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Solução_Calculo_Stewart_6e

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F.<br />

300 ¤ CHAPTER 7 TECHNIQUES OF INTEGRATION<br />

TX.10<br />

67. Using the formula for volumes of rotation and the figure, we see that<br />

Volume = d<br />

0 πb2 dy − c<br />

0 πa2 dy − d<br />

c π[g(y)]2 dy = πb 2 d − πa 2 c − d<br />

c π[g(y)]2 dy. Lety = f(x),<br />

which gives dy = f 0 (x) dx and g(y) =x, sothatV = πb 2 d − πa 2 c − π b<br />

a x2 f 0 (x) dx.<br />

Now integrate by parts with u = x 2 ,anddv = f 0 (x) dx ⇒ du =2xdx, v = f(x), and<br />

b<br />

a x2 f 0 (x) dx = x 2 f(x) b<br />

a − b<br />

<br />

V = πb 2 d − πa 2 c − π b 2 d − a 2 c − <br />

b<br />

2xf(x) dx a<br />

2xf(x) dx = a b2 f(b) − a 2 f(a) − b<br />

2xf(x) dx,butf(a) =c and f(b) =d ⇒<br />

a<br />

= b<br />

2πx f(x) dx.<br />

a<br />

7.2 Trigonometric Integrals<br />

The symbols<br />

s = and c = indicate the use of the substitutions {u =sinx, du =cosxdx} and {u =cosx, du = − sin xdx}, respectively.<br />

<br />

1. sin 3 x cos 2 xdx = sin 2 x cos 2 x sin xdx= (1 − cos 2 x)cos 2 x sin xdx= c (1 − u 2 )u 2 (−du)<br />

= (u 2 − 1)u 2 du = (u 4 − u 2 ) du = 1 5 u5 − 1 3 u3 + C = 1 5 cos5 x − 1 3 cos3 x + C<br />

3.<br />

3π/4<br />

sin 5 x cos 3 xdx = 3π/4<br />

sin 5 x cos 2 x cos xdx= 3π/4<br />

sin 5 x (1 − sin 2 x)cosxdx= s √ 2/2<br />

u 5 (1 − u 2 ) du<br />

π/2 π/2 π/2 1<br />

= √ 2/2<br />

(u 5 − u 7 ) du = 1<br />

1 6 u6 − 1 8 u8√ 2/2<br />

=<br />

1<br />

<br />

1/8<br />

− 1/16<br />

6 8<br />

5. Let y = πx,sody = πdxand<br />

<br />

sin 2 (πx) cos 5 (πx) dx = 1 π sin 2 y cos 5 ydy= 1 π sin 2 y cos 4 y cos ydy<br />

<br />

− 1<br />

− 1<br />

6 8 = −<br />

11<br />

384<br />

= 1 π<br />

= 1 π<br />

<br />

sin 2 y (1 − sin 2 y) 2 cos ydy = s 1<br />

π u 2 (1 − u 2 ) 2 du = 1 π (u 2 − 2u 4 + u 6 ) du<br />

1<br />

3 u3 − 2 5 u5 + 1 7 u7 + C = 1<br />

3π sin3 y − 2<br />

5π sin5 y + 1<br />

7π sin7 y + C<br />

= 1<br />

3π sin3 (πx) − 2<br />

5π sin5 (πx)+ 1<br />

7π sin7 (πx)+C<br />

7.<br />

π/2<br />

cos 2 θdθ = π/2<br />

0 0<br />

= 1 2<br />

1<br />

(1 + cos 2θ) dθ [half-angle identity]<br />

2<br />

θ +<br />

1<br />

sin 2θ π/2 <br />

= 1 π +0 − (0 + 0) = π 2 0 2 2 4<br />

9.<br />

π<br />

0<br />

sin4 (3t) dt = π<br />

0<br />

<br />

= 1 π<br />

4 0<br />

= 1 4<br />

<br />

sin 2 (3t) 2 dt = π<br />

1 (1 − cos <br />

0 2 6t)2 dt = 1 π (1 − 2cos6t 4 0 +cos2 6t) dt<br />

3 − 2cos6t + 1 cos 12t 2 2<br />

dt<br />

<br />

1 − 2cos6t +<br />

1<br />

2 (1 + cos 12t) dt = 1 4<br />

3<br />

2 t − 1 3<br />

sin 6t +<br />

1<br />

24 sin 12t π<br />

0 = 1 4<br />

3π<br />

2 − 0+0 − (0 − 0+0) = 3π 8<br />

π<br />

0<br />

<br />

11. (1 + cos θ) 2 dθ = <br />

(1 + 2 cos θ +cos 2 θ) dθ = θ +2sinθ + 1 2 (1 + cos 2θ) dθ<br />

= θ +2sinθ + 1 θ + 1 sin 2θ + C = 3 θ +2sinθ + 1 sin 2θ + C<br />

2 4 2 4<br />

13.<br />

π/2<br />

sin 2 x cos 2 xdx = π/2 1<br />

(4 0 0 4 sin2 x cos 2 x) dx = π/2 1<br />

(2 sin x cos <br />

0 4 x)2 dx = 1 π/2<br />

4<br />

= 1 4<br />

π/2<br />

0<br />

1<br />

2 (1 − cos 4x) dx = 1 8<br />

π/2<br />

0<br />

(1 − cos 4x) dx = 1 8<br />

sin 2 2xdx<br />

0<br />

x −<br />

1<br />

sin 4x π/2 <br />

= 1 π<br />

4 0 8 2<br />

=<br />

π<br />

16

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