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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

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