What Are the Implications of Kepler's First Law on Planetary Motion?

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Discussion Overview

The discussion revolves around the implications of Kepler's First Law of planetary motion, specifically addressing the assumptions and derivations related to elliptical orbits and the role of mass in the two-body problem. Participants explore theoretical aspects, mathematical formulations, and the conditions under which Kepler's law holds true.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant questions the derivation of Kepler's First Law, noting that it relies on a potential dependent on distance and suggests that the assumption of the sun being much more massive than the orbiting body is not explicitly stated in the derivation.
  • Another participant agrees that the elliptical path is based on the approximation of the sun's mass being significantly larger than that of the orbiting body, indicating that this assumption is implicit in treating the sun as a fixed point.
  • A third participant introduces the concept of reduced mass in the context of two-body interactions, explaining that the motion can be simplified to a single particle problem with the sun treated as fixed due to its larger mass.
  • There is a clarification regarding the potential energy, emphasizing that it must be specifically proportional to -1/r for the derivation of elliptical orbits to hold.

Areas of Agreement / Disagreement

Participants express differing views on the assumptions underlying Kepler's First Law, particularly regarding the treatment of mass and the implications of the potential used in the derivation. There is no consensus on the clarity of these assumptions or their presentation in the textbook.

Contextual Notes

Participants highlight limitations in the derivation, including the dependence on the assumption of mass ratios and the specific form of the potential energy function. These factors may affect the interpretation of Kepler's First Law.

UJS
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The textbook I'm using states Kepler's first law in the following form: all planets move in elliptical paths with the sun at one of the foci. If I'm understanding this claim correctly, I've got some problems with it..

This conclusion was reached using a potential that depends only on the distance between the two objects. In that case (no external forces), the center of mass of the two-body system shouldn't accelerate. But with one stationary object and another circling around it, this can never be the case. It seems like an approximation in which one of the two objects (the sun) is much more massive than the other, but I don't see that assumption appearing anywhere in the derivation.

The kinetic energy is first expressed in terms of the velocity of the center of mass and the relative velocity of the objects. In polar coordinates the Lagrangian leads to three equations of motion, and filling in the 1/r potential immediately gives elliptical paths.

What's going on?
 
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UJS said:
The textbook I'm using states Kepler's first law in the following form: all planets move in elliptical paths with the sun at one of the foci. If I'm understanding this claim correctly, I've got some problems with it..

This conclusion was reached using a potential that depends only on the distance between the two objects. In that case (no external forces), the center of mass of the two-body system shouldn't accelerate. But with one stationary object and another circling around it, this can never be the case. It seems like an approximation in which one of the two objects (the sun) is much more massive than the other, but I don't see that assumption appearing anywhere in the derivation.
Yes, it is true that the "elliptic path" with the sun at one focus is based upon the approximation that the sun is much more massive than the orbiting body. It "appears" in the derivation with the assumption that the sun is a fixed point.

The kinetic energy is first expressed in terms of the velocity of the center of mass and the relative velocity of the objects. In polar coordinates the Lagrangian leads to three equations of motion, and filling in the 1/r potential immediately gives elliptical paths.

What's going on?
The "kinetic energy" of what? I suspect you mean the kinetic energy of the orbiting object. With the sun assumed stationary (typically at the origin of a coordinate system) then its kinetic energy is 0.
 
For two bodies with mass m1 and m2 respectively interacting via a central force, the problem separates into two single-particle problems, one involving a mass M=m1+m2 and one involving a "reduced mass" mu=m1m2/(m1+m2). The motion of particle 1 as viewed from particle 2 is the same as if particle 2 were fixed and particle 1 had mass mu. Kepler's law as stated in the textbook is a statement of what he observed. It is approximately true because the mass of the sun is so much larger than that of any single satellite.
 
UJS said:
This conclusion was reached using a potential that depends only on the distance between the two objects.

The potential has to be specifically proportional to -1/r, not just depend only on the distance.
 

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