Physics for Scientists and Engineers: A Strategic Approach with Modern Physics (3rd Edition)

Published by Pearson
ISBN 10: 0321740904
ISBN 13: 978-0-32174-090-8

Chapter 14 - Oscillations - Exercises and Problems - Page 405: 58

Answer

$9.74\;\rm m/s^2$

Work Step by Step

We are here dealing with a system that we can consider a small-angle physical pendulum without damping. Now we need to find the frequency of our physical pendulum and we know that the angular frequency of such one is given by $$\omega=2\pi f=\sqrt{\dfrac{Mgl}{I}}$$ So, $$f=\dfrac{1}{2\pi}\sqrt{\dfrac{Mgl}{I}}$$ Squaring both sides; $$f^2=\dfrac{1}{4\pi^2}\dfrac{Mgl}{I}$$ Recall that the moment of inertia of a thin-uniform rod around one end is $\frac{1}{3}ML^2$. $$f^2=\dfrac{1}{4\pi^2}\dfrac{ \color{red}{\bf\not} Mgl}{ \frac{1}{3} \color{red}{\bf\not} ML^2}$$ Noting that $l$ is the distance from the pivot point to the center of mass of the rod which is $L/2$, $$f^2=\dfrac{1}{4\pi^2}\dfrac{3g \color{red}{\bf\not} L}{2L^{ \color{red}{\bf\not} 2}}$$ Hence, $$f^2= \dfrac{3g }{8\pi^2 }\dfrac{1}{L}$$ Now this is a form of a straight line formula where $y=f^2$, $x=\dfrac{1}{L}$, and the slope of this line is given by $$ {\rm Slope}=\dfrac{3g }{8\pi^2 }$$ Hence, $$g=\dfrac{ 8\pi^2\;\cdot{\rm Slope}}{3}\tag 1 $$ So we have to draw the best-fit line from the given data and then find its slope then we can find the free-fall acceleration. \begin{array}{|c|c|c|} \hline \dfrac{1}{L}\;({\rm m^{-1}})& f^2\;({\rm Hz^2}) \\ \hline \hline \dfrac{1}{1.0}=1 & 0.61^2 \\ \hline \dfrac{1}{0.8}=1.25& 0.67^2\\ \hline \dfrac{1}{0.6} =\dfrac{5}{3}& 0.79^2\\ \hline \dfrac{1}{0.4}=2.5&0.96^2\\ \hline \end{array} Plug these data into any software calculator, as we can see below. From the figure below, we can see that the slope is 0.37, plug that into (1). $$g=\dfrac{ 8\pi^2\; (0.37)}{3}=\color{red}{\bf 9.74}\;\rm m/s^2 $$ which is a closer answer to $9.8\;\rm m/s^2$ but the difference may appear due to the uncertainty of measurements.
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