MATH 140 Calculus 1 • McGill University, Montreal

Corrected exercises: antiderivatives (MATH 140)

This is the corrected exercise set for antiderivatives in MATH 140, Calculus 1, at McGill University, section 4.9 of Stewart and the last chapter of the course. It turns differentiation around: given ff, find every FF with F′=fF' = f. In MATH 141 the same family will be written as an indefinite integral; here it is simply the general antiderivative, and no area appears anywhere. Every number is exact and chosen to be done by hand, and each solution names the rule it reads backwards.

The thread running through the whole set: antidifferentiation has no product rule, no quotient rule and no chain rule, so the function is REWRITTEN first, as a sum of lines of the table, and every answer is CHECKED by differentiating it. The answer is a family: one constant per antidifferentiation and per interval of the domain, and only a condition, an initial value, a point, a tangency or continuity at a junction, picks one member.

The traps named in the solutions: the power rule applied to x−1x^{-1} or to 10x10^x, the product of two antiderivatives, the missing 1a\frac{1}{a} of a linear inside function, a division by the derivative of a nonlinear inside, ln⁡x\ln x written without its absolute value, a single constant forced across a gap in the domain, the same constant used twice for a second derivative, a condition that repeats another, and an antiderivative read as increasing because ff increases.

10 corrected exercises • 100 points • 150 minutes

Revision sheet for this chapter → Every MATH 140 chapter →

Self-checking set Type your answers under each question: the page tells you right or wrong before you open the solution. With an account, every answer right on the first try earns points.

Course recap

  • • FF is an antiderivative of ff on an interval II if F′=fF' = f on II; then every antiderivative on II is F+CF + C.
  • • xn↦xn+1n+1x^n \mapsto \frac{x^{n+1}}{n+1} for n≠−1n \ne -1; 1x↦ln⁡∣x∣\frac{1}{x} \mapsto \ln|x|; ex↦exe^x \mapsto e^x; bx↦bxln⁡bb^x \mapsto \frac{b^x}{\ln b}.
  • • cos⁡x↦sin⁡x\cos x \mapsto \sin x, sin⁡x↦−cos⁡x\sin x \mapsto -\cos x, sec⁡2x↦tan⁡x\sec^2 x \mapsto \tan x, csc⁡2x↦−cot⁡x\csc^2 x \mapsto -\cot x, sec⁡xtan⁡x↦sec⁡x\sec x\tan x \mapsto \sec x, csc⁡xcot⁡x↦−csc⁡x\csc x\cot x \mapsto -\csc x.
  • • 11+x2↦arctan⁡x\frac{1}{1 + x^2} \mapsto \arctan x; 11−x2↦arcsin⁡x\frac{1}{\sqrt{1 - x^2}} \mapsto \arcsin x on (−1,1)(-1, 1).
  • • Linear inside only: if F′=fF' = f and a≠0a \ne 0, then 1aF(ax+b)\frac{1}{a}F(ax + b) is an antiderivative of f(ax+b)f(ax + b).
  • • Motion: v′=av' = a and s′=vs' = v; the constants are v(0)v(0) and s(0)s(0), or come from continuity at a junction.

Part A: the basics (/50)

Exercise 1: The general antiderivative: read the table backwards, then differentiate

A function FF is an antiderivative of ff on an interval II when F′(x)=f(x)F'(x) = f(x) for every xx in II. If FF is one antiderivative, the most general antiderivative of ff on II is F(x)+CF(x) + C, with CC an arbitrary constant: two antiderivatives on an INTERVAL differ by a constant, a consequence of the Mean Value Theorem.

Every line of the table of antiderivatives is a line of the table of derivatives read from right to left, and so every answer can be checked in one line by differentiating it. That check is part of the answer on this set, and it is the only protection against a missing factor.

  • a) Find the most general antiderivative of f(x)=8x3−6x+3x4f(x) = 8x^3 - 6\sqrt{x} + \frac{3}{x^4}, and state the interval on which it is valid.
  • b) Same question for g(x)=5x+4ex−21+x2g(x) = \frac{5}{x} + 4e^x - \frac{2}{1 + x^2}.
  • c) Same question for h(θ)=3cos⁡θ−2sec⁡2θ+sec⁡θtan⁡θh(\theta) = 3\cos\theta - 2\sec^2\theta + \sec\theta\tan\theta.
  • d) Same question for k(x)=31−x2+10xk(x) = \frac{3}{\sqrt{1 - x^2}} + 10^x on (−1,1)(-1, 1). A student answers 3arcsin⁡x+10x+1x+1+C3\arcsin x + \frac{10^{x+1}}{x+1} + C: find the error by differentiating.
  • e) The table has no line for ln⁡x\ln x. Decide, by differentiating, which of F1(x)=xln⁡x−x+7F_1(x) = x\ln x - x + 7, F2(x)=(ln⁡x)22F_2(x) = \frac{(\ln x)^2}{2} and F3(x)=xln⁡xF_3(x) = x\ln x are antiderivatives of ln⁡x\ln x on (0,∞)(0, \infty).

Type your answers, the page tells you right or wrong 0/7

a)
b)
c)
d)
e)
Show the solution

Answers

  • a) F(x)=2x4−4x3/2−x−3+CF(x) = 2x^4 - 4x^{3/2} - x^{-3} + C on (0,∞)(0, \infty)
  • b) G(x)=5ln⁡∣x∣+4ex−2arctan⁡x+CG(x) = 5\ln|x| + 4e^x - 2\arctan x + C, one constant on (−∞,0)(-\infty, 0) and one on (0,∞)(0, \infty)
  • c) H(θ)=3sin⁡θ−2tan⁡θ+sec⁡θ+CH(\theta) = 3\sin\theta - 2\tan\theta + \sec\theta + C on each interval where cos⁡θ≠0\cos\theta \ne 0
  • d) K(x)=3arcsin⁡x+10xln⁡10+CK(x) = 3\arcsin x + \frac{10^x}{\ln 10} + C; the power rule does not apply to 10x10^x
  • e) Only F1F_1: F1′(x)=ln⁡xF_1'(x) = \ln x, F2′(x)=ln⁡xxF_2'(x) = \frac{\ln x}{x}, F3′(x)=ln⁡x+1F_3'(x) = \ln x + 1

a) Rewrite every term as a power of xx BEFORE reading the table: f(x)=8x3−6x1/2+3x−4f(x) = 8x^3 - 6x^{1/2} + 3x^{-4}. The power rule backwards, xn↦xn+1n+1x^n \mapsto \frac{x^{n+1}}{n+1} for n≠−1n \ne -1, gives 8⋅x44=2x48 \cdot \frac{x^4}{4} = 2x^4, then −6⋅x3/23/2=−4x3/2-6 \cdot \frac{x^{3/2}}{3/2} = -4x^{3/2}, then 3⋅x−3−3=−x−33 \cdot \frac{x^{-3}}{-3} = -x^{-3}. So F(x)=2x4−4x3/2−x−3+CF(x) = 2x^4 - 4x^{3/2} - x^{-3} + C. The domain of ff is (0,∞)(0, \infty), because of x\sqrt x and of x−4x^{-4} together: it is ONE interval, so one constant suffices. Check: F′(x)=8x3−4⋅32x1/2+3x−4=8x3−6x+3x4F'(x) = 8x^3 - 4 \cdot \frac{3}{2}x^{1/2} + 3x^{-4} = 8x^3 - 6\sqrt x + \frac{3}{x^4}. The classic slip is 3x4↦3x5⋅15\frac{3}{x^4} \mapsto \frac{3}{x^5} \cdot \frac{1}{5}, raising the exponent in the denominator: the exponent of x−4x^{-4} goes UP to −3-3, and the differentiation catches the error at once.

b) 5⋅1x5 \cdot \frac{1}{x} comes from 5ln⁡∣x∣5\ln|x|, 4ex4e^x from 4ex4e^x, and −21+x2-\frac{2}{1 + x^2} from −2arctan⁡x-2\arctan x, since (arctan⁡x)′=11+x2(\arctan x)' = \frac{1}{1 + x^2}. Check: G′(x)=5x+4ex−21+x2G'(x) = \frac{5}{x} + 4e^x - \frac{2}{1 + x^2}. The domain of gg is x≠0x \ne 0, which is TWO intervals, (−∞,0)(-\infty, 0) and (0,∞)(0, \infty): the most general antiderivative carries one constant on each, G(x)=5ln⁡∣x∣+4ex−2arctan⁡x+C1G(x) = 5\ln|x| + 4e^x - 2\arctan x + C_1 for x>0x > 0 and +C2+ C_2 for x<0x < 0. Exercise 5 is devoted to this. Writing ln⁡x\ln x without the absolute value gives an antiderivative on (0,∞)(0, \infty) only, and loses half of the domain.

c) Read three lines of the derivative table backwards: (sin⁡θ)′=cos⁡θ(\sin\theta)' = \cos\theta, (tan⁡θ)′=sec⁡2θ(\tan\theta)' = \sec^2\theta, (sec⁡θ)′=sec⁡θtan⁡θ(\sec\theta)' = \sec\theta\tan\theta. So H(θ)=3sin⁡θ−2tan⁡θ+sec⁡θ+CH(\theta) = 3\sin\theta - 2\tan\theta + \sec\theta + C. Check: H′(θ)=3cos⁡θ−2sec⁡2θ+sec⁡θtan⁡θH'(\theta) = 3\cos\theta - 2\sec^2\theta + \sec\theta\tan\theta. The signs are where the marks go: the antiderivative of cos⁡\cos is +sin⁡+\sin, of sin⁡\sin is −cos⁡-\cos, and a student who remembers only that a minus sign appears somewhere gets half of them wrong. The domain excludes the zeros of cos⁡θ\cos\theta, so the formula holds on each interval (−π2+kπ,π2+kπ)\left(-\frac{\pi}{2} + k\pi, \frac{\pi}{2} + k\pi\right), with its own constant.

