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21b. Differentials · Newton's Method — Practice

Drill sheet for 21. Differentials · Newton's Method. Book-style solved ideas as guided checks and regenerable worksheets.


1. Linear approximations​

(a) 1243\sqrt[3]{124}: x=125x=125, Δx=−1\Delta x=-1, f′(125)=1/75f'(125)=1/75

1243∼5−175=37475≈4.9867\sqrt[3]{124}\sim 5-\frac1{75}=\frac{374}{75}\approx 4.9867

(true ≈4.9866\approx 4.9866).

(b) sin⁡61∘\sin 61^\circ: use radians — x=π/3x=\pi/3, Δx=π/180\Delta x=\pi/180, f′=cos⁡(π/3)=1/2f'=\cos(\pi/3)=1/2

sin⁡61∘∼32+π360≈0.8747\sin 61^\circ\sim \frac{\sqrt3}{2}+\frac{\pi}{360}\approx 0.8747

(true ≈0.8746\approx 0.8746).

Radians

Trig derivatives in calculus assume the argument is in radians. Convert 1∘=π/1801^\circ=\pi/180.

Linear approximation

Roots, sine, percent change
(1)Approximate 1243\sqrt[3]{124} using f(x)=x1/3f(x)=x^{1/3}, x=125x=125, Δx=−1\Delta x=-1.
f(125)=5f(125)=5, f′(x)=13x−2/3f'(x)=\frac13 x^{-2/3}, f′(125)=1/75f'(125)=1/75.
1243≈5+(1/75)(−1)=374/75≈4.9867\sqrt[3]{124}\approx 5+(1/75)(-1)=374/75\approx 4.9867.
≈4.9867\approx 4.9867 (true ≈4.9866\approx 4.9866).
(2)Approximate 174\sqrt[4]{17} from x=16x=16, Δx=1\Delta x=1.
f=x1/4f=x^{1/4}, f(16)=2f(16)=2, f′(16)=1/(4⋅8)=1/32f'(16)=1/(4\cdot 8)=1/32.
2+(1/32)=2.031252+(1/32)=2.03125.
2.031252.03125.

2. Cube volume, 1%1\% side increase​

V=x3V=x^{3}, Δx=0.01x\Delta x=0.01x:

ΔV∼3x2⋅(0.01x)=0.03x3.\Delta V\sim 3x^{2}\cdot(0.01x)=0.03x^{3}.

Volume grows by roughly 3%3\%.


3. Find dydy​

yydydy
x3+4x2−5x+6x^{3}+4x^{2}-5x+6(3x2+8x−5) dx(3x^{2}+8x-5)\,dx
(2x3+5)3/2(2x^{3}+5)^{3/2}9x22x3+5 dx9x^{2}\sqrt{2x^{3}+5}\,dx
x3+2x+1x2+3\dfrac{x^{3}+2x+1}{x^{2}+3}x4+7x2−2x+6(x2+3)2 dx\dfrac{x^{4}+7x^{2}-2x+6}{(x^{2}+3)^{2}}\,dx
cos⁡22x+sin⁡3x\cos^{2}2x+\sin 3x(−2sin⁡4x+3cos⁡3x) dx(-2\sin 4x+3\cos 3x)\,dx

Compute dy

Polynomial · chain · quotient · trig
(1)Find dydy if y=x3+4x2−5x+6y=x^{3}+4x^{2}-5x+6.
dy=(3x2+8x−5) dxdy=(3x^{2}+8x-5)\,dx.
(3x2+8x−5) dx(3x^{2}+8x-5)\,dx.
(2)Find dydy if y=(2x3+5)3/2y=(2x^{3}+5)^{3/2}.
dy=32(2x3+5)1/2⋅6x2 dx=9x2(2x3+5)1/2 dxdy=\tfrac32(2x^{3}+5)^{1/2}\cdot 6x^{2}\,dx=9x^{2}(2x^{3}+5)^{1/2}\,dx.
9x22x3+5 dx9x^{2}\sqrt{2x^{3}+5}\,dx.

4. dy/dxdy/dx via differentials​

(a) xy+x−2y=5xy+x-2y=5 ⇒ dydx=−y+1x−2\dfrac{dy}{dx}=-\dfrac{y+1}{x-2}.

