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

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SUMMARY

The discussion focuses on deriving the average of the cube of the semimajor axis to position ratio, specifically \((a/r)^3\), with respect to time in celestial mechanics. Participants highlight the challenge of expressing the distance \(r\) as a function of time and suggest converting \(dt\) to \(d\theta\) using Kepler's laws. The final solution is indicated to involve the term \((1-e^2)^{-3/2}\), emphasizing the importance of understanding the relationship between the semimajor axis \(a\), distance \(r\), and the true anomaly \(\theta\).

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antythingyani
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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]
 
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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.
 
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PeroK said:
... which it does.
The 1-e^2 terms cancel and then again we will be left with a/r isn't it?!?
 
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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.
 
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