d) (arcsin⁡x)′=11−x2(\arcsin x)' = \frac{1}{\sqrt{1 - x^2}} on (−1,1)(-1, 1), and (10x)′=10xln⁡10(10^x)' = 10^x \ln 10, so 10x10^x comes from 10xln⁡10\frac{10^x}{\ln 10}: K(x)=3arcsin⁡x+10xln⁡10+CK(x) = 3\arcsin x + \frac{10^x}{\ln 10} + C. Check: K′(x)=31−x2+10xln⁡10ln⁡10K'(x) = \frac{3}{\sqrt{1 - x^2}} + \frac{10^x \ln 10}{\ln 10}. The student's term 10x+1x+1\frac{10^{x+1}}{x+1} applies the power rule to an EXPONENTIAL: the variable is in the exponent, not in the base. Differentiating it by the quotient rule gives 10x+1ln⁡10⋅(x+1)−10x+1(x+1)2\frac{10^{x+1}\ln 10 \cdot (x+1) - 10^{x+1}}{(x+1)^2}, which at x=0x = 0 equals 10ln⁡10−10≈1310\ln 10 - 10 \approx 13, while 100=110^0 = 1. The power rule is for xnx^n with a fixed exponent, never for bxb^x.

e) F1′(x)=(1⋅ln⁡x+x⋅1x)−1+0=ln⁡xF_1'(x) = \left(1 \cdot \ln x + x \cdot \frac{1}{x}\right) - 1 + 0 = \ln x, by the product rule: F1F_1 IS an antiderivative of ln⁡x\ln x, and the constant 77 changes nothing. F2′(x)=2ln⁡x2⋅1x=ln⁡xxF_2'(x) = \frac{2\ln x}{2} \cdot \frac{1}{x} = \frac{\ln x}{x}, by the chain rule with inner function ln⁡x\ln x: not ln⁡x\ln x. F3′(x)=ln⁡x+1F_3'(x) = \ln x + 1: off by the constant 11, so no. Only F1F_1 works, and the general antiderivative is xln⁡x−x+Cx\ln x - x + C. No line of the table produced it, and none will until MATH 141; but checking a PROPOSED antiderivative needs nothing more than the rules of differentiation, which is why a claimed antiderivative is never accepted without the check.

Tick the exercises you have done or want to review: a free account, no password, keeps your ticks from one visit to the next and tells you which chapter to tackle next. Create your space, an email is enough.

Exercise 2: Rewrite before antidifferentiating: no product rule and no quotient rule backwards

The derivative table has a product rule, a quotient rule and a chain rule. The antiderivative table has NONE of them: the antiderivative of a product is not the product of the antiderivatives, and the antiderivative of a quotient is not the quotient. Before any table is read, the function is rewritten as a SUM of table entries, by expanding, by splitting a fraction over a single-term denominator, or by a long division.

One composition is allowed in MATH 140, the one with a LINEAR inside function: if F′=fF' = f and a≠0a \ne 0, then 1aF(ax+b)\frac{1}{a}F(ax + b) is an antiderivative of f(ax+b)f(ax + b). It is guessed, then proved by the chain rule, never assumed.

  • a) Find the most general antiderivative of p(x)=(x2+1)(2x−3)p(x) = (x^2 + 1)(2x - 3). A student answers (x33+x)(x2−3x)+C\left(\frac{x^3}{3} + x\right)(x^2 - 3x) + C: show that it is wrong by comparing derivatives at x=1x = 1.
  • b) Same question for q(x)=x4−3x2+6x3q(x) = \frac{x^4 - 3x^2 + 6}{x^3}.
  • c) Same question for r(x)=x2x2+1r(x) = \frac{x^2}{x^2 + 1}. Hint: add and subtract 11 in the numerator.
  • d) Same question for s(x)=x+3x+1s(x) = \frac{x + 3}{x + 1}. Guess the antiderivative of 1x+1\frac{1}{x + 1} and verify it.
  • e) Prove the rule for f(ax+b)f(ax + b) stated above, then find antiderivatives of (3x−1)4(3x - 1)^4 and of e5−2xe^{5 - 2x}. A student writes (3x−1)55\frac{(3x - 1)^5}{5}: what does its derivative give?

Type your answers, the page tells you right or wrong 0/9

a)
b)
c)
d)
e)
Show the solution

Answers

  • a) x42−x3+x2−3x+C\frac{x^4}{2} - x^3 + x^2 - 3x + C; at x=1x = 1 the student's derivative is −163-\frac{16}{3}, not p(1)=−2p(1) = -2
  • b) x22−3ln⁡∣x∣−3x2+C\frac{x^2}{2} - 3\ln|x| - \frac{3}{x^2} + C, one constant on each side of 00
  • c) x−arctan⁡x+Cx - \arctan x + C
  • d) x+2ln⁡∣x+1∣+Cx + 2\ln|x + 1| + C, one constant on each side of −1-1
  • e) (3x−1)515+C\frac{(3x - 1)^5}{15} + C and −12e5−2x+C-\frac{1}{2}e^{5 - 2x} + C; the student's answer differentiates to 3(3x−1)43(3x - 1)^4

a) Expand first: p(x)=2x3−3x2+2x−3p(x) = 2x^3 - 3x^2 + 2x - 3, a sum of powers. Term by term, P(x)=x42−x3+x2−3x+CP(x) = \frac{x^4}{2} - x^3 + x^2 - 3x + C, and P′(x)=2x3−3x2+2x−3=p(x)P'(x) = 2x^3 - 3x^2 + 2x - 3 = p(x). The student multiplied the antiderivatives of the two factors, x33+x\frac{x^3}{3} + x and x2−3xx^2 - 3x. By the product rule, the derivative of that product is (x2+1)(x2−3x)+(x33+x)(2x−3)(x^2 + 1)(x^2 - 3x) + \left(\frac{x^3}{3} + x\right)(2x - 3), which at x=1x = 1 equals 2⋅(−2)+43⋅(−1)=−1632 \cdot (-2) + \frac{4}{3} \cdot (-1) = -\frac{16}{3}, while p(1)=2⋅(−1)=−2p(1) = 2 \cdot (-1) = -2. One point of disagreement is enough to reject a candidate. The reason is structural: differentiating a product produces TWO terms, so undoing a product cannot give one.

b) Split over the single-term denominator: q(x)=x4x3−3x2x3+6x3=x−3x+6x−3q(x) = \frac{x^4}{x^3} - \frac{3x^2}{x^3} + \frac{6}{x^3} = x - \frac{3}{x} + 6x^{-3}. Now each term is in the table: x22\frac{x^2}{2}, then −3ln⁡∣x∣-3\ln|x| (the exponent −1-1 is the one case of the power rule that does NOT apply), then 6⋅x−2−2=−3x−26 \cdot \frac{x^{-2}}{-2} = -3x^{-2}. So Q(x)=x22−3ln⁡∣x∣−3x2+CQ(x) = \frac{x^2}{2} - 3\ln|x| - \frac{3}{x^2} + C, with a constant on each of (−∞,0)(-\infty, 0) and (0,∞)(0, \infty). Check: Q′(x)=x−3x+6x−3Q'(x) = x - \frac{3}{x} + 6x^{-3}. Dividing a sum by a single term is legal term by term; dividing BY a sum, 1x2+1\frac{1}{x^2 + 1}, is not, and c) shows what to do then.

c) The denominator is a sum, so the fraction does not split. Make the numerator contain the denominator: x2x2+1=(x2+1)−1x2+1=1−1x2+1\frac{x^2}{x^2 + 1} = \frac{(x^2 + 1) - 1}{x^2 + 1} = 1 - \frac{1}{x^2 + 1}, the result of a long division. Both pieces are in the table: R(x)=x−arctan⁡x+CR(x) = x - \arctan x + C, valid on all of R\mathbb{R}, a single interval. Check: R′(x)=1−11+x2=x21+x2R'(x) = 1 - \frac{1}{1 + x^2} = \frac{x^2}{1 + x^2}. A student who writes x3/3arctan⁡x\frac{x^3/3}{\arctan x}, the quotient of two antiderivatives, obtains a function whose derivative has nothing to do with rr: the quotient rule does not run backwards either.

d) Same gesture: x+3x+1=(x+1)+2x+1=1+2x+1\frac{x + 3}{x + 1} = \frac{(x + 1) + 2}{x + 1} = 1 + \frac{2}{x + 1}. For 1x+1\frac{1}{x + 1}, guess ln⁡∣x+1∣\ln|x + 1| and verify with the chain rule, inner function u=x+1u = x + 1 with u′=1u' = 1: ddxln⁡∣x+1∣=1x+1⋅1\frac{d}{dx}\ln|x + 1| = \frac{1}{x + 1} \cdot 1. So S(x)=x+2ln⁡∣x+1∣+CS(x) = x + 2\ln|x + 1| + C, one constant on (−∞,−1)(-\infty, -1) and one on (−1,∞)(-1, \infty). Check: S′(x)=1+2x+1=x+3x+1S'(x) = 1 + \frac{2}{x + 1} = \frac{x + 3}{x + 1}. Here the inner derivative is 11 and no factor appears; in e) it is not 11.

e) If F′=fF' = f, the chain rule with inner function u=ax+bu = ax + b, u′=au' = a, gives ddx[1aF(ax+b)]=1a⋅f(ax+b)⋅a=f(ax+b)\frac{d}{dx}\left[\frac{1}{a}F(ax + b)\right] = \frac{1}{a} \cdot f(ax + b) \cdot a = f(ax + b), which proves the rule; a≠0a \ne 0 is needed to divide. For (3x−1)4(3x - 1)^4: F(u)=u55F(u) = \frac{u^5}{5} and a=3a = 3, so (3x−1)515+C\frac{(3x - 1)^5}{15} + C. For e5−2xe^{5 - 2x}: a=−2a = -2, so −12e5−2x+C-\frac{1}{2}e^{5 - 2x} + C, and the check gives −12⋅e5−2x⋅(−2)=e5−2x-\frac{1}{2} \cdot e^{5 - 2x} \cdot (-2) = e^{5 - 2x}. The student's (3x−1)55\frac{(3x - 1)^5}{5} differentiates to (3x−1)4⋅3(3x - 1)^4 \cdot 3, three times too much: the factor 1a\frac{1}{a} is exactly what the chain rule will put back. The rule works only because aa is a CONSTANT; with x2+1x^2 + 1 inside, dividing by 2x2x fails, as Exercise 8 shows.

