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Solução_Calculo_Stewart_6e

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F.<br />

TX.10<br />

CHAPTER 6 REVIEW ¤ 289<br />

29. (a) The parabola has equation y = ax 2 with vertex at the origin and passing through<br />

(4, 4). 4=a · 4 2 ⇒ a = 1 4<br />

⇒ y = 1 4 x2 ⇒ x 2 =4y ⇒<br />

x =2 y. Each circular disk has radius 2 y and is moved 4 − y ft.<br />

W = 4<br />

2 π 2 4<br />

y<br />

0 62.5(4 − y) dy = 250π y(4 − y) dy<br />

0<br />

= 250π 2y 2 − 1 y3 4<br />

=250π <br />

3<br />

32 − 64<br />

0 3 =<br />

8000π<br />

3<br />

≈ 8378 ft-lb<br />

(b) In part (a) we knew the final water level (0) but not the amount of work done. Here<br />

we use the same equation, except with the work fixed, and the lower limit of<br />

integration (that is, the final water level — call it h) unknown: W = 4000<br />

250π 2y 2 − 1 y3 4<br />

16<br />

3<br />

=4000 ⇔ = <br />

h π<br />

32 − 64 3 − 2h 2 − 1 h3 3<br />

⇔<br />

⇔<br />

h 3 − 6h 2 +32− 48 =0. We graph the function f(h) π =h3 − 6h 2 +32− 48<br />

π<br />

on the interval [0, 4] to see where it is 0. From the graph, f(h) =0for h ≈ 2.1.<br />

So the depth of water remaining is about 2.1 ft.<br />

31. lim<br />

h→0<br />

f ave =lim<br />

h→0<br />

1<br />

(x + h) − x<br />

x+h<br />

x<br />

F (x + h) − F (x)<br />

f(t) dt =lim<br />

,whereF (x) = x<br />

f(t) dt. But we recognize this<br />

h→0 h<br />

a<br />

limit as being F 0 (x) by the definition of a derivative. Therefore, lim<br />

h→0<br />

f ave = F 0 (x) =f(x) by FTC1.

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