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) replaces a function near a point, and the differential dy=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=81, a reciprocal, never a negative number); the sign of the increment x−a; the constant factored out before (1+x)k≈1+kx can be used (9.18=31.02); a derivative brought to a single fraction; the quotient ydy simplified to kxdx 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 16−3/4 as a negative number, losing the sign of x−a, using degrees in tanx, flipping 3/41 the wrong way, applying (1+x)k to 2+x without factoring, trusting the rule when kx is not small, confusing dy with Δy and with the error, writing 0.02 as 0.02%, putting the error of a circumference or a diameter on the radius, and forgetting that the exponent multiplies the relative error.
Self-checking setType 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.
Exercise 1: The fourth root at 16: the exponent at the centre, the sign of x - a, the side
The linearization of f at a is L(x)=f(a)+f′(a)(x−a), and f(x)≈L(x) is the standard linear approximation of f at a (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) with its sign, and the side of the error, read on the sign of 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)∣. The figure shows y=4x and its tangent at (16,2).
a) Find the linearization L of f(x)=4x at a=16. Write 16−3/4 as a fraction before using it.
b) Use L to approximate 417 and 415.5, as exact decimals.
c) Use 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−3/2 at a=4, approximate 4.2−3/2, give the side of the error, and compare with the calculator.
e) Approximate 416.5 with the same L and compute the actual error. About how many times smaller is it than the error at 17? Explain.
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Answers
a)f′(16)=41⋅16−3/4=321, so L(x)=2+321(x−16)
b)417≈2.03125, 415.5≈1.984375
c)Both too large (f′′<0); calculator 2.030543 and 1.984188; errors 0.000707 and 0.000187
d)Lg(x)=81−643(x−4); 4.2−3/2≈0.115625, too small; calculator 0.116179
e)416.5≈2.015625, error 0.000180, about 4 times smaller: half the distance, a quarter of the error
a) f(x)=x1/4, so by the power rule f′(x)=41x−3/4. At the centre, the algebra first: 16−3/4=163/41=(416)31=231=81. Take the root FIRST, then the power, then the reciprocal: 163 is 4096, a number nobody wants to root. A negative exponent means a reciprocal, never a negative number: writing 16−3/4=−8 or −12 makes the slope negative although the figure shows a rising curve. Hence f(16)=2, f′(16)=41⋅81=321, and L(x)=2+321(x−16). Check: L(16)=2=f(16).
b) 417≈L(17)=2+321=2.03125. For 15.5 the increment is NEGATIVE: x−a=15.5−16=−0.5, so 415.5≈2−320.5=2−641=1.984375. Losing the sign gives 2.015625, a value above 2 for a number below 16, which a rising function cannot produce.
c) f′′(x)=41⋅(−43)x−7/4=−163x−7/4<0 for x>0: the curve is concave down, it lies below each of its tangents (the figure shows it on both sides of (16,2)), so BOTH estimates are too large. The calculator agrees: 417=2.030543 and 415.5=1.984188 to six decimals. Actual errors: 2.03125−2.030543=0.000707 and 1.984375−1.984188=0.000187, both positive as predicted. As percentages of the true values, about 0.035% and 0.009%: the tangent is excellent this close to 16.
d) g(x)=x−3/2 gives g′(x)=−23x−5/2. At 4: 4−3/2=(4)31=81 and 4−5/2=(4)51=321, so g(4)=81 and g′(4)=−23⋅321=−643. Then Lg(x)=81−643(x−4) and 4.2−3/2≈0.125−643(0.2)=0.125−0.009375=0.115625. Side: g′′(x)=415x−7/2>0, concave up, the tangent lies BELOW the curve, so the estimate is too small. Calculator: 4.2−3/2=0.116179, larger than 0.115625 as predicted, error 0.000554. 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+320.5=2.015625 and the calculator gives 416.5=2.015445, an error of 0.000180. At 17 the error was 0.000707: the ratio is 0.0001800.000707, about 3.9, so about 4. The distance to the centre was halved, from 1 to 0.5, and the error was divided by about 22=4, not by 2. The error of a linearization behaves like a constant times (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 a is not chosen because it is a nice number, but because f(a) and f′(a) are EXACT there and a is close to the target. For ex near 0.7, that point is ln2, where eln2=2: an ugly number with perfect values. For a trigonometric function, the angle is in RADIANS, because (tanx)′=sec2x 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=tanx and its tangent at (4π,1).