Exercise 3: Trigonometric functions: an identity first, then the table

The table knows six trigonometric antiderivatives, those of cos⁡x\cos x, sin⁡x\sin x, sec⁡2x\sec^2 x, csc⁡2x\csc^2 x, sec⁡xtan⁡x\sec x\tan x and csc⁡xcot⁡x\csc x\cot x. It knows neither cos⁡2x\cos^2 x, nor a quotient of trigonometric functions, nor a square of a sum. Each function below becomes a sum of table entries after ONE identity: sin⁡2x+cos⁡2x=1\sin^2 x + \cos^2 x = 1, cos⁡2x=cos⁡2x−sin⁡2x\cos 2x = \cos^2 x - \sin^2 x, the half-angle forms cos⁡2x=1+cos⁡2x2\cos^2 x = \frac{1 + \cos 2x}{2} and sin⁡2x=1−cos⁡2x2\sin^2 x = \frac{1 - \cos 2x}{2}, or a multiplication by a conjugate.

Work on an interval where every expression is defined, and check each answer by differentiating.

  • a) Find the most general antiderivative of sec⁡x(sec⁡x+tan⁡x)\sec x(\sec x + \tan x) on (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right).
  • b) Same question for cos⁡2xcos⁡x−sin⁡x\frac{\cos 2x}{\cos x - \sin x} on (−3π4,π4)\left(-\frac{3\pi}{4}, \frac{\pi}{4}\right).
  • c) Same question for 11+cos⁡x\frac{1}{1 + \cos x} on (0,π)(0, \pi). Hint: multiply numerator and denominator by 1−cos⁡x1 - \cos x.
  • d) Same question for cos⁡2x\cos^2 x on R\mathbb{R}.
  • e) A student writes that an antiderivative of sin⁡2x\sin^2 x is sin⁡3x3\frac{\sin^3 x}{3}. Differentiate it to find the error, then give a correct antiderivative.

Type your answers, the page tells you right or wrong 0/6

a)
b)
c)
d)
e)
Show the solution

Answers

  • a) tan⁡x+sec⁡x+C\tan x + \sec x + C
  • b) sin⁡x−cos⁡x+C\sin x - \cos x + C
  • c) csc⁡x−cot⁡x+C\csc x - \cot x + C
  • d) x2+sin⁡2x4+C\frac{x}{2} + \frac{\sin 2x}{4} + C
  • e) (sin⁡3x3)′=sin⁡2xcos⁡x\left(\frac{\sin^3 x}{3}\right)' = \sin^2 x\cos x; correct: x2−sin⁡2x4+C\frac{x}{2} - \frac{\sin 2x}{4} + C

a) Distribute: sec⁡x(sec⁡x+tan⁡x)=sec⁡2x+sec⁡xtan⁡x\sec x(\sec x + \tan x) = \sec^2 x + \sec x\tan x, two lines of the table. So the answer is tan⁡x+sec⁡x+C\tan x + \sec x + C on (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right), where cos⁡x≠0\cos x \ne 0. Check: (tan⁡x+sec⁡x)′=sec⁡2x+sec⁡xtan⁡x(\tan x + \sec x)' = \sec^2 x + \sec x\tan x. Nothing here needs more than expanding a product, the gesture of Exercise 2 a): products are opened before the table is read, whatever the functions.

b) Factor the numerator with cos⁡2x=cos⁡2x−sin⁡2x=(cos⁡x−sin⁡x)(cos⁡x+sin⁡x)\cos 2x = \cos^2 x - \sin^2 x = (\cos x - \sin x)(\cos x + \sin x). On the given interval cos⁡x−sin⁡x≠0\cos x - \sin x \ne 0 (it vanishes only at x=π4+kπx = \frac{\pi}{4} + k\pi), so the factor cancels: the function is cos⁡x+sin⁡x\cos x + \sin x, and its antiderivative is sin⁡x−cos⁡x+C\sin x - \cos x + C. Check: (sin⁡x−cos⁡x)′=cos⁡x+sin⁡x(\sin x - \cos x)' = \cos x + \sin x. The cancellation is legitimate only where the factor is not zero, and naming the interval says exactly that. Without the identity, no rule of the table touches a quotient.

c) On (0,π)(0, \pi), 1+cos⁡x≠01 + \cos x \ne 0 and sin⁡x≠0\sin x \ne 0. Multiply by the conjugate: 11+cos⁡x⋅1−cos⁡x1−cos⁡x=1−cos⁡x1−cos⁡2x=1−cos⁡xsin⁡2x\frac{1}{1 + \cos x} \cdot \frac{1 - \cos x}{1 - \cos x} = \frac{1 - \cos x}{1 - \cos^2 x} = \frac{1 - \cos x}{\sin^2 x}. Split over the single-term denominator: 1sin⁡2x−cos⁡xsin⁡2x=csc⁡2x−csc⁡xcot⁡x\frac{1}{\sin^2 x} - \frac{\cos x}{\sin^2 x} = \csc^2 x - \csc x\cot x. Read backwards: (−cot⁡x)′=csc⁡2x(-\cot x)' = \csc^2 x and (−csc⁡x)′=csc⁡xcot⁡x(-\csc x)' = \csc x\cot x, so the antiderivative is −cot⁡x+csc⁡x+C-\cot x + \csc x + C. Check: (csc⁡x−cot⁡x)′=−csc⁡xcot⁡x+csc⁡2x(\csc x - \cot x)' = -\csc x\cot x + \csc^2 x. At x=π2x = \frac{\pi}{2}, the function is 11+0=1\frac{1}{1 + 0} = 1 and the check gives −1⋅0+1=1-1 \cdot 0 + 1 = 1. The two minus signs of (cot⁡x)′(\cot x)' and (csc⁡x)′(\csc x)' are where this question is lost.

d) The half-angle identity turns a square into a first power: cos⁡2x=12+12cos⁡2x\cos^2 x = \frac{1}{2} + \frac{1}{2}\cos 2x. The second term has a linear inside function, 2x2x, so by the rule of Exercise 2 e) its antiderivative is 12⋅sin⁡2x2\frac{1}{2} \cdot \frac{\sin 2x}{2}. Hence x2+sin⁡2x4+C\frac{x}{2} + \frac{\sin 2x}{4} + C. Check: 12+2cos⁡2x4=1+cos⁡2x2=cos⁡2x\frac{1}{2} + \frac{2\cos 2x}{4} = \frac{1 + \cos 2x}{2} = \cos^2 x. Forgetting the 12\frac{1}{2} of the linear rule gives x2+sin⁡2x2\frac{x}{2} + \frac{\sin 2x}{2}, whose derivative 12+cos⁡2x\frac{1}{2} + \cos 2x reaches 32\frac{3}{2} at x=0x = 0, more than the maximum 11 of cos⁡2x\cos^2 x.

e) By the chain rule with inner function sin⁡x\sin x: (sin⁡3x3)′=3sin⁡2x3⋅cos⁡x=sin⁡2xcos⁡x\left(\frac{\sin^3 x}{3}\right)' = \frac{3\sin^2 x}{3} \cdot \cos x = \sin^2 x\cos x. The factor cos⁡x\cos x, the derivative of the inside, is the proof that the power rule does not apply to a POWER OF A FUNCTION: it applies to a power of xx. At x=π3x = \frac{\pi}{3} the student's derivative is 34⋅12=38\frac{3}{4} \cdot \frac{1}{2} = \frac{3}{8}, while sin⁡2π3=34\sin^2\frac{\pi}{3} = \frac{3}{4}. The right way is the other half-angle identity, sin⁡2x=1−cos⁡2x2\sin^2 x = \frac{1 - \cos 2x}{2}, which gives x2−sin⁡2x4+C\frac{x}{2} - \frac{\sin 2x}{4} + C. Check: 12−cos⁡2x2=sin⁡2x\frac{1}{2} - \frac{\cos 2x}{2} = \sin^2 x. Adding d) and e): the antiderivative of cos⁡2x+sin⁡2x=1\cos^2 x + \sin^2 x = 1 is x2+x2=x\frac{x}{2} + \frac{x}{2} = x, as it must be.

Exercise 4: Initial value problems: one condition for each constant

An initial value problem gives a derivative and one or more values of the unknown function, and asks for THE function. The method never changes: antidifferentiate, writing the constant at the very line where it appears; then use each condition to find one constant; then check both the equation and the conditions.

