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Exercicios resolvidos James Stewart vol. 2 7ª ed - ingles

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D<br />

PROBLEMS PLUS<br />

1. Since three-dimensional situations are often difficult to visualize and work with, let<br />

us first try to find an analogous problem in two dimensions. The analogue of a cube<br />

is a square and the analogue of a sphere is a circle. Thus a similar problem in two<br />

dimensions is the following: if five circles with the same radius rare contain<strong>ed</strong> in a<br />

square of side 1 m so that the circles touch each other and four of the circles touch<br />

two sides ofthe square, find r.<br />

The diagonal of the square is .J2. The diagonal is a lso 4r + 2x . But x is the diagonal of a smaller square of side r . Therefore<br />

x = .J2r ~ .J2=4r+2x =4r+2.J2r= (4+2.J2)r ~ r = 4<br />

/{,/2.<br />

Let's use these ideas to solve the original three-dimensional problem. The diagonal of the cube is \/12 + 12 + 12 = v'a.<br />

The diagonal of the cube is also 4r + 2x where x is the diagonal of a smaller cube with <strong>ed</strong>ger. Therefore<br />

r;; r;; v'3 2 v'a - 3<br />

x = Jr 2 + 1·~ + r 2 = v'3 r ~ v'a = 4r+2x .=4r+2v3r = (4+2v3)r.Thus r= r;;=<br />

4 + 2v3 2<br />

The radius of each ball is ( v'3 - ~) m.<br />

3. (a) We find the line of intersection L as in Example 12.5. 7(b). Observe that the point ( - 1, c, c) lies on both planes. Now since<br />

L lies in both planes, it is perpendicular to both of the normal vectors n1 and n 2, and thus parallel to their cross product<br />

j<br />

k<br />

n 1 x n 2 = c 1 1 = (2c, -c 2 + 1, -c 2 - 1). So symmetric equations of L can be written as<br />

1 - c c<br />

-- x +1 = y - c z - c<br />

~<br />

1 =<br />

- 2c (..- - ~ c + 1<br />

, provid<strong>ed</strong> that c I 0, ±1.<br />

If c = 0, then the two planes are given by y + z = 0 and x = - 1, so symmetric· equations of L are x = - 1, y = - z. If<br />

c = - 1, then the two planes are given by -x + y + z = - 1 and x + y + z = -1, and they intersect in the line x = 0,<br />

y = - z - 1. If c = 1, then the two planes are given by x + y + z = 1 and x - y + z = 1, and they intersect in the line<br />

y = 0, X = 1- Z.<br />

(b) If we set z = t in the symmet~i c equations and solve for x andy separately, we get x + 1 = (t - c)( - 2 c)<br />

c 2 + 1<br />

(t- c)(c 2 - 1)<br />

y - c = c2 +1<br />

- 2ct + (c 2 - 1) (c 2 - 1)t + 2c El. . . fr th .<br />

~ x = c 2 + 1<br />

, Y = & + 1<br />

. unmatmg c om ese equattons, we<br />

have x 2 + y 2 = t 2 + 1. So the curve trac<strong>ed</strong> out by L in the plane z = tis a circle with center~~ (0, 0, t) and<br />

radius J fl + 1.<br />

© 2012 Cc:ngoge le=ling. All Rights Resorvoo. Moy nol be sconn<strong>ed</strong>, copi<strong>ed</strong>, or duplicalcd, or posll:d to o publicly occcssiblc wcbsito, in whole or in pori. 147

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