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 501<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 />
*R1–32. <strong>The</strong> collar has a mass <strong>of</strong> 2 kg and travels along the<br />
smooth <strong>horizontal</strong> rod defined by the equiangular spiral<br />
r = (e u ) m, where u is in radians. Determine the tangential<br />
force F and the normal force N acting on the collar when<br />
u if force maintains a constant angular motion<br />
u # = 90°, F<br />
= 2 rad>s.<br />
F<br />
r<br />
r e u<br />
r = e u<br />
r # = e u u #<br />
r $ = e u (u # ) 2 + e u u $<br />
u<br />
At u = 90°<br />
u # = 2 rad>s<br />
u # = 0<br />
r = 4.8105 m<br />
r # = 9.6210 m>s<br />
r $ = 19.242 m>s 2<br />
a r = r $ - r(u # ) 2 = 19.242 - 4.8105(2) 2 = 0<br />
a u = r u $ + 2 r # u # = 0 + 2(9.6210)(2) = 38.4838 m>s 2<br />
tan c =<br />
r<br />
A dr<br />
du B<br />
c = u = 45°<br />
= e u >e u = 1<br />
+ c ©F t = m a t ; -N cos 45° + F cos 45° = 2(0)<br />
; + ©F u = m a u ; F sin 45° + N sin 45° = 2(38.4838)<br />
N t = 54.4 N<br />
F = 54.4 N<br />
Ans.<br />
Ans.<br />
501