Principle of Least Action - Straight Worldline on a Geodesic

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Discussion Overview

The discussion revolves around the principle of least action and its implications for motion along straight worldlines and geodesics in the context of physics. Participants explore the relationship between action, geodesic motion, and the conditions under which these concepts apply, touching on both conceptual and mathematical aspects.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions whether action is zero for geodesic motion and seeks to understand the implications of the principle of least action for straight versus curved worldlines.
  • Another participant explains that geodesics represent the straightest paths through curved spacetime and relate this to the principle of least action, comparing it to Fermat's principle of least time for light.
  • A different participant clarifies that while the action does not have to be zero, its variation is what is relevant, and the action taken can depend on the presence of external forces, which can alter the geodesic equation.
  • One participant suggests resources for basic information on the principle of least action, noting the variety of approaches available and the potential challenges in finding suitable materials.

Areas of Agreement / Disagreement

Participants express differing views on the nature of action in relation to geodesics, with some asserting that action does not need to be zero while others explore the implications of external forces on the geodesic equation. The discussion remains unresolved regarding the specific conditions under which action relates to straight and curved worldlines.

Contextual Notes

The discussion highlights the dependence on definitions and the context of forces acting on particles, which may influence the interpretation of the principle of least action and its application to geodesics.

runner108
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What does it mean to say that something moves on a straight wordline in terms of the principle of least action? I know it generally means that action is minimum or stationary but since I only really know some physics from a conceptual standpoint and not a mathematical one I don't really know what this means. Does it mean for geodesic motion that action is Zero?

Another way of putting the question is, is there anyway to tell from the output of the Principle of Least Action that something is moving on a straight worldline as opposed to a curved one? Does one always reduce to 0 and the other is non-zero? Or is that wrong.

I'm trying to figure out the privileged status of movement along a geodesic in terms of the principle of least action.
 
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Geodesics are just the straightest possible "lines" through curved spacetime. The principle of least action is basically like a version of Fermat's principle of least time... only for material bodies instead of light. Recall that Fermat's principle says that light always travels the path between two points that takes the least amount of time. In curved spacetime that would be a null geodesic. Material bodies without any forces acting on them move along timelike geodesics in general relativity. So the statement that it moves along a straight worldline is just saying that it follows a timelike geodesic (has no forces acting on it)...that it makes use of the principle of least action...all things do that.
 
runner108 said:
What does it mean to say that something moves on a straight wordline in terms of the principle of least action? I know it generally means that action is minimum or stationary but since I only really know some physics from a conceptual standpoint and not a mathematical one I don't really know what this means. Does it mean for geodesic motion that action is Zero?
No, the action doesn't have to be zero, but its variation.


Another way of putting the question is, is there anyway to tell from the output of the Principle of Least Action that something is moving on a straight worldline as opposed to a curved one? Does one always reduce to 0 and the other is non-zero? Or is that wrong.

I'm trying to figure out the privileged status of movement along a geodesic in terms of the principle of least action.
This depends on the action you take. For instance, without external force fields (but with the probability of gravity) you just have as the action of a particle the length of the worldline. This gives you the geodesic equation. In the presence of, say, electromagnetic fields you get extra terms with your geodesic equation and the solution won't be a geodesic anymore.

I'm not sure if I understand your question.
 
If the OP is just looking for some basic information about the principle of least action, E F Taylor's website might help.

http://www.eftaylor.com/leastaction.html

There are a LOT of papers about the topic there - it's a bit of a crapshoot to guess which must be most helpful, but I'd say http://www.eftaylor.com/pub/ForceEnergyPredictMotion.pdf is one of the more elementary ones, as it manages to avoid using Lagrangian mechanics. I suppose I should mention that their approach is a bit unusual, but that's part of the appeal - most "standard" appraoches require a lot more knowledge.

Some might not like the "let's take a guess and then show that it gives the right answer" approach, though...
 
Thanks Pervect, I'll look into it.
 

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