23.04.2014 Views

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

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

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

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!