MATH 203 Calculus I • Concordia University, Montreal

Corrected exercises: linearization and differentials (MATH 203)

This is the corrected exercise set for linearization and differentials in MATH 203, Differential and Integral Calculus I, at Concordia University, section 3.11 of Thomas' Calculus. The tangent line becomes a tool: L(x)=f(a)+f′(a)(x−a)L(x) = f(a) + f'(a)(x - a) replaces a function near a point, and the differential dy=f′(x) dxdy = f'(x)\,dx measures how a small change, or a measuring error, travels into a computed quantity. A scientific calculator is allowed in MATH 203, so every estimate here is made by hand and then compared with the calculator: the actual error and the percentage error are part of the answer.

The thread of the whole set: the calculus is one line, the marks are lost in the ALGEBRA around it. A fractional or negative exponent evaluated at the centre (16−3/4=1816^{-3/4} = \frac{1}{8}, a reciprocal, never a negative number); the sign of the increment x−ax - a; the constant factored out before (1+x)k≈1+kx(1 + x)^k \approx 1 + kx can be used (9.18=31.02\sqrt{9.18} = 3\sqrt{1.02}); a derivative brought to a single fraction; the quotient dyy\frac{dy}{y} simplified to kdxxk\frac{dx}{x} before any number goes in. Each solution names the algebra step where the points are won or lost.

The traps named in the solutions: reading 16−3/416^{-3/4} as a negative number, losing the sign of x−ax - a, using degrees in tan⁡x\tan x, flipping 13/4\frac{1}{\sqrt{3/4}} the wrong way, applying (1+x)k(1 + x)^k to 2+x2 + x without factoring, trusting the rule when kxkx is not small, confusing dydy with Δy\Delta y and with the error, writing 0.020.02 as 0.02%0.02\%, putting the error of a circumference or a diameter on the radius, and forgetting that the exponent multiplies the relative error.

10 corrected exercises • 100 points • 150 minutes

Revision sheet for this chapter → Every MATH 203 chapter →

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Course recap

  • • Linearization of ff at aa: L(x)=f(a)+f′(a)(x−a)L(x) = f(a) + f'(a)(x - a), and f(x)≈L(x)f(x) \approx L(x) near aa. Check: L(a)=f(a)L(a) = f(a).
  • • Centre: close to the target, with f(a)f(a) and f′(a)f'(a) exact (ln⁡2\ln 2 for exe^x, π4\frac{\pi}{4} for tan⁡x\tan x, a perfect power for a root). Angles in radians.
  • • Negative and fractional exponents: a−m/n=1(an)ma^{-m/n} = \frac{1}{\left(\sqrt[n]{a}\right)^m}, root first, then power, then reciprocal.
  • • Standard linear approximation: (1+x)k≈1+kx(1 + x)^k \approx 1 + kx when kxkx is small; factor the constant first, (c+x)k=ck(1+xc)k(c + x)^k = c^k\left(1 + \frac{x}{c}\right)^k.
  • • Side: f′′>0f'' > 0 between aa and xx, LL underestimates; f′′<0f'' < 0, LL overestimates.
  • • Differentials: dy=f′(x) dxdy = f'(x)\,dx, Δy=f′(a) dx+ε dx\Delta y = f'(a)\,dx + \varepsilon\,dx with ε→0\varepsilon \to 0; d(uv)=u dv+v dud(uv) = u\,dv + v\,du.
  • • Propagated error: dydy; relative error dyy\frac{dy}{y}; percentage 100dyy100\frac{dy}{y}; for y=cxky = cx^k, dyy=kdxx\frac{dy}{y} = k\frac{dx}{x}.

Part A: the basics (/50)

Exercise 1: The fourth root at 16: the exponent at the centre, the sign of x - a, the side

The linearization of ff at aa is L(x)=f(a)+f′(a)(x−a)L(x) = f(a) + f'(a)(x - a), and f(x)≈L(x)f(x) \approx L(x) is the standard linear approximation of ff at aa (Thomas 3.11). The calculus fits in one line. The marks go to the algebra around it: the value of a fractional or NEGATIVE exponent at the centre, the factor (x−a)(x - a) with its sign, and the side of the error, read on the sign of f′′f''.

A scientific calculator is allowed. Compute every estimate by hand first, then use the calculator to measure the actual error ∣f(x)−L(x)∣|f(x) - L(x)|. The figure shows y=x4y = \sqrt[4]{x} and its tangent at (16,2)(16, 2).

481216202428320.511.522.53y = ∜xtangent at (16, 2)x
  • a) Find the linearization LL of f(x)=x4f(x) = \sqrt[4]{x} at a=16a = 16. Write 16−3/416^{-3/4} as a fraction before using it.
  • b) Use LL to approximate 174\sqrt[4]{17} and 15.54\sqrt[4]{15.5}, as exact decimals.
  • c) Use f′′f'' to decide whether the two estimates are too large or too small. Then give the calculator values to six decimal places and the actual error of each estimate.
  • d) Find the linearization of g(x)=x−3/2g(x) = x^{-3/2} at a=4a = 4, approximate 4.2−3/24.2^{-3/2}, give the side of the error, and compare with the calculator.
  • e) Approximate 16.54\sqrt[4]{16.5} with the same LL and compute the actual error. About how many times smaller is it than the error at 1717? Explain.

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  • a) f′(16)=14⋅16−3/4=132f'(16) = \frac{1}{4} \cdot 16^{-3/4} = \frac{1}{32}, so L(x)=2+132(x−16)L(x) = 2 + \frac{1}{32}(x - 16)
  • b) 174≈2.03125\sqrt[4]{17} \approx 2.03125, 15.54≈1.984375\sqrt[4]{15.5} \approx 1.984375
  • c) Both too large (f′′<0f'' < 0); calculator 2.0305432.030543 and 1.9841881.984188; errors 0.0007070.000707 and 0.0001870.000187
  • d) Lg(x)=18−364(x−4)L_g(x) = \frac{1}{8} - \frac{3}{64}(x - 4); 4.2−3/2≈0.1156254.2^{-3/2} \approx 0.115625, too small; calculator 0.1161790.116179
  • e) 16.54≈2.015625\sqrt[4]{16.5} \approx 2.015625, error 0.0001800.000180, about 44 times smaller: half the distance, a quarter of the error

a) f(x)=x1/4f(x) = x^{1/4}, so by the power rule f′(x)=14x−3/4f'(x) = \frac{1}{4}x^{-3/4}. At the centre, the algebra first: 16−3/4=1163/4=1(164)3=123=1816^{-3/4} = \frac{1}{16^{3/4}} = \frac{1}{\left(\sqrt[4]{16}\right)^3} = \frac{1}{2^3} = \frac{1}{8}. Take the root FIRST, then the power, then the reciprocal: 16316^{3} is 40964096, a number nobody wants to root. A negative exponent means a reciprocal, never a negative number: writing 16−3/4=−816^{-3/4} = -8 or −12-12 makes the slope negative although the figure shows a rising curve. Hence f(16)=2f(16) = 2, f′(16)=14⋅18=132f'(16) = \frac{1}{4} \cdot \frac{1}{8} = \frac{1}{32}, and L(x)=2+132(x−16)L(x) = 2 + \frac{1}{32}(x - 16). Check: L(16)=2=f(16)L(16) = 2 = f(16).

b) 174≈L(17)=2+132=2.03125\sqrt[4]{17} \approx L(17) = 2 + \frac{1}{32} = 2.03125. For 15.515.5 the increment is NEGATIVE: x−a=15.5−16=−0.5x - a = 15.5 - 16 = -0.5, so 15.54≈2−0.532=2−164=1.984375\sqrt[4]{15.5} \approx 2 - \frac{0.5}{32} = 2 - \frac{1}{64} = 1.984375. Losing the sign gives 2.0156252.015625, a value above 22 for a number below 1616, which a rising function cannot produce.

c) f′′(x)=14⋅(−34)x−7/4=−316x−7/4<0f''(x) = \frac{1}{4} \cdot \left(-\frac{3}{4}\right)x^{-7/4} = -\frac{3}{16}x^{-7/4} < 0 for x>0x > 0: the curve is concave down, it lies below each of its tangents (the figure shows it on both sides of (16,2)(16, 2)), so BOTH estimates are too large. The calculator agrees: 174=2.030543\sqrt[4]{17} = 2.030543 and 15.54=1.984188\sqrt[4]{15.5} = 1.984188 to six decimals. Actual errors: 2.03125−2.030543=0.0007072.03125 - 2.030543 = 0.000707 and 1.984375−1.984188=0.0001871.984375 - 1.984188 = 0.000187, both positive as predicted. As percentages of the true values, about 0.035%0.035\% and 0.009%0.009\%: the tangent is excellent this close to 1616.

d) g(x)=x−3/2g(x) = x^{-3/2} gives g′(x)=−32x−5/2g'(x) = -\frac{3}{2}x^{-5/2}. At 44: 4−3/2=1(4)3=184^{-3/2} = \frac{1}{(\sqrt 4)^3} = \frac{1}{8} and 4−5/2=1(4)5=1324^{-5/2} = \frac{1}{(\sqrt 4)^5} = \frac{1}{32}, so g(4)=18g(4) = \frac{1}{8} and g′(4)=−32⋅132=−364g'(4) = -\frac{3}{2} \cdot \frac{1}{32} = -\frac{3}{64}. Then Lg(x)=18−364(x−4)L_g(x) = \frac{1}{8} - \frac{3}{64}(x - 4) and 4.2−3/2≈0.125−364(0.2)=0.125−0.009375=0.1156254.2^{-3/2} \approx 0.125 - \frac{3}{64}(0.2) = 0.125 - 0.009375 = 0.115625. Side: g′′(x)=154x−7/2>0g''(x) = \frac{15}{4}x^{-7/2} > 0, concave up, the tangent lies BELOW the curve, so the estimate is too small. Calculator: 4.2−3/2=0.1161794.2^{-3/2} = 0.116179, larger than 0.1156250.115625 as predicted, error 0.0005540.000554. Two exponents with a minus sign, two reciprocals: the algebra of exponents is where this question is won or lost.

e) L(16.5)=2+0.532=2.015625L(16.5) = 2 + \frac{0.5}{32} = 2.015625 and the calculator gives 16.54=2.015445\sqrt[4]{16.5} = 2.015445, an error of 0.0001800.000180. At 1717 the error was 0.0007070.000707: the ratio is 0.0007070.000180\frac{0.000707}{0.000180}, about 3.93.9, so about 44. The distance to the centre was halved, from 11 to 0.50.5, and the error was divided by about 22=42^2 = 4, not by 22. The error of a linearization behaves like a constant times (x−a)2(x - a)^2: this is why a centre CLOSE to the target matters more than anything else.