Each antidifferentiation brings its own constant. A second derivative therefore produces two constants, f(x)=G(x)+Cx+Df(x) = G(x) + Cx + D, and needs two conditions.

  • a) Find ff if f′(x)=3x2−4x+1f'(x) = 3x^2 - 4x + 1 and f(2)=5f(2) = 5.
  • b) Find ff if f′(x)=x (3−x)f'(x) = \sqrt{x}\,(3 - x) for x>0x > 0 and f(4)=0f(4) = 0. Then give f(1)f(1).
  • c) Find ff if f′(x)=11+x2f'(x) = \frac{1}{1 + x^2} and f(1)=0f(1) = 0. Then give f(−1)f(-1) and lim⁡x→∞f(x)\lim_{x\to\infty} f(x).
  • d) Find ff if f′′(x)=6x+2f''(x) = 6x + 2, f(0)=1f(0) = 1 and f(1)=4f(1) = 4.
  • e) Find ff if f′′(x)=12x2+4e2xf''(x) = 12x^2 + 4e^{2x}, f(0)=0f(0) = 0 and f′(0)=1f'(0) = 1. A student writes f′(x)=4x3+2e2x+Cf'(x) = 4x^3 + 2e^{2x} + C, then f(x)=x4+e2x+Cf(x) = x^4 + e^{2x} + C: find what is wrong.

Type your answers, the page tells you right or wrong 0/9

a)
b)
c)
d)
e)
Show the solution

Answers

  • a) f(x)=x3−2x2+x+3f(x) = x^3 - 2x^2 + x + 3
  • b) f(x)=2x3/2−25x5/2−165f(x) = 2x^{3/2} - \frac{2}{5}x^{5/2} - \frac{16}{5}, and f(1)=−85f(1) = -\frac{8}{5}
  • c) f(x)=arctan⁡x−π4f(x) = \arctan x - \frac{\pi}{4}; f(−1)=−π2f(-1) = -\frac{\pi}{2}; limit π4\frac{\pi}{4}
  • d) f(x)=x3+x2+x+1f(x) = x^3 + x^2 + x + 1
  • e) f(x)=x4+e2x−x−1f(x) = x^4 + e^{2x} - x - 1; the student lost the term CxCx and used one constant for two

a) The general antiderivative is f(x)=x3−2x2+x+Cf(x) = x^3 - 2x^2 + x + C, the constant written at once. The condition gives f(2)=8−8+2+C=2+C=5f(2) = 8 - 8 + 2 + C = 2 + C = 5, so C=3C = 3 and f(x)=x3−2x2+x+3f(x) = x^3 - 2x^2 + x + 3. Check: f′(x)=3x2−4x+1f'(x) = 3x^2 - 4x + 1 and f(2)=8−8+2+3=5f(2) = 8 - 8 + 2 + 3 = 5. The student who writes f(x)=x3−2x2+xf(x) = x^3 - 2x^2 + x and then notices that f(2)=2≠5f(2) = 2 \ne 5 has nowhere to go: without CC, the condition cannot be satisfied, and the question loses all its marks at the very first line.

b) Expand before reading the table: f′(x)=3x1/2−x3/2f'(x) = 3x^{1/2} - x^{3/2}. Then f(x)=3⋅x3/23/2−x5/25/2+C=2x3/2−25x5/2+Cf(x) = 3 \cdot \frac{x^{3/2}}{3/2} - \frac{x^{5/2}}{5/2} + C = 2x^{3/2} - \frac{2}{5}x^{5/2} + C. With 43/2=84^{3/2} = 8 and 45/2=324^{5/2} = 32: f(4)=16−645+C=165+C=0f(4) = 16 - \frac{64}{5} + C = \frac{16}{5} + C = 0, so C=−165C = -\frac{16}{5}. Then f(1)=2−25−165=−85f(1) = 2 - \frac{2}{5} - \frac{16}{5} = -\frac{8}{5}. Check: f′(x)=3x1/2−x3/2=x (3−x)f'(x) = 3x^{1/2} - x^{3/2} = \sqrt{x}\,(3 - x). Evaluating 45/24^{5/2} as (4)5=25(\sqrt 4)^5 = 2^5, root first, keeps the numbers small without a calculator.

c) f(x)=arctan⁡x+Cf(x) = \arctan x + C on R\mathbb{R}, one interval, one constant. f(1)=π4+C=0f(1) = \frac{\pi}{4} + C = 0 gives C=−π4C = -\frac{\pi}{4}. Then f(−1)=−π4−π4=−π2f(-1) = -\frac{\pi}{4} - \frac{\pi}{4} = -\frac{\pi}{2}, since arctan⁡\arctan is odd, and lim⁡x→∞f(x)=π2−π4=π4\lim_{x\to\infty} f(x) = \frac{\pi}{2} - \frac{\pi}{4} = \frac{\pi}{4}. The answers are exact: C=−π4C = -\frac{\pi}{4}, never −0.785-0.785. The limit shows something the formula makes plain: this ff increases for ever, since f′>0f' > 0, and yet stays below π4\frac{\pi}{4}.

d) First antiderivative: f′(x)=3x2+2x+Cf'(x) = 3x^2 + 2x + C. Second: f(x)=x3+x2+Cx+Df(x) = x^3 + x^2 + Cx + D. Two constants, two conditions: f(0)=D=1f(0) = D = 1, then f(1)=1+1+C+1=4f(1) = 1 + 1 + C + 1 = 4, so C=1C = 1. Hence f(x)=x3+x2+x+1f(x) = x^3 + x^2 + x + 1. Check: f′(x)=3x2+2x+1f'(x) = 3x^2 + 2x + 1, f′′(x)=6x+2f''(x) = 6x + 2, f(0)=1f(0) = 1, f(1)=4f(1) = 4. The two conditions here are both on ff, at two different points: nothing requires one of them to be on f′f', only that together they fix both constants.

e) f′(x)=4x3+2e2x+C1f'(x) = 4x^3 + 2e^{2x} + C_1, using the linear rule for e2xe^{2x}. f′(0)=2+C1=1f'(0) = 2 + C_1 = 1, so C1=−1C_1 = -1. Then f(x)=x4+e2x−x+C2f(x) = x^4 + e^{2x} - x + C_2, and f(0)=1+C2=0f(0) = 1 + C_2 = 0, so C2=−1C_2 = -1: f(x)=x4+e2x−x−1f(x) = x^4 + e^{2x} - x - 1. Check: f′(x)=4x3+2e2x−1f'(x) = 4x^3 + 2e^{2x} - 1, f′′(x)=12x2+4e2xf''(x) = 12x^2 + 4e^{2x}, f′(0)=1f'(0) = 1, f(0)=0f(0) = 0. The student made two errors in one line: the antiderivative of the constant CC is CxCx, not CC, and a second antidifferentiation brings a NEW constant. His f(x)=x4+e2x+Cf(x) = x^4 + e^{2x} + C has f′(0)=2f'(0) = 2 whatever CC is, so the condition f′(0)=1f'(0) = 1 can never hold. Name the constants C1C_1, C2C_2 from the start and find C1C_1 BEFORE the second antidifferentiation.

Exercise 5: One constant per interval: when the domain has a gap

The statement two antiderivatives differ by a constant comes from the Mean Value Theorem: if F′=G′F' = G' on an INTERVAL, then F−GF - G has zero derivative there, so it is constant. On a domain made of several intervals, the theorem applies on each piece separately, and the constant may change from one piece to the next.

The figure shows y=ln⁡∣x∣y = \ln|x| in blue and another function GG in orange, defined for x≠0x \ne 0: on each side of 00, the orange curve is the blue one moved vertically. The red points are on the graph of GG.

-4-3-2-11234-3-2-1123y = ln|x|y = G(x)(1, 1)(-1, -1)x
  • a) Prove that ddxln⁡∣x∣=1x\frac{d}{dx}\ln|x| = \frac{1}{x} for every x≠0x \ne 0, treating x>0x > 0 and x<0x < 0 separately.
  • b) Read GG on the figure and write its formula. Show that G′(x)=1xG'(x) = \frac{1}{x} for every x≠0x \ne 0, and yet that G−ln⁡∣x∣G - \ln|x| is not constant. Why is there no contradiction? Write the most general antiderivative of 1x\frac{1}{x}.
  • c) Find ff such that f′(x)=1x2f'(x) = \frac{1}{x^2} for x≠0x \ne 0, f(1)=0f(1) = 0 and f(−1)=0f(-1) = 0. A classmate claims that no such ff exists, because −1x+1-\frac{1}{x} + 1 gives f(−1)=2f(-1) = 2: answer him.
  • d) Find ff on (−π2,3π2)\left(-\frac{\pi}{2}, \frac{3\pi}{2}\right) minus the point π2\frac{\pi}{2} such that f′(x)=sec⁡2xf'(x) = \sec^2 x, f(0)=0f(0) = 0 and f(π)=1f(\pi) = 1.
  • e) Find ff such that f′(x)=1x−2f'(x) = \frac{1}{x - 2} for x≠2x \ne 2, f(3)=0f(3) = 0 and f(0)=1f(0) = 1.

