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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 3:54 PM Page 498<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 />

R1–27. <strong>The</strong> 150-lb man lies against the cushion for which<br />

the coefficient <strong>of</strong> static friction is m s = 0.5. Determine the<br />

resultant normal and frictional forces the cushion exerts on<br />

him if, due to rotation about the z axis, he has a constant<br />

speed v = 20 ft>s. Neglect the size <strong>of</strong> the man. Take<br />

u = 60°.<br />

z<br />

8 ft<br />

G<br />

u<br />

+a ©F y = m(a n ) y ; N - 150 cos 60° = 150<br />

32.2 a 202 b sin 60°<br />

8<br />

N = 277 lb<br />

Ans.<br />

+b©F x = m(a n ) x ; -F + 150 sin 60° = 150<br />

32.2 a 202 b cos 60°<br />

8<br />

F = 13.4 lb<br />

Ans.<br />

Note: No slipping occurs<br />

Since m s N = 138.4 lb 7 13.4 lb<br />

*R1–28. <strong>The</strong> 150-lb man lies against the cushion for which<br />

the coefficient <strong>of</strong> static friction is m s = 0.5. If he rotates<br />

about the z axis with a constant speed v = 30 ft>s, determine<br />

the smallest angle u <strong>of</strong> the cushion at which he will begin to<br />

slip up the cushion.<br />

z<br />

8 ft<br />

G<br />

u<br />

; + ©F n = ma n ; 0.5N cos u + N sin u = 150<br />

32.2 a (30)2<br />

8 b<br />

+ c ©F b = 0; -150 + N cos u - 0.5 N sin u = 0<br />

N =<br />

150<br />

cos u - 0.5 sin u<br />

(0.5 cos u + sin u)150<br />

(cos u - 0.5 sin u)<br />

= 150<br />

32.2 a (30)2<br />

8 b<br />

0.5 cos u + sin u = 3.493 79 cos u - 1.746 89 sin u<br />

u = 47.5°<br />

Ans.<br />

498

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