30.04.2015 Views

Solução_Calculo_Stewart_6e

Solução_Calculo_Stewart_6e

Solução_Calculo_Stewart_6e

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

F.<br />

448 ¤ CHAPTER 10 PARAMETRIC EQUATIONS AND POLAR COORDINATES TX.10<br />

11. r =cos3θ.Thisisa<br />

three-leaved rose. The curve is<br />

traced twice.<br />

13. r =1+cos2θ. Thecurveis<br />

symmetric about the pole and<br />

both the horizontal and vertical<br />

axes.<br />

3<br />

15. r =<br />

⇒ e =2> 1, so the conic is a hyperbola. de =3 ⇒<br />

1+2sinθ<br />

d = 3 2<br />

and the form “+2 sin θ” imply that the directrix is above the focus at<br />

the origin and has equation y = 3 . The vertices are <br />

1, π 2 2 and −3,<br />

3π<br />

2 .<br />

2<br />

17. x + y =2 ⇔ r cos θ + r sin θ =2 ⇔ r(cos θ +sinθ) =2 ⇔ r =<br />

cos θ +sinθ<br />

19. r =(sinθ)/θ. Asθ → ±∞, r → 0.<br />

As θ → 0, r → 1. Inthefirst figure,<br />

there are an infinite number of<br />

x-intercepts at x = πn, n a nonzero<br />

integer. These correspond to pole<br />

points in the second figure.<br />

21. x =lnt, y =1+t 2 ; t =1. dy dx<br />

=2t and<br />

dt dt = 1 dy<br />

,so<br />

t dx = dy/dt<br />

dx/dt = 2t<br />

1/t =2t2 .<br />

When t =1, (x, y) =(0, 2) and dy/dx =2.<br />

23. r = e −θ ⇒ y = r sin θ = e −θ sin θ and x = r cos θ = e −θ cos θ ⇒<br />

dy<br />

dx = dy/dθ dr<br />

dx/dθ = sin θ + r cos θ<br />

dθ<br />

dr<br />

cos θ − r sin θ = −e−θ sin θ + e −θ cos θ<br />

−e −θ cos θ − e −θ sin θ · −eθ sin θ − cos θ<br />

=<br />

−eθ cos θ +sinθ .<br />

dθ<br />

When θ = π, dy<br />

dx = 0 − (−1)<br />

−1+0 = 1 −1 = −1.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!