Type your answers, the page tells you right or wrong 0/8

b)
c)
d)
e)
Show the solution

Answers

  • a) For x>0x > 0, (ln⁡x)′=1x(\ln x)' = \frac{1}{x}; for x<0x < 0, (ln⁡(−x))′=−1−x=1x(\ln(-x))' = \frac{-1}{-x} = \frac{1}{x}
  • b) G(x)=ln⁡x+1G(x) = \ln x + 1 for x>0x > 0, ln⁡(−x)−1\ln(-x) - 1 for x<0x < 0; G−ln⁡∣x∣G - \ln|x| is 11 on the right, −1-1 on the left; general: ln⁡∣x∣+C1\ln|x| + C_1 (x>0x > 0), ln⁡∣x∣+C2\ln|x| + C_2 (x<0x < 0)
  • c) f(x)=1−1xf(x) = 1 - \frac{1}{x} for x>0x > 0 and f(x)=−1−1xf(x) = -1 - \frac{1}{x} for x<0x < 0
  • d) f(x)=tan⁡xf(x) = \tan x on (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right) and f(x)=tan⁡x+1f(x) = \tan x + 1 on (π2,3π2)\left(\frac{\pi}{2}, \frac{3\pi}{2}\right)
  • e) f(x)=ln⁡∣x−2∣f(x) = \ln|x - 2| for x>2x > 2 and f(x)=ln⁡∣x−2∣+1−ln⁡2f(x) = \ln|x - 2| + 1 - \ln 2 for x<2x < 2

a) For x>0x > 0, ∣x∣=x|x| = x and (ln⁡x)′=1x(\ln x)' = \frac{1}{x} from the table. For x<0x < 0, ∣x∣=−x>0|x| = -x > 0 and, by the chain rule with inner function u=−xu = -x, u′=−1u' = -1: (ln⁡(−x))′=1−x⋅(−1)=1x(\ln(-x))' = \frac{1}{-x} \cdot (-1) = \frac{1}{x}. So ln⁡∣x∣\ln|x| is an antiderivative of 1x\frac{1}{x} on (−∞,0)(-\infty, 0) AND on (0,∞)(0, \infty). Writing ln⁡x\ln x alone covers only the right half: on (−∞,0)(-\infty, 0), ln⁡x\ln x is not even defined, while 1x\frac{1}{x} is.

b) The orange right branch passes through (1,1)(1, 1) and is the blue one shifted up by 11: G(x)=ln⁡x+1G(x) = \ln x + 1 for x>0x > 0. The left branch passes through (−1,−1)(-1, -1) where ln⁡∣−1∣=0\ln|{-1}| = 0, so it is shifted DOWN by 11: G(x)=ln⁡(−x)−1G(x) = \ln(-x) - 1 for x<0x < 0. On each side, adding a constant does not change the derivative, so G′(x)=1xG'(x) = \frac{1}{x} for every x≠0x \ne 0. Yet G(x)−ln⁡∣x∣G(x) - \ln|x| equals 11 for x>0x > 0 and −1-1 for x<0x < 0: not constant. No contradiction, because the domain x≠0x \ne 0 is not an interval, and the Mean Value Theorem only works between two points of an interval on which the function is differentiable; 11 and −1-1 are separated by the hole at 00. The most general antiderivative of 1x\frac{1}{x} is ln⁡∣x∣+C1\ln|x| + C_1 for x>0x > 0 and ln⁡∣x∣+C2\ln|x| + C_2 for x<0x < 0, two independent constants.

c) On each interval, f(x)=−1x+Cf(x) = -\frac{1}{x} + C, since (−x−1)′=x−2\left(-x^{-1}\right)' = x^{-2}. For x>0x > 0: f(1)=−1+C1=0f(1) = -1 + C_1 = 0, so C1=1C_1 = 1. For x<0x < 0: f(−1)=1+C2=0f(-1) = 1 + C_2 = 0, so C2=−1C_2 = -1. Hence f(x)=1−1xf(x) = 1 - \frac{1}{x} for x>0x > 0 and f(x)=−1−1xf(x) = -1 - \frac{1}{x} for x<0x < 0. Check: f′(x)=1x2f'(x) = \frac{1}{x^2} on both sides, f(1)=0f(1) = 0, f(−1)=−1+1=0f(-1) = -1 + 1 = 0. The classmate forced ONE constant on a domain with two pieces; with one condition per piece, the problem has exactly one solution. The two conditions are not redundant: f(1)=0f(1) = 0 says nothing at all about the left branch.

d) The function sec⁡2x\sec^2 x is undefined at π2\frac{\pi}{2}, so the domain consists of the two intervals (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right) and (π2,3π2)\left(\frac{\pi}{2}, \frac{3\pi}{2}\right), and f(x)=tan⁡x+Cf(x) = \tan x + C on each, with its own constant. f(0)=tan⁡0+C1=0f(0) = \tan 0 + C_1 = 0 gives C1=0C_1 = 0; f(π)=tan⁡π+C2=0+C2=1f(\pi) = \tan\pi + C_2 = 0 + C_2 = 1 gives C2=1C_2 = 1. So f=tan⁡xf = \tan x on the first interval and tan⁡x+1\tan x + 1 on the second. A single formula tan⁡x+C\tan x + C would require C=0C = 0 and C=1C = 1 at once: the gap at π2\frac{\pi}{2}, a vertical asymptote of tan⁡\tan, is what makes room for two constants.

e) By the linear rule, (ln⁡∣x−2∣)′=1x−2(\ln|x - 2|)' = \frac{1}{x - 2}, with inner derivative 11. On (2,∞)(2, \infty): f(3)=ln⁡1+C1=C1=0f(3) = \ln 1 + C_1 = C_1 = 0. On (−∞,2)(-\infty, 2): f(0)=ln⁡∣−2∣+C2=ln⁡2+C2=1f(0) = \ln|{-2}| + C_2 = \ln 2 + C_2 = 1, so C2=1−ln⁡2C_2 = 1 - \ln 2. Hence f(x)=ln⁡(x−2)f(x) = \ln(x - 2) for x>2x > 2 and f(x)=ln⁡(2−x)+1−ln⁡2f(x) = \ln(2 - x) + 1 - \ln 2 for x<2x < 2. Check at x=0x = 0: ln⁡2+1−ln⁡2=1\ln 2 + 1 - \ln 2 = 1. The exact constant is 1−ln⁡21 - \ln 2; its size, about 0.310.31 with ln⁡2≈0.69\ln 2 \approx 0.69, is a check, never the answer.

Part B: problems and reasoning (/50)

Exercise 6: Sketching an antiderivative from the graph of f: slopes, not guesses

The figure shows the graph of a continuous function ff on [0,6][0, 6], made of two line segments: from (0,2)(0, 2) to (2,−2)(2, -2), then from (2,−2)(2, -2) to (6,2)(6, 2). Let FF be the antiderivative of ff on [0,6][0, 6] such that F(0)=0F(0) = 0.

The graph of ff is the graph of the SLOPES of FF: the sign of ff gives the direction of FF, and the direction of ff gives the concavity of FF. Values of FF come from formulas, found piece by piece and joined by continuity.

123456-3-2-1123y = f(x)x
  • a) On which intervals is FF increasing, decreasing? Where does FF have a local maximum, a local minimum? Justify with ff only.
  • b) Where is FF concave up, concave down? Give the inflection point of FF.
  • c) Read the two formulas of ff on the figure, and find FF on [0,2][0, 2], then on [2,6][2, 6]. Explain how the second constant is found.
  • d) Compute F(1)F(1), F(2)F(2), F(4)F(4) and F(6)F(6), and sketch the graph of FF.
  • e) A student's sketch shows a corner in the graph of FF at x=2x = 2, because the graph of ff has one there. Correct the sketch, and say what the corner of ff becomes on the graph of FF.

Type your answers, the page tells you right or wrong 0/13

a)
FF decreases on ,
b)
Concave up on ,
c)
d)
e)
Show the solution

Answers

  • a) FF increases on [0,1][0, 1] and [4,6][4, 6], decreases on [1,4][1, 4]; local max at x=1x = 1, local min at x=4x = 4
  • b) Concave down on (0,2)(0, 2), concave up on (2,6)(2, 6); inflection point (2,0)(2, 0)
  • c) F(x)=2x−x2F(x) = 2x - x^2 on [0,2][0, 2]; F(x)=x22−4x+6F(x) = \frac{x^2}{2} - 4x + 6 on [2,6][2, 6], constant from FF continuous at 22
  • d) F(1)=1F(1) = 1, F(2)=0F(2) = 0, F(4)=−2F(4) = -2, F(6)=0F(6) = 0
  • e) No corner: F′(2)=f(2)=−2F'(2) = f(2) = -2 from both sides; the corner of ff is the inflection point of FF.

a) F′=fF' = f, so FF increases where f>0f > 0 and decreases where f<0f < 0. The first segment crosses the axis at x=1x = 1, the second at x=4x = 4 (from −2-2 at x=2x = 2 to 22 at x=6x = 6, it rises 11 per unit). So f>0f > 0 on [0,1)[0, 1), f<0f < 0 on (1,4)(1, 4), f>0f > 0 on (4,6](4, 6]: FF increases on [0,1][0, 1], decreases on [1,4][1, 4], increases on [4,6][4, 6]. By the first derivative test, FF has a local maximum at x=1x = 1, where ff changes from ++ to −-, and a local minimum at x=4x = 4, where ff changes from −- to ++. Note what was NOT used: the height of ff. The highest point of ff, at x=0x = 0, is not an extremum of FF at all.

b) F′′=f′F'' = f': FF is concave up where ff increases and concave down where ff decreases. On (0,2)(0, 2), ff decreases (slope −2-2), so FF is concave down; on (2,6)(2, 6), ff increases (slope 11), so FF is concave up. The concavity changes at x=2x = 2, where ff reaches its minimum, and FF is continuous there: x=2x = 2 is the inflection point, and d) gives F(2)=0F(2) = 0. The reading to memorize: the zeros of ff give the extrema of FF, the extrema of ff give the inflection points of FF.