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Exercise 2: Choosing the centre: e to the 0.7, tan 44 degrees, arcsin 0.52 and ln 2.7

The centre aa is not chosen because it is a nice number, but because f(a)f(a) and f′(a)f'(a) are EXACT there and aa is close to the target. For exe^x near 0.70.7, that point is ln⁡2\ln 2, where eln⁡2=2e^{\ln 2} = 2: an ugly number with perfect values. For a trigonometric function, the angle is in RADIANS, because (tan⁡x)′=sec⁡2x(\tan x)' = \sec^2 x only holds in radians.

Calculator allowed, but only for the arithmetic of the increment and for the final comparison. Give the estimates and calculator values to six decimal places. The figure shows y=tan⁡xy = \tan x and its tangent at (π4,1)\left(\frac{\pi}{4}, 1\right).

0.20.40.60.811.21.4-11234y = tan xtangent at (π/4, 1)x (rad)
  • a) Find the linearization of f(x)=exf(x) = e^x at a=ln⁡2a = \ln 2 and use it to approximate e0.7e^{0.7}. Is the estimate too large or too small? Compare with the calculator.
  • b) Write 44∘44^\circ as π4+h\frac{\pi}{4} + h with hh in radians. Linearize tan⁡x\tan x at π4\frac{\pi}{4} and approximate tan⁡44∘\tan 44^\circ, with the side of the error (use the figure and f′′f''). Compare with the calculator.
  • c) Linearize arcsin⁡x\arcsin x at a=12a = \frac{1}{2}, writing f′(12)f'\left(\frac{1}{2}\right) as a simplified fraction, and approximate arcsin⁡0.52\arcsin 0.52, with the side. Compare with the calculator.
  • d) Linearize ln⁡x\ln x at a=ea = e and show that the estimate of ln⁡2.7\ln 2.7 simplifies to 2.7e\frac{2.7}{e}. Give its value, the side, and compare with the calculator.
  • e) A student centres exe^x at 00 and writes e0.7≈1.7e^{0.7} \approx 1.7. Compute the percentage error of this estimate, and explain why ln⁡2\ln 2 is the right centre although it is not a simple number.

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  • a) L(x)=2+2(x−ln⁡2)L(x) = 2 + 2(x - \ln 2); e0.7≈2.013706e^{0.7} \approx 2.013706, too small; calculator 2.0137532.013753
  • b) h=−π180h = -\frac{\pi}{180}; tan⁡44∘≈1−π90=0.965093\tan 44^\circ \approx 1 - \frac{\pi}{90} = 0.965093, too small; calculator 0.9656890.965689
  • c) f′(12)=23f'\left(\frac{1}{2}\right) = \frac{2}{\sqrt 3}; arcsin⁡0.52≈π6+0.043=0.546693\arcsin 0.52 \approx \frac{\pi}{6} + \frac{0.04}{\sqrt 3} = 0.546693, too small; calculator 0.5468510.546851
  • d) L(2.7)=1+2.7−ee=2.7e=0.993274L(2.7) = 1 + \frac{2.7 - e}{e} = \frac{2.7}{e} = 0.993274, too large; calculator 0.9932520.993252
  • e) About 15.58%15.58\%; 0.70.7 is far from 00 but only 0.00690.0069 from ln⁡2\ln 2, where ff and f′f' are exactly 22.

a) f(ln⁡2)=eln⁡2=2f(\ln 2) = e^{\ln 2} = 2 and f′(x)=exf'(x) = e^x, so f′(ln⁡2)=2f'(\ln 2) = 2 as well. Hence L(x)=2+2(x−ln⁡2)L(x) = 2 + 2(x - \ln 2). The calculator gives the increment, 0.7−ln⁡2=0.0068530.7 - \ln 2 = 0.006853, and e0.7≈2+2(0.006853)=2.013706e^{0.7} \approx 2 + 2(0.006853) = 2.013706. Side: (ex)′′=ex>0(e^x)'' = e^x > 0, the curve is concave up and lies above its tangent, so the estimate is too small. Calculator: e0.7=2.013753e^{0.7} = 2.013753, larger indeed, an error of 0.0000470.000047. Keep ln⁡2\ln 2 exact inside LL; round only the final number.

b) 44∘=45∘−1∘=π4−π18044^\circ = 45^\circ - 1^\circ = \frac{\pi}{4} - \frac{\pi}{180}, so h=−π180h = -\frac{\pi}{180} rad. For f(x)=tan⁡xf(x) = \tan x: f(π4)=1f\left(\frac{\pi}{4}\right) = 1 and f′(x)=sec⁡2xf'(x) = \sec^2 x, sec⁡2π4=1cos⁡2(π/4)=11/2=2\sec^2\frac{\pi}{4} = \frac{1}{\cos^2(\pi/4)} = \frac{1}{1/2} = 2. So L(x)=1+2(x−π4)L(x) = 1 + 2\left(x - \frac{\pi}{4}\right) and tan⁡44∘≈1+2(−π180)=1−π90=0.965093\tan 44^\circ \approx 1 + 2\left(-\frac{\pi}{180}\right) = 1 - \frac{\pi}{90} = 0.965093. With h=−1h = -1, the degree left unconverted, one gets L=−1L = -1, a negative tangent for an acute angle. Side: f′′(x)=2sec⁡2xtan⁡x>0f''(x) = 2\sec^2 x \tan x > 0 on (0,π2)\left(0, \frac{\pi}{2}\right), the curve bends up away from its tangent on both sides (figure): too small. Calculator in degree mode: tan⁡44∘=0.965689\tan 44^\circ = 0.965689, error 0.0005950.000595.

c) f(x)=arcsin⁡xf(x) = \arcsin x, f(12)=π6f\left(\frac{1}{2}\right) = \frac{\pi}{6}, and f′(x)=11−x2f'(x) = \frac{1}{\sqrt{1 - x^2}}. The algebra: 1−14=341 - \frac{1}{4} = \frac{3}{4}, 34=32\sqrt{\frac{3}{4}} = \frac{\sqrt 3}{2}, and its reciprocal is 23\frac{2}{\sqrt 3}, not 32\frac{\sqrt 3}{2}: the fraction is flipped by the 1…\frac{1}{\ldots}. So L(x)=π6+23(x−12)L(x) = \frac{\pi}{6} + \frac{2}{\sqrt 3}\left(x - \frac{1}{2}\right) and arcsin⁡0.52≈π6+23(0.02)=π6+0.043=0.523599+0.023094=0.546693\arcsin 0.52 \approx \frac{\pi}{6} + \frac{2}{\sqrt 3}(0.02) = \frac{\pi}{6} + \frac{0.04}{\sqrt 3} = 0.523599 + 0.023094 = 0.546693. Side: f′′(x)=x(1−x2)−3/2>0f''(x) = x(1 - x^2)^{-3/2} > 0 for 0<x<10 < x < 1: too small. Calculator (radian mode): arcsin⁡0.52=0.546851\arcsin 0.52 = 0.546851, error 0.0001580.000158.

d) ln⁡e=1\ln e = 1 and (ln⁡x)′=1x(\ln x)' = \frac{1}{x} gives 1e\frac{1}{e}: L(x)=1+1e(x−e)L(x) = 1 + \frac{1}{e}(x - e). At 2.72.7: 1+2.7−ee=1+2.7e−ee=2.7e1 + \frac{2.7 - e}{e} = 1 + \frac{2.7}{e} - \frac{e}{e} = \frac{2.7}{e}. Distributing the 1e\frac{1}{e} over (x−e)(x - e) makes the 11 disappear, a simplification worth doing BEFORE the calculator. Value: 2.7e=0.993274\frac{2.7}{e} = 0.993274. Side: (ln⁡x)′′=−1x2<0(\ln x)'' = -\frac{1}{x^2} < 0, concave down, too large. Calculator: ln⁡2.7=0.993252\ln 2.7 = 0.993252, error 0.0000230.000023.

e) Centred at 00: e0.7≈1+0.7=1.7e^{0.7} \approx 1 + 0.7 = 1.7, and the percentage error is 2.013753−1.72.013753×100\frac{2.013753 - 1.7}{2.013753} \times 100, about 15.58%15.58\%, against 0.002%0.002\% in a). The target 0.70.7 is at distance 0.70.7 from 00 but only 0.00690.0069 from ln⁡2\ln 2. The centre is chosen for two properties together: f(a)f(a) and f′(a)f'(a) exact (here both equal 22), and ∣x−a∣|x - a| small. Whether aa itself looks simple does not matter, since only f(a)f(a) and f′(a)f'(a) enter the computation.

