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8.66: The total mass of the car is changing, but the speed of the sand as it leaves the car<br />

is the same as the speed of the car, so there is no change in the velocity of either the car<br />

or the sand (the sand acquires a downward velocity after it leaves the car, and is stopped<br />

on the tracks after it leaves the car). Another way of regarding the situation is that vex<br />

in<br />

Equations (8.37), (8.38) and (8.39) is zero, and the car does not accelerate. In any event,<br />

the speed of the car remains constant at 15.0 m/s. In Exercise 8.24, the rain is given as<br />

falling vertically, so its velocity relative to the car as it hits the car is not zero.<br />

8.67: a) The ratio of the kinetic energy of the Nash to that of the Packard is<br />

2<br />

m<br />

v<br />

2<br />

mPvP<br />

=<br />

2<br />

( 840 kg)( 9 m s)<br />

2<br />

( 1620 kg)( 5 m s)<br />

mPvP<br />

= 1.68. b) The ratio of the momentum of the Nash to that of the<br />

mv<br />

(840 kg)(9 m/s)<br />

Packard is = = 0.933, therefore the Packard has the greater magnitude<br />

(1620 kg)(5 m/s)<br />

of momentum. c) The force necessary to stop an object with momentum P in time t is<br />

F = − P/<br />

t. Since the Packard has the greater momentum, it will require the greater force<br />

to stop it. The ratio is the same since the time is the same, therefore F / = 0.933. d)<br />

F P<br />

By the work-kinetic energy theorem, F = ∆ k<br />

d<br />

. Therefore, since the Nash has the greater<br />

kinetic energy, it will require the greater force to stop it in a given distance. Since the<br />

distance is the same, the ratio of the forces is the same as that of the kinetic energies,<br />

F <br />

/ F P<br />

= 1.68.<br />

8.68: The recoil force is the momentum delivered to each bullet times the rate at which<br />

the bullets are fired,<br />

F =<br />

3<br />

⎛1000 bullets/min ⎞<br />

36.4 N.<br />

ave<br />

(7.45× 10<br />

− kg) (293 m/s) ⎜<br />

⎟ =<br />

⎝ 60 s/ min ⎠

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