(b) 2xy−3yx=8\dfrac{2x}{y}-\dfrac{3y}{x}=8 ⇒ dydx=yx\dfrac{dy}{dx}=\dfrac{y}{x} (after canceling 2x2+3y2≠02x^{2}+3y^{2}\neq 0).

(c) Parametric x=3cos⁡θ−cos⁡3θx=3\cos\theta-\cos 3\theta, y=3sin⁡θ−sin⁡3θy=3\sin\theta-\sin 3\theta:

dydx=cos⁡θ−cos⁡3θ−sin⁡θ+sin⁡3θ.\frac{dy}{dx}=\frac{\cos\theta-\cos 3\theta}{-\sin\theta+\sin 3\theta}.

dy/dx from differentials

Implicit and parametric
(1)Parametric: x=3cos⁡θ−cos⁡3θx=3\cos\theta-\cos 3\theta, y=3sin⁡θ−sin⁡3θy=3\sin\theta-\sin 3\theta. Find dy/dxdy/dx.
dx=(−3sin⁡θ+3sin⁡3θ) dθdx=(-3\sin\theta+3\sin 3\theta)\,d\theta, dy=(3cos⁡θ−3cos⁡3θ) dθdy=(3\cos\theta-3\cos 3\theta)\,d\theta.
dy/dx=(cos⁡θ−cos⁡3θ)/(−sin⁡θ+sin⁡3θ)dy/dx=(\cos\theta-\cos 3\theta)/(-\sin\theta+\sin 3\theta).
cos⁡θ−cos⁡3θ−sin⁡θ+sin⁡3θ\dfrac{\cos\theta-\cos 3\theta}{-\sin\theta+\sin 3\theta}.
(2)From xy=sin⁡(x−y)xy=\sin(x-y), find dy/dxdy/dx.
x dy+y dx=cos⁡(x−y)(dx−dy)x\,dy+y\,dx=\cos(x-y)(dx-dy).
dy/dx=cos⁡(x−y)−ycos⁡(x−y)+xdy/dx=\dfrac{\cos(x-y)-y}{\cos(x-y)+x}.
cos⁡(x−y)−ycos⁡(x−y)+x\dfrac{\cos(x-y)-y}{\cos(x-y)+x}.

5. Newton: x3+2x−5=0x^{3}+2x-5=0​

One real root between 11 and 22. With x0=1x_0=1:

xn+1=2xn3+53xn2+2.x_{n+1}=\frac{2x_n^{3}+5}{3x_n^{2}+2}.

x1=1.4x_1=1.4; stabilizes at ≈1.328268856\approx 1.328268856.


6. Newton: 2cos⁡x−x2=02\cos x-x^{2}=0​

Even ff ⇒ roots ±r\pm r. From x0=1x_0=1:

xn+1=xn2+2(xnsin⁡xn+cos⁡xn)2(xn+sin⁡xn),x_{n+1}=\frac{x_n^{2}+2(x_n\sin x_n+\cos x_n)}{2(x_n+\sin x_n)},

converging to r≈1.02168995r\approx 1.02168995 (and −r-r).

Newton roots

Cubic and trig–polynomial
(1)Newton for 2cos⁡x−x2=02\cos x-x^{2}=0 with x0=1x_{0}=1. Approximate the positive root.
f′=−2(x+sin⁡x)f'=-2(x+\sin x); even ff ⇒ roots ±r\pm r.
Converges to r≈1.02168995r\approx 1.02168995.
≈±1.02169\approx\pm 1.02169.
(2)Newton x−cos⁡x=0x-\cos x=0 to four decimals.
Fixed-point of cos⁡\cos; ≈0.7391\approx 0.7391.
0.73910.7391.