Exercise 3: (1 + x) to the k: factor first, and check that kx is small

Thomas lists one linearization above all others: (1+x)k≈1+kx(1 + x)^k \approx 1 + kx for xx near 00 and any number kk. It applies ONLY to the form 1+1 + (something small), so a quantity like 9.18\sqrt{9.18} or (2+x)−2(2 + x)^{-2} must first be rewritten by FACTORING the constant out: that factoring is the algebra step where most of the marks are lost.

The figure shows y=(1+x)5y = (1 + x)^5 and its tangent y=1+5xy = 1 + 5x at 00, with x=0.08x = 0.08 marked. Calculator allowed for the comparisons, six decimal places.

0.040.080.120.160.211.21.41.61.822.22.42.6y = (1 + x)⁵y = 1 + 5xx = 0.08x
  • a) Show that the linearization of (1+x)k(1 + x)^k at 00 is 1+kx1 + kx. Deduce the linearizations at 00 of 11−x\frac{1}{1 - x} and of 1+x\sqrt{1 + x}.
  • b) Approximate (1.002)25(1.002)^{25}. Is the estimate too large or too small? Give the calculator value and the percentage error.
  • c) Write 9.18=9(1.02)9.18 = 9(1.02) and approximate 9.18\sqrt{9.18}, with the side of the error. Compare with the calculator.
  • d) Show that (2+x)−2≈14−x4(2 + x)^{-2} \approx \frac{1}{4} - \frac{x}{4} near 00 and approximate 12.062\frac{1}{2.06^2}; compare with the calculator. A student writes (2+x)−2≈1−2x(2 + x)^{-2} \approx 1 - 2x: what did he forget, and how does x=0x = 0 expose it?
  • e) Approximate (1.08)5(1.08)^5 and compute the percentage error with the calculator. Compare with b) and explain, with the figure, what must be small for the rule to work.

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  • a) f(0)=1f(0) = 1, f′(0)=kf'(0) = k; 11−x≈1+x\frac{1}{1 - x} \approx 1 + x, 1+x≈1+x2\sqrt{1 + x} \approx 1 + \frac{x}{2}
  • b) (1.002)25≈1.05(1.002)^{25} \approx 1.05, too small; calculator 1.0512191.051219, error about 0.12%0.12\%
  • c) 9.18=31.02≈3.03\sqrt{9.18} = 3\sqrt{1.02} \approx 3.03, too large; calculator 3.0298513.029851
  • d) (2+x)−2=14(1+x2)−2≈14(1−x)(2 + x)^{-2} = \frac{1}{4}\left(1 + \frac{x}{2}\right)^{-2} \approx \frac{1}{4}(1 - x); 12.062≈0.235\frac{1}{2.06^2} \approx 0.235, calculator 0.2356490.235649; the factor 14\frac{1}{4} is missing, 1−2x1 - 2x gives 1≠141 \ne \frac{1}{4} at x=0x = 0
  • e) (1.08)5≈1.4(1.08)^5 \approx 1.4, calculator 1.4693281.469328, error about 4.72%4.72\%: kx=0.4kx = 0.4 is not small, while kx=0.05kx = 0.05 in b)

a) f(x)=(1+x)kf(x) = (1 + x)^k gives f(0)=1f(0) = 1 and, by the chain rule with inner function 1+x1 + x, f′(x)=k(1+x)k−1f'(x) = k(1 + x)^{k-1}, so f′(0)=kf'(0) = k. Hence L(x)=1+kxL(x) = 1 + kx. For 11−x=(1+(−x))−1\frac{1}{1 - x} = (1 + (-x))^{-1}, replace xx by −x-x and kk by −1-1: 1+(−1)(−x)=1+x1 + (-1)(-x) = 1 + x. The two minus signs multiply to a plus, and dropping one of them gives 1−x1 - x, the classic slip. For 1+x=(1+x)1/2\sqrt{1 + x} = (1 + x)^{1/2}: 1+x21 + \frac{x}{2}.

b) (1.002)25=(1+0.002)25≈1+25(0.002)=1.05(1.002)^{25} = (1 + 0.002)^{25} \approx 1 + 25(0.002) = 1.05. Side: f′′(x)=k(k−1)(1+x)k−2=600(1+x)23>0f''(x) = k(k - 1)(1 + x)^{k-2} = 600(1 + x)^{23} > 0, concave up, the tangent is below: too small. Calculator: (1.002)25=1.051219(1.002)^{25} = 1.051219, and the percentage error is 1.051219−1.051.051219×100\frac{1.051219 - 1.05}{1.051219} \times 100, about 0.12%0.12\%.

c) The rule needs 1+1 + something small, and 9.189.18 is not of that form. Factor: 9.18=9×1.02=9 1.02=3(1+0.02)1/2≈3(1+0.022)=3(1.01)=3.03\sqrt{9.18} = \sqrt{9 \times 1.02} = \sqrt 9\,\sqrt{1.02} = 3(1 + 0.02)^{1/2} \approx 3\left(1 + \frac{0.02}{2}\right) = 3(1.01) = 3.03. Applying the rule to 9.18=1+8.189.18 = 1 + 8.18 instead gives 1+8.182=5.091 + \frac{8.18}{2} = 5.09, a tangent at 11 used eight units away. Side: (1+x)1/2(1 + x)^{1/2} is concave down (k(k−1)=−14<0k(k - 1) = -\frac{1}{4} < 0), so 3.033.03 is too large. Calculator: 9.18=3.029851\sqrt{9.18} = 3.029851; and 3.032=9.1809>9.183.03^2 = 9.1809 > 9.18 confirms it.

d) (2+x)−2=(2(1+x2))−2=2−2(1+x2)−2=14(1+x2)−2≈14(1−2⋅x2)=14(1−x)=14−x4(2 + x)^{-2} = \left(2\left(1 + \frac{x}{2}\right)\right)^{-2} = 2^{-2}\left(1 + \frac{x}{2}\right)^{-2} = \frac{1}{4}\left(1 + \frac{x}{2}\right)^{-2} \approx \frac{1}{4}\left(1 - 2 \cdot \frac{x}{2}\right) = \frac{1}{4}(1 - x) = \frac{1}{4} - \frac{x}{4}. The factored constant is raised to the power −2-2 too: 2−2=142^{-2} = \frac{1}{4}. At x=0.06x = 0.06: 14(0.94)=0.235\frac{1}{4}(0.94) = 0.235. Calculator: 12.062=0.235649\frac{1}{2.06^2} = 0.235649 (the estimate is too small, (1+u)−2(1 + u)^{-2} being concave up). The student applied (1+x)k(1 + x)^k to 2+x2 + x as if the 22 were a 11: he forgot to factor out 2−22^{-2} and to halve xx. At x=0x = 0 his formula gives 11 while (2+0)−2=14(2 + 0)^{-2} = \frac{1}{4}: any linearization must be exact at its centre, and this one is not.

e) (1.08)5≈1+5(0.08)=1.4(1.08)^5 \approx 1 + 5(0.08) = 1.4, while the calculator gives 1.4693281.469328: a percentage error of 1.469328−1.41.469328×100\frac{1.469328 - 1.4}{1.469328} \times 100, about 4.72%4.72\%, forty times worse than in b). Yet x=0.08x = 0.08 looks small. What enters the approximation is the product kxkx: 25×0.002=0.0525 \times 0.002 = 0.05 in b), 5×0.08=0.45 \times 0.08 = 0.4 here. On the figure the tangent y=1+5xy = 1 + 5x and the curve are almost together up to about x=0.02x = 0.02, then separate: at x=0.08x = 0.08 the gap between the two marked points is about 0.070.07. The rule is safe when kxkx is small, not merely when xx is.

Exercise 4: Finding dy: the differential as a formula, and the algebra that simplifies it

For y=f(x)y = f(x), the differential is dy=f′(x) dxdy = f'(x)\,dx, where dxdx is an independent increment. Every rule has a differential form: d(u+v)=du+dvd(u + v) = du + dv, d(uv)=u dv+v dud(uv) = u\,dv + v\,du, d(uv)=v du−u dvv2d\left(\frac{u}{v}\right) = \frac{v\,du - u\,dv}{v^2}. A question that says “find dydy” expects dydy written as ONE simplified expression times dxdx.

The calculus is routine here; the marks go to the simplification: a common denominator after the product rule, a numerator reduced after the quotient rule, a common factor pulled out. Calculator allowed for the numerical values, six decimal places.

