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Solução_Calculo_Stewart_6e

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F.<br />

132 ¤ CHAPTER 13 VECTORSANDTHEGEOMETRYOFSPACE ETTX.10<br />

CHAPTER 12<br />

(b) The intersection of this sphere with the yz-plane is the set of points on the sphere whose x-coordinate is 0. Putting x =0<br />

into the equation, we have (y − 2) 2 +(z − 1) 2 =68,x=0which represents a circle in the yz-plane with center (0, 2, 1)<br />

and radius √ 68.<br />

(c) Completing squares gives (x − 4) 2 +(y +1) 2 +(z +3) 2 = −1+16+1+9=25. Thus the sphere is centered at<br />

(4, −1, −3) and has radius 5.<br />

3. u · v = |u||v| cos 45 ◦ =(2)(3) √ 2<br />

2 =3√ 2. |u × v| = |u||v| sin 45 ◦ =(2)(3) √ 2<br />

2 =3√ 2.<br />

By the right-hand rule, u × v is directed out of the page.<br />

5. For the two vectors to be orthogonal, we need h3, 2,xi·h2x, 4,xi =0 ⇔ (3)(2x) + (2)(4) + (x)(x) =0 ⇔<br />

x 2 +6x +8=0 ⇔ (x +2)(x +4)=0 ⇔ x = −2 or x = −4.<br />

7. (a) (u × v) · w = u · (v × w) =2<br />

(b) u · (w × v) =u · [− (v × w)] = −u · (v × w) =−2<br />

(c) v · (u × w) =(v × u) · w = − (u × v) · w = −2<br />

(d) (u × v) · v = u · (v × v) =u · 0 =0<br />

9. For simplicity, consider a unit cube positioned with its back left corner at the origin. Vector representations of the diagonals<br />

11.<br />

joining the points (0, 0, 0) to (1, 1, 1) and (1, 0, 0) to (0, 1, 1) are h1, 1, 1i and h−1, 1, 1i. Letθ be the angle between these<br />

two vectors. h1, 1, 1i·h−1, 1, 1i = −1+1+1=1=|h1, 1, 1i| |h−1, 1, 1i| cos θ =3cosθ ⇒ cos θ = 1 3<br />

⇒<br />

θ =cos −1 1<br />

3<br />

<br />

≈ 71 ◦ .<br />

−→<br />

AB = h1, 0, −1i, −→<br />

AC = h0, 4, 3i,so<br />

(a) a vector perpendicular to the plane is −→<br />

AB × −→<br />

AC = h0+4, −(3 + 0), 4 − 0i = h4, −3, 4i.<br />

(b) 1 2<br />

−→<br />

AB × −→<br />

√<br />

AC = 1 √<br />

2 16 + 9 + 16 = 41<br />

. 2<br />

13. Let F 1 be the magnitude of the force directed 20 ◦ away from the direction of shore, and let F 2 be the magnitude of the other<br />

force. Separating these forces into components parallel to the direction of the resultant force and perpendicular to it gives<br />

F 1 cos 20 ◦ + F 2 cos 30 ◦ =255 (1),andF 1 sin 20 ◦ − F 2 sin 30 ◦ sin 30 ◦<br />

=0 ⇒ F 1 = F 2 (2). Substituting (2)<br />

sin 20◦ into (1) gives F 2 (sin 30 ◦ cot 20 ◦ +cos30 ◦ )=255 ⇒ F 2 ≈ 114 N. Substituting this into (2) gives F 1 ≈ 166 N.<br />

15. The line has direction v = h−3, 2, 3i. LettingP 0 =(4, −1, 2), parametric equations are<br />

x =4− 3t, y = −1+2t, z =2+3t.<br />

17. A direction vector for the line is a normal vector for the plane, n = h2, −1, 5i, and parametric equations for the line are<br />

x = −2+2t, y =2− t, z =4+5t.

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