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 />
1<br />
(b) The maximum speed occurs at the equilibrium position where PE s = 0. Thus, E mv<br />
2<br />
2 max<br />
, or<br />
v<br />
max<br />
2 E k<br />
250 N m<br />
A 0.035 m 0.78 m s<br />
m m<br />
0.50 kg<br />
(c) The acceleration is a F/ m kx/<br />
m . Thus, a = a max at x = x max = A.<br />
a<br />
max<br />
k A k<br />
m m<br />
A<br />
250 N m 0.035 m 18 m s<br />
0.50 kg<br />
2<br />
<strong>13</strong>.19 The maximum speed occurs at the equilibrium position and is<br />
v<br />
max<br />
k<br />
m<br />
A<br />
Thus,<br />
m<br />
kA<br />
v<br />
2<br />
2<br />
max<br />
16.0 N m 0.200 m<br />
0.400 m s<br />
2<br />
2<br />
4.00 kg ,<br />
and<br />
Fg<br />
mg<br />
4.00 kg 9.80 m s2<br />
39.2 N<br />
<strong>13</strong>.20<br />
k<br />
v A x<br />
m<br />
2 2<br />
10.0 N m<br />
50.0 10<br />
-3<br />
kg<br />
2 2<br />
0.250 m 0.125 m 3.06 m s<br />
<strong>13</strong>.21 (a) The motion is simple harmonic because the tire is rotating with constant velocity and you are looking at the<br />
uniform circular motion of the “bump” projected on a plane perpendicular to the tire.<br />
(b)<br />
Note that the tangential speed of a point on the rim of a rolling tire is the same as the translational speed of the<br />
axle. Thus, v v 3.00 m s and the angular velocity of the tire is<br />
t<br />
car<br />
v t<br />
r<br />
3.00 m s<br />
0.300 m<br />
10.0 rad s<br />
Therefore, the period of the motion is<br />
T<br />
2 2<br />
10.0 rad s<br />
0.628 s<br />
Page <strong>13</strong>.8