  • a) For y=x1−x2y = x\sqrt{1 - x^2}, find dydy as a single fraction times dxdx. Evaluate it for x=0.6x = 0.6 and dx=0.02dx = 0.02.
  • b) For y=x−1x+3y = \frac{x - 1}{x + 3}, find dydy, simplifying the numerator. For x=1x = 1 and dx=0.2dx = 0.2, compute dydy and the exact change Δy\Delta y.
  • c) For y=x2e−xy = x^2 e^{-x}, find dydy in factored form, then its value for x=1x = 1 and dx=0.1dx = 0.1.
  • d) The point (1,2)(1, 2) lies on the curve xy2+y=6xy^2 + y = 6. Differentiate the equation in differential form and express dydy in terms of dxdx at (1,2)(1, 2). Use it to estimate the yy of the point of the curve with x=1.05x = 1.05 near (1,2)(1, 2), and compare with the exact value given by the quadratic formula.
  • e) Two quantities have values u=3u = 3 and v=5v = 5 and small changes du=0.1du = 0.1 and dv=−0.2dv = -0.2. Compute d(uv)d(uv) and d(uv)d\left(\frac{u}{v}\right).

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  • a) dy=1−2x21−x2 dxdy = \frac{1 - 2x^2}{\sqrt{1 - x^2}}\,dx; for x=0.6x = 0.6, dx=0.02dx = 0.02: dy=0.35×0.02=0.007dy = 0.35 \times 0.02 = 0.007
  • b) dy=4(x+3)2 dxdy = \frac{4}{(x + 3)^2}\,dx; dy=0.05dy = 0.05, Δy=0.24.2=0.047619\Delta y = \frac{0.2}{4.2} = 0.047619
  • c) dy=x(2−x)e−x dxdy = x(2 - x)e^{-x}\,dx; dy=0.1e=0.036788dy = \frac{0.1}{e} = 0.036788
  • d) y2 dx+2xy dy+dy=0y^2\,dx + 2xy\,dy + dy = 0, dy=−y22xy+1 dx=−0.8 dxdy = -\frac{y^2}{2xy + 1}\,dx = -0.8\,dx; y≈1.96y \approx 1.96, exact 1.9612351.961235
  • e) d(uv)=3(−0.2)+5(0.1)=−0.1d(uv) = 3(-0.2) + 5(0.1) = -0.1; d(uv)=5(0.1)−3(−0.2)25=0.044d\left(\frac{u}{v}\right) = \frac{5(0.1) - 3(-0.2)}{25} = 0.044

a) Product rule, then the chain rule on 1−x2\sqrt{1 - x^2} with inner function 1−x21 - x^2: dydx=1−x2+x⋅−2x21−x2=1−x2−x21−x2\frac{dy}{dx} = \sqrt{1 - x^2} + x \cdot \frac{-2x}{2\sqrt{1 - x^2}} = \sqrt{1 - x^2} - \frac{x^2}{\sqrt{1 - x^2}}. Common denominator, the step that costs the marks: 1−x2=1−x21−x2\sqrt{1 - x^2} = \frac{1 - x^2}{\sqrt{1 - x^2}}, so dydx=1−x2−x21−x2=1−2x21−x2\frac{dy}{dx} = \frac{1 - x^2 - x^2}{\sqrt{1 - x^2}} = \frac{1 - 2x^2}{\sqrt{1 - x^2}} and dy=1−2x21−x2 dxdy = \frac{1 - 2x^2}{\sqrt{1 - x^2}}\,dx. At x=0.6x = 0.6: 1−2(0.36)=0.281 - 2(0.36) = 0.28 and 1−0.36=0.8\sqrt{1 - 0.36} = 0.8, so dy=0.280.8(0.02)=0.35×0.02=0.007dy = \frac{0.28}{0.8}(0.02) = 0.35 \times 0.02 = 0.007.

b) Quotient rule: dydx=(x+3)−(x−1)(x+3)2\frac{dy}{dx} = \frac{(x + 3) - (x - 1)}{(x + 3)^2}. The numerator needs its brackets: (x+3)−(x−1)=x+3−x+1=4(x + 3) - (x - 1) = x + 3 - x + 1 = 4; without them one gets x+3−x−1=2x + 3 - x - 1 = 2, half the answer. So dy=4(x+3)2 dxdy = \frac{4}{(x + 3)^2}\,dx. At x=1x = 1, dx=0.2dx = 0.2: dy=416(0.2)=0.05dy = \frac{4}{16}(0.2) = 0.05. Exact change: y(1.2)−y(1)=0.24.2−0=0.047619y(1.2) - y(1) = \frac{0.2}{4.2} - 0 = 0.047619. The differential is close, and slightly too large, the function being concave down there (y′′=−8(x+3)3<0y'' = -\frac{8}{(x + 3)^3} < 0).

c) Product rule and chain rule on e−xe^{-x} (inner function −x-x): dydx=2xe−x+x2(−e−x)=2xe−x−x2e−x\frac{dy}{dx} = 2xe^{-x} + x^2(-e^{-x}) = 2xe^{-x} - x^2e^{-x}. Factor out the common xe−xxe^{-x}: dydx=x(2−x)e−x\frac{dy}{dx} = x(2 - x)e^{-x}, so dy=x(2−x)e−x dxdy = x(2 - x)e^{-x}\,dx. The factored form shows at once where dy=0dy = 0 (x=0x = 0 and x=2x = 2) and makes the evaluation clean: at x=1x = 1, dy=1⋅1⋅e−1(0.1)=0.1e=0.036788dy = 1 \cdot 1 \cdot e^{-1}(0.1) = \frac{0.1}{e} = 0.036788.

d) Take the differential of each term: d(xy2)=y2 dx+x⋅2y dyd(xy^2) = y^2\,dx + x \cdot 2y\,dy (product rule in differential form) and d(y)=dyd(y) = dy, while d(6)=0d(6) = 0. So y2 dx+2xy dy+dy=0y^2\,dx + 2xy\,dy + dy = 0, that is (2xy+1) dy=−y2 dx(2xy + 1)\,dy = -y^2\,dx and dy=−y22xy+1 dxdy = -\frac{y^2}{2xy + 1}\,dx. Check the point: 1⋅4+2=61 \cdot 4 + 2 = 6. At (1,2)(1, 2): dy=−45 dx=−0.8 dxdy = -\frac{4}{5}\,dx = -0.8\,dx. With dx=0.05dx = 0.05: dy=−0.04dy = -0.04, so y≈2−0.04=1.96y \approx 2 - 0.04 = 1.96. Exactly, 1.05y2+y−6=01.05y^2 + y - 6 = 0 gives y=−1+1+4(1.05)(6)2(1.05)=−1+26.22.1=1.961235y = \frac{-1 + \sqrt{1 + 4(1.05)(6)}}{2(1.05)} = \frac{-1 + \sqrt{26.2}}{2.1} = 1.961235 (the positive root, the one near 22). The estimate is off by about 0.00120.0012.

e) d(uv)=u dv+v du=3(−0.2)+5(0.1)=−0.6+0.5=−0.1d(uv) = u\,dv + v\,du = 3(-0.2) + 5(0.1) = -0.6 + 0.5 = -0.1: the product decreases slightly although uu increased. And d(uv)=v du−u dvv2=5(0.1)−3(−0.2)25=0.5+0.625=1.125=0.044d\left(\frac{u}{v}\right) = \frac{v\,du - u\,dv}{v^2} = \frac{5(0.1) - 3(-0.2)}{25} = \frac{0.5 + 0.6}{25} = \frac{1.1}{25} = 0.044. The minus sign of the quotient rule meets the minus sign of dvdv: two negatives, a plus. These two forms are exactly what propagates measurement errors through a product or a quotient.

Exercise 5: dy against Delta y, and Thomas' epsilon

When xx moves from aa to a+dxa + dx, the true change is Δy=f(a+dx)−f(a)\Delta y = f(a + dx) - f(a), measured along the CURVE, while dy=f′(a) dxdy = f'(a)\,dx is measured along the TANGENT. Thomas writes the gap as Δy=f′(a) dx+ε dx\Delta y = f'(a)\,dx + \varepsilon\,dx, where ε→0\varepsilon \to 0 as dx→0dx \to 0: the error is small compared with dxdx itself. With f(a)f(a) as reference, Δy\Delta y is the absolute change, Δyf(a)\frac{\Delta y}{f(a)} the relative change, and 100Δyf(a)100\frac{\Delta y}{f(a)} the percentage change.

The figure shows y=x3/2y = x^{3/2} near P(4,8)P(4, 8) with a deliberately large dx=2dx = 2: RR is level with PP, TT lies on the tangent at PP and QQ on the curve, all at x=6x = 6. Calculator allowed, six decimal places.

33.544.555.566.576810121416PRTQdx = 2y = x^(3/2)tangent at P
  • a) Find dydy for y=x3/2y = x^{3/2}. With x=4x = 4 and dx=2dx = 2, compute dydy and Δy\Delta y, and say which segments of the figure they are.
  • b) At x=4x = 4, compute dydy and Δy\Delta y for dx=0.1dx = 0.1, then for dx=0.01dx = 0.01.
  • c) Compute ε=Δy−dydx\varepsilon = \frac{\Delta y - dy}{dx} for dx=2dx = 2, 0.10.1 and 0.010.01, to four decimal places, and conclude.
  • d) Estimate with differentials the absolute, relative and percentage change of yy when xx goes from 44 to 4.14.1.
  • e) Compute dydy and Δy\Delta y for dx=−0.1dx = -0.1. In both directions, which of dydy and Δy\Delta y is larger? Explain with f′′f'' and the figure.

