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Solução_Calculo_Stewart_6e

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F.<br />

246 ¤ CHAPTER 16 MULTIPLE INTEGRALS ET CHAPTER 15<br />

TX.10<br />

37. m = E ρ(x, y, z) dV = 1<br />

0<br />

= 1<br />

<br />

0 2y +2xy + y<br />

2 y= √ x<br />

dx = 1<br />

y=0 0<br />

√ x<br />

1+x+y<br />

2 dz dy dx = 1<br />

√ x<br />

0 0 0<br />

<br />

<br />

2 √ x +2x 3/2 + x<br />

0<br />

2(1 + x + y) dy dx<br />

dx =<br />

<br />

1<br />

4<br />

3 x3/2 + 4 5 x5/2 + 1 2 x2 = 79<br />

30<br />

0<br />

M yz = xρ(x, y, z) dV = 1<br />

√ x<br />

1+x+y<br />

2xdzdydx= 1<br />

√ x<br />

2x(1 + x + y) dy dx<br />

E 0 0 0 0 0<br />

= 1<br />

<br />

0 2xy +2x 2 y + xy 2 y= √ x<br />

dx = <br />

1<br />

1<br />

y=0 0 (2x3/2 +2x 5/2 + x 2 4<br />

) dx =<br />

5 x5/2 + 4 7 x7/2 + 1 3 x3 = 179<br />

105<br />

0<br />

M xz = E yρ(x, y, z) dV = 1<br />

0<br />

= 1<br />

0<br />

<br />

y 2 + xy 2 + 2 3 y3 y= √ x<br />

y=0<br />

M xy = E zρ(x, y, z) dV = 1<br />

0<br />

√ x<br />

1+x+y<br />

2ydzdydx= 1<br />

√ x<br />

0 0 0<br />

dx = 1<br />

0<br />

x + x 2 + 2 3 x3/2 <br />

dx =<br />

√ x<br />

1+x+y<br />

2zdzdydx= 1<br />

0 0 0<br />

2y(1 + x + y) dy dx<br />

0<br />

<br />

1<br />

1<br />

2 x2 + 1 3 x3 + 4 15 x5/2 = 11<br />

10<br />

0<br />

√ x<br />

0<br />

z<br />

2 z=1+x+y<br />

= 1<br />

√ x<br />

(1 + 2x +2y +2xy + x 2 + y 2 ) dy dx = 1<br />

<br />

0 0 0 y +2xy + y 2 + xy 2 + x 2 y + 1 y3 y= √ x<br />

3<br />

= <br />

1 √x <br />

0 +<br />

7<br />

3 x3/2 + x + x 2 + x 5/2 dx =<br />

z=0<br />

<br />

1<br />

2<br />

3 x3/2 + 14<br />

15 x5/2 + 1 2 x2 + 1 3 x3 + 2 7 x7/2 = 571<br />

210<br />

0<br />

<br />

Thus the mass is 79 and the center of mass is (x, y, z) = Myz<br />

30<br />

m , Mxz<br />

m , Mxy 358<br />

=<br />

m 553 , 33<br />

79 , 571 <br />

.<br />

553<br />

dy dx = 1<br />

√ x<br />

(1 + x + y) 2 dy dx<br />

0 0<br />

y=0<br />

dx<br />

39. m = a a<br />

0 0<br />

= a<br />

0<br />

M yz = a a<br />

a<br />

0 0 0<br />

= a<br />

0<br />

a<br />

0 (x2 + y 2 + z 2 ) dx dy dz = a a<br />

1<br />

0 0 3 x3 + xy 2 + xz 2 x=a<br />

dy dz = a a<br />

1<br />

x=0 0 0 3 a3 + ay 2 + az 2 dy dz<br />

1<br />

3 a3 y + 1 3 ay3 + ayz 2 y=a<br />

dz = a<br />

2<br />

y=0 0 3 a4 + a 2 z 2 dz = 2<br />

3 a4 z + 1 3 a2 z 3 a<br />

= 2 0 3 a5 + 1 3 a5 = a 5<br />

<br />

x 3 + x(y 2 + z 2 ) dx dy dz = a<br />

a<br />

1<br />

0 0 4 a4 + 1 2 a2 (y 2 + z 2 ) dy dz<br />

1<br />

4 a5 + 1 6 a5 + 1 2 a3 z 2 dz = 1 4 a6 + 1 3 a6 = 7 12 a6 = M xz = M xy by symmetry of E and ρ(x, y, z)<br />

Hence (x, y, z) = 7<br />

12 a, 7<br />

12 a, 7 12 a .<br />

41. I x = L L<br />

L<br />

0 0 0<br />

k(y2 + z 2 ) dz dy dx = k L L<br />

0 0<br />

By symmetry, I x = I y = I z = 2 3 kL5 .<br />

<br />

Ly 2 + 1 3 L3 dy dx = k L<br />

0<br />

2<br />

3 L4 dx = 2 3 kL5 .<br />

43. I z = E (x2 + y 2 ) ρ(x, y, z) dV = <br />

h<br />

0 k(x2 + y 2 ) dz dA = <br />

k(x 2 + y 2 )hdA<br />

x 2 +y 2 ≤a 2 x 2 +y 2 ≤a 2<br />

= kh 2π a<br />

0 0 (r2 ) rdrdθ= kh 2π<br />

dθ a<br />

0 0 r3 dr = kh(2π) 1<br />

a<br />

4 0 4 a4 = 1 2 πkha4<br />

45. (a) m = 3<br />

−3<br />

√ √<br />

9−x2<br />

−<br />

5−y<br />

9−x 2 1<br />

<br />

x2 + y 2 dz dy dx<br />

<br />

Myz<br />

(b) (x, y, z) =<br />

m , Mxz<br />

m , Mxy<br />

where<br />

m<br />

M yz = 3<br />

−3<br />

M xy = 3<br />

−3<br />

(c) I z = 3<br />

−3<br />

√ √<br />

9−x2<br />

−<br />

√ √<br />

9−x2<br />

−<br />

√<br />

√<br />

9−x2<br />

−<br />

9−x 2 5−y<br />

9−x 2 5−y<br />

9−x 2 5−y<br />

1<br />

x x 2 + y 2 dz dy dx, M xz = 3<br />

1<br />

z x 2 + y 2 dz dy dx.<br />

1<br />

(x 2 + y 2 ) x 2 + y 2 dz dy dx = 3<br />

−3<br />

−3<br />

√ 9−x<br />

√<br />

2<br />

−<br />

√ 9−x<br />

√<br />

2<br />

−<br />

9−x 2 5−y<br />

9−x 2 5−y<br />

1<br />

y x 2 + y 2 dz dy dx, and<br />

1<br />

(x 2 + y 2 ) 3/2 dz dy dx

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