a) Find the linearization of f(x)=ex at a=ln2 and use it to approximate e0.7. Is the estimate too large or too small? Compare with the calculator.
b) Write 44∘ as 4π+h with h in radians. Linearize tanx at 4π and approximate tan44∘, with the side of the error (use the figure and f′′). Compare with the calculator.
c) Linearize arcsinx at a=21, writing f′(21) as a simplified fraction, and approximate arcsin0.52, with the side. Compare with the calculator.
d) Linearize lnx at a=e and show that the estimate of ln2.7 simplifies to e2.7. Give its value, the side, and compare with the calculator.
e) A student centres ex at 0 and writes e0.7≈1.7. Compute the percentage error of this estimate, and explain why ln2 is the right centre although it is not a simple number.
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Answers
a)L(x)=2+2(x−ln2); e0.7≈2.013706, too small; calculator 2.013753
b)h=−180π; tan44∘≈1−90π=0.965093, too small; calculator 0.965689
c)f′(21)=32; arcsin0.52≈6π+30.04=0.546693, too small; calculator 0.546851
d)L(2.7)=1+e2.7−e=e2.7=0.993274, too large; calculator 0.993252
e)About 15.58%; 0.7 is far from 0 but only 0.0069 from ln2, where f and f′ are exactly 2.
a) f(ln2)=eln2=2 and f′(x)=ex, so f′(ln2)=2 as well. Hence L(x)=2+2(x−ln2). The calculator gives the increment, 0.7−ln2=0.006853, and e0.7≈2+2(0.006853)=2.013706. Side: (ex)′′=ex>0, the curve is concave up and lies above its tangent, so the estimate is too small. Calculator: e0.7=2.013753, larger indeed, an error of 0.000047. Keep ln2 exact inside L; round only the final number.
b) 44∘=45∘−1∘=4π−180π, so h=−180π rad. For f(x)=tanx: f(4π)=1 and f′(x)=sec2x, sec24π=cos2(π/4)1=1/21=2. So L(x)=1+2(x−4π) and tan44∘≈1+2(−180π)=1−90π=0.965093. With h=−1, the degree left unconverted, one gets L=−1, a negative tangent for an acute angle. Side: f′′(x)=2sec2xtanx>0 on (0,2π), the curve bends up away from its tangent on both sides (figure): too small. Calculator in degree mode: tan44∘=0.965689, error 0.000595.
c) f(x)=arcsinx, f(21)=6π, and f′(x)=1−x21. The algebra: 1−41=43, 43=23, and its reciprocal is 32, not 23: the fraction is flipped by the …1. So L(x)=6π+32(x−21) and arcsin0.52≈6π+32(0.02)=6π+30.04=0.523599+0.023094=0.546693. Side: f′′(x)=x(1−x2)−3/2>0 for 0<x<1: too small. Calculator (radian mode): arcsin0.52=0.546851, error 0.000158.
d) lne=1 and (lnx)′=x1 gives e1: L(x)=1+e1(x−e). At 2.7: 1+e2.7−e=1+e2.7−ee=e2.7. Distributing the e1 over (x−e) makes the 1 disappear, a simplification worth doing BEFORE the calculator. Value: e2.7=0.993274. Side: (lnx)′′=−x21<0, concave down, too large. Calculator: ln2.7=0.993252, error 0.000023.
e) Centred at 0: e0.7≈1+0.7=1.7, and the percentage error is 2.0137532.013753−1.7×100, about 15.58%, against 0.002% in a). The target 0.7 is at distance 0.7 from 0 but only 0.0069 from ln2. The centre is chosen for two properties together: f(a) and f′(a) exact (here both equal 2), and ∣x−a∣ small. Whether a itself looks simple does not matter, since only f(a) and 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 for x near 0 and any number k. It applies ONLY to the form 1+ (something small), so a quantity like 9.18 or (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)5 and its tangent y=1+5x at 0, with x=0.08 marked. Calculator allowed for the comparisons, six decimal places.
a) Show that the linearization of (1+x)k at 0 is 1+kx. Deduce the linearizations at 0 of 1−x1 and of 1+x.