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  • a) dy=32x1/2 dxdy = \frac{3}{2}x^{1/2}\,dx; dy=6=RTdy = 6 = RT, Δy=63/2−8=6.696938=RQ\Delta y = 6^{3/2} - 8 = 6.696938 = RQ
  • b) dx=0.1dx = 0.1: dy=0.3dy = 0.3, Δy=0.301867\Delta y = 0.301867; dx=0.01dx = 0.01: dy=0.03dy = 0.03, Δy=0.030019\Delta y = 0.030019
  • c) ε=0.3485\varepsilon = 0.3485, 0.01870.0187, 0.00190.0019: ε→0\varepsilon \to 0 as dx→0dx \to 0
  • d) dy=0.3dy = 0.3; relative 0.38=0.0375\frac{0.3}{8} = 0.0375; percentage 3.75%3.75\%
  • e) dy=−0.3dy = -0.3, Δy=−0.298117\Delta y = -0.298117; Δy>dy\Delta y > dy in both directions (f′′>0f'' > 0, curve above tangent)

a) dydx=32x1/2\frac{dy}{dx} = \frac{3}{2}x^{1/2}, so dy=32x dxdy = \frac{3}{2}\sqrt x\,dx. At x=4x = 4: 32⋅2=3\frac{3}{2} \cdot 2 = 3, and with dx=2dx = 2, dy=6dy = 6. The true change is Δy=63/2−43/2=66−8=14.696938−8=6.696938\Delta y = 6^{3/2} - 4^{3/2} = 6\sqrt 6 - 8 = 14.696938 - 8 = 6.696938. Note 43/2=(4)3=84^{3/2} = (\sqrt 4)^3 = 8: root first, then the cube. On the figure, the tangent y=8+3(x−4)y = 8 + 3(x - 4) reaches T(6,14)T(6, 14) and the curve reaches Q(6,66)Q(6, 6\sqrt 6): dydy is the segment RTRT, Δy\Delta y the segment RQRQ, and TQTQ, about 0.700.70, is the error of the linear approximation.

b) For dx=0.1dx = 0.1: dy=3(0.1)=0.3dy = 3(0.1) = 0.3 and Δy=4.13/2−8=8.301867−8=0.301867\Delta y = 4.1^{3/2} - 8 = 8.301867 - 8 = 0.301867. For dx=0.01dx = 0.01: dy=0.03dy = 0.03 and Δy=4.013/2−8=0.030019\Delta y = 4.01^{3/2} - 8 = 0.030019. On a calculator, enter 4.11.54.1^{1.5} or 4.1×4.14.1 \times \sqrt{4.1}; typing 4.13/24.1^{3/2} without brackets computes 4.132\frac{4.1^3}{2}, a slip worth checking.

c) ε=Δy−dydx\varepsilon = \frac{\Delta y - dy}{dx}: for dx=2dx = 2, 6.696938−62=0.3485\frac{6.696938 - 6}{2} = 0.3485; for dx=0.1dx = 0.1, 0.0018670.1=0.0187\frac{0.001867}{0.1} = 0.0187; for dx=0.01dx = 0.01, 0.00001870.01=0.0019\frac{0.0000187}{0.01} = 0.0019. Each time dxdx is divided by 1010, ε\varepsilon is divided by about 1010 too, so ε→0\varepsilon \to 0. The gap Δy−dy=ε dx\Delta y - dy = \varepsilon\,dx is therefore divided by about 100100: it is small compared with dxdx, not merely small. That is Thomas' statement that the differential is the best linear estimate of the change.

d) Absolute change: dy=3(0.1)=0.3dy = 3(0.1) = 0.3 (true value 0.3018670.301867). Relative change: dyy(4)=0.38=0.0375\frac{dy}{y(4)} = \frac{0.3}{8} = 0.0375. Percentage change: 3.75%3.75\%. Keep the two last ones apart: 0.03750.0375 IS 3.75%3.75\%, and writing 0.0375%0.0375\% divides the answer by a hundred. Faster, with the algebra done first: dyy=32x1/2 dxx3/2=32dxx=32⋅0.14=0.0375\frac{dy}{y} = \frac{\frac{3}{2}x^{1/2}\,dx}{x^{3/2}} = \frac{3}{2}\frac{dx}{x} = \frac{3}{2} \cdot \frac{0.1}{4} = 0.0375.

e) dy=3(−0.1)=−0.3dy = 3(-0.1) = -0.3 and Δy=3.93/2−8=7.701883−8=−0.298117\Delta y = 3.9^{3/2} - 8 = 7.701883 - 8 = -0.298117. So Δy>dy\Delta y > dy here too: the function drops LESS than the tangent says. With dx=0.1dx = 0.1, Δy=0.301867>0.3=dy\Delta y = 0.301867 > 0.3 = dy. In both directions the curve is above its tangent, because f′′(x)=34x−1/2>0f''(x) = \frac{3}{4}x^{-1/2} > 0: concave up, as the figure shows on the right of PP and would show on its left. When dx<0dx < 0, being above the tangent means a change that is less negative, not larger in size: compare signed numbers, never sizes.

Part B: problems and reasoning (/50)

Exercise 6: Propagated error: a ball measured with a tape around its equator

A quantity xx is measured with a maximum error dxdx; a quantity computed from it, y=f(x)y = f(x), then carries the propagated error dy=f′(x) dxdy = f'(x)\,dx. Its relative error is dyy\frac{dy}{y} and its percentage error 100dyy100\frac{dy}{y}. The whole method rests on one rule: write yy as a function of the quantity that was actually MEASURED, not of the one that appears in the textbook formula.

The circumference of a ball is measured with a tailor's tape around its equator: C=75C = 75 cm, with a maximum error of 0.50.5 cm. The radius is never measured. Calculator allowed; give lengths, areas and volumes to two decimal places unless told otherwise.

rtape: C = 75 cm
  • a) Express the radius rr, the surface area SS and the volume VV of the ball in terms of CC, simplifying the powers of π\pi. Compute VV to the nearest cm3^3.
  • b) Use a differential to estimate the maximum error in the computed volume. Give the relative error and the percentage error.
  • c) Same questions for the surface area.
  • d) A student writes dr=0.5dr = 0.5 cm and dV=4πr2 drdV = 4\pi r^2\,dr. What does he find, and what is the actual error on the radius?
  • e) How precisely must CC be measured for the volume to be known within 1%1\%? Finally, compute the exact change ΔV\Delta V when CC goes from 7575 to 75.575.5, and compare with b).

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  • a) r=C2πr = \frac{C}{2\pi}, S=C2πS = \frac{C^2}{\pi}, V=C36π2V = \frac{C^3}{6\pi^2}; V≈7124V \approx 7124 cm3^3
  • b) dV=C22π2 dC=142.48dV = \frac{C^2}{2\pi^2}\,dC = 142.48 cm3^3; dVV=3dCC=0.02\frac{dV}{V} = 3\frac{dC}{C} = 0.02, that is 2%2\%
  • c) dS=2Cπ dC=75π=23.87dS = \frac{2C}{\pi}\,dC = \frac{75}{\pi} = 23.87 cm2^2; dSS=2dCC\frac{dS}{S} = 2\frac{dC}{C}, about 1.33%1.33\%
  • d) 895.25895.25 cm3^3, 2π2\pi times too large; dr=dC2π=0.0796dr = \frac{dC}{2\pi} = 0.0796 cm
  • e) 3dCC≤0.013\frac{dC}{C} \le 0.01, so dC≤0.25dC \le 0.25 cm; ΔV=143.43\Delta V = 143.43 cm3^3 against dV=142.48dV = 142.48 cm3^3

a) C=2πrC = 2\pi r, so r=C2πr = \frac{C}{2\pi}. Then S=4πr2=4π⋅C24π2=C2πS = 4\pi r^2 = 4\pi \cdot \frac{C^2}{4\pi^2} = \frac{C^2}{\pi}, and V=43πr3=43π⋅C3(2π)3=43π⋅C38π3=C36π2V = \frac{4}{3}\pi r^3 = \frac{4}{3}\pi \cdot \frac{C^3}{(2\pi)^3} = \frac{4}{3}\pi \cdot \frac{C^3}{8\pi^3} = \frac{C^3}{6\pi^2}. The power applies to the whole bracket: (2π)3=8π3(2\pi)^3 = 8\pi^3, and writing 2π32\pi^3 divides the volume by four. With C=75C = 75: V=421 8756π2=7124.15V = \frac{421\,875}{6\pi^2} = 7124.15, about 71247124 cm3^3.

b) dVdC=3C26π2=C22π2\frac{dV}{dC} = \frac{3C^2}{6\pi^2} = \frac{C^2}{2\pi^2}, so dV=C22π2 dC=56252π2(0.5)=142.48dV = \frac{C^2}{2\pi^2}\,dC = \frac{5625}{2\pi^2}(0.5) = 142.48 cm3^3. Relative error, with the algebra done before the numbers: dVV=C2/(2π2)C3/(6π2) dC=6π22π2⋅dCC=3dCC=3⋅0.575=0.02\frac{dV}{V} = \frac{C^2/(2\pi^2)}{C^3/(6\pi^2)}\,dC = \frac{6\pi^2}{2\pi^2} \cdot \frac{dC}{C} = 3\frac{dC}{C} = 3 \cdot \frac{0.5}{75} = 0.02, that is 2%2\%. The π\pi's cancel: simplifying the quotient first avoids two rounded divisions and shows that the exponent 33 triples the 23%\frac{2}{3}\% error of the tape.

