How Does a Charged Particle Behave in an Electromagnetic Field?

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Homework Help Overview

The discussion revolves around the behavior of a charged particle in an electromagnetic field, specifically examining the transition from the relativistic Hamiltonian to the equations of motion involving electric and magnetic fields. Participants are analyzing the mathematical relationships and identities involved in this context.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants are attempting to understand the transition between different forms of momentum and the implications of Hamilton's equations. Questions are raised about the identities needed to relate the vector potential to the equations of motion.

Discussion Status

The discussion is ongoing, with participants exploring various mathematical identities and relationships. Some guidance has been offered regarding the distinction between kinematic and canonical momentum, but no consensus has been reached on a simpler method for deriving the desired results.

Contextual Notes

There is mention of a potential difference in approaches, specifically between Hamiltonian and Lagrangian formalisms. Participants are also grappling with the implications of electromagnetic potentials on momentum definitions.

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If you go to the relativistic Hamiltonian, what allows us to go from
[tex]\dot{\vec{P}} = - \frac{\partial \mathcal{H}}{\partial \vec{x}} = e (\vec{\nabla} \vec{A}) \cdot \dot{\vec{x}} - e \vec{\nabla} \phi[/tex]
to
[tex]\frac{d}{d t}\left(\frac{m \dot{\vec{x}}} {\sqrt {1 - \frac{\dot{\vec{x}}^2}{c^2}}}\right) = e \vec{E} + e \dot{\vec{x}} \times \vec{B}[/tex]

Is there some identity with
[tex]\frac{\partial A^i}{\partial x^i}[/tex]
that turns it into a curl that I'm missing?
 
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You should try using both Hamilton equations to find the relation between P and the velocity. Then get rid of P.

For a somewhat different Hamiltonian - see the attached gif form Cordinalesi, "Classical mechanics for physics graduate students".

Cordinalesi p. 251.gif
 
Last edited:
Both Hamilton's equations are used to get to the first line. I'm looking at the RHS and wondering how to go from the RHS of eqn 1 to the RHS of eqn 2. I'm having trouble coming up with an identity that will give me a curl and divergence of the vector potential from its form in eqn 1.
 
The LHS is not the same, so the RHS are also different - not a surprise.
 
I'm missing something. Why are the two LHS not the same? P is the relativistic momentum, so dP/dt is the LHS, no?
 
There are two kinds of momenta: kinematic (or "kinetic") momentum and canonical momentum. When there is an electromagnetic potential present, they are not equal. You can find the difference from your Hamiltonian. P there is the canonical momentum, not the kinetic momentum.
 
Ah, I see. So yeah, like you said earlier, I can get a relationship between x'' and p', then go through a whole bunch of tedious algebra to get the result. :(
 
Sometimes it is like that. We have to go through the whole bunch of tedious algebra to get, at the end, simple result. In such cases we are entled to think: "There must be a simple method!". And often, though not always, there is indeed one. In this case, I personally, do not know, right now, a simple method. Maybe someone knows it? Probably using Lagrangian formalism, rather than Hamiltonian one, is a simpler method. But you have asked about the Hamiltonian ...
 

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