+C\int\frac{dx}{2x+1}=\ln|2x+1|+C.
  • c) ∫sec⁡xtan⁡x dx=sec⁡x+C\int\sec x\tan x\,dx=\sec x+C.
  • d) ∫e−xdx=e−x+C\int e^{-x}dx=e^{-x}+C.
  • e) ∫dx(1+x)2=−11+x+C\int\frac{dx}{(1+x)^{2}}=-\frac{1}{1+x}+C.

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  • a) False: xln⁡x−x+Cx\ln x-x+C
  • b) False: 12ln⁡∣2x+1∣+C\frac{1}{2}\ln|2x+1|+C
  • c) True
  • d) False: −e−x+C-e^{-x}+C
  • e) True
a)

FALSE. (1x)′=−1x2\left(\frac{1}{x}\right)'=-\frac{1}{x^{2}}, not ln⁡x\ln x: the paper gave the DERIVATIVE of ln⁡x\ln x instead of an antiderivative. The correct answer is xln⁡x−x+Cx\ln x-x+C, which we check: (xln⁡x−x)′=ln⁡x+1−1=ln⁡x\left(x\ln x-x\right)'=\ln x+1-1=\ln x ✓. It is obtained by parts in the next chapter.

b)

FALSE. (ln⁡∣2x+1∣)′=22x+1\left(\ln|2x+1|\right)'=\frac{2}{2x+1}: twice too much. The chain rule brings out the factor 22 of the linear argument, so you must divide: ∫dx2x+1=12ln⁡∣2x+1∣+C\int\frac{dx}{2x+1}=\frac{1}{2}\ln|2x+1|+C.

c)

TRUE. (sec⁡x)′=(1cos⁡x)′=sin⁡xcos⁡2x=sec⁡xtan⁡x\left(\sec x\right)'=\left(\frac{1}{\cos x}\right)'=\frac{\sin x}{\cos^{2}x}=\sec x\tan x ✓. It is a row of the table of derivatives, read backwards.

d)

FALSE. (e−x)′=−e−x\left(e^{-x}\right)'=-e^{-x}: the sign is wrong. The correct answer is −e−x+C-e^{-x}+C, since the argument −x-x has coefficient −1-1.

e)

TRUE. (−11+x)′=−(−1(1+x)2)=1(1+x)2\left(-\frac{1}{1+x}\right)'=-\left(-\frac{1}{(1+x)^{2}}\right)=\frac{1}{(1+x)^{2}} ✓. With u=1+xu=1+x: ∫u−2du=−u−1+C\int u^{-2}du=-u^{-1}+C. Verdict on the paper: two correct answers out of five, and the three wrong ones all fell to differentiation, in under a minute.

Exercise 14: Problem: the deflection of a cantilever beam

A horizontal beam of length L=3L=3 m is built into a wall at x=0x=0 and free at the other end. Under a distributed load, its deflection curve y(x)y(x) (in metres, negative downward) satisfies y′′(x)=−k(L−x)2y''(x)=-k\left(L-x\right)^{2} with k=0.0004k=0.0004 m−3^{-3}. The built-in end forces y(0)=0y(0)=0 and y′(0)=0y'(0)=0: the beam leaves the wall horizontally.

The figure below shows the situation; it is not to scale.

distributed loadL = 3 mfree endwall
  • a) Compute y′(x)y'(x) in terms of kk, LL and xx. Watch the sign produced by the argument L−xL-x.
  • b) Compute y(x)y(x) in terms of kk, LL and xx.
  • c) Show that the deflection at the free end is y(L)=−kL44y(L)=-\frac{kL^{4}}{4}, then compute it in millimetres.
  • d) Compute the slope y′(L)y'(L) at the end of the beam.
  • e) The beam is replaced by a beam with the same cross-section that is twice as long, under the same load per metre. By what factor is the deflection multiplied?

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  • a) y′(x)=k(L−x)33−kL33y'(x)=\frac{k(L-x)^{3}}{3}-\frac{kL^{3}}{3}
  • b) y(x)=−k(L−x)412−kL3x3+kL412y(x)=-\frac{k(L-x)^{4}}{12}-\frac{kL^{3}x}{3}+\frac{kL^{4}}{12}
  • c) y(L)=−kL44=−8.1y(L)=-\frac{kL^{4}}{4}=-8.1 mm
  • d) y′(L)=−0.0036y'(L)=-0.0036
  • e) Deflection in L4L^{4}: multiplied by 1616
a)

With u=L−xu=L-x, du=−dxdu=-dx: ∫−k(L−x)2dx=k∫u2du=k(L−x)33+C1\int-k(L-x)^{2}dx=k\int u^{2}du=\frac{k(L-x)^{3}}{3}+C_{1}. The minus sign of du=−dxdu=-dx has changed the sign of the antiderivative. The condition y′(0)=0y'(0)=0 gives kL33+C1=0\frac{kL^{3}}{3}+C_{1}=0, so y′(x)=k(L−x)33−kL33y'(x)=\frac{k(L-x)^{3}}{3}-\frac{kL^{3}}{3}.

b)