c) dS=2Cπ dC=150π(0.5)=75π=23.87dS = \frac{2C}{\pi}\,dC = \frac{150}{\pi}(0.5) = \frac{75}{\pi} = 23.87 cm2^2, for S=5625π=1790.49S = \frac{5625}{\pi} = 1790.49 cm2^2. Relative error: dSS=2C/πC2/π dC=2dCC=175\frac{dS}{S} = \frac{2C/\pi}{C^2/\pi}\,dC = 2\frac{dC}{C} = \frac{1}{75}, about 1.33%1.33\%. The square doubles the relative error, the cube triples it.

d) With r=752π=11.94r = \frac{75}{2\pi} = 11.94 cm and dr=0.5dr = 0.5: 4πr2(0.5)=895.254\pi r^2(0.5) = 895.25 cm3^3, more than six times the right answer. The error of 0.50.5 cm is on the CIRCUMFERENCE; since r=C2πr = \frac{C}{2\pi}, dr=dC2π=0.52π=0.0796dr = \frac{dC}{2\pi} = \frac{0.5}{2\pi} = 0.0796 cm. With that value, 4πr2 dr=4πr2⋅dC2π=C22π2 dC4\pi r^2\,dr = 4\pi r^2 \cdot \frac{dC}{2\pi} = \frac{C^2}{2\pi^2}\,dC, the 142.48142.48 cm3^3 of b): both routes agree once the measured quantity is respected. The student's answer is exactly 2π2\pi times too large.

e) We need 3dCC≤0.013\frac{dC}{C} \le 0.01, so dCC≤1300\frac{dC}{C} \le \frac{1}{300} and dC≤75300=0.25dC \le \frac{75}{300} = 0.25 cm: the tape must be read twice as precisely. The exact change: ΔV=75.53−7536π2=143.43\Delta V = \frac{75.5^3 - 75^3}{6\pi^2} = 143.43 cm3^3, against dV=142.48dV = 142.48 cm3^3. The differential misses by less than 11 cm3^3, under 1%1\% of the error itself, which is itself only known to one significant figure: dVdV is all the precision that makes sense.

Exercise 7: A pendulum clock in summer: a longer rod, a slower clock

The period of a pendulum of length LL is T=2πLgT = 2\pi\sqrt{\frac{L}{g}}, with gg constant. A pendulum clock counts oscillations: if the period becomes a little longer, every oscillation takes a little more real time and the clock falls behind. Its metal rod expands with heat, and a clockmaker adjusts it with a screw under the bob. The clock of this exercise has L=0.994L = 0.994 m, which gives T=2T = 2 s with g=9.81g = 9.81 m/s2^2.

Write p=dLLp = \frac{dL}{L} for the relative change of the length. The exact ratio of the new period to the old one is then 1+p\sqrt{1 + p}, and its linearization is 1+p21 + \frac{p}{2}. The figure shows y=1+py = \sqrt{1 + p} and y=1+p2y = 1 + \frac{p}{2} on a deliberately wide window. Calculator allowed.

-0.8-0.6-0.4-0.20.20.40.60.811.20.20.40.60.811.21.41.61.8y = 1 + p/2y = √(1 + p)p
  • a) Write TT in the form cLkcL^k, then use differentials to express the relative change of the period in terms of the relative change pp of the length. Why do 2π2\pi and gg play no role?
  • b) On a hot day the rod lengthens by 0.3%0.3\%. Estimate the percentage change of the period with differentials, then compute the exact percentage change to four decimal places.
  • c) With that lengthening, use the estimate of b) to find how many seconds the clock loses in one week (604 800604\,800 s).
  • d) Another clock of the same length GAINS 3030 s per day (86 40086\,400 s). By what percentage must its rod be lengthened (four decimal places), and by how many millimetres (two decimal places)?
  • e) Compute the estimated and the exact percentage change of TT for p=0.21p = 0.21 and for p=−0.19p = -0.19. Where is the tangent with respect to the curve on the figure? Deduce whether the differential overestimates or underestimates the size of a RISE of the period, and of a DROP.

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  • a) dTT=π dL/gL2πL/g=12dLL\frac{dT}{T} = \frac{\pi\,dL/\sqrt{gL}}{2\pi\sqrt{L/g}} = \frac{1}{2}\frac{dL}{L}; 2π2\pi and gg cancel
  • b) Estimate +0.15%+0.15\%; exact 1.003−1\sqrt{1.003} - 1, about +0.1499%+0.1499\%
  • c) 0.0015×604 800=907.20.0015 \times 604\,800 = 907.2 s, about 1515 minutes per week
  • d) dTT=3086 400=12880\frac{dT}{T} = \frac{30}{86\,400} = \frac{1}{2880}, so dLL=22880\frac{dL}{L} = \frac{2}{2880}, about 0.0694%0.0694\%, that is 0.690.69 mm
  • e) p=0.21p = 0.21: estimate +10.5%+10.5\%, exact +10%+10\%; p=−0.19p = -0.19: estimate −9.5%-9.5\%, exact −10%-10\%. Tangent above the curve: a rise is overestimated, a drop underestimated.

a) T=2πg−1/2L1/2T = 2\pi g^{-1/2}L^{1/2}, so dTdL=2πg−1/2⋅12L−1/2=πgL\frac{dT}{dL} = 2\pi g^{-1/2} \cdot \frac{1}{2}L^{-1/2} = \frac{\pi}{\sqrt{gL}} and dT=πgL dLdT = \frac{\pi}{\sqrt{gL}}\,dL. Divide by TT before substituting anything: dTT=πgL⋅12πgL dL=12dLL\frac{dT}{T} = \frac{\pi}{\sqrt{gL}} \cdot \frac{1}{2\pi}\sqrt{\frac{g}{L}}\,dL = \frac{1}{2}\frac{dL}{L}. The π\pi's cancel, and gg=1\frac{\sqrt g}{\sqrt g} = 1, 1L⋅L=1L\frac{1}{\sqrt L \cdot \sqrt L} = \frac{1}{L}: the algebra of the quotient leaves only the exponent 12\frac{1}{2} of LL. That is the rule dyy=kdxx\frac{dy}{y} = k\frac{dx}{x} for y=cxky = cx^k, with k=12k = \frac{1}{2}.

b) dLL=0.003\frac{dL}{L} = 0.003 gives dTT=12(0.003)=0.0015\frac{dT}{T} = \frac{1}{2}(0.003) = 0.0015: the period grows by about 0.15%0.15\%. Exactly, Tnew=2π1.003Lg=1.003 TT_{\text{new}} = 2\pi\sqrt{\frac{1.003L}{g}} = \sqrt{1.003}\,T, and 1.003=1.0014989\sqrt{1.003} = 1.0014989, so the change is +0.1499%+0.1499\%. For a change this small the differential is excellent: the two agree to within one part in a thousand of the change itself.

c) Each oscillation lasts 0.15%0.15\% longer than the clock believes, so in a week of real time the clock counts about 0.15%0.15\% too few seconds: it loses about 0.0015×604 800=907.20.0015 \times 604\,800 = 907.2 s, roughly 1515 minutes. A lengthening of three millimetres per metre, invisible to the eye, is a quarter of an hour a week: this is why pendulum rods were made of materials that barely expand.

d) Gaining 3030 s per day means the period is too SHORT by the fraction 3086 400=12880\frac{30}{86\,400} = \frac{1}{2880}, so we need dTT=12880\frac{dT}{T} = \frac{1}{2880}. Going back from the period to the length, divide by the exponent 12\frac{1}{2}, that is multiply by 22: dLL=2⋅12880=11440\frac{dL}{L} = 2 \cdot \frac{1}{2880} = \frac{1}{1440}, about 0.0694%0.0694\%. On 0.9940.994 m: dL=0.9941440=0.00069dL = \frac{0.994}{1440} = 0.00069 m, that is 0.690.69 mm, one or two turns of the adjusting screw. Halving instead of doubling, 15760\frac{1}{5760}, would correct only a quarter of the fault.

e) For p=0.21p = 0.21: estimate 1+0.212=1.1051 + \frac{0.21}{2} = 1.105, a rise of 10.5%10.5\%; exactly 1.21=1.1\sqrt{1.21} = 1.1, a rise of 10%10\%. For p=−0.19p = -0.19: estimate 1−0.095=0.9051 - 0.095 = 0.905, a drop of 9.5%9.5\%; exactly 0.81=0.9\sqrt{0.81} = 0.9, a drop of 10%10\%. The function 1+p\sqrt{1 + p} has second derivative −14(1+p)−3/2<0-\frac{1}{4}(1 + p)^{-3/2} < 0: it is concave down and lies BELOW its tangent 1+p21 + \frac{p}{2} on both sides of 00, as the figure shows. So the linear estimate of the new period is always too large: a rise is OVERestimated (10.5%10.5\% against 10%10\%) and the size of a drop UNDERestimated (9.5%9.5\% against 10%10\%). These large values of pp only make the side visible; for the 0.3%0.3\% of b) the gap is negligible.

Exercise 8: Five statements to correct

Each statement below was written by a student on a MATH 203 assignment, and each one is false. Say what is wrong, settle it with a short computation, and write the correct statement. A calculator may be used for the checks.