b) Approximate (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) and approximate 9.18, with the side of the error. Compare with the calculator.
d) Show that (2+x)−2≈41−4x near 0 and approximate 2.0621; compare with the calculator. A student writes (2+x)−2≈1−2x: what did he forget, and how does x=0 expose it?
e) Approximate (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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Answers
a)f(0)=1, f′(0)=k; 1−x1≈1+x, 1+x≈1+2x
b)(1.002)25≈1.05, too small; calculator 1.051219, error about 0.12%
c)9.18=31.02≈3.03, too large; calculator 3.029851
d)(2+x)−2=41(1+2x)−2≈41(1−x); 2.0621≈0.235, calculator 0.235649; the factor 41 is missing, 1−2x gives 1=41 at x=0
e)(1.08)5≈1.4, calculator 1.469328, error about 4.72%: kx=0.4 is not small, while kx=0.05 in b)
a) f(x)=(1+x)k gives f(0)=1 and, by the chain rule with inner function 1+x, f′(x)=k(1+x)k−1, so f′(0)=k. Hence L(x)=1+kx. For 1−x1=(1+(−x))−1, replace x by −x and k by −1: 1+(−1)(−x)=1+x. The two minus signs multiply to a plus, and dropping one of them gives 1−x, the classic slip. For 1+x=(1+x)1/2: 1+2x.
b) (1.002)25=(1+0.002)25≈1+25(0.002)=1.05. Side: f′′(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, and the percentage error is 1.0512191.051219−1.05×100, about 0.12%.
c) The rule needs 1+ something small, and 9.18 is not of that form. Factor: 9.18=9×1.02=91.02=3(1+0.02)1/2≈3(1+20.02)=3(1.01)=3.03. Applying the rule to 9.18=1+8.18 instead gives 1+28.18=5.09, a tangent at 1 used eight units away. Side: (1+x)1/2 is concave down (k(k−1)=−41<0), so 3.03 is too large. Calculator: 9.18=3.029851; and 3.032=9.1809>9.18 confirms it.
d) (2+x)−2=(2(1+2x))−2=2−2(1+2x)−2=41(1+2x)−2≈41(1−2⋅2x)=41(1−x)=41−4x. The factored constant is raised to the power −2 too: 2−2=41. At x=0.06: 41(0.94)=0.235. Calculator: 2.0621=0.235649 (the estimate is too small, (1+u)−2 being concave up). The student applied (1+x)k to 2+x as if the 2 were a 1: he forgot to factor out 2−2 and to halve x. At x=0 his formula gives 1 while (2+0)−2=41: any linearization must be exact at its centre, and this one is not.
e) (1.08)5≈1+5(0.08)=1.4, while the calculator gives 1.469328: a percentage error of 1.4693281.469328−1.4×100, about 4.72%, forty times worse than in b). Yet x=0.08 looks small. What enters the approximation is the product kx: 25×0.002=0.05 in b), 5×0.08=0.4 here. On the figure the tangent y=1+5x and the curve are almost together up to about x=0.02, then separate: at x=0.08 the gap between the two marked points is about 0.07. The rule is safe when kx is small, not merely when x is.
Exercise 4: Finding dy: the differential as a formula, and the algebra that simplifies it
For y=f(x), the differential is dy=f′(x)dx, where dx is an independent increment. Every rule has a differential form: d(u+v)=du+dv, d(uv)=udv+vdu, d(vu)=v2vdu−udv. A question that says “find dy” expects dy written as ONE simplified expression times dx.
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−x2, find dy as a single fraction times dx. Evaluate it for x=0.6 and dx=0.02.
b) For y=x+3x−1, find dy, simplifying the numerator. For x=1 and dx=0.2, compute dy and the exact change Δy.
c) For y=x2e−x, find dy in factored form, then its value for x=1 and dx=0.1.
d) The point (1,2) lies on the curve xy2+y=6. Differentiate the equation in differential form and express dy in terms of dx at (1,2). Use it to estimate the y of the point of the curve with x=1.05 near (1,2), and compare with the exact value given by the quadratic formula.
e) Two quantities have values u=3 and v=5 and small changes du=0.1 and dv=−0.2. Compute d(uv) and d(vu).
