Physics Technology Update (4th Edition)

Published by Pearson
ISBN 10: 0-32190-308-0
ISBN 13: 978-0-32190-308-2

Chapter 11 - Rotational Dynamics and Static Equilibrium - Problems and Conceptual Exercises - Page 369: 38

Answer

a) $N=0.983N$ b) $f_x=0.492N$ c) $f_y=1.25N$

Work Step by Step

(a) We can find the required force as follows: $\Sigma \tau=0=-(\frac{1}{2}lcos\theta)mg+N(\frac{H}{sin\theta})$ This simplifies to: $N=\frac{sin\theta (\frac{1}{2}lcos\theta)mg}{H}$ $\implies N=\frac{mglsin\theta cos\theta}{2R(1+cos\theta)}$ We plug in the known values to obtain: $N=\frac{(0.214)(9.81)(0.436)sin30.0^{\circ}cos30.0^{\circ}}{2(\frac{1}{2}\times 0.216)(1+cos 30.0^{\circ})}$ $N=0.983N$ (b) We can find the required horizontal component of the force as $F_x=f_x-Nsin\theta=0$ $\implies f_x=Nsin\theta$ We plug in the known values to obtain: $f_x=(0.983N)sin30.0^{\circ}$ $f_x=0.492N$ (c) We can find the vertical component of the force as $\Sigma F_y=f_y-mg+Ncos\theta=0$ $f_y=mg-Ncos\theta$ We plug in the known values to obtain: $f_y=(0.214)(9.81)-(0.983)cos 30^{\circ}$ $f_y=1.25N$
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