Mixed review​

Differentials & Newton mixed

Approx · errors · dy · implicit · roots · failures
(1)Piecewise f=±∣x−2∣f=\pm\sqrt{|x-2|} with x0=3x_{0}=3: what goes wrong?
Cusp / infinite slope at the root x=2x=2; tangent from x0=3x_{0}=3 does not settle.
Not a smooth simple root; Newton leaves the basin.
(2)Circular plate: radius 5→5.065\to 5.06. Estimate ΔA\Delta A for A=πr2A=\pi r^{2}.
dA=2πr dr=2π⋅5⋅0.06=0.6π≈1.88dA=2\pi r\,dr=2\pi\cdot 5\cdot 0.06=0.6\pi\approx 1.88 in².
0.6π≈1.880.6\pi\approx 1.88 in².
(3)Approximate sin⁡61∘\sin 61^\circ from sin⁡(π/3)\sin(\pi/3) with Δx=π/180\Delta x=\pi/180.
f=sin⁡f=\sin, f(π/3)=3/2f(\pi/3)=\sqrt{3}/2, f′=cos⁡(π/3)=1/2f'=\cos(\pi/3)=1/2.
sin⁡61∘≈3/2+(π/360)≈0.8747\sin 61^\circ\approx \sqrt{3}/2+(\pi/360)\approx 0.8747.
≈0.8747\approx 0.8747 (true ≈0.8746\approx 0.8746).
(4)Piecewise f=±∣x−2∣f=\pm\sqrt{|x-2|} with x0=3x_{0}=3: what goes wrong?
Cusp / infinite slope at the root x=2x=2; tangent from x0=3x_{0}=3 does not settle.
Not a smooth simple root; Newton leaves the basin.
(5)From xy=sin⁡(x−y)xy=\sin(x-y), find dy/dxdy/dx.
x dy+y dx=cos⁡(x−y)(dx−dy)x\,dy+y\,dx=\cos(x-y)(dx-dy).
dy/dx=cos⁡(x−y)−ycos⁡(x−y)+xdy/dx=\dfrac{\cos(x-y)-y}{\cos(x-y)+x}.
cos⁡(x−y)−ycos⁡(x−y)+x\dfrac{\cos(x-y)-y}{\cos(x-y)+x}.
(6)Approximate Δ(1/x)\Delta(1/x) as xx goes 1→0.981\to 0.98.
d(1/x)=−dx/x2=−(−0.02)/1=0.02d(1/x)=-dx/x^{2}=-( -0.02)/1=0.02.
0.020.02 (value increases).

Supplementary Problems​

7–10. More linear approximations and Δy\Delta y​

#SetupAns
7174\sqrt[4]{17}; 10205\sqrt[5]{1020}; cos⁡59∘\cos 59^\circ; tan⁡44∘\tan 44^\circ2.031252.03125; 3.996883.99688; 0.51510.5151; 0.96510.9651
8Δ(x3)\Delta(x^{3}) for 5→5.015\to 5.01; Δ(1/x)\Delta(1/x) for 1→0.981\to 0.980.750.75; 0.020.02
9Plate r:5→5.06r:5\to 5.06ΔA≈0.6π≈1.88\Delta A\approx 0.6\pi\approx 1.88 in²
10Ice ball r:10→9.8r:10\to 9.8ΔV≈−80π\Delta V\approx -80\pi; ΔS≈−16π\Delta S\approx -16\pi

11–16. Measurement error and surfaces​

  • 11. v=64.4hv=\sqrt{64.4 h}, h=100±0.5h=100\pm 0.5 ⇒ ∣Δv∣≈0.2|\Delta v|\approx 0.2 ft/s.
  • 12. Flight 22 mi above equator: extra ≈2π⋅2≈12.6\approx 2\pi\cdot 2\approx 12.6 mi.
  • 13. ∣dr∣≤0.001|dr|\le 0.001, need ∣dA∣≤0.1|dA|\le 0.1 ⇒ r≤16r\le 16 in.
  • 14. pV=20pV=20, p=5±0.02p=5\pm 0.02 ⇒ V=4±0.016V=4\pm 0.016.
  • 15. F=1/r2F=1/r^{2}, F=4±0.05F=4\pm 0.05 ⇒ r=0.5±0.003r=0.5\pm 0.003.
  • 16. Cone total surface S=πrr2+h2+πr2S=\pi r\sqrt{r^{2}+h^{2}}+\pi r^{2}:
    • (a) fixed rr: dS=πrhr2+h2 ΔhdS=\dfrac{\pi r h}{\sqrt{r^{2}+h^{2}}}\,\Delta h
    • (b) fixed hh: dS=π ⁣(h2+2r2r2+h2+2r)ΔrdS=\pi\!\left(\dfrac{h^{2}+2r^{2}}{\sqrt{r^{2}+h^{2}}}+2r\right)\Delta r