  • a) For f(x)=x2/3f(x) = x^{2/3}, f′(8)=23⋅8−1/3=23(−2)=−43f'(8) = \frac{2}{3} \cdot 8^{-1/3} = \frac{2}{3}(-2) = -\frac{4}{3}, so L(x)=4−43(x−8)L(x) = 4 - \frac{4}{3}(x - 8).
  • b) 4.04=4+0.04≈2+0.042=2.02\sqrt{4.04} = \sqrt{4 + 0.04} \approx 2 + \frac{0.04}{2} = 2.02.
  • c) The relative error on the volume is dVV=0.02\frac{dV}{V} = 0.02, so the volume is known to within 0.02%0.02\%.
  • d) For f(x)=x2f(x) = x^2 at x=5x = 5 with dx=0.2dx = 0.2, the error made by the linear approximation is dy=2dy = 2.
  • e) exe^x is concave up, so its tangent at 00 lies above the curve and e0.1≈1.1e^{0.1} \approx 1.1 is an overestimate.

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  • a) False: 8−1/3=128^{-1/3} = \frac{1}{2}, f′(8)=13f'(8) = \frac{1}{3}, L(x)=4+13(x−8)L(x) = 4 + \frac{1}{3}(x - 8).
  • b) False: f′(4)=14f'(4) = \frac{1}{4}, so 4.04≈2+0.044=2.01\sqrt{4.04} \approx 2 + \frac{0.04}{4} = 2.01 (calculator 2.0099752.009975).
  • c) False: 0.02=2%0.02 = 2\%.
  • d) False: dy=2dy = 2 estimates the change; Δy=2.04\Delta y = 2.04, the error is Δy−dy=0.04\Delta y - dy = 0.04.
  • e) False: the tangent 1+x1 + x lies below, e0.1=1.105171>1.1e^{0.1} = 1.105171 > 1.1: an underestimate.

a) A negative exponent is a reciprocal, not a sign: 8−1/3=181/3=128^{-1/3} = \frac{1}{8^{1/3}} = \frac{1}{2}. So f′(8)=23⋅12=13f'(8) = \frac{2}{3} \cdot \frac{1}{2} = \frac{1}{3}, and with f(8)=(83)2=4f(8) = (\sqrt[3]{8})^2 = 4, L(x)=4+13(x−8)L(x) = 4 + \frac{1}{3}(x - 8). The student's line has a negative slope for an increasing function: x2/3x^{2/3} increases for x>0x > 0, so f′(8)<0f'(8) < 0 should have raised the alarm. Check: L(8.3)=4.1L(8.3) = 4.1 while the calculator gives 8.32/3=4.0993858.3^{2/3} = 4.099385; the student's line would give 3.63.6.

b) The derivative of x\sqrt x at 44 is 124=14\frac{1}{2\sqrt 4} = \frac{1}{4}, not 12\frac{1}{2}: the student used the slope of x\sqrt x at 11. Correct statement: 4.04≈2+14(0.04)=2.01\sqrt{4.04} \approx 2 + \frac{1}{4}(0.04) = 2.01. Or, factoring as in the standard linear approximation: 4.04=21.01≈2(1+0.012)=2.01\sqrt{4.04} = 2\sqrt{1.01} \approx 2\left(1 + \frac{0.01}{2}\right) = 2.01. The calculator gives 2.0099752.009975, so 2.012.01 is off by 0.0000250.000025 and 2.022.02 by 0.010.01. Check any root estimate by squaring: 2.022=4.08042.02^2 = 4.0804, far from 4.044.04.

c) A relative error is a pure fraction, and a percentage is that fraction times 100100: 0.02=2100=2%0.02 = \frac{2}{100} = 2\%. Writing 0.02%0.02\% claims a precision a hundred times better than the measurement gives. Correct statement: dVV=0.02\frac{dV}{V} = 0.02, so the volume is known to within 2%2\%.

d) dy=f′(5) dx=10(0.2)=2dy = f'(5)\,dx = 10(0.2) = 2 is the ESTIMATED change of yy, read along the tangent. The true change is Δy=5.22−52=27.04−25=2.04\Delta y = 5.2^2 - 5^2 = 27.04 - 25 = 2.04, and the error of the approximation is Δy−dy=0.04\Delta y - dy = 0.04, which here equals (dx)2(dx)^2. Correct statement: dy=2dy = 2 approximates Δy=2.04\Delta y = 2.04, with an error of 0.040.04.

e) Concave up means the curve bends UP away from its tangents: the tangent lies BELOW the curve. The tangent to exe^x at 00 is y=1+xy = 1 + x, and the calculator gives e0.1=1.105171>1.1e^{0.1} = 1.105171 > 1.1. Correct statement: since (ex)′′=ex>0(e^x)'' = e^x > 0, the estimate e0.1≈1.1e^{0.1} \approx 1.1 is an underestimate. Memory aid: concave up, tangent under, estimate under.

Exercise 9: A cylindrical tank: two measurements, one volume, and the error budget

A vertical cylindrical water tank is measured on site. Its inner diameter is D=2.4D = 2.4 m, measured with a maximum error of 11 cm, and its height is h=3.5h = 3.5 m. Written with the MEASURED quantity, its volume is V=π4D2hV = \frac{\pi}{4}D^2h. Recall that 11 m3=1000^3 = 1000 L.

The figure shows the tank. Calculator allowed; give volumes in litres to two decimal places and percentages to two decimal places.

D = 2.4 mh = 3.5 m
  • a) Take hh as exact. Compute VV, exactly in terms of π\pi and in m3^3, then use a differential to estimate the maximum error in VV, in litres.
  • b) Give the relative and percentage error of VV. A student writes V=πr2hV = \pi r^2h with r=1.2r = 1.2 and dr=0.01dr = 0.01: what maximum error does he find, and what went wrong?
  • c) The height is also measured, with a maximum error of 22 cm. Using d(uv)=u dv+v dud(uv) = u\,dv + v\,du, show that in the worst case ∣dVV∣=2∣dDD∣+∣dhh∣\left|\frac{dV}{V}\right| = 2\left|\frac{dD}{D}\right| + \left|\frac{dh}{h}\right|. Compute the percentage error and the maximum error in litres.
  • d) With hh exact again, how precisely must DD be measured for the volume to be known within 0.5%0.5\%? Answer in millimetres.
  • e) With hh exact, compute the exact change ΔV\Delta V when DD goes from 2.42.4 to 2.412.41 m, in litres. How far is it from dVdV, and what does the difference represent in the formula?

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  • a) V=5.04π=15.83V = 5.04\pi = 15.83 m3^3; dV=π2Dh dD=0.042πdV = \frac{\pi}{2}Dh\,dD = 0.042\pi m3=131.95^3 = 131.95 L
  • b) dVV=2dDD=1120\frac{dV}{V} = 2\frac{dD}{D} = \frac{1}{120}, about 0.83%0.83\%; the student gets 263.89263.89 L: dr=dD2=0.005dr = \frac{dD}{2} = 0.005 m, not 0.010.01
  • c) dVV=2dDD+dhh=1120+1175\frac{dV}{V} = 2\frac{dD}{D} + \frac{dh}{h} = \frac{1}{120} + \frac{1}{175}, about 1.40%1.40\%, that is 222.42222.42 L
  • d) 2dDD≤0.0052\frac{dD}{D} \le 0.005, so dD≤0.006dD \le 0.006 m =6= 6 mm
  • e) ΔV=132.22\Delta V = 132.22 L, 0.270.27 L more than dVdV: the term π4h(dD)2\frac{\pi}{4}h(dD)^2 dropped by the differential

a) V=π4(2.4)2(3.5)=π4(5.76)(3.5)=5.04πV = \frac{\pi}{4}(2.4)^2(3.5) = \frac{\pi}{4}(5.76)(3.5) = 5.04\pi, about 15.8315.83 m3^3. With hh constant, dVdD=π4⋅2Dh=π2Dh\frac{dV}{dD} = \frac{\pi}{4} \cdot 2Dh = \frac{\pi}{2}Dh, so dV=π2Dh dD=π2(2.4)(3.5)(0.01)=0.042πdV = \frac{\pi}{2}Dh\,dD = \frac{\pi}{2}(2.4)(3.5)(0.01) = 0.042\pi m3^3. In litres: 0.042π×1000=131.950.042\pi \times 1000 = 131.95 L. Convert the error to metres BEFORE substituting: 11 cm =0.01= 0.01 m; keeping dD=1dD = 1 with DD in metres multiplies the answer by a hundred.

b) dVV=π2Dh dDπ4D2h=2dDD=2⋅0.012.4=1120\frac{dV}{V} = \frac{\frac{\pi}{2}Dh\,dD}{\frac{\pi}{4}D^2h} = 2\frac{dD}{D} = 2 \cdot \frac{0.01}{2.4} = \frac{1}{120}, about 0.83%0.83\%. The fraction simplifies before any number goes in: π\pi, hh and one DD cancel. The student: dV=2πrh dr=2π(1.2)(3.5)(0.01)=0.084πdV = 2\pi rh\,dr = 2\pi(1.2)(3.5)(0.01) = 0.084\pi m3^3, that is 263.89263.89 L, exactly twice too much. The radius is half the diameter, so its error is half too: dr=dD2=0.005dr = \frac{dD}{2} = 0.005 m. With it, 2π(1.2)(3.5)(0.005)=0.042π2\pi(1.2)(3.5)(0.005) = 0.042\pi, the answer of a).

