Angular momentum in eliptical orbits

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Discussion Overview

The discussion revolves around the application of angular momentum conservation in elliptical orbits, specifically addressing the differences in results when using different reference points (the focus of the ellipse versus the center). Participants explore the implications of these choices on the conservation of angular momentum and the effects of gravitational forces on torque.

Discussion Character

  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant presents a calculation using conservation of angular momentum with respect to the focus of the ellipse, leading to a different result when using the center as the reference point.
  • Another participant explains that the gravitational force does not exert a torque about the focus, which allows for the conservation of angular momentum at that point.
  • There is a challenge regarding the assertion that angular momentum is not conserved when using the center of the ellipse as a reference point.
  • A participant questions the reasoning behind the conservation of angular momentum and the role of torque, particularly when considering the net torque at different points in the orbit.
  • It is noted that the gravitational force is only antiparallel to the radius vector at specific points in the orbit, suggesting that torque is not zero throughout the entire orbit.

Areas of Agreement / Disagreement

Participants express differing views on the conservation of angular momentum when switching reference points, with some asserting that it is not conserved at the center of the ellipse while others challenge this claim. The discussion remains unresolved regarding the implications of torque and the conditions under which angular momentum is conserved.

Contextual Notes

Participants highlight the dependence on the choice of reference point and the conditions under which gravitational forces exert torque, indicating that assumptions about the nature of forces and torques are critical to the discussion.

arunma
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OK, I'm sure I must be doing something wrong here, because I've run into a seeming contradiction. Please refer to the image I've attached below: an ellipse with the center and a focus marked. If there is a massive body at point P, then an object can orbit in the ellipse shown. If I know the velocity of the object at point B, and want to compute the velocity at point A, I can use conservation of angular momentum,

[tex]mv_{A}r_{PA} = mv_{B}r_{PB}[/tex]

[tex]v_{A} = v_{B} \dfrac{r_{PB}}{r_{PA}}[/tex]

Here, [tex]r_{PA}[/tex] and [tex]r_{PB}[/tex] are the distances from the focus to points A and B respectively.

However, if I switch coordinate systems and measure angular momentum with respect to the center of the ellipse, then I can write,

[tex]mv_{A}a = mv_{B}a[/tex]

[tex]v_{A} = v_{B}[/tex]

Where a is the semimajor axis of the ellipse.

OK, clearly I can't do this, since switching coordinate systems gives me a different result. Can someone explain why the latter is an invalid means to solve this problem? Thanks.
 

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The reason why taking the focus (P) as your reference point works so easily is that the gravitational force on the orbiting body never exerts a torque about that point. (The force is radial towards P.) That's why angular momentum about point P is conserved. But if you take the center of the ellipse as your reference point, angular momentum is no longer conserved.
 
Doc Al said:
But if you take the center of the ellipse as your reference point, angular momentum is no longer conserved.

You're sure about that?
 
Am I wrong? How could it be conserved?
 
Doc Al said:
The reason why taking the focus (P) as your reference point works so easily is that the gravitational force on the orbiting body never exerts a torque about that point. (The force is radial towards P.) That's why angular momentum about point P is conserved. But if you take the center of the ellipse as your reference point, angular momentum is no longer conserved.

Thanks, this makes qualitative sense. But one point still confuses me. If we take O as the origin, then the net torque on the orbiting body is equal to the cross product of the radius vector and the force. And since the force is still antiparallel to the radius vector, the net torque on the body should still be zero.

Am I still missing something here?
 
arunma said:
And since the force is still antiparallel to the radius vector, the net torque on the body should still be zero.
They are only antiparallel at those two points in the orbit. In general, they are not. As the body goes from A to B, gravity exerts a torque about point O.
 
Doc Al said:
They are only antiparallel at those two points in the orbit. In general, they are not. As the body goes from A to B, gravity exerts a torque about point O.

Oh, I understand now. Thank you.
 

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