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8.63: The total momentum must be zero, and the velocity vectors must be three vectors of<br />

the same magnitude that sum to zero, and hence must form the sides of an equilateral<br />

triangle. One puck will move 60 ° north of east and the other will move 60°<br />

south of east.<br />

8.64: a) m<br />

AvAx<br />

+ mBvBx<br />

+ mCvCx<br />

= mtotvx<br />

, therefore<br />

v<br />

Cx<br />

v<br />

Cx<br />

( 0.100 kg)(0.50 m s) − (0.020 kg)( −1.50 m s) − (0.030 kg)( −0.50m s)cos60°<br />

=<br />

0.050kg<br />

= 1.75m s<br />

Similarly,<br />

v<br />

Cy<br />

v<br />

Cy<br />

( 0.100kg)(0m s) − (0.020kg)(0 m s) − (0.030 kg)( −0.50m s)sin 60°<br />

=<br />

0.050 kg<br />

= 0.26 m s<br />

b)<br />

∆K =<br />

−<br />

1<br />

2<br />

1<br />

2<br />

(0.100 kg)(0.5 m<br />

s)<br />

(0.050 kg) × [(1.75 m<br />

2<br />

−<br />

s)<br />

1<br />

2<br />

2<br />

(0.020 kg)(1.50 m<br />

s)<br />

1<br />

2<br />

2<br />

+ (0.26 m s) ] = −0.092 J<br />

2<br />

−<br />

(0.030 kg)( −0.50m<br />

s)<br />

2<br />

8.65: a) To throw the mass sideways, a sideways force must be exerted on the mass, and<br />

hence a sideways force is exerted on the car. The car is given to remain on track, so some<br />

other force (the tracks on the car) act to give a net horizontal force of zero on the car,<br />

which continues at 5.00 m s east.<br />

b) If the mass is thrown with backward with a speed of 5 .00 m s relative to the initial<br />

motion of the car, the mass is at rest relative to the ground, and has zero momentum. The<br />

( 200 kg)<br />

speed of the car is then 5.00 m s) = 5.71m s, and the car is still moving east.<br />

(<br />

kg<br />

( 175 )<br />

c) The combined momentum of the mass and car must be same before and after the<br />

( 200 kg)( 5.00 m s) + ( 25.0 kg)( −6.00<br />

m s)<br />

mass hits the car, so the speed is = 3.78 m s, with the car still<br />

moving east.<br />

( 225 kg )

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