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Solução_Calculo_Stewart_6e

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F.<br />

274 ¤ CHAPTER 6 APPLICATIONS OF INTEGRATION<br />

TX.10<br />

39. V = π<br />

π<br />

0<br />

CAS<br />

= 11 8 π2<br />

sin 2 x − (−1) 2<br />

− [0 − (−1)]<br />

2 dx<br />

41. π π/2<br />

cos 2 xdxdescribes the volume of the solid obtained by rotating the region R = (x, y) | 0 ≤ x ≤ π 0 2<br />

, 0 ≤ y ≤ cos x<br />

43. π<br />

of the xy-plane about the x-axis.<br />

1<br />

0<br />

(y 4 − y 8 ) dy = π<br />

1<br />

0<br />

<br />

(y 2 ) 2 − (y 4 ) 2 dy describes the volume of the solid obtained by rotating the region<br />

R = (x, y) | 0 ≤ y ≤ 1,y 4 ≤ x ≤ y 2 of the xy-plane about the y-axis.<br />

45. There are 10 subintervals over the 15-cm length, so we’ll use n =10/2 =5for the Midpoint Rule.<br />

V = 15<br />

0<br />

A(x) dx ≈ M 5 = 15−0<br />

5<br />

[A(1.5) + A(4.5) + A(7.5) + A(10.5) + A(13.5)]<br />

= 3(18 + 79 + 106 + 128 + 39) = 3 · 370 = 1110 cm 3<br />

47. (a) V = 10<br />

<br />

π [f(x)] 2 dx ≈ π 10 − 2<br />

2 4 [f(3)] 2 +[f(5)] 2 +[f(7)] 2 +[f(9)] 2<br />

≈ 2π (1.5) 2 +(2.2) 2 +(3.8) 2 +(3.1) 2 ≈ 196 units 3<br />

(b) V = 4<br />

π (outer radius) 2 − (inner radius) 2 dy<br />

0<br />

<br />

≈ π 4 − 0<br />

4 (9.9) 2 − (2.2) 2 + (9.7) 2 − (3.0) 2 + (9.3) 2 − (5.6) 2 + (8.7) 2 − (6.5) 2<br />

≈ 838 units 3<br />

49. We’ll form a right circular cone with height h and base radius r by<br />

revolving the line y = r x about the x-axis.<br />

h<br />

V = π<br />

h<br />

0<br />

r<br />

h x 2dx<br />

= π<br />

h<br />

= π r2<br />

h 2 1<br />

3 h3 <br />

= 1 3 πr2 h<br />

0<br />

r 2<br />

h 2 x2 dx = π r2<br />

h 2 1<br />

3 x3 h<br />

0<br />

Another solution: Revolve x = − r y + r about the y-axis.<br />

h<br />

h <br />

V = π − r 2dy<br />

h<br />

<br />

h y + r = ∗ r<br />

2<br />

<br />

π<br />

h 2 y2 − 2r2<br />

h y + r2 dy<br />

0<br />

0<br />

r<br />

2<br />

h<br />

= π<br />

3h 2 y3 − r2<br />

h y2 + r y 2 = π 1<br />

3 r2 h − r 2 h + r 2 h = 1 3 πr2 h<br />

0<br />

∗ Or use substitution with u = r − r h y and du = − r dy to get<br />

h<br />

0<br />

<br />

π u 2 − h <br />

r r du = −π h 0 1<br />

r 3 u3 = −π h − 1 <br />

r<br />

r 3 r3 = 1 3 πr2 h.

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