c) The first segment passes through (0,2)(0, 2) with slope −2-2: f(x)=2−2xf(x) = 2 - 2x on [0,2][0, 2]. The second passes through (4,0)(4, 0) with slope 11: f(x)=x−4f(x) = x - 4 on [2,6][2, 6]. On [0,2][0, 2], F(x)=2x−x2+C1F(x) = 2x - x^2 + C_1, and F(0)=0F(0) = 0 gives C1=0C_1 = 0. On [2,6][2, 6], F(x)=x22−4x+C2F(x) = \frac{x^2}{2} - 4x + C_2. There is no condition given at a point of [2,6][2, 6], but FF is differentiable, hence CONTINUOUS, at x=2x = 2: the two formulas must agree there. 2⋅2−4=02 \cdot 2 - 4 = 0 on the left, 2−8+C22 - 8 + C_2 on the right, so C2=6C_2 = 6 and F(x)=x22−4x+6F(x) = \frac{x^2}{2} - 4x + 6 on [2,6][2, 6]. Continuity is the condition that fixes the constant of every piece after the first.

d) F(1)=2−1=1F(1) = 2 - 1 = 1, F(2)=4−4=0F(2) = 4 - 4 = 0, F(4)=8−16+6=−2F(4) = 8 - 16 + 6 = -2, F(6)=18−24+6=0F(6) = 18 - 24 + 6 = 0. The sketch, shown in the solution figure: starting at the origin, FF rises to its local maximum (1,1)(1, 1) along an arc that bends down, falls through (2,0)(2, 0), where the bending changes, to its local minimum (4,−2)(4, -2), then rises back to (6,0)(6, 0) bending up. Every feature of the sketch comes from a) and b); the four values of d) only place it. Check on one piece: F′(x)=x−4=f(x)F'(x) = x - 4 = f(x) on [2,6][2, 6].

e) FF is an antiderivative of the continuous function ff, so FF is differentiable at x=2x = 2 with F′(2)=f(2)=−2F'(2) = f(2) = -2. Both formulas agree: on the left, F′(x)=2−2xF'(x) = 2 - 2x gives −2-2; on the right, F′(x)=x−4F'(x) = x - 4 gives −2-2. The graph of FF has ONE tangent line at (2,0)(2, 0), of slope −2-2: no corner. A corner in the graph of FF would need a JUMP in the values of ff. The corner of ff is a jump in the slope of ff, that is in F′′F'', which goes from −2-2 to 11: it shows up as the change of concavity, the inflection point of b). Each derivative smooths the picture by one level: a jump in ff gives a corner in FF, a corner in ff gives only a change of bending.

123456-3-2-112max (1, 1)inflection (2, 0)min (4, -2)y = F(x)x

Exercise 7: A family of curves: which conditions pick one member, and which pick none

The antiderivatives of f′(x)=3x2−3f'(x) = 3x^2 - 3 form the family y=x3−3x+Cy = x^3 - 3x + C. The figure shows three members, for C=2C = 2, C=0C = 0 and C=−2C = -2, and the point P(2,1)P(2, 1).

Every member is a vertical translate of the others. One condition on ff picks one member; a second derivative needs two conditions, and those two conditions must actually reach the two constants.

-3-2-1123-5-4-3-2-112345C = 2C = 0C = -2P(2, 1)x
  • a) Explain, with f′f', why all the members have the same slope at a given xx, and why no two of them ever meet. Which member passes through PP?
  • b) Which member has its local minimum ON the xx-axis? For which values of CC does the member have three xx-intercepts?
  • c) Find ff if f′′(x)=6xf''(x) = 6x, f(0)=1f(0) = 1 and f(1)=0f(1) = 0.
  • d) Same equation f′′(x)=6xf''(x) = 6x, with the conditions f′(−1)=3f'(-1) = 3 and f′(1)=3f'(1) = 3. How many solutions are there? Same question with f′(−1)=3f'(-1) = 3 and f′(1)=5f'(1) = 5.
  • e) Find ff if f′′(x)=12x−4f''(x) = 12x - 4 and the graph of ff is tangent to the line y=5x−3y = 5x - 3 at the point where x=1x = 1.

Type your answers, the page tells you right or wrong 0/9

a)
b)
CC for three xx-intercepts ,
c)
d)
e)
Show the solution

Answers

  • a) Slope 3x2−33x^2 - 3 for every member; two members differ by a nonzero constant; through PP: C=−1C = -1
  • b) C=2C = 2; three intercepts exactly when −2<C<2-2 < C < 2
  • c) f(x)=x3−2x+1f(x) = x^3 - 2x + 1
  • d) Infinitely many: f(x)=x3+Df(x) = x^3 + D; none with f′(1)=5f'(1) = 5
  • e) f(x)=2x3−2x2+3x−1f(x) = 2x^3 - 2x^2 + 3x - 1

a) Every member has derivative 3x2−33x^2 - 3, so at a given xx all the members have the same slope: their tangent lines above that xx are parallel, which is why the curves look like copies slid up and down. Two members differ by the constant C1−C2≠0C_1 - C_2 \ne 0 at EVERY xx, so they never meet: exactly one member passes through each point of the plane. For P(2,1)P(2, 1): 8−6+C=18 - 6 + C = 1, so C=−1C = -1, the member between the grey and green curves. The figure does not show it, and it does not need to: one point, one equation, one constant.

b) F′(x)=3x2−3=3(x−1)(x+1)F'(x) = 3x^2 - 3 = 3(x - 1)(x + 1) vanishes at x=±1x = \pm 1, and changes from −- to ++ at x=1x = 1: the local minimum is F(1)=1−3+C=C−2F(1) = 1 - 3 + C = C - 2, and the local maximum is F(−1)=−1+3+C=C+2F(-1) = -1 + 3 + C = C + 2. The minimum is on the axis when C=2C = 2, the blue curve, which touches the axis at (1,0)(1, 0). Three intercepts require the maximum above the axis and the minimum below: C+2>0C + 2 > 0 and C−2<0C - 2 < 0, that is −2<C<2-2 < C < 2. Indeed, the member then goes from −∞-\infty up to a positive maximum, down to a negative minimum and up to +∞+\infty, and the Intermediate Value Theorem gives one root on each of the three stretches. At C=±2C = \pm 2 one root is double; the grey member C=0C = 0 has three: x=0x = 0 and x=±3x = \pm\sqrt 3.

c) f′(x)=3x2+Cf'(x) = 3x^2 + C and f(x)=x3+Cx+Df(x) = x^3 + Cx + D. f(0)=D=1f(0) = D = 1; f(1)=1+C+1=0f(1) = 1 + C + 1 = 0, so C=−2C = -2. Hence f(x)=x3−2x+1f(x) = x^3 - 2x + 1. Check: f′′(x)=6xf''(x) = 6x, f(0)=1f(0) = 1, f(1)=1−2+1=0f(1) = 1 - 2 + 1 = 0. Each condition was used for the constant it can reach: f(0)f(0) kills CxCx and isolates DD, which is why it is used first.

d) f′(x)=3x2+Cf'(x) = 3x^2 + C. Then f′(−1)=3+C=3f'(-1) = 3 + C = 3 and f′(1)=3+C=3f'(1) = 3 + C = 3 give the SAME equation, C=0C = 0: the second condition repeats the first, because f′f' is even. Then f(x)=x3+Df(x) = x^3 + D with DD free: infinitely many solutions, since no condition touches DD. With f′(1)=5f'(1) = 5 instead, the conditions demand C=0C = 0 and C=2C = 2 at once: NO solution. Two conditions for two constants is necessary, not sufficient: both conditions on f′f' leave DD untouched, and two conditions on the same quantity can repeat or contradict each other.

e) Tangent to y=5x−3y = 5x - 3 at x=1x = 1 means two conditions: same slope, f′(1)=5f'(1) = 5, and same point, f(1)=5−3=2f(1) = 5 - 3 = 2. Now f′(x)=6x2−4x+Cf'(x) = 6x^2 - 4x + C and f′(1)=2+C=5f'(1) = 2 + C = 5 gives C=3C = 3. Then f(x)=2x3−2x2+3x+Df(x) = 2x^3 - 2x^2 + 3x + D and f(1)=3+D=2f(1) = 3 + D = 2 gives D=−1D = -1. So f(x)=2x3−2x2+3x−1f(x) = 2x^3 - 2x^2 + 3x - 1. Check: f′′(x)=12x−4f''(x) = 12x - 4, f′(1)=6−4+3=5f'(1) = 6 - 4 + 3 = 5, f(1)=2−2+3−1=2f(1) = 2 - 2 + 3 - 1 = 2. A tangency hidden in words is the most frequent way an exam gives two conditions in one sentence; reading only the point, and forgetting the slope, leaves CC undetermined.

Exercise 8: Five statements to correct

Each statement below was written by a student on a MATH 140 assignment, and each is false. Say what is wrong, settle it by differentiating or with a counterexample, and write the correct statement.

  • a) The most general antiderivative of 1x3\frac{1}{x^3} is ln⁡∣x3∣+C\ln|x^3| + C.
  • b) An antiderivative of 12x+5\frac{1}{2x + 5} is ln⁡∣2x+5∣\ln|2x + 5|.
  • c) An antiderivative of ex2e^{x^2} is ex22x\frac{e^{x^2}}{2x}, dividing by the derivative of the exponent as for e2xe^{2x}.
  • d) (x+1)22\frac{(x + 1)^2}{2} and x22+x\frac{x^2}{2} + x are different functions, so they cannot both be antiderivatives of x+1x + 1.
  • e) If ff is increasing on R\mathbb{R}, then every antiderivative of ff is increasing on R\mathbb{R}.

