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8.25: m + m )(3.00 m s) = m (4.00 m s) + m (2.25 m s), so<br />

(<br />

Kim Ken<br />

Kim<br />

Ken<br />

m<br />

m<br />

Ken<br />

(3.00 m s) − (2.25 m s)<br />

=<br />

(4.00 m s) − (3.00 m s)<br />

Kim<br />

=<br />

and Kim weighs ( 0.750)(700 N) = 525 N.<br />

0.750,<br />

4<br />

8.26: The original momentum is (24,000 kg)(4.00 m s) = 9.60 × 10 kg ⋅ m s, the<br />

final mass is 24 ,000 kg + 3000 kg = 27,000 kg, and so the final speed is<br />

4<br />

9.60×<br />

10 kg ⋅ m s<br />

4<br />

2.70 × 10 kg<br />

= 3.56 m s.<br />

8.27: Denote the final speeds as v<br />

A<br />

and vB<br />

and the initial speed of puck A as v<br />

0<br />

, and<br />

omit the common mass. Then, the condition for conservation of momentum is<br />

v = v A<br />

cos 30.0°<br />

+ v<br />

0 B<br />

0 = v<br />

sin 30.0°<br />

−<br />

A<br />

v B<br />

o<br />

cos 45.0<br />

o<br />

sin 45.0 .<br />

The 45 .0°<br />

angle simplifies the algebra, in that sin 45 .0° = cos 45.0°<br />

, and so the<br />

vB<br />

terms cancel when the equations are added, giving<br />

v A<br />

v<br />

=<br />

cos 30.0° + sin 30.0°<br />

0<br />

=<br />

29.3m s<br />

From the second equation, v = v A<br />

= 20.7 m<br />

B<br />

s. b) Again neglecting the common mass,<br />

2<br />

K<br />

K<br />

2 2<br />

2<br />

(1 2)( vA<br />

+ vB<br />

) (29.3 m s) + (20.7 m s)<br />

=<br />

=<br />

2<br />

2<br />

(1 2) v<br />

(40.0 m s)<br />

2<br />

2<br />

=<br />

1<br />

so 19.6% of the original energy is dissipated.<br />

0<br />

0.804,

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