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fisica1-youn-e-freedman-exercicios-resolvidos

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3.52: a) Setting y = −h<br />

in Eq. (3.27) (h being the stuntwoman’s initial height above the<br />

ground) and rearranging gives<br />

2<br />

2<br />

2 2v0<br />

sin α0<br />

cos α0<br />

2v0x<br />

x −<br />

x − h = 0,<br />

g<br />

g<br />

The easier thing to do here is to recognize that this can be put in the form<br />

2<br />

2v<br />

2 0xv0<br />

y 2v0<br />

x<br />

x − x − h = 0,<br />

g g<br />

the solution to which is<br />

v<br />

[ ] 0 x<br />

2<br />

x = v0<br />

+ v0<br />

+ 2gh<br />

=<br />

y y<br />

55.5 m (south).<br />

g<br />

b) The graph of v x<br />

(t)<br />

is a horizontal line.<br />

3.53: The distance is the horizontal speed times the time of free fall,<br />

2y<br />

2(90 m)<br />

v x<br />

= (64.0 m/s)<br />

= 274 m.<br />

2<br />

g<br />

(9.80 m/s )<br />

3.54: In terms of the range R and the time t that the balloon is in the air, the car’s original<br />

distance is d = R + v t . The time t can be expressed in terms of the range and the<br />

car<br />

R<br />

vcar<br />

horizontal component of velocity, t so d = R( + )<br />

= . Using<br />

v0<br />

cos α<br />

, 1<br />

0<br />

v0<br />

cos α0<br />

2<br />

R = v0<br />

sin 2α0<br />

/ g and the given values yields d = 29.5 m .

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