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Chapter 13 Solutions - Mosinee School District

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<strong>Chapter</strong> <strong>13</strong><br />

k<br />

Fs<br />

x<br />

mg<br />

x<br />

50 N<br />

5.0 10<br />

-2<br />

m<br />

1.0 103<br />

N m<br />

F Fs<br />

kx<br />

1.0 103 N m 0.11 m 1.1 102<br />

N<br />

(b) The graph will be a straight line passing through the origin with a slope equal to k 1.0 103<br />

N m .<br />

<strong>13</strong>.5 When the system is in equilibrium, the tension in the spring F k x must equal the weight of the object. Thus,<br />

k x<br />

mg giving<br />

m<br />

k x<br />

g<br />

47.5 N 5.00 10<br />

2<br />

m<br />

9.80 m s<br />

2<br />

0.242 kg<br />

<strong>13</strong>.6 (a) The free-body diagram of the point in the center of the string is<br />

given at the right. From this, we see that<br />

F 0 F 2T<br />

sin 35.0 0<br />

x<br />

or<br />

T<br />

F 375 N<br />

2 sin 35.0 2 sin 35.0<br />

327 N<br />

(b)<br />

Since the bow requires an applied horizontal force of 375 N to hold the string at 35.0° from the vertical, the<br />

tension in the spring must be 375 N when the spring is stretched 30.0 cm. Thus, the spring constant is<br />

k<br />

F<br />

x<br />

375 N<br />

0.300 m<br />

1.25 103<br />

N m<br />

<strong>13</strong>.7 (a) When the block comes to equilibrium, Fy<br />

ky0 mg 0 giving<br />

y<br />

0<br />

mg<br />

k<br />

10.0 kg 9.80 m s<br />

475 N m<br />

2<br />

0.206 m<br />

or the equilibrium position is 0.206 m below the unstretched position of the lower end of the spring.<br />

(b) When the elevator (and everything in it) has an upward acceleration of a 2.00 m s2<br />

second law to the block gives<br />

, applying Newton’s<br />

Fy<br />

k y0<br />

y mg ma y or y 0<br />

F ky mg ky ma<br />

y<br />

Page <strong>13</strong>.2

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