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 - Chapter Review Exercises - Page 754: 42

Answer

It takes Mercury to travel $5.74$ days longer from $A'$ to $B'$ than from $B'$ to $A$.

Work Step by Step

From Exercise 41, we obtain the area swept out by the planet from $A'$ to $B'$ is ${A_{A'B'}} = ab\left( {\frac{1}{4}\pi + \frac{1}{2}e} \right)$ Therefore, the area swept out by the planet from $B'$ to $A$ is ${A_{B'A}} = \frac{1}{2}\pi ab - ab\left( {\frac{1}{4}\pi + \frac{1}{2}e} \right) = \frac{1}{4}\pi ab - \frac{1}{2}abe$ ${A_{B'A}} = ab\left( {\frac{1}{4}\pi - \frac{1}{2}e} \right)$ Using Kepler's Second Law we find the time required to travel from $B'$ to $A$: $\frac{{{A_{B'A}}}}{A} = \frac{{{t_{B'A}}}}{T}$ $\frac{{ab\left( {\frac{1}{4}\pi - \frac{1}{2}e} \right)}}{{\pi ab}} = \frac{{{t_{B'A}}}}{T}$ ${t_{B'A}} = \left( {\frac{1}{4} - \frac{e}{{2\pi }}} \right)T$ From Exercise 41, we obtain the time required to travel from $A'$ to $B'$ is ${t_{A'B'}} = \left( {\frac{1}{4} + \frac{e}{{2\pi }}} \right)T$ Thus, ${t_{A'B'}} - {t_{B'A}} = \left( {\frac{1}{4} + \frac{e}{{2\pi }}} \right)T - \left( {\frac{1}{4} - \frac{e}{{2\pi }}} \right)T$ ${t_{A'B'}} - {t_{B'A}} = \frac{e}{\pi }T$ We have for Mercury $T=88$ days and $e=0.205$. So, ${t_{A'B'}} - {t_{B'A}} = \frac{{0.205}}{\pi }88 \simeq 5.74$ Hence, it takes Mercury to travel $5.74$ days longer from $A'$ to $B'$ than from $B'$ to $A$.
Update this answer!

You can help us out by revising, improving and updating this answer.

Update this answer

After you claim an answer you’ll have 24 hours to send in a draft. An editor will review the submission and either publish your submission or provide feedback.