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3.20: a) If air resistance is to be ignored, the components of acceleration are 0<br />

2<br />

horizontally and − g = −9.80 m s vertically.<br />

b) The x-component of velocity is constant at v = ( 12.0 m s)cos51.0°<br />

= 7.55 m s . The<br />

y-component is v = (12.0 m s)sin 51.0°<br />

9.32 m s at release and<br />

0 y<br />

=<br />

2<br />

0<br />

−<br />

v y<br />

− gt = (10.57 m s) − (9.80 m s )(2.08 s) = 11.06 m s when the shot hits.<br />

c) v0 x<br />

t = (7.55 m s)(2.08 s) = 15.<br />

7 m .<br />

d) The initial and final heights are not the same.<br />

e) With y = 0 and v 0y as found above, solving Eq. (3.18) for y = 1.81<br />

0<br />

m .<br />

x<br />

f)<br />

3.21: a) The time the quarter is in the air is the horizontal distance divided by the<br />

horizontal component of velocity. Using this time in Eq. (3.18),<br />

2<br />

x gx<br />

y − y0<br />

= v0<br />

y<br />

−<br />

2<br />

v 2v<br />

0x<br />

= tanα<br />

0<br />

x −<br />

v<br />

2<br />

0<br />

0x<br />

2<br />

gx<br />

2<br />

2cos α<br />

0<br />

2<br />

2<br />

(9.80 m s )(2.1 m)<br />

= tan 60°<br />

(2.1m) −<br />

= 1.53 m rounded.<br />

2 2<br />

2(6.4 m s) cos 60°<br />

b) Using the same expression for the time in terms of the horizontal distance in<br />

Eq. (3.17),<br />

2<br />

gx<br />

(9.80 m s )(2.1 m)<br />

v y<br />

= v0 sinα<br />

0<br />

− = (6.4 m s)sin 60° −<br />

= −0.89 m s.<br />

v cosα<br />

(6.4 m s)cos60°<br />

0<br />

0

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