Type your answers, the page tells you right or wrong 0/6

a)
b)
c)
d)
e)
Show the solution

Answers

  • a) False: (ln⁡∣x3∣)′=3x(\ln|x^3|)' = \frac{3}{x}. Correct: −12x2+C-\frac{1}{2x^2} + C, one constant on each side of 00.
  • b) False: its derivative is 22x+5\frac{2}{2x + 5}. Correct: 12ln⁡∣2x+5∣\frac{1}{2}\ln|2x + 5|.
  • c) False: the derivative is ex2−ex22x2e^{x^2} - \frac{e^{x^2}}{2x^2}. Dividing by the inner derivative works for LINEAR inner functions only.
  • d) False: they differ by the constant 12\frac{1}{2}, and both have derivative x+1x + 1.
  • e) False: f(x)=xf(x) = x, F(x)=x22F(x) = \frac{x^2}{2} decreases on (−∞,0](-\infty, 0]. FF increases where f>0f > 0.

a) FALSE. The exponent is −3-3, not −1-1: the power rule applies, x−3↦x−2−2=−12x2x^{-3} \mapsto \frac{x^{-2}}{-2} = -\frac{1}{2x^2}. The logarithm is reserved for the exponent −1-1 alone. Differentiating the student's answer settles it: ln⁡∣x3∣=3ln⁡∣x∣\ln|x^3| = 3\ln|x|, whose derivative is 3x\frac{3}{x}, not 1x3\frac{1}{x^3}; at x=2x = 2, 32\frac{3}{2} against 18\frac{1}{8}. Correct statement: the most general antiderivative of 1x3\frac{1}{x^3} is −12x2+C1-\frac{1}{2x^2} + C_1 on (0,∞)(0, \infty) and −12x2+C2-\frac{1}{2x^2} + C_2 on (−∞,0)(-\infty, 0). Check: (−12x−2)′=x−3\left(-\frac{1}{2}x^{-2}\right)' = x^{-3}.

b) FALSE. By the chain rule with inner function 2x+52x + 5, whose derivative is 22: (ln⁡∣2x+5∣)′=22x+5(\ln|2x + 5|)' = \frac{2}{2x + 5}, twice the target. Correct statement: 12ln⁡∣2x+5∣\frac{1}{2}\ln|2x + 5| is an antiderivative of 12x+5\frac{1}{2x + 5} on each of the intervals x>−52x > -\frac{5}{2} and x<−52x < -\frac{5}{2}, which is the linear rule 1aF(ax+b)\frac{1}{a}F(ax + b) with a=2a = 2. The missing 1a\frac{1}{a} is the single most frequent error of the chapter, and differentiating catches it in one line every time.

c) FALSE. By the quotient rule, (ex22x)′=2xex2⋅2x−2ex24x2=ex2−ex22x2\left(\frac{e^{x^2}}{2x}\right)' = \frac{2x e^{x^2} \cdot 2x - 2e^{x^2}}{4x^2} = e^{x^2} - \frac{e^{x^2}}{2x^2}: an extra term appears, because the xx in the denominator is NOT a constant and gets differentiated too. Dividing by the derivative of the inside works for e2xe^{2x} because that derivative is the constant 22, which passes through the differentiation untouched. Correct statement: for a LINEAR inside ax+bax + b, 1aF(ax+b)\frac{1}{a}F(ax + b) is an antiderivative of f(ax+b)f(ax + b); for any other inside, the division fails. In fact ex2e^{x^2}, which is continuous, does have antiderivatives, but none can be written with the functions of this course.

d) FALSE. Expand: (x+1)22=x22+x+12\frac{(x + 1)^2}{2} = \frac{x^2}{2} + x + \frac{1}{2}. The two functions differ by the constant 12\frac{1}{2}, and both have derivative x+1x + 1: both are antiderivatives, two members of the same family. Correct statement: two antiderivatives of the same function on an interval differ by a constant, and they may LOOK different. That is why two correct answers on a test can disagree in form: compare them by subtracting, or by differentiating both, never by their appearance.

e) FALSE. Take f(x)=xf(x) = x, increasing on R\mathbb{R}. Its antiderivative F(x)=x22F(x) = \frac{x^2}{2} decreases on (−∞,0](-\infty, 0], where f<0f < 0. What decides whether FF increases is the SIGN of f=F′f = F', not its direction. Correct statement: an antiderivative of ff increases on any interval where f>0f > 0 and decreases where f<0f < 0; that ff increases says that F′F' increases, that is, FF is concave up. This is the same reading as in Exercise 6: zeros and sign of ff for the direction of FF, slope of ff for its bending.

Exercise 9: A stone thrown up from a bridge: the equations of motion rebuilt from the acceleration

A stone is thrown straight up at 14.714.7 m/s from a bridge whose parapet is 44.144.1 m above a river, and falls into the water, missing the bridge. Air resistance is neglected, so the acceleration is −9.8-9.8 m/s2^2 throughout the flight. Measure the height s(t)s(t), in metres, upward from the surface of the water, with tt in seconds from the throw.

No formula of kinematics is given: velocity and position are recovered from the acceleration by two antiderivatives, v′=av' = a and s′=vs' = v, each with its constant. Every time asked for is exact.

44.1 mthrown upat 14.7 m/sriver: s = 0
  • a) Find v(t)v(t) and s(t)s(t), and say what each constant of antidifferentiation represents.
  • b) When does the stone reach its highest point, and how high above the water is it then?
  • c) When does it pass back at the level of the parapet, and with what velocity?
  • d) When does it hit the water? Give the exact time and the exact velocity at impact, then estimate both with 5≈2.236\sqrt 5 \approx 2.236.
  • e) With what initial speed should the stone be thrown up, from the same parapet, to hit the water exactly 55 s after the throw?

Type your answers, the page tells you right or wrong 0/9

a)
b)
c)
d)
e)
Show the solution

Answers

  • a) v(t)=14.7−9.8tv(t) = 14.7 - 9.8t, s(t)=44.1+14.7t−4.9t2s(t) = 44.1 + 14.7t - 4.9t^2; the constants are v(0)v(0) and s(0)s(0)
  • b) At t=1.5t = 1.5 s, at 55.12555.125 m above the water
  • c) At t=3t = 3 s, with v(3)=−14.7v(3) = -14.7 m/s
  • d) t=3+352≈4.85t = \frac{3 + 3\sqrt 5}{2} \approx 4.85 s, v=−14.75≈−32.9v = -14.7\sqrt 5 \approx -32.9 m/s
  • e) v0=15.68v_0 = 15.68 m/s

a) v′(t)=a(t)=−9.8v'(t) = a(t) = -9.8, so v(t)=−9.8t+C1v(t) = -9.8t + C_1. At t=0t = 0, v(0)=C1v(0) = C_1: the first constant IS the initial velocity, C1=14.7C_1 = 14.7, positive because the throw is upward on an upward axis. Then s′(t)=v(t)=14.7−9.8ts'(t) = v(t) = 14.7 - 9.8t gives s(t)=14.7t−4.9t2+C2s(t) = 14.7t - 4.9t^2 + C_2, and s(0)=C2s(0) = C_2 is the initial height, 44.144.1. So v(t)=14.7−9.8tv(t) = 14.7 - 9.8t and s(t)=44.1+14.7t−4.9t2s(t) = 44.1 + 14.7t - 4.9t^2. Check: s′′=−9.8s'' = -9.8, s(0)=44.1s(0) = 44.1, s′(0)=14.7s'(0) = 14.7. The formula s=s0+v0t+12at2s = s_0 + v_0 t + \frac{1}{2}at^2 of physics is exactly this computation with letters, and it holds only while aa is constant, which Exercise 10 will not be.

b) At the highest point the stone stops rising: v(t)=0v(t) = 0, so t=14.79.8=1.5t = \frac{14.7}{9.8} = 1.5 s. Then s(1.5)=44.1+14.7⋅1.5−4.9⋅2.25=44.1+22.05−11.025=55.125s(1.5) = 44.1 + 14.7 \cdot 1.5 - 4.9 \cdot 2.25 = 44.1 + 22.05 - 11.025 = 55.125 m above the water, that is 11.02511.025 m above the parapet. It is a maximum because v>0v > 0 before t=1.5t = 1.5 and v<0v < 0 after: the first derivative test, with s′=vs' = v. The trap is to give 11.02511.025 m, the rise above the hand, when the question measures from the water: the axis was fixed in the statement, and ss is measured on it.

c) s(t)=44.1s(t) = 44.1 means 14.7t−4.9t2=014.7t - 4.9t^2 = 0, that is 4.9t(3−t)=04.9t(3 - t) = 0: t=0t = 0, the throw, or t=3t = 3 s. Then v(3)=14.7−29.4=−14.7v(3) = 14.7 - 29.4 = -14.7 m/s: the same speed as the throw, downward. The flight above the parapet is symmetric about the top, 1.51.5 s up and 1.51.5 s down, because ss is a parabola whose axis is t=1.5t = 1.5. The sign of vv is part of the answer: −14.7-14.7 m/s says down, and a velocity given as 14.714.7 m/s is a speed, which is a different word.