∫k(L−x)33dx=−k(L−x)412\int\frac{k(L-x)^{3}}{3}dx=-\frac{k(L-x)^{4}}{12}, by the same substitution. Hence y(x)=−k(L−x)412−kL33x+C2y(x)=-\frac{k(L-x)^{4}}{12}-\frac{kL^{3}}{3}x+C_{2}, and y(0)=0y(0)=0 gives −kL412+C2=0-\frac{kL^{4}}{12}+C_{2}=0: y(x)=−k(L−x)412−kL3x3+kL412y(x)=-\frac{k(L-x)^{4}}{12}-\frac{kL^{3}x}{3}+\frac{kL^{4}}{12}.

c)

At x=Lx=L, the first term vanishes: y(L)=−kL43+kL412=−4kL4−kL412=−kL44y(L)=-\frac{kL^{4}}{3}+\frac{kL^{4}}{12}=-\frac{4kL^{4}-kL^{4}}{12}=-\frac{kL^{4}}{4}. Numerically: −0.0004×814=−0.0081-\frac{0.0004\times 81}{4}=-0.0081 m, that is, a deflection of 8.18.1 mm downward.

d)

y′(L)=0−kL33=−0.0004×273=−0.0036y'(L)=0-\frac{kL^{3}}{3}=-\frac{0.0004\times 27}{3}=-0.0036. The beam drops 3.63.6 mm per metre at its end, where it is most steeply inclined.

e)

The deflection is proportional to L4L^{4}: doubling the length multiplies it by 24=162^{4}=16. That is why a balcony twice as deep does not need a beam twice as strong, but far more than that. The figure in the solution plots the deflection curve in millimetres.

0.511.522.53-10-8-6-4-22deflection: −8.1 mmx (m)y (mm)

Exercise 15: Problem: the sales of a game launched without advertising

A small studio launches a game with no advertising campaign: sales come from word of mouth, which starts slowly and then runs out of steam. The sales rate is modelled by S′(t)=5000 t e−t2/2S'(t)=5000\,t\,e^{-t^{2}/2} copies per week, with tt in weeks after release, and S(0)=0S(0)=0.

  • a) Using a substitution that you state, find S(t)S(t).
  • b) How many copies are sold during the first two weeks?
  • c) What value does S(t)S(t) approach as t→+∞t\to+\infty? Interpret.
  • d) After how many weeks will the studio have sold 9090 percent of that total?
  • e) At what time is the sales rate at its maximum, and how many copies per week are being sold then?

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  • a) S(t)=5000(1−e−t2/2)S(t)=5000\left(1-e^{-t^{2}/2}\right)
  • b) ≈4323\approx 4323 copies
  • c) 50005000 copies in total
  • d) t=2ln⁡10≈2.15t=\sqrt{2\ln 10}\approx 2.15 weeks
  • e) At t=1t=1 week, ≈3033\approx 3033 per week
a)

Set u=−t22u=-\frac{t^{2}}{2}, so du=−t dtdu=-t\,dt and t dt=−dut\,dt=-du: ∫5000 t e−t2/2dt=−5000∫eudu=−5000e−t2/2+C\int 5000\,t\,e^{-t^{2}/2}dt=-5000\int e^{u}du=-5000e^{-t^{2}/2}+C. The condition S(0)=0S(0)=0 gives −5000+C=0-5000+C=0, so C=5000C=5000 and S(t)=5000(1−e−t2/2)S(t)=5000\left(1-e^{-t^{2}/2}\right).

b)

S(2)=5000(1−e−2)≈5000×0.8647≈4323S(2)=5000\left(1-e^{-2}\right)\approx 5000\times 0.8647\approx 4323 copies.

c)

e−t2/2→0e^{-t^{2}/2}\to 0, so S(t)→5000S(t)\to 5000. The model predicts a total of 50005000 copies: that is exactly the constant of integration, which here measures the market that word of mouth will eventually reach.

d)

5000(1−e−t2/2)=45005000\left(1-e^{-t^{2}/2}\right)=4500 gives e−t2/2=0.1e^{-t^{2}/2}=0.1, that is, t22=ln⁡10\frac{t^{2}}{2}=\ln 10 and t=2ln⁡10≈2.15t=\sqrt{2\ln 10}\approx 2.15 weeks. Most of the sales therefore happen in just over two weeks.

e)

Differentiate the rate: (t e−t2/2)′=e−t2/2−t2e−t2/2=(1−t2)e−t2/2\left(t\,e^{-t^{2}/2}\right)'=e^{-t^{2}/2}-t^{2}e^{-t^{2}/2}=\left(1-t^{2}\right)e^{-t^{2}/2}, positive before t=1t=1 and negative after. The rate is at its maximum at t=1t=1 week and equals 5000e−1/2≈30335000e^{-1/2}\approx 3033 copies per week. The figure in the solution shows both curves: the rate peaks at the inflection point of the cumulative sales.

123410002000300040005000S(t), cumulative salesS′(t), sales rate5000
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Next chapter Partial fraction decomposition, 201-SN3-RE

© Ahmed Squalli Houssaini. Exercise set published at www.letuteurscientifique.ca/en/exercices/cegep-calc2-antiderivatives. Free for personal and classroom use; republishing it elsewhere requires written permission (legal notice).

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