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: 23

Answer

(a) Using the result ${r_{per}} = a\left( {1 - e} \right)$ from Exercise 13, we show that $C{F_1} = ae$ (b) Using $r = \frac{p}{{1 + e\cos \theta }}$ we show that $a = \frac{p}{{1 - {e^2}}}$ (c) We obtain ${F_1}B = {F_2}B = a$. Thus, ${F_1}B + {F_2}B = 2a$. (d) Using Pythagorean Theorem and the result from part (b) we prove that $b = \sqrt {pa} $

Work Step by Step

(a) From Figure 10, we see that ${F_1}A = {r_{per}}$. From Exercise 13, we obtain ${r_{per}} = a\left( {1 - e} \right)$. Thus, $C{F_1} = CA - {F_1}A$ $C{F_1} = a - a\left( {1 - e} \right) = ae$ Hence, $C{F_1} = ae$. (b) We have $r = \frac{p}{{1 + e\cos \theta }}$, ${\ \ \ }$ where $p = {J^2}/k$. So, at $\theta = 0$ we get ${r_{per}} = \frac{p}{{1 + e}}$. From Exercise 13, we obtain ${r_{per}} = a\left( {1 - e} \right)$. Thus, $a\left( {1 - e} \right) = \frac{p}{{1 + e}}$ $p = a\left( {1 - {e^2}} \right)$ Hence, $a = \frac{p}{{1 - {e^2}}}$. (c) From part (a) we obtain $C{F_1} = ae$. From Figure 10, we see that ${F_1}A = a - C{F_1}$ and ${F_2}A = {F_2}C + a$. Since ${F_2}C = C{F_1}$, so ${F_2}A = C{F_1} + a$. Thus, ${F_1}A + {F_2}A = a - C{F_1} + C{F_1} + a$ Hence, ${F_1}A + {F_2}A = 2a$. Since the $\vartriangle BC{F_1}$ is a right triangle, so ${F_1}B = \sqrt {{{\left( {CB} \right)}^2} + {{\left( {C{F_1}} \right)}^2}} $ ${F_1}B = \sqrt {{b^2} + {a^2}{e^2}} = a\sqrt {\frac{{{b^2}}}{{{a^2}}} + {e^2}} $ Since $\frac{{{b^2}}}{{{a^2}}} = 1 - {e^2}$, so ${F_1}B = a$. By symmetry we obtain ${F_1}B = {F_2}B = a$. Thus, we conclude that ${F_1}B + {F_2}B = 2a$. (d) By the Pythagorean Theorem: $C{B^2} = {\left( {{F_1}B} \right)^2} - {\left( {C{F_1}} \right)^2}$ Since $CB = b$, ${F_1}B = a$, and $C{F_1} = ae$, so ${b^2} = {a^2} - {a^2}{e^2} = {a^2}\left( {1 - {e^2}} \right)$ $\frac{{{b^2}}}{{{a^2}}} = 1 - {e^2}$ From part (b), we obtain $a = \frac{p}{{1 - {e^2}}}$. So, $p = a\left( {1 - {e^2}} \right)$ $p = a\frac{{{b^2}}}{{{a^2}}} = \frac{{{b^2}}}{a}$ Hence, $b = \sqrt {pa} $.
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