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 384: 78d

Answer

The work done to replace A is negative.

Work Step by Step

We can find the gravitational potential energy of the three-particle system: $U_3 = -\frac{G~m_B~m_C}{r_{BC}}-\frac{G~m_B~m_D}{r_{BD}}-\frac{G~m_C~m_D}{r_{CD}}$ $U_3 = -\frac{(6.67\times 10^{-11}~N~m^2/kg^2)~(35~kg)~(200~kg)}{0.80~m}-\frac{(6.67\times 10^{-11}~N~m^2/kg^2)~(35~kg)~(50~kg)}{0.40~m}-\frac{(6.67\times 10^{-11}~N~m^2/kg^2)~(200~kg)~(50~kg)}{1.20~m}$ $U_3 = -1.4\times 10^{-6}~J$ We can write an expression for the gravitational potential energy of the four-particle system when A is put back in place: $U_4 = U_3-\frac{G~m_A~m_B}{r_{AB}}-\frac{G~m_A~m_C}{r_{AC}}-\frac{G~m_A~m_D}{r_{AD}}$ Suppose we begin with a three-particle system and then replace A in the system. We can find the change in gravitational potential energy: $\Delta U = U_4-U_3$ $\Delta U = (U_3-\frac{G~m_A~m_B}{r_{AB}}-\frac{G~m_A~m_C}{r_{AC}}-\frac{G~m_A~m_D}{r_{AD}})-(U_3)$ $\Delta U = -\frac{G~m_A~m_B}{r_{AB}}-\frac{G~m_A~m_C}{r_{AC}}-\frac{G~m_A~m_D}{r_{AD}}$ We can see that $~~\Delta U \lt 0$ Since $~~Work = \Delta U,~~$ the work done to replace A is negative.
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