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8.99: The information is not sufficient to use conservation of energy. Denote the emitted<br />

neutron that moves in the + y - direction by the subscript 1 and the emitted neutron that<br />

moves in the –y-direction by the subscript 2. Using conservation of momentum in the x-<br />

and y-directions, neglecting the common factor of the mass of neutron,<br />

v<br />

0<br />

= (2v<br />

0 = (2v<br />

0<br />

0<br />

3)cos10° + v<br />

3)sin 10° + v<br />

1<br />

1<br />

cos 45° + v<br />

sin 45° − v<br />

2<br />

2<br />

cos 30°<br />

sin 30°<br />

.<br />

With sin 45° = cos 45°<br />

, these two relations may be subtracted to eliminate v 1,<br />

and<br />

rearrangement gives<br />

v<br />

0<br />

( 1−<br />

(2 3) cos10° + (2 3)sin 10°<br />

) = v2(cos 30° + sin 30°<br />

),<br />

3<br />

3<br />

from which v<br />

2<br />

= 1.01×<br />

10 m s or 1.0×<br />

10 m s to two figures. Substitution of this into<br />

either of the momentum relations gives v = 221m<br />

1<br />

s. All that is known is that there is no<br />

z - component of momentum, and so only the ratio of the speeds can be determined. The<br />

ratio is the inverse of the ratio of the masses, so v = ( 1.5 v .<br />

Kr<br />

)<br />

Ba<br />

mA<br />

8.100: a) With block B initially at rest, vcm<br />

=<br />

m m<br />

v<br />

A + B A1<br />

. b) Since there is no net external<br />

force, the center of mass moves with constant velocity, and so a frame that moves with<br />

the center of mass is an inertial reference frame. c) The velocities have only x -<br />

components, and the x -components are<br />

mB<br />

m A<br />

u = v − v = v u = −v<br />

= u . Then, P m u + m u 0 .<br />

A1 A1<br />

cm<br />

A1, B1<br />

cm<br />

−<br />

m A + mB<br />

m A + mB<br />

A1<br />

cm<br />

=<br />

A A1<br />

B B1<br />

=<br />

d) Since there is zero momentum in the center-of-mass frame before the collision, there<br />

can be no momentum after the collision; the momentum of each block after the collision<br />

must be reversed in direction. The only way to conserve kinetic energy is if the<br />

momentum of each has the same magnitude so in the center-of-mass frame, the blocks<br />

change direction but have the same speeds. Symbolically, uA2<br />

= −uA<br />

1, uB2<br />

= −uB<br />

1. e) The<br />

velocities all have only x –components; these components are<br />

0.200<br />

0.400<br />

u .00 m s = 2.00m s, u = − 6.00 m s = −4.00 m s, u = −2.00m s, u 4.<br />

A1 =<br />

0.600<br />

6<br />

B1<br />

0.600<br />

A2<br />

B2<br />

=<br />

1<br />

v<br />

A2 = + 2.00<br />

m s, vB2<br />

= 8.00 m and Equation (8.24) predicts v<br />

A2 +<br />

3<br />

v<br />

A1<br />

and s.<br />

4<br />

(8.25) predicts v<br />

B<br />

= u<br />

1<br />

, which are in agreement with the above.<br />

2 3 A<br />

= and Eq.

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