Classical Electrodynamics: Explaining the Lorentz Gauge Condition

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Discussion Overview

The discussion revolves around the physical meaning and implications of the Lorentz gauge condition in classical electrodynamics. Participants explore its role in simplifying equations, its historical attribution, and its suitability for various physical problems.

Discussion Character

  • Exploratory, Technical explanation, Debate/contested

Main Points Raised

  • One participant asks for the physical meaning of the Lorentz gauge condition in classical electrodynamics.
  • Another participant explains that the constraint leads to simpler wave equations for the scalar and vector potentials, which can be easily solved under certain conditions.
  • A different participant expresses confusion regarding the speed-of-light factor in the gauge condition and provides a covariant notation, suggesting that the gauge should be attributed to Ludvig Lorenz rather than Hendrik Antoon Lorentz.
  • This participant also notes that the Lorentz gauge is Poincare invariant, which is beneficial for radiation problems, while other gauges may be more suitable for different contexts, such as the Coulomb gauge for bound states in quantum mechanics.
  • One participant reiterates the question about the physical meaning of the Lorentz gauge condition and points out the discrepancy between the number of Maxwell equations and the quantities to determine.

Areas of Agreement / Disagreement

Participants express differing views on the attribution of the gauge condition and its physical implications. There is no consensus on the best gauge for all problems, indicating multiple competing perspectives.

Contextual Notes

Some participants mention the historical confusion between Lorenz and Lorentz, and the discussion highlights the dependence of gauge choice on specific physical problems, suggesting that the appropriateness of a gauge may vary.

nrjsingh413
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what is physical meaning of Lorentz gauge condition in classical electrodynamics??
 
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Actually the constraint

$$
\frac{1}{c^2}\frac{\partial\phi}{\partial t} + \nabla \cdot \mathbf A = 0
$$

is due to Lorenz (Lorenz and Lorentz are easily confused):

https://en.wikipedia.org/wiki/Lorenz_gauge_condition

This equation is sometimes used because it leads to simple and symmetric wave equations for the scalar and vector potential, which are then easily solved for known charge and current distribution and initial conditions on the field.

The potentials are auxiliary functions without direct physical meaning. The meaning of the constraint is really just simplification of the relativistic equations so they become nice and simple.
 
You confuse me a bit with the speed-of-light factor. In relativistically covariant notation, it's
[tex]\partial_{\mu} A^{\mu}=0.[/tex]
Split into temporal and spatial components this reads
[tex]\partial_0 A^0+\vec{\nabla} \cdot \vec{A}=\frac{1}{c} \partial_t \Phi + \vec{\nabla} \cdot \vec{A}.[/tex]
This is, of course, in Heaviside-Lorentz units.

The good thing with this particular gauge, which should indeed be named after the Danish physicists Ludvig Lorenz instead of the Dutch physicist Hendrik Antoon Lorentz, because Lorenz was the first, using this gauge condition.

The physical merit of this particular gauge is clear: It's a Poincare invariant condition, leading to Poincare invariant equations of motion for the four-potential that at the same time separate into the components. This makes it particularly nice for radiation problems.

For other problems like the description of bound states in quantum mechanics other gauges are more convenient. In this case the Coulomb gauge is good.

It always depends on the physical problem you want to solve, what's the most appropriate gauge constraint. Choosing a gauge is an art comparable to the one to find the most convenient set of coordinates to solve a problem.
 
nrjsingh413 said:
what is physical meaning of Lorentz gauge condition in classical electrodynamics??
Can you see that maxwell eqn are total 8 in numbers but there are only 6 quantities to determine.
 

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