Averaging the cube of semimajor axis to position ratio wrt to time

AI Thread Summary
The discussion revolves around deriving the average of the cube of the semimajor axis to position ratio in celestial mechanics, specifically in the context of elliptical Keplerian orbits. The main challenge is converting the time differential (dt) into the true anomaly differential (dθ) to facilitate the calculation. Participants suggest expressing the distance (r) as a function of the semimajor axis (a) and true anomaly (θ), and reference Kepler's laws to aid in the derivation. There is some confusion regarding the cancellation of terms and the overall approach to the problem. The conversation emphasizes the need for clarity in mathematical notation and the use of LaTeX for better communication.
antythingyani
Messages
5
Reaction score
2
Thread moved from the technical forums to the schoolwork forums
Summary:: Averaging (a power of) semimajor axis to position ratio wrt to time - celestial mechanics

I evaluated it this far, but i don't know how to change the dt to d theta ... the final solution is

Sideways equation 01.jpg

supposedly (1-e^2)^-(3/2) . Any help will be appreciated.photo1638096644.jpeg

[Image re-inserted with correct orientation by Mentor]
 
Last edited by a moderator:
Physics news on Phys.org
It's not very easy to read your post or to understand precisely what question you are asking.
 
PeroK said:
It's not very easy to read your post or to understand precisely what question you are asking.
The question is basically : derive the average of (a/r)^3 taking time as an independent variable. (where a is the semi major axis and r is the distance in an elliptical keplerian orbit.
 
antythingyani said:
The question is basically : derive the average of (a/r)^3 taking time as an independent variable. (where a is the semi major axis and r is the distance in an elliptical keplerian orbit.
Given that we cannot easily express ##r## as a function of time, what is your strategy?
 
we can express r as a function of semimajor axis (a) and the true anomaly (theta). In that case maybe finding a way to turn dt into dtheta would be handy... or trying to express theta as a function of t.
 
antythingyani said:
we can express r as a function of semimajor axis (a) and the true anomaly (theta). In that case maybe finding a way to turn dt into dtheta would be handy... or trying to express theta as a function of t.
I don't think you can get ##\theta## as a function of ##t## either. We have: $$\frac{d\theta}{dt} = \frac{L}{mr^2}$$But I don't know that solves the problem. There might be some trick using Kepler's law.
 
... we also have $$\frac{a(1 - e^2)}{r} = 1 + e\cos \theta$$ Perhaps that does the trick?
 
... which it does.
 
  • Like
Likes antythingyani
PeroK said:
... which it does.
The 1-e^2 terms cancel and then again we will be left with a/r isn't it?!?
 
  • #10
antythingyani said:
The 1-e^2 terms cancel and then again we will be left with a/r isn't it?!?
I'm not sure what you mean by that. I used my notes on the derivation of elliptical orbits to find the relevant equations. This looks like a tricky problem where you'll need to do the same. I've given you the two equations to get you started.

At this level, I think you need to learn a little Latex:

https://www.physicsforums.com/help/latexhelp/

If you reply to my posts you'll see what I've typed to render the mathematics.
 
  • Like
Likes berkeman
Back
Top