Fundamentals of Physics Extended (10th Edition)

Published by Wiley
ISBN 10: 1-11823-072-8
ISBN 13: 978-1-11823-072-5

Chapter 13 - Gravitation - Problems - Page 380: 16

Answer

The Magnitude Of The Force On The Mass $m_1$ Due To The Rod Is : $3.01\times10^{-10}$$N$.

Work Step by Step

Consider a small segment of the rod with length $dr$ at a distance of $r$ from the point mass $m_1$. Let the linear mass density of the rod is $\lambda$. The the mass of the segment $dm$ is $\lambda$$dr$ Gravitational force on the mass $m_1$ due to the small segment acts along $x-axis$ and is given by : $$dF = \frac{Gm_1dm}{r^2}$$ $$dF = \frac{Gm_1\lambda dr}{r^2}$$ Total force on the point mass $m_1$ is : $$F= \int_{d}^{d+L}\frac{Gm_1\lambda}{r^2}dr$$ Where $d$ is the distance between the end of rod closer to the point mass $m_1$ and $L$ is the length of the rod. $$F= Gm_1\lambda\int_{d}^{d+L}\frac{1}{r^2}dr$$ $$F=-Gm_1\lambda\frac{1}{r}\left. \right|_{d} ^{d+L}$$ $$F=-Gm_1\lambda(\frac{1}{d+L}-\frac{1}{d})$$ $$F=Gm_1\lambda(\frac{1}{d}-\frac{1}{d+L})$$ $$F=Gm_1\lambda L(\frac{1}{d\times(d+L)})$$ $$ \lambda = \frac{M}{L}$$ Where $M$ is the mass of the rod. Therefore, $$F=Gm_1M (\frac{1}{d\times(d+L)})$$ Substituting for the values, we get : $$F= 6.67\times10^{-11}\times0.67\times5(\frac{1}{0.23\times(0.23+3)})$$ $$F= 22.3\times10^{-11}\times(\frac{1}{0.23\times(3.23)})$$ $$F= 22.3\times10^{-11}\times(\frac{1}{0.74})$$ $$F= 30.1\times10^{-11}$$ Therefore magnitude of force on the point mass $m_1$ is : $$F= 3.01\times10^{-10}$$
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