\documentstyle[11pt]{article} \textheight 22cm \textwidth 16cm \hoffset= -0.6in \voffset= -0.5in \setlength{\parindent}{0cm} \setlength{\parskip}{15pt plus 2pt minus 2pt} \pagenumbering{roman} \setcounter{page}{-9} \newcommand{\be}{\begin{equation}} \newcommand{\ee}{\end{equation}} \newcommand{\bd}{\begin{displaymath}} \newcommand{\ed}{\end{displaymath}} \begin{document} \begin{center} {\Large ASTR450 Homework \# 3 -- Central Force Motion\\ Due Tuesday, February 28} \end{center} Reading: Start Danby's Chapter 6. 1. Danby: Page 82, Problem 8. To start, draw a picture of the elliptical orbit and label the semimajor axis, semiminor axis and latus rectum. The fact that a particle sweeps out equal areas in equal times for all central forces will be useful for this problem. You will need to look up some hairy integrals! 2. Danby: Page 84, Problem 10. You can assume that the force is gravity. Draw a picture to start and use the equation that describes the velocity of a particle in terms of $a$ and $r$. Under what conditions will the future orbit be a circle? An ellipse? A parabola? A hyperbola? 3. Danby: Page 84, Problem 14. The ``apsidal angle'' is the angle between two successive turning points (apses) - it is 180 degrees for a Keplerian ellipse. You'll need a good understanding of the derivation on page 60 to do this problem. 4. Danby: Page 85, Problem 25. The six cases refer to how r varies with time; r increasing monotonically with time from 0 to infinity is one case. Use the Central Force Integrator to determine numerically what happens to each of the six cases when the force law is changed to $r^{-2.9}$. 5. Danby: Page 86, Problem 31. Find $h$ and $C$ and use Eq. 4.3.1. Sketch the orbit for several different values of a. \enddocument}