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6.47: The power is P = F ⋅v<br />

. F is the weight, mg, so<br />

2<br />

P = (700 kg) (9.8 m s ) (2.5 m s) = 17.15 kW. So, 17 .15 kW 75 kW. = 0.23, or about<br />

23% of the engine power is used in climbing.<br />

6.48: a) The number per minute would be the average power divided by the work (mgh)<br />

required to lift one box,<br />

(0.50 hp) (746 W hp)<br />

= 1.41 s,<br />

2<br />

(30 kg) (9.80 m s ) (0.90 m)<br />

or 84 .6 min. b) Similarly,<br />

(100 W)<br />

(30 kg) (9.80 m s ) (0.90 m)<br />

or<br />

22 .7<br />

min.<br />

2<br />

=<br />

0.378<br />

s,<br />

6.49: The total mass that can be raised is<br />

(40.0 hp) (746 W hp)(16.0 s)<br />

(9.80 m s ) (20.0 m)<br />

2<br />

=<br />

1836 kg<br />

so the maximum number of passengers is = 28.<br />

65.0 kg<br />

2436 kg,<br />

6.50: From any of Equations (6.15), (6.16), (6.18) or (6.19),<br />

Wh ( 3800 N) (2.80 m)<br />

3<br />

P = =<br />

= 2.66×<br />

10 W = 3.57 hp.<br />

t (4.00 s)<br />

( 0.70) P (0.70) (280,000 hp)(746 W hp)<br />

6<br />

6.51: F =<br />

ave =<br />

= 8.1 10 N.<br />

v (65 km h) ((1km h) (3.6 m s))<br />

×<br />

6.52: Here, Eq. (6.19) is the most direct. Gravity is doing negative work, so the rope<br />

must do positive work to lift the skiers. The force F r is gravity, and F = mg,<br />

where <br />

is the number of skiers on the rope. The power is then<br />

P = ( mg)<br />

( v)<br />

cosφ<br />

=<br />

(50) (70 kg) (9.80 m<br />

2<br />

⎛<br />

s ) (12.0 km h) ⎜<br />

⎝<br />

1m s<br />

3.6 km h<br />

⎞<br />

⎟ cos (90.0° −15.0°<br />

)<br />

⎠<br />

4<br />

= 2.96×<br />

10 W.<br />

Note that Eq. (1.18) uses φ as the angle between the force and velocity vectors; in this<br />

case, the force is vertical, but the angle 15 .0°<br />

is measured from the horizontal, so<br />

φ = 90.0° −15.<br />

0°<br />

is used.

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