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Answers
a)dy=1−x21−2x2dx; for x=0.6, dx=0.02: dy=0.35×0.02=0.007
a) Product rule, then the chain rule on 1−x2 with inner function 1−x2: dxdy=1−x2+x⋅21−x2−2x=1−x2−1−x2x2. Common denominator, the step that costs the marks: 1−x2=1−x21−x2, so dxdy=1−x21−x2−x2=1−x21−2x2 and dy=1−x21−2x2dx. At x=0.6: 1−2(0.36)=0.28 and 1−0.36=0.8, so dy=0.80.28(0.02)=0.35×0.02=0.007.
b) Quotient rule: dxdy=(x+3)2(x+3)−(x−1). The numerator needs its brackets: (x+3)−(x−1)=x+3−x+1=4; without them one gets x+3−x−1=2, half the answer. So dy=(x+3)24dx. At x=1, dx=0.2: dy=164(0.2)=0.05. Exact change: y(1.2)−y(1)=4.20.2−0=0.047619. The differential is close, and slightly too large, the function being concave down there (y′′=−(x+3)38<0).
c) Product rule and chain rule on e−x (inner function −x): dxdy=2xe−x+x2(−e−x)=2xe−x−x2e−x. Factor out the common xe−x: dxdy=x(2−x)e−x, so dy=x(2−x)e−xdx. The factored form shows at once where dy=0 (x=0 and x=2) and makes the evaluation clean: at x=1, dy=1⋅1⋅e−1(0.1)=e0.1=0.036788.
d) Take the differential of each term: d(xy2)=y2dx+x⋅2ydy (product rule in differential form) and d(y)=dy, while d(6)=0. So y2dx+2xydy+dy=0, that is (2xy+1)dy=−y2dx and dy=−2xy+1y2dx. Check the point: 1⋅4+2=6. At (1,2): dy=−54dx=−0.8dx. With dx=0.05: dy=−0.04, so y≈2−0.04=1.96. Exactly, 1.05y2+y−6=0 gives y=2(1.05)−1+1+4(1.05)(6)=2.1−1+26.2=1.961235 (the positive root, the one near 2). The estimate is off by about 0.0012.
e) d(uv)=udv+vdu=3(−0.2)+5(0.1)=−0.6+0.5=−0.1: the product decreases slightly although u increased. And d(vu)=v2vdu−udv=255(0.1)−3(−0.2)=250.5+0.6=251.1=0.044. The minus sign of the quotient rule meets the minus sign of dv: 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 x moves from a to a+dx, the true change is Δy=f(a+dx)−f(a), measured along the CURVE, while dy=f′(a)dx is measured along the TANGENT. Thomas writes the gap as Δy=f′(a)dx+εdx, where ε→0 as dx→0: the error is small compared with dx itself. With f(a) as reference, Δy is the absolute change, f(a)Δy the relative change, and 100f(a)Δy the percentage change.
The figure shows y=x3/2 near P(4,8) with a deliberately large dx=2: R is level with P, T lies on the tangent at P and Q on the curve, all at x=6. Calculator allowed, six decimal places.
a) Find dy for y=x3/2. With x=4 and dx=2, compute dy and Δy, and say which segments of the figure they are.
b) At x=4, compute dy and Δy for dx=0.1, then for dx=0.01.
c) Compute ε=dxΔy−dy for dx=2, 0.1 and 0.01, to four decimal places, and conclude.
d) Estimate with differentials the absolute, relative and percentage change of y when x goes from 4 to 4.1.
e) Compute dy and Δy for dx=−0.1. In both directions, which of dy and Δy is larger? Explain with f′′ and the figure.
e)dy=−0.3, Δy=−0.298117; Δy>dy in both directions (f′′>0, curve above tangent)
a) dxdy=23x1/2, so dy=23xdx. At x=4: 23⋅2=3, and with dx=2, dy=6. The true change is Δy=63/2−43/2=66−8=14.696938−8=6.696938. Note 43/2=(4)3=8: root first, then the cube. On the figure, the tangent y=8+3(x−4) reaches T(6,14) and the curve reaches Q(6,66): dy is the segment RT, Δy the segment RQ, and TQ, about 0.70, is the error of the linear approximation.
b) For dx=0.1: dy=3(0.1)=0.3 and Δy=4.13/2−8=8.301867−8=0.301867. For dx=0.01: dy=0.03 and Δy=4.013/2−8=0.030019. On a calculator, enter 4.11.5 or 4.1×4.1; typing 4.13/2 without brackets computes 24.13, a slip worth checking.