c) V=π4uvV = \frac{\pi}{4}uv with u=D2u = D^2 and v=hv = h. Then dV=π4(u dv+v du)=π4(D2 dh+h⋅2D dD)dV = \frac{\pi}{4}(u\,dv + v\,du) = \frac{\pi}{4}(D^2\,dh + h \cdot 2D\,dD). Dividing by V=π4D2hV = \frac{\pi}{4}D^2h: dVV=dhh+2dDD\frac{dV}{V} = \frac{dh}{h} + 2\frac{dD}{D}. The two errors may have either sign; in the worst case they add, so ∣dVV∣≤2∣dDD∣+∣dhh∣=1120+0.023.5=1120+1175=0.014048\left|\frac{dV}{V}\right| \le 2\left|\frac{dD}{D}\right| + \left|\frac{dh}{h}\right| = \frac{1}{120} + \frac{0.02}{3.5} = \frac{1}{120} + \frac{1}{175} = 0.014048, about 1.40%1.40\%. Maximum error: 0.014048×15.8336=0.222420.014048 \times 15.8336 = 0.22242 m3^3, that is 222.42222.42 L. The diameter, squared in the formula, weighs double: its 0.42%0.42\% becomes 0.83%0.83\%, while the height brings only 0.57%0.57\%.

d) We need 2dDD≤0.0052\frac{dD}{D} \le 0.005, so dDD≤0.0025\frac{dD}{D} \le 0.0025 and dD≤0.0025×2.4=0.006dD \le 0.0025 \times 2.4 = 0.006 m, that is 66 mm. Dividing by the exponent 22 is the step that gets forgotten: 0.5%0.5\% of 2.42.4 m, 1212 mm, would allow twice too much.

e) ΔV=π4(2.412−2.42)(3.5)=π4(0.0481)(3.5)=0.132222\Delta V = \frac{\pi}{4}(2.41^2 - 2.4^2)(3.5) = \frac{\pi}{4}(0.0481)(3.5) = 0.132222 m3^3, that is 132.22132.22 L, against dV=131.95dV = 131.95 L: a difference of 0.270.27 L, about 0.2%0.2\% of the error itself. Algebraically, (D+dD)2−D2=2D dD+(dD)2(D + dD)^2 - D^2 = 2D\,dD + (dD)^2: the differential keeps 2D dD2D\,dD and drops (dD)2(dD)^2, so the difference is exactly π4h(dD)2=π4(3.5)(0.0001)=0.000275\frac{\pi}{4}h(dD)^2 = \frac{\pi}{4}(3.5)(0.0001) = 0.000275 m3^3. That is the ε dx\varepsilon\,dx of Thomas, negligible for a measuring error.

Exercise 10: A final exam problem: linearizing a curve given by an equation

The curve x3+y3=9x^3 + y^3 = 9 passes through (1,2)(1, 2). Near that point it is the graph of a function y(x)y(x), and implicit differentiation gives its slope without solving for yy. The linearization is then the tangent line, and the side of the error comes from y′′y'', which is simplified by using the EQUATION of the curve: the algebra step on which this question is marked.

The figure shows the curve, its tangent at (1,2)(1, 2), and the point (93,0)(\sqrt[3]{9}, 0) with its vertical tangent dashed. Calculator allowed, six decimal places.

-0.50.511.522.53-1-0.50.511.522.53x³ + y³ = 9tangent at (1, 2)(∛9, 0)x
  • a) Check that (1,2)(1, 2) lies on the curve. Find dydx\frac{dy}{dx} by implicit differentiation and write the linearization L(x)L(x) of yy at x=1x = 1.
  • b) Use LL to estimate the yy-coordinate of the points of the curve with x=1.1x = 1.1 and x=0.9x = 0.9.
  • c) Show that y′′=−18xy5y'' = -\frac{18x}{y^5} on the curve, using its equation to simplify. Compute y′′y'' at (1,2)(1, 2) and deduce the side of both estimates.
  • d) Solve the equation for yy and compute the exact values at x=1.1x = 1.1 and x=0.9x = 0.9 with the calculator. Give the actual errors and check the side found in c).
  • e) Why has yy no linearization, as a function of xx, at the point (93,0)(\sqrt[3]{9}, 0)? Linearize xx as a function of yy there instead, estimate the xx of the point with y=0.3y = 0.3, and compare with the exact value.

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  • a) 1+8=91 + 8 = 9; dydx=−x2y2=−14\frac{dy}{dx} = -\frac{x^2}{y^2} = -\frac{1}{4}; L(x)=2−14(x−1)L(x) = 2 - \frac{1}{4}(x - 1)
  • b) y(1.1)≈1.975y(1.1) \approx 1.975, y(0.9)≈2.025y(0.9) \approx 2.025
  • c) y′′=−2x(x3+y3)y5=−18xy5y'' = -\frac{2x(x^3 + y^3)}{y^5} = -\frac{18x}{y^5}; y′′(1)=−916y''(1) = -\frac{9}{16}: both estimates too large
  • d) y=9−x33y = \sqrt[3]{9 - x^3}: 1.9720271.972027 and 2.0223332.022333; errors 0.0029730.002973 and 0.0026670.002667, both positive
  • e) dydx=−x2y2\frac{dy}{dx} = -\frac{x^2}{y^2} is undefined at y=0y = 0 (vertical tangent); dxdy=0\frac{dx}{dy} = 0 there, so x≈93=2.080084x \approx \sqrt[3]{9} = 2.080084; exact 2.0780022.078002

a) 13+23=1+8=91^3 + 2^3 = 1 + 8 = 9: the point is on the curve. Differentiating both sides with respect to xx, yy being a function of xx (chain rule on y3y^3): 3x2+3y2dydx=03x^2 + 3y^2\frac{dy}{dx} = 0, so dydx=−x2y2\frac{dy}{dx} = -\frac{x^2}{y^2}. At (1,2)(1, 2): −14-\frac{1}{4}. Hence L(x)=2−14(x−1)L(x) = 2 - \frac{1}{4}(x - 1), the orange line of the figure, which falls by 14\frac{1}{4} for each unit to the right.

b) L(1.1)=2−0.14=1.975L(1.1) = 2 - \frac{0.1}{4} = 1.975 and L(0.9)=2−−0.14=2+0.025=2.025L(0.9) = 2 - \frac{-0.1}{4} = 2 + 0.025 = 2.025. The minus of the slope meets the minus of the increment 0.9−1=−0.10.9 - 1 = -0.1: the estimate at 0.90.9 is ABOVE 22, as it must be on a decreasing curve.

c) Differentiate y′=−x2y−2y' = -x^2y^{-2} again, by the product rule, with yy still a function of xx: y′′=−2xy−2+2x2y−3y′y'' = -2xy^{-2} + 2x^2y^{-3}y'. Substitute y′=−x2y2y' = -\frac{x^2}{y^2}: y′′=−2xy2−2x4y5=−2xy3+2x4y5=−2x(x3+y3)y5y'' = -\frac{2x}{y^2} - \frac{2x^4}{y^5} = -\frac{2xy^3 + 2x^4}{y^5} = -\frac{2x(x^3 + y^3)}{y^5}. Now use the equation, x3+y3=9x^3 + y^3 = 9: y′′=−18xy5y'' = -\frac{18x}{y^5}. That substitution is the step that turns a messy expression into a clean one; without it, the value at (1,2)(1, 2) is still reachable but the sign on a whole interval is not. At (1,2)(1, 2): y′′=−1832=−916<0y'' = -\frac{18}{32} = -\frac{9}{16} < 0, and more generally y′′<0y'' < 0 wherever x>0x > 0 and y>0y > 0, hence on the whole arc between x=0.9x = 0.9 and x=1.1x = 1.1. Concave down: the tangent lies above the curve, and both estimates are too large.

d) y3=9−x3y^3 = 9 - x^3, so y=9−x33y = \sqrt[3]{9 - x^3}. At x=1.1x = 1.1: 9−1.331=7.6699 - 1.331 = 7.669 and y=1.972027y = 1.972027. At x=0.9x = 0.9: 9−0.729=8.2719 - 0.729 = 8.271 and y=2.022333y = 2.022333. Actual errors: 1.975−1.972027=0.0029731.975 - 1.972027 = 0.002973 and 2.025−2.022333=0.0026672.025 - 2.022333 = 0.002667. Both are positive, as c) predicted: the estimates are too large on both sides of x=1x = 1.

e) At (93,0)(\sqrt[3]{9}, 0), the formula dydx=−x2y2\frac{dy}{dx} = -\frac{x^2}{y^2} has a zero denominator and a nonzero numerator: the tangent is vertical (dashed on the figure), so no line y=f(a)+f′(a)(x−a)y = f(a) + f'(a)(x - a) exists. Exchange the roles: 3x2dxdy+3y2=03x^2\frac{dx}{dy} + 3y^2 = 0 gives dxdy=−y2x2\frac{dx}{dy} = -\frac{y^2}{x^2}, which is 00 at y=0y = 0. So near that point x≈93+0⋅yx \approx \sqrt[3]{9} + 0 \cdot y, and for y=0.3y = 0.3 the estimate is 93=2.080084\sqrt[3]{9} = 2.080084. Exactly, x=9−0.0273=8.9733=2.078002x = \sqrt[3]{9 - 0.027} = \sqrt[3]{8.973} = 2.078002, an error of 0.0020820.002082. A vertical tangent is not an obstacle to linearizing, only to linearizing in the wrong variable.

© Ahmed Squalli Houssaini. Exercise set published at www.letuteurscientifique.ca/en/exercices/math203-linearization-differentials. Free for personal and classroom use; republishing it elsewhere requires written permission (legal notice).

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