Error & small-change estimates

Plates · spheres · gas law · equator
(1)Area to ±0.1\pm 0.1 in²; ∣dr∣≤0.001|dr|\le 0.001. Max rr for A=πr2A=\pi r^{2}?
∣dA∣=2πr∣dr∣≤0.1|dA|=2\pi r|dr|\le 0.1 ⇒ r≤0.1/(2π⋅0.001)≈16r\le 0.1/(2\pi\cdot 0.001)\approx 16.
r≤16r\le 16 in.
(2)Area to ±0.1\pm 0.1 in²; ∣dr∣≤0.001|dr|\le 0.001. Max rr for A=πr2A=\pi r^{2}?
∣dA∣=2πr∣dr∣≤0.1|dA|=2\pi r|dr|\le 0.1 ⇒ r≤0.1/(2π⋅0.001)≈16r\le 0.1/(2\pi\cdot 0.001)\approx 16.
r≤16r\le 16 in.
(3)pV=20pV=20, p=5±0.02p=5\pm 0.02. Estimate VV.
V=4V=4; dV=−20 dp/p2=−20(0.02)/25=−0.016dV=-20\,dp/p^{2}=-20(0.02)/25=-0.016.
V=4±0.016V=4\pm 0.016.

17–18. More dydy and implicit dy/dxdy/dx​

(17) y=(5−x)3y=(5-x)^{3}, sin⁡x/x\sin x/x, arccos⁡(2x)\arccos(2x), cos⁡(bx2)\cos(bx^{2}) — answers in the worksheet pool.

(18) 2xy3+3x2y=12xy^{3}+3x^{2}y=1 and xy=sin⁡(x−y)xy=\sin(x-y) — see dy/dxdy/dx worksheet.

19–22, 25–26. Newton (calculator)​

Equation / target≈ answer
x3+3x+1=0x^{3}+3x+1=0−0.3222-0.3222
x−cos⁡x=0x-\cos x=00.73910.7391
x3+2x2−4=0x^{3}+2x^{2}-4=01.13041.1304
34\sqrt[4]{3}; 2475\sqrt[5]{247}1.31611.3161; 3.00983.0098
Heron r\sqrt{r}: x←12(x+r/x)x\leftarrow\tfrac12(x+r/x); 5\sqrt{5}2.23612.2361
x3+x2−3=0x^{3}+x^{2}-3=0 in (1,2)(1,2)1.17461.1746
cos⁡x+1=0\cos x+1=0 (→ π\pi)3.1415926543.141592654 (slow: f′(π)=0f'(\pi)=0)
cos⁡x=x/2\cos x=x/2 (positive)1.0298665291.029866529

23–24. Failure cases​

  • 23. x1/3=0x^{1/3}=0, x0=1x_0=1: update x↦−2xx\mapsto -2x diverges.
  • 24. (a) f′(1)=0f'(1)=0; (b) bad basin / horizontal issues; (c) cusp at root x=2x=2.

Newton failures

Why the iteration breaks
(1)Piecewise f=±∣x−2∣f=\pm\sqrt{|x-2|} with x0=3x_{0}=3: what goes wrong?
Cusp / infinite slope at the root x=2x=2; tangent from x0=3x_{0}=3 does not settle.
Not a smooth simple root; Newton leaves the basin.
(2)For x3−3x2+3x+2=0x^{3}-3x^{2}+3x+2=0 with x0=1x_{0}=1, why does Newton fail?
f′(x)=3(x−1)2f'(x)=3(x-1)^{2}; f′(1)=0f'(1)=0 — division by zero / horizontal tangent.
f′(x0)=0f'(x_{0})=0.

Self-check​

Quiz

Differentials & Newton review

1 / 7

∛124 ≈ 5 − 1/75 uses f′(125) = …

Pick an answer to see if you are right.

Further Reading​