Classical Electrodynamics: Explaining the Lorentz Gauge Condition

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SUMMARY

The Lorentz gauge condition in classical electrodynamics, expressed as $$\frac{1}{c^2}\frac{\partial\phi}{\partial t} + \nabla \cdot \mathbf A = 0$$, simplifies the wave equations for scalar and vector potentials, facilitating solutions for known charge and current distributions. This gauge, named after Ludvig Lorenz, is Poincare invariant, making it particularly effective for radiation problems. While the potentials themselves lack direct physical meaning, the gauge condition streamlines the relativistic equations, enhancing clarity in problem-solving. For certain scenarios, such as bound states in quantum mechanics, alternative gauges like the Coulomb gauge may be more suitable.

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  • Understanding of classical electrodynamics principles
  • Familiarity with wave equations and potential theory
  • Knowledge of Poincare invariance in physics
  • Basic grasp of gauge theory and its applications
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  • Research the implications of the Lorentz gauge condition in solving electromagnetic problems
  • Study the differences between Lorentz and Coulomb gauges in various physical contexts
  • Explore the role of gauge invariance in quantum field theory
  • Learn about the Heaviside-Lorentz units and their application in electrodynamics
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Physicists, electrical engineers, and students of classical electrodynamics seeking to deepen their understanding of gauge conditions and their applications in solving electromagnetic problems.

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
\partial_{\mu} A^{\mu}=0.
Split into temporal and spatial components this reads
\partial_0 A^0+\vec{\nabla} \cdot \vec{A}=\frac{1}{c} \partial_t \Phi + \vec{\nabla} \cdot \vec{A}.
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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