c) ε=dxΔy−dy: for dx=2, 26.696938−6=0.3485; for dx=0.1, 0.10.001867=0.0187; for dx=0.01, 0.010.0000187=0.0019. Each time dx is divided by 10, ε is divided by about 10 too, so ε→0. The gap Δy−dy=εdx is therefore divided by about 100: it is small compared with dx, 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)=0.3 (true value 0.301867). Relative change: y(4)dy=80.3=0.0375. Percentage change: 3.75%. Keep the two last ones apart: 0.0375 IS 3.75%, and writing 0.0375% divides the answer by a hundred. Faster, with the algebra done first: ydy=x3/223x1/2dx=23xdx=23⋅40.1=0.0375.
e) dy=3(−0.1)=−0.3 and Δy=3.93/2−8=7.701883−8=−0.298117. So Δy>dy here too: the function drops LESS than the tangent says. With dx=0.1, Δy=0.301867>0.3=dy. In both directions the curve is above its tangent, because f′′(x)=43x−1/2>0: concave up, as the figure shows on the right of P and would show on its left. When dx<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 x is measured with a maximum error dx; a quantity computed from it, y=f(x), then carries the propagated error dy=f′(x)dx. Its relative error is ydy and its percentage error 100ydy. The whole method rests on one rule: write y 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=75 cm, with a maximum error of 0.5 cm. The radius is never measured. Calculator allowed; give lengths, areas and volumes to two decimal places unless told otherwise.
a) Express the radius r, the surface area S and the volume V of the ball in terms of C, simplifying the powers of π. Compute V to the nearest cm3.
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=0.5 cm and dV=4πr2dr. What does he find, and what is the actual error on the radius?
e) How precisely must C be measured for the volume to be known within 1%? Finally, compute the exact change ΔV when C goes from 75 to 75.5, and compare with b).
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Answers
a)r=2πC, S=πC2, V=6π2C3; V≈7124 cm3
b)dV=2π2C2dC=142.48 cm3; VdV=3CdC=0.02, that is 2%
c)dS=π2CdC=π75=23.87 cm2; SdS=2CdC, about 1.33%
d)895.25 cm3, 2π times too large; dr=2πdC=0.0796 cm
e)3CdC≤0.01, so dC≤0.25 cm; ΔV=143.43 cm3 against dV=142.48 cm3
a) C=2πr, so r=2πC. Then S=4πr2=4π⋅4π2C2=πC2, and V=34πr3=34π⋅(2π)3C3=34π⋅8π3C3=6π2C3. The power applies to the whole bracket: (2π)3=8π3, and writing 2π3 divides the volume by four. With C=75: V=6π2421875=7124.15, about 7124 cm3.
b) dCdV=6π23C2=2π2C2, so dV=2π2C2dC=2π25625(0.5)=142.48 cm3. Relative error, with the algebra done before the numbers: VdV=C3/(6π2)C2/(2π2)dC=2π26π2⋅CdC=3CdC=3⋅750.5=0.02, that is 2%. The π's cancel: simplifying the quotient first avoids two rounded divisions and shows that the exponent 3 triples the 32% error of the tape.
c) dS=π2CdC=π150(0.5)=π75=23.87 cm2, for S=π5625=1790.49 cm2. Relative error: SdS=C2/π2C/πdC=2CdC=751, about 1.33%. The square doubles the relative error, the cube triples it.
d) With r=2π75=11.94 cm and dr=0.5: 4πr2(0.5)=895.25 cm3, more than six times the right answer. The error of 0.5 cm is on the CIRCUMFERENCE; since r=2πC, dr=2πdC=2π0.5=0.0796 cm. With that value, 4πr2dr=4πr2⋅2πdC=2π2C2dC, the 142.48 cm3 of b): both routes agree once the measured quantity is respected. The student's answer is exactly 2π times too large.
e) We need 3CdC≤0.01, so CdC≤3001 and dC≤30075=0.25 cm: the tape must be read twice as precisely. The exact change: ΔV=6π275.53−753=143.43 cm3, against dV=142.48 cm3. The differential misses by less than 1 cm3, under 1% of the error itself, which is itself only known to one significant figure: dV 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 L is T=2πgL, with g 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=0.994 m, which gives T=2 s with g=9.81 m/s2.
