I What Is the Descriptive Meaning of \(- \frac{e}{c}\vec A\)?

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The term \(- \frac{e}{c}\vec A\) represents the modification of momentum in the presence of an electromagnetic field, specifically indicating the momentum imparted through electromagnetic forces. In the context of Hamiltonian mechanics, the classical Hamiltonian combines kinetic and potential energy, with the potential energy in an electromagnetic field expressed as \(V = e\phi\). The replacement of kinetic momentum \(p\) with canonical momentum \(P - \frac{e}{c}\vec A\) is crucial for accurately describing a particle's dynamics in such fields. The distinction between kinetic momentum \(p\) and canonical momentum \(P\) is essential for understanding how particles behave under electromagnetic influences. This framework allows for a comprehensive analysis of particle dynamics in electromagnetic contexts.
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If you want to modify the Hamiltonian by introducing the effect of an electromagnetic field, then the replacement \vec p \rightarrow \vec p - \frac{e}{c}\vec A is applied.

Now my question is, whether there is a descriptive meaning of that extra term - \frac{e}{c}\vec A. As what can I think of that?
Thank you in advance
 
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One way to look at it is that it is the momentum imparted through the electromagnetic force,

Momentum wikipedia -
The classical Hamiltonian ℋ for a particle in any field equals the total energy of the system – the kinetic energy T = p2/2m (where p2 = p · p, see dot product) plus the potential energy V. For a particle in an electromagnetic field, the potential energy is V = , and since the kinetic energy T always corresponds to the kinetic momentum p, replacing the kinetic momentum by the above equation (p = PqA) leads to the Hamiltonian in the table.
 
say_cheese said:
For a particle in an electromagnetic field, the potential energy is V = , and since the kinetic energy T always corresponds to the kinetic momentum p, replacing the kinetic momentum by the above equation (p = PqA) leads to the Hamiltonian in the table.
If small type p is the kinetic momentum, what then is capital P?
 
Anton Alice said:
If small type p is the kinetic momentum, what then is capital P?
It's the canonical momentum, i.e., the total momentum of the particle.
 
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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