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3.40: a) The plane’s northward component of velocity relative to the air must be 80.0<br />

80.8<br />

km/h, so the heading must be arcsin 320<br />

= 14°<br />

north of west. b) Using the angle found in<br />

part (a), ( 320 km/h) cos14° = 310 km/h . Equivalently,<br />

(320 km/h)<br />

2<br />

2<br />

− (80.0 km/h) = 310 km/h .<br />

2<br />

2<br />

2.0<br />

3.41: a) ( 2.0 m/s) + (4.2 m/s) = 4.7 m/s, arctan<br />

4.2<br />

= 25. 5°<br />

, south of east.<br />

b) 800 m/4.2 m/s = 190 s .<br />

c) 2 .0 m/s × 190 s = 381 m .<br />

3.42: a) The speed relative to the water is still 4.2 m/s; the necessary heading of the boat<br />

is arcsin 2.0 4.2<br />

= 28°<br />

north of east. b) 2<br />

2<br />

(4.2 m/s) − (2.0 m/s) = 3.7 m/s , east. d)<br />

800 m/3.7 m/s = 217 s , rounded to three significant figures.<br />

3.43: a)<br />

b) x : −(10 m/s) cos 45°<br />

= −7.1m/s.<br />

y : = −(35 m/s) − (10 m/s)sin 45°<br />

= −42.1m/s<br />

.<br />

2<br />

2<br />

− 42.1<br />

c) −7.1m/s)<br />

+ ( −42.1m/s)<br />

= 42.7 m/s, arctan = 80°<br />

, south of west.<br />

(<br />

−7.<br />

1<br />

3.44: a) Using generalizations of Equations 2.17 and 2.18,<br />

α 3<br />

2<br />

v v t , v v βt<br />

− γ<br />

α 4<br />

β 2 γ 3<br />

= + = + t , and x = v t + t , y = v t + t − t . b) Setting<br />

x<br />

0 x<br />

3<br />

y<br />

0 y<br />

2<br />

γ 2<br />

v = 0 yields a quadratic in t, 0 = v + βt<br />

− t , which has as the positive solution<br />

y<br />

0 y<br />

0 x<br />

12<br />

0 y<br />

2<br />

2<br />

[ β + β + 2v0<br />

] = 13.59 s,<br />

1<br />

t = γ<br />

γ<br />

keeping an extra place in the intermediate calculation. Using this time in the expression<br />

for y(t) gives a maximum height of 341 m.<br />

2<br />

6

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