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