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479 Horizontal Motion: The horizontal component of velocity ... - Wuala

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91962_05_R1_p0<strong>479</strong>-0512 6/5/09 3:53 PM Page 484<br />

© 2010 Pearson Education, Inc., Upper Saddle River, NJ. All rights reserved. This material is protected under all copyright laws as they currently<br />

exist. No portion <strong>of</strong> this material may be reproduced, in any form or by any means, without permission in writing from the publisher.<br />

R1–7. <strong>The</strong> man A has a weight <strong>of</strong> 100 lb and jumps from<br />

rest onto the platform P that has a weight <strong>of</strong> 60 lb. <strong>The</strong><br />

platform is mounted on a spring, which has a stiffness<br />

k = 200 lb>ft. If the coefficient <strong>of</strong> restitution between the<br />

man and the platform is e = 0.6, and the man holds himself<br />

rigid during the motion, determine the required height h <strong>of</strong><br />

the jump if the maximum compression <strong>of</strong> the spring is 2 ft.<br />

h<br />

A<br />

Conservation <strong>of</strong> Energy: <strong>The</strong> datum is set at the initial position <strong>of</strong> platform P. When<br />

the man falls from a height <strong>of</strong> h above the datum, his initial gravitational potential<br />

energy is 100h. Applying Eq. 14–21, we have<br />

P<br />

Conservation <strong>of</strong> Momentum:<br />

T 1 + V 1 = T 2 + V 2<br />

0 + 100h = 1 2 a 100<br />

32.2 b(y M) 2 1 + 0<br />

(y H ) 1 = 264.4h<br />

m M (y M ) 1 + m P (y P ) 1 = m M (y M ) 2 + m P (y P ) 2<br />

( +T) a 100<br />

100<br />

b(264.4h) + 0 = a<br />

32.2 32.2 b(y M) 2 + a 60<br />

32.2 b(y P) 2<br />

[1]<br />

Coefficient <strong>of</strong> Restitution:<br />

e = (y p) 2 - (y M ) 2<br />

(y M ) 1 - (y p ) 1<br />

( +T) 0.6 = (y p) 2 - (y M ) 2<br />

264.4h - 0<br />

[2]<br />

Solving Eqs. [1] and [2] yields<br />

(y p ) 2 = 264.4h T (y M ) 2 = 0.4264.4h T<br />

Conservation <strong>of</strong> Energy: <strong>The</strong> datum is set at the spring’s compressed position.<br />

60<br />

Initially, the spring has been compressed = 0.3 ft and the elastic potential<br />

200<br />

1<br />

energy is<br />

. Here, the compression <strong>of</strong> the spring caused by<br />

2 (200) A0.32 B = 9.00 ft # lb<br />

impact is (2 - 0.3) ft = 1.7 ft. When platform P is at a height <strong>of</strong> 1.7 ft above the<br />

datum, its initial gravitational potential energy is<br />

60(1.7) = 102 ft # lb . When<br />

platform P stops momentary, the spring has been compressed to its maximum and<br />

1<br />

the elastic potential energy at this instant is<br />

. Applying<br />

2 (200)A22 B = 400 ft # lb<br />

Eq. 14–21, we have<br />

T 1 + V 1 = T 2 + V 2<br />

1<br />

2 a 60<br />

32.2 b A 264.4hB2 + 102 + 9.00 = 400<br />

h = 4.82 ft<br />

Ans.<br />

484

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