Calculus (3rd Edition)

Published by W. H. Freeman
ISBN 10: 1464125260
ISBN 13: 978-1-46412-526-3

Chapter 14 - Calculus of Vector-Valued Functions - 14.6 Planetary Motion According to Kepler and Newton - Exercises - Page 752: 22

Answer

Since ${a_A} > {a_B}$, so by Kepler's Third Law: ${T_A} > {T_B}$. Hence, $A$'s orbital period ${T_A}$ will increase and she will fall farther and farther behind $B$.

Work Step by Step

From Exercise 20, we obtain the total energy: $E = - \frac{{GMm}}{{2a}}$. Since $A$ and $B$ orbit the earth along the same solid trajectory, their total energies are the same. Notice that the larger the value of $a$, the larger is the total energy. Thus, shuttle $A$ will move off into a larger orbit if its pilot increases the shuttle's kinetic energy. Let ${a_B} = a$. Let ${a_A}$ denote the semi-major axis of $A$ after it moves off into a larger orbit. So, ${a_A} > {a_B}$. By Kepler's Third Law, we have ${T_A}^2 = \left( {\frac{{4{\pi ^2}}}{{GM}}} \right){a_A}^3$ ${\ \ \ }$ and ${\ \ \ }$ ${T_B}^2 = \left( {\frac{{4{\pi ^2}}}{{GM}}} \right){a_B}^3$ Since ${a_A} > {a_B}$, so ${T_A} > {T_B}$. Hence, $A$'s orbital period ${T_A}$ will increase and she will fall farther and farther behind $B$.
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