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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

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