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7.39: a) At constant speed, the upward force of the three ropes must balance the force,<br />

so the tension in each is one-third of the man’s weight. The tension in the rope is the<br />

2<br />

force he exerts, or (70.0 kg)(9.80 m s ) 3 = 229 N.<br />

b) The man has risen 1.20 m, and so<br />

the increase in his potential energy is (70.0 kg)(9.80 m s )(1.20 m) = 823 J.<br />

In moving up<br />

a given distance, the total length of the rope between the pulleys and the platform<br />

changes by three times this distance, so the length of rope that passes through the man’s<br />

hands is 3 × 1.20 m = 3.60 m,<br />

and ( 229 N)(3.6 m) = 824 J.<br />

2<br />

7.40: First find the acceleration:<br />

2 2<br />

2<br />

v − v0<br />

(3.00 m s)<br />

2<br />

a = =<br />

= 3.75 m s<br />

2( x − x0)<br />

2(1.20 m)<br />

Then, choosing motion in the direction of the more massive block as positive:<br />

F = Mg − mg = ( M + m)<br />

a = Ma + ma<br />

net<br />

M ( g − a)<br />

= m(<br />

g + a)<br />

M<br />

m<br />

g + a (9.80 + 3.75) m s<br />

= =<br />

g − a (9.80 − 3.75) m s<br />

M = 2.24 m<br />

Since M + m = 15.0 kg :<br />

2.24m<br />

+ m = 15.0 kg<br />

m = 4.63 kg<br />

M = 15.<br />

0 kg − 4.63 kg = 10.<br />

4 kg<br />

2<br />

2<br />

= 2.24<br />

7.41: a) K<br />

1<br />

+ U1<br />

+ Wother<br />

= K2<br />

+ U<br />

2<br />

U<br />

1<br />

= U<br />

2<br />

= K2<br />

= 0<br />

W = W<br />

f<br />

= −µ<br />

mgs, with s = 280 ft<br />

other k<br />

=<br />

85.3 m<br />

The work-energy expression gives 1 2<br />

mv − µ mgs = 0<br />

v 1<br />

= 2µ k<br />

gs = 22.4 m s = 50 mph; the driver was speeding.<br />

a) 15 mph over speed limit so $150 ticket.<br />

2<br />

1<br />

k

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