Relationship between Principle of Least Action and Continuity Equation

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The discussion explores the relationship between the Principle of Least Action and the Continuity Equation, questioning whether one can be derived from the other. It emphasizes that the Continuity Equation pertains to behaviors at individual points in space, while the Principle of Least Action concerns paths taken over time. Some participants argue that while you cannot deduce path behavior solely from point behavior, continuity equations can emerge from symmetries in Lagrangians. Specifically, if a Lagrangian remains unchanged under certain transformations, it can lead to conservation laws expressed by continuity equations. Overall, the conversation highlights the complexities and nuances in relating these two fundamental concepts in physics.
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Is there a profound relationship between Principle of Least Action and Continuity Equation? Can we derive one from another?
 
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What is the "Continuity Equation"?
 
UltrafastPED said:
What is the "Continuity Equation"?

http://en.wikipedia.org/wiki/Continuity_equation


I've never heard of a profound relation between the two nor have I seen one derived from the other.
 
Why should you be able to derive one from the other? The continuity equation is about what happens at a single point in space. Least action is about what happens along a path.

If you have done any real analysis, it should be clear you can't deduce what happens in an interval (i.e. a path) from what happens at each individual point. For example think about the difference between "convergence" and "uniform convergence".
 
Not from continuity alone, that is too little information. For example, time-asymmetric system of equations can move continuously (system with friction), but it cannot be described by Hamilton's principle.

On the other hand, from Hamilton's principle the continuity does follow.

In my opinion, the most instructive way to arrive at Hamilton's principle is from the Newtonian equations of motion (of certain kind, like particles moving under potential forces).

Why should you be able to derive one from the other? The continuity equation is about what happens at a single point in space. Least action is about what happens along a path.

If you have done any real analysis, it should be clear you can't deduce what happens in an interval (i.e. a path) from what happens at each individual point. For example think about the difference between "convergence" and "uniform
convergence".

Although I agree with you answer, I do not understand your argument. It is perfectly possible to derive what happens to integral quantity from the knowledge of what happens at one point.

We can derive the variational condition from the Euler-Lagrange differential equations, for example.
 
hmm. If we have a Lagrangian, and we have some symmetries, then we can derive continuity equations from them. (This follows from the requirement that the Action is stationary). For example, if our Lagrangian does not change when we make a small spatial translation, then we get a continuity equation for conservation of momentum. And in quantum field theories, if we have some complex field such that our Lagrangian is unchanged by making a small rotation (of the value of the field) in the complex plane, then we get a continuity equation for the conservation of charge. But yeah, if your system does not have a Lagrangian, then I'm pretty sure this method cannot be used to derive continuity equations.
 
So I know that electrons are fundamental, there's no 'material' that makes them up, it's like talking about a colour itself rather than a car or a flower. Now protons and neutrons and quarks and whatever other stuff is there fundamentally, I want someone to kind of teach me these, I have a lot of questions that books might not give the answer in the way I understand. Thanks
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