Write p=LdL for the relative change of the length. The exact ratio of the new period to the old one is then 1+p, and its linearization is 1+2p. The figure shows y=1+p and y=1+2p on a deliberately wide window. Calculator allowed.
a) Write T in the form cLk, then use differentials to express the relative change of the period in terms of the relative change p of the length. Why do 2π and g play no role?
b) On a hot day the rod lengthens by 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 (604800 s).
d) Another clock of the same length GAINS 30 s per day (86400 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 T for p=0.21 and for p=−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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Answers
a)TdT=2πL/gπdL/gL=21LdL; 2π and g cancel
b)Estimate +0.15%; exact 1.003−1, about +0.1499%
c)0.0015×604800=907.2 s, about 15 minutes per week
d)TdT=8640030=28801, so LdL=28802, about 0.0694%, that is 0.69 mm
e)p=0.21: estimate +10.5%, exact +10%; p=−0.19: estimate −9.5%, exact −10%. Tangent above the curve: a rise is overestimated, a drop underestimated.
a) T=2πg−1/2L1/2, so dLdT=2πg−1/2⋅21L−1/2=gLπ and dT=gLπdL. Divide by T before substituting anything: TdT=gLπ⋅2π1LgdL=21LdL. The π's cancel, and gg=1, L⋅L1=L1: the algebra of the quotient leaves only the exponent 21 of L. That is the rule ydy=kxdx for y=cxk, with k=21.
b) LdL=0.003 gives TdT=21(0.003)=0.0015: the period grows by about 0.15%. Exactly, Tnew=2πg1.003L=1.003T, and 1.003=1.0014989, so the change is +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% longer than the clock believes, so in a week of real time the clock counts about 0.15% too few seconds: it loses about 0.0015×604800=907.2 s, roughly 15 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 30 s per day means the period is too SHORT by the fraction 8640030=28801, so we need TdT=28801. Going back from the period to the length, divide by the exponent 21, that is multiply by 2: LdL=2⋅28801=14401, about 0.0694%. On 0.994 m: dL=14400.994=0.00069 m, that is 0.69 mm, one or two turns of the adjusting screw. Halving instead of doubling, 57601, would correct only a quarter of the fault.
e) For p=0.21: estimate 1+20.21=1.105, a rise of 10.5%; exactly 1.21=1.1, a rise of 10%. For p=−0.19: estimate 1−0.095=0.905, a drop of 9.5%; exactly 0.81=0.9, a drop of 10%. The function 1+p has second derivative −41(1+p)−3/2<0: it is concave down and lies BELOW its tangent 1+2p on both sides of 0, as the figure shows. So the linear estimate of the new period is always too large: a rise is OVERestimated (10.5% against 10%) and the size of a drop UNDERestimated (9.5% against 10%). These large values of p only make the side visible; for the 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)=x2/3, f′(8)=32⋅8−1/3=32(−2)=−34, so L(x)=4−34(x−8).
b) 4.04=4+0.04≈2+20.04=2.02.
c) The relative error on the volume is VdV=0.02, so the volume is known to within 0.02%.
d) For f(x)=x2 at x=5 with dx=0.2, the error made by the linear approximation is dy=2.
e) ex is concave up, so its tangent at 0 lies above the curve and e0.1≈1.1 is an overestimate.
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Answers
a)False: 8−1/3=21, f′(8)=31, L(x)=4+31(x−8).
b)False: f′(4)=41, so 4.04≈2+40.04=2.01 (calculator 2.009975).
c)False: 0.02=2%.
d)False: dy=2 estimates the change; Δy=2.04, the error is Δy−dy=0.04.
e)False: the tangent 1+x lies below, e0.1=1.105171>1.1: an underestimate.
a) A negative exponent is a reciprocal, not a sign: 8−1/3=81/31=21. So f′(8)=32⋅21=31, and with f(8)=(38)2=4, L(x)=4+31(x−8). The student's line has a negative slope for an increasing function: x2/3 increases for x>0, so f′(8)<0 should have raised the alarm. Check: L(8.3)=4.1 while the calculator gives 8.32/3=4.099385; the student's line would give 3.6.
