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Solução_Calculo_Stewart_6e

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F.<br />

TX.10<br />

CHAPTER 10 REVIEW ¤ 445<br />

the length of the orbit is<br />

L =<br />

2π<br />

0<br />

<br />

r2 +(dr/dθ) 2 dθ = a(1 − e 2 )<br />

2π<br />

0<br />

√<br />

1+e2 − 2e cos θ<br />

(1 − e cos θ) 2 dθ ≈ 3.6 × 10 8 km<br />

This seems reasonable, since Mercury’s orbit is nearly circular, and the circumference of a circle of radius a<br />

is 2πa ≈ 3.6 × 10 8 km.<br />

10 Review<br />

1. (a) A parametric curve is a set of points of the form (x, y) =(f(t),g(t)), wheref and g are continuous functions of a<br />

variable t.<br />

(b)Sketchingaparametriccurve,likesketching the graph of a function, is difficult to do in general. We can plot points on the<br />

curve by finding f(t) and g(t) for various values of t, either by hand or with a calculator or computer. Sometimes, when<br />

f and g are given by formulas, we can eliminate t from the equations x = f(t) and y = g(t) to get a Cartesian equation<br />

relating x and y. It may be easier to graph that equation than to work with the original formulas for x and y in terms of t.<br />

2. (a) You can find dy<br />

dy<br />

as a function of t by calculating<br />

dx dx = dy/dt<br />

dx/dt<br />

[if dx/dt 6= 0].<br />

(b) Calculate the area as b<br />

a ydx= β<br />

α g(t) f 0 (t)dt [or α<br />

β g(t) f 0 (t)dt if the leftmost point is (f(β),g(β)) rather<br />

than (f(α),g(α))].<br />

3. (a) L = β<br />

<br />

(dx/dt)2 +(dy/dt)<br />

α<br />

2 dt = β<br />

<br />

α [f 0<br />

(t)] 2 +[g 0 (t)] 2 dt<br />

(b) S = β<br />

α 2πy (dx/dt) 2 +(dy/dt) 2 dt = β<br />

α 2πg(t) [f 0 (t)] 2 +[g 0 (t)] 2 dt<br />

4. (a) See Figure 5 in Section 10.3.<br />

(b) x = r cos θ, y = r sin θ<br />

(c) To find a polar representation (r, θ) with r ≥ 0 and 0 ≤ θ

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