Chapter 13 Solutions - Mosinee School District
Chapter 13 Solutions - Mosinee School District
Chapter 13 Solutions - Mosinee School District
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<strong>Chapter</strong> <strong>13</strong><br />
v<br />
2<br />
588 N m 0.050 0 m<br />
2 9.80 m s2<br />
0.050 0 m 0.700 m s<br />
3.00 kg<br />
<strong>13</strong>.68 (a) We apply conservation of mechanical energy from just after the collision until the block comes to rest.<br />
KE PE s KE PE f<br />
s<br />
gives 1 2 1<br />
0 k x 2 0<br />
i<br />
f MV<br />
2 2<br />
or the speed of the block just after the collision is<br />
V<br />
kx2<br />
f<br />
M<br />
900 N m 0.050 0 m<br />
1.00 kg<br />
2<br />
1.50 m s<br />
Now, we apply conservation of momentum from just before impact to immediately after the collision. This<br />
gives<br />
m v 0 m v MV<br />
bullet<br />
i<br />
bullet<br />
f<br />
or<br />
M<br />
vbullet<br />
v<br />
f bullet V<br />
i<br />
m<br />
1.00 kg<br />
400 m s 1.5 m s 100 m s<br />
5.00 10<br />
-3<br />
kg<br />
(b)<br />
The mechanical energy converted into internal energy during the collision is<br />
1 2 1 2 1<br />
i f bullet i<br />
bullet f<br />
E KE KE 2 m v 2 m v 2<br />
MV<br />
2<br />
or<br />
E<br />
1 1<br />
2 2<br />
3<br />
2 2 2<br />
5.00 10 kg 400 m s 100 m s 1.00 kg 1.50 m s<br />
E<br />
374 J<br />
<strong>13</strong>.69 Choose PE g = 0 when the blocks start from rest. Then, using conservation of mechanical energy from when the<br />
blocks are released until the spring returns to its unstretched length gives<br />
KE PE PE KE PE PE , or<br />
g s<br />
f<br />
g s<br />
i<br />
Page <strong>13</strong>.26