d) s(t)=0s(t) = 0: 4.9t2−14.7t−44.1=04.9t^2 - 14.7t - 44.1 = 0. Dividing by 4.94.9, since 14.7=3⋅4.914.7 = 3 \cdot 4.9 and 44.1=9⋅4.944.1 = 9 \cdot 4.9: t2−3t−9=0t^2 - 3t - 9 = 0, so t=3±9+362=3±352t = \frac{3 \pm \sqrt{9 + 36}}{2} = \frac{3 \pm 3\sqrt 5}{2}. The negative root is rejected, the flight starts at t=0t = 0: t=3+352t = \frac{3 + 3\sqrt 5}{2} s. Then v=14.7−9.8⋅3+352=14.7−14.7−14.75=−14.75v = 14.7 - 9.8 \cdot \frac{3 + 3\sqrt 5}{2} = 14.7 - 14.7 - 14.7\sqrt 5 = -14.7\sqrt 5 m/s. Estimates: t≈3+6.7082≈4.85t \approx \frac{3 + 6.708}{2} \approx 4.85 s and v≈−32.9v \approx -32.9 m/s. Check by energy, independent of the time: v2=v02+2⋅9.8⋅44.1=216.09+864.36=1080.45=5⋅14.72v^2 = v_0^2 + 2 \cdot 9.8 \cdot 44.1 = 216.09 + 864.36 = 1080.45 = 5 \cdot 14.7^2. Dividing by 4.94.9 first is what makes the computation possible by hand.

e) Keep the initial speed as the unknown v0v_0: the same two antiderivatives give s(t)=44.1+v0t−4.9t2s(t) = 44.1 + v_0 t - 4.9t^2. The condition s(5)=0s(5) = 0 reads 44.1+5v0−122.5=044.1 + 5v_0 - 122.5 = 0, so 5v0=78.45v_0 = 78.4 and v0=15.68v_0 = 15.68 m/s. Check: s(5)=44.1+78.4−122.5=0s(5) = 44.1 + 78.4 - 122.5 = 0. This is an initial value problem run backwards: the condition at t=5t = 5 fixes the constant C1=v0C_1 = v_0 instead of the value at t=0t = 0. Faster than the 14.714.7 m/s of the statement, as expected, since the flight is longer than 4.854.85 s.

123456102030405060top: t = 1.5 sbridge level: t = 3 swatert (s)s (m)

Exercise 10: A final exam question: stopping distance when the braking builds up

A car travels at 1818 m/s, that is 64.864.8 km/h, on a straight road. At t=0t = 0 the driver brakes. The deceleration is not instantaneous: it grows linearly during the first second, a(t)=−6ta(t) = -6t m/s2^2 for 0≤t≤10 \le t \le 1, then stays at a(t)=−6a(t) = -6 m/s2^2 until the car stops, as the figure shows.

Measure the position s(t)s(t), in metres, from the point where braking starts, in the direction of motion. This is the shape of a long final exam question: two pieces, two antiderivatives on each, constants fixed by continuity, and no calculator.

0.511.522.533.54-7-6-5-4-3-2-11a = -6t on [0, 1]a = -6 until the stopt (s)a (m/s²)
  • a) Find v(t)v(t) and s(t)s(t) for 0≤t≤10 \le t \le 1, then v(1)v(1) and s(1)s(1).
  • b) Find v(t)v(t) and s(t)s(t) for t≥1t \ge 1, until the car stops. Explain how the constants are found, and give the time at which the car stops.
  • c) Find the stopping distance.
  • d) Compare with an ideal braking at −6-6 m/s2^2 from t=0t = 0. How many metres does the ramp cost, and why?
  • e) With the same braking profile, what is the largest initial speed v0v_0 for which the stopping distance is at most 2020 m? Give the exact value, then bracket it without a calculator.

Type your answers, the page tells you right or wrong 0/8

a)
b)
c)
d)
e)
Show the solution

Answers

  • a) v(t)=18−3t2v(t) = 18 - 3t^2, s(t)=18t−t3s(t) = 18t - t^3; v(1)=15v(1) = 15 m/s, s(1)=17s(1) = 17 m
  • b) v(t)=21−6tv(t) = 21 - 6t, s(t)=−3t2+21t−1s(t) = -3t^2 + 21t - 1 by continuity at t=1t = 1; stop at t=3.5t = 3.5 s
  • c) s(3.5)=35.75s(3.5) = 35.75 m
  • d) 2727 m for the ideal braking: the ramp costs 8.758.75 m
  • e) v0=−3+67v_0 = -3 + 6\sqrt 7 m/s, between 12.8412.84 and 12.912.9 m/s, about 4646 km/h

a) On [0,1][0, 1], v′(t)=−6tv'(t) = -6t gives v(t)=−3t2+C1v(t) = -3t^2 + C_1, and v(0)=18v(0) = 18 gives C1=18C_1 = 18: v(t)=18−3t2v(t) = 18 - 3t^2. Then s′(t)=v(t)s'(t) = v(t) gives s(t)=18t−t3+C2s(t) = 18t - t^3 + C_2, and s(0)=0s(0) = 0 gives C2=0C_2 = 0. So v(1)=15v(1) = 15 m/s and s(1)=18−1=17s(1) = 18 - 1 = 17 m. During the ramp the car loses only 33 m/s in the first second, half of what a full braking would take away: the acceleration is not constant, so no equation of constant acceleration may be used on this piece, only antiderivatives.

b) On [1,∞)[1, \infty), v′(t)=−6v'(t) = -6 gives v(t)=−6t+C3v(t) = -6t + C_3. No value of vv is given at a time of this piece, but the velocity is continuous (it cannot jump without an infinite force): v(1)=15v(1) = 15, so −6+C3=15-6 + C_3 = 15 and C3=21C_3 = 21, v(t)=21−6tv(t) = 21 - 6t. Then s(t)=21t−3t2+C4s(t) = 21t - 3t^2 + C_4, and continuity of the position at t=1t = 1 gives 21−3+C4=1721 - 3 + C_4 = 17, so C4=−1C_4 = -1: s(t)=−3t2+21t−1s(t) = -3t^2 + 21t - 1. The car stops when v(t)=0v(t) = 0: t=3.5t = 3.5 s. Four constants, four conditions: two initial values and two junction conditions, exactly as in Exercise 6.

c) The car moves forward during the whole braking (v>0v > 0 on [0,3.5)[0, 3.5)), so the stopping distance is s(3.5)=−3⋅12.25+73.5−1=−36.75+72.5=35.75s(3.5) = -3 \cdot 12.25 + 73.5 - 1 = -36.75 + 72.5 = 35.75 m. Check: s′(t)=21−6t=v(t)s'(t) = 21 - 6t = v(t) and s(1)=−3+21−1=17s(1) = -3 + 21 - 1 = 17, the value of a). Using the second formula before t=1t = 1, or the first after, is the classic error of piecewise motion: each formula is valid on its own piece only.

d) Ideal braking: v(t)=18−6tv(t) = 18 - 6t and s(t)=18t−3t2s(t) = 18t - 3t^2, from the same two antiderivatives. The car stops at t=3t = 3 s, after s(3)=54−27=27s(3) = 54 - 27 = 27 m. The ramp costs 35.75−27=8.7535.75 - 27 = 8.75 m, about two car lengths. Why: after one second the ramped car still moves at 1515 m/s, having covered 1717 m, while the ideal car is at 1212 m/s after 1515 m. From there both decelerate at 66 m/s2^2; a car at speed uu then needs u212\frac{u^2}{12} metres, since v=u−6τv = u - 6\tau stops at τ=u6\tau = \frac{u}{6} after uτ−3τ2=u212u\tau - 3\tau^2 = \frac{u^2}{12}. That is 18.7518.75 m for the ramped car against 1212 m. The whole loss is decided in the first second.

e) For an initial speed v0>3v_0 > 3, the ramp gives v(t)=v0−3t2v(t) = v_0 - 3t^2 and s(t)=v0t−t3s(t) = v_0 t - t^3, so v(1)=v0−3v(1) = v_0 - 3 and s(1)=v0−1s(1) = v_0 - 1; the remaining distance is (v0−3)212\frac{(v_0 - 3)^2}{12} by d). The stopping distance is D(v0)=v0−1+(v0−3)212D(v_0) = v_0 - 1 + \frac{(v_0 - 3)^2}{12}, increasing in v0v_0. Check: D(18)=17+22512=35.75D(18) = 17 + \frac{225}{12} = 35.75. Solve D(v0)=20D(v_0) = 20: 12v0−12+v02−6v0+9=24012v_0 - 12 + v_0^2 - 6v_0 + 9 = 240, that is v02+6v0−243=0v_0^2 + 6v_0 - 243 = 0, so v0=−3+9+243=−3+252=−3+67v_0 = -3 + \sqrt{9 + 243} = -3 + \sqrt{252} = -3 + 6\sqrt 7 m/s, the negative root rejected. Bracket: 2.642=6.9696<7<7.0225=2.6522.64^2 = 6.9696 < 7 < 7.0225 = 2.65^2, so 15.84<67<15.915.84 < 6\sqrt 7 < 15.9 and 12.84<v0<12.912.84 < v_0 < 12.9 m/s, about 4646 km/h. It exceeds 33, as the formula for DD assumed. The fastest speed for a 2020 m stop is far below the 1818 m/s of the statement.

© Ahmed Squalli Houssaini. Exercise set published at www.letuteurscientifique.ca/en/exercices/math140-antiderivatives. Free for personal and classroom use; republishing it elsewhere requires written permission (legal notice).

See also

Struggling with MATH 140?

I tutor first-year calculus at McGill and Concordia, in English or in French, in Montreal or online. Get in touch for a first session.

Site by Studio Squalli