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what is physical meaning of Lorentz gauge condition in classical electrodynamics??
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.
PREREQUISITESPhysicists, electrical engineers, and students of classical electrodynamics seeking to deepen their understanding of gauge conditions and their applications in solving electromagnetic problems.
Can you see that maxwell eqn are total 8 in numbers but there are only 6 quantities to determine.nrjsingh413 said:what is physical meaning of Lorentz gauge condition in classical electrodynamics??