b) The derivative of x at 4 is 241=41, not 21: the student used the slope of x at 1. Correct statement: 4.04≈2+41(0.04)=2.01. Or, factoring as in the standard linear approximation: 4.04=21.01≈2(1+20.01)=2.01. The calculator gives 2.009975, so 2.01 is off by 0.000025 and 2.02 by 0.01. Check any root estimate by squaring: 2.022=4.0804, far from 4.04.
c) A relative error is a pure fraction, and a percentage is that fraction times 100: 0.02=1002=2%. Writing 0.02% claims a precision a hundred times better than the measurement gives. Correct statement: VdV=0.02, so the volume is known to within 2%.
d) dy=f′(5)dx=10(0.2)=2 is the ESTIMATED change of y, read along the tangent. The true change is Δy=5.22−52=27.04−25=2.04, and the error of the approximation is Δy−dy=0.04, which here equals (dx)2. Correct statement: dy=2 approximates Δy=2.04, with an error of 0.04.
e) Concave up means the curve bends UP away from its tangents: the tangent lies BELOW the curve. The tangent to ex at 0 is y=1+x, and the calculator gives e0.1=1.105171>1.1. Correct statement: since (ex)′′=ex>0, the estimate e0.1≈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=2.4 m, measured with a maximum error of 1 cm, and its height is h=3.5 m. Written with the MEASURED quantity, its volume is V=4πD2h. Recall that 1 m3=1000 L.
The figure shows the tank. Calculator allowed; give volumes in litres to two decimal places and percentages to two decimal places.
a) Take h as exact. Compute V, exactly in terms of π and in m3, then use a differential to estimate the maximum error in V, in litres.
b) Give the relative and percentage error of V. A student writes V=πr2h with r=1.2 and dr=0.01: what maximum error does he find, and what went wrong?
c) The height is also measured, with a maximum error of 2 cm. Using d(uv)=udv+vdu, show that in the worst case VdV=2DdD+hdh. Compute the percentage error and the maximum error in litres.
d) With h exact again, how precisely must D be measured for the volume to be known within 0.5%? Answer in millimetres.
e) With h exact, compute the exact change ΔV when D goes from 2.4 to 2.41 m, in litres. How far is it from dV, and what does the difference represent in the formula?
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Answers
a)V=5.04π=15.83 m3; dV=2πDhdD=0.042π m3=131.95 L
b)VdV=2DdD=1201, about 0.83%; the student gets 263.89 L: dr=2dD=0.005 m, not 0.01
c)VdV=2DdD+hdh=1201+1751, about 1.40%, that is 222.42 L
d)2DdD≤0.005, so dD≤0.006 m =6 mm
e)ΔV=132.22 L, 0.27 L more than dV: the term 4πh(dD)2 dropped by the differential
a) V=4π(2.4)2(3.5)=4π(5.76)(3.5)=5.04π, about 15.83 m3. With h constant, dDdV=4π⋅2Dh=2πDh, so dV=2πDhdD=2π(2.4)(3.5)(0.01)=0.042π m3. In litres: 0.042π×1000=131.95 L. Convert the error to metres BEFORE substituting: 1 cm =0.01 m; keeping dD=1 with D in metres multiplies the answer by a hundred.
b) VdV=4πD2h2πDhdD=2DdD=2⋅2.40.01=1201, about 0.83%. The fraction simplifies before any number goes in: π, h and one D cancel. The student: dV=2πrhdr=2π(1.2)(3.5)(0.01)=0.084π m3, that is 263.89 L, exactly twice too much. The radius is half the diameter, so its error is half too: dr=2dD=0.005 m. With it, 2π(1.2)(3.5)(0.005)=0.042π, the answer of a).
c) V=4πuv with u=D2 and v=h. Then dV=4π(udv+vdu)=4π(D2dh+h⋅2DdD). Dividing by V=4πD2h: VdV=hdh+2DdD. The two errors may have either sign; in the worst case they add, so VdV≤2DdD+hdh=1201+3.50.02=1201+1751=0.014048, about 1.40%. Maximum error: 0.014048×15.8336=0.22242 m3, that is 222.42 L. The diameter, squared in the formula, weighs double: its 0.42% becomes 0.83%, while the height brings only 0.57%.
