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Solução_Calculo_Stewart_6e

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F.<br />

SECTIONTX.10<br />

17.6 PARAMETRIC SURFACES AND THEIR AREAS ET SECTION 16.6 ¤ 289<br />

31. (a) Replacing cos u by sin u and sin u by cos u gives parametric equations<br />

x =(2+sinv)sinu, y =(2+sinv)cosu, z = u +cosv. From the graph, it<br />

appears that the direction of the spiral is reversed. We can verify this observation by<br />

noting that the projection of the spiral grid curves onto the xy-plane, given by<br />

x =(2+sinv)sinu, y =(2+sinv)cosu, z =0,drawsacircleintheclockwise<br />

direction for each value of v. The original equations, on the other hand, give circular<br />

projections drawn in the counterclockwise direction. The equation for z is identical in<br />

both surfaces, so as z increases, these grid curves spiral up in opposite directions for<br />

the two surfaces.<br />

(b) Replacing cos u by cos 2u and sin u by sin 2u gives parametric equations<br />

x =(2+sinv)cos2u, y =(2+sinv)sin2u, z = u +cosv. From the graph, it<br />

appears that the number of coils in the surface doubles within the same parametric<br />

domain. We can verify this observation by noting that the projection of the spiral grid<br />

curves onto the xy-plane, given by x =(2+sinv)cos2u, y =(2+sinv)sin2u,<br />

z =0(where v is constant), complete circular revolutions for 0 ≤ u ≤ π while the<br />

original surface requires 0 ≤ u ≤ 2π for a complete revolution. Thus, the new<br />

surface winds around twice as fast as the original surface, and since the equation for z<br />

is identical in both surfaces, we observe twice as many circular coils in the same<br />

z-interval.<br />

33. r(u, v) =(u + v) i +3u 2 j +(u − v) k.<br />

r u = i +6u j + k and r v = i − k,sor u × r v = −6u i +2j − 6u k.<br />

Since the point (2, 3, 0) corresponds to u =1, v =1, a normal vector<br />

to the surface at (2, 3, 0) is −6 i +2j − 6 k, and an equation of the<br />

tangent plane is −6x +2y − 6z = −6 or 3x − y +3z =3.<br />

35. r(u, v) =u 2 i +2u sin v j + u cos v k ⇒ r(1, 0) = (1, 0, 1).<br />

r u =2u i +2sinv j +cosv k and r v =2u cos v j − u sin v k,<br />

so a normal vector to the surface at the point (1, 0, 1) is<br />

r u (1, 0) × r v (1, 0) = (2 i + k) × (2 j) =−2 i +4k.<br />

Thus an equation of the tangent plane at (1, 0, 1) is<br />

−2(x − 1) + 0(y − 0) + 4(z − 1) = 0 or −x +2z =1.

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