d) We need 2DdD≤0.005, so DdD≤0.0025 and dD≤0.0025×2.4=0.006 m, that is 6 mm. Dividing by the exponent 2 is the step that gets forgotten: 0.5% of 2.4 m, 12 mm, would allow twice too much.
e) ΔV=4π(2.412−2.42)(3.5)=4π(0.0481)(3.5)=0.132222 m3, that is 132.22 L, against dV=131.95 L: a difference of 0.27 L, about 0.2% of the error itself. Algebraically, (D+dD)2−D2=2DdD+(dD)2: the differential keeps 2DdD and drops (dD)2, so the difference is exactly 4πh(dD)2=4π(3.5)(0.0001)=0.000275 m3. That is the εdx of Thomas, negligible for a measuring error.
Exercise 10: A final exam problem: linearizing a curve given by an equation
The curve x3+y3=9 passes through (1,2). Near that point it is the graph of a function y(x), and implicit differentiation gives its slope without solving for y. The linearization is then the tangent line, and the side of the error comes from 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), and the point (39,0) with its vertical tangent dashed. Calculator allowed, six decimal places.
a) Check that (1,2) lies on the curve. Find dxdy by implicit differentiation and write the linearization L(x) of y at x=1.
b) Use L to estimate the y-coordinate of the points of the curve with x=1.1 and x=0.9.
c) Show that y′′=−y518x on the curve, using its equation to simplify. Compute y′′ at (1,2) and deduce the side of both estimates.
d) Solve the equation for y and compute the exact values at x=1.1 and x=0.9 with the calculator. Give the actual errors and check the side found in c).
e) Why has y no linearization, as a function of x, at the point (39,0)? Linearize x as a function of y there instead, estimate the x of the point with y=0.3, and compare with the exact value.
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Answers
a)1+8=9; dxdy=−y2x2=−41; L(x)=2−41(x−1)
b)y(1.1)≈1.975, y(0.9)≈2.025
c)y′′=−y52x(x3+y3)=−y518x; y′′(1)=−169: both estimates too large
d)y=39−x3: 1.972027 and 2.022333; errors 0.002973 and 0.002667, both positive
e)dxdy=−y2x2 is undefined at y=0 (vertical tangent); dydx=0 there, so x≈39=2.080084; exact 2.078002
a) 13+23=1+8=9: the point is on the curve. Differentiating both sides with respect to x, y being a function of x (chain rule on y3): 3x2+3y2dxdy=0, so dxdy=−y2x2. At (1,2): −41. Hence L(x)=2−41(x−1), the orange line of the figure, which falls by 41 for each unit to the right.
b) L(1.1)=2−40.1=1.975 and L(0.9)=2−4−0.1=2+0.025=2.025. The minus of the slope meets the minus of the increment 0.9−1=−0.1: the estimate at 0.9 is ABOVE 2, as it must be on a decreasing curve.
c) Differentiate y′=−x2y−2 again, by the product rule, with y still a function of x: y′′=−2xy−2+2x2y−3y′. Substitute y′=−y2x2: y′′=−y22x−y52x4=−y52xy3+2x4=−y52x(x3+y3). Now use the equation, x3+y3=9: y′′=−y518x. That substitution is the step that turns a messy expression into a clean one; without it, the value at (1,2) is still reachable but the sign on a whole interval is not. At (1,2): y′′=−3218=−169<0, and more generally y′′<0 wherever x>0 and y>0, hence on the whole arc between x=0.9 and x=1.1. Concave down: the tangent lies above the curve, and both estimates are too large.
d) y3=9−x3, so y=39−x3. At x=1.1: 9−1.331=7.669 and y=1.972027. At x=0.9: 9−0.729=8.271 and y=2.022333. Actual errors: 1.975−1.972027=0.002973 and 2.025−2.022333=0.002667. Both are positive, as c) predicted: the estimates are too large on both sides of x=1.
e) At (39,0), the formula dxdy=−y2x2 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) exists. Exchange the roles: 3x2dydx+3y2=0 gives dydx=−x2y2, which is 0 at y=0. So near that point x≈39+0⋅y, and for y=0.3 the estimate is 39=2.080084. Exactly, x=39−0.027=38.973=2.078002, an error of 0.002082. A vertical tangent is not an obstacle to linearizing, only to linearizing in the wrong variable.