Advanced Electromagnetic and Mathematic Concepts

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SUMMARY

The discussion centers on the quasistatic approximation in electromagnetic theory, specifically regarding the wave equation derived from the Lorentz gauge condition for the magnetic vector potential. Participants clarify that the term d²A/dt² can be ignored under certain conditions, allowing the equation to be simplified to a Poisson Equation. This simplification is valid when the displacement current is negligible compared to the actual current, typically in scenarios involving slowly varying fields, such as a wire loop in a magnetic field. Ignoring the Maxwell term leads to the omission of electromagnetic wave phenomena, which is acceptable when the system's dimensions are much smaller than the wavelength of interest.

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  • Understanding of electromagnetic theory and Maxwell's equations
  • Familiarity with the Lorentz gauge condition
  • Knowledge of wave equations and their applications
  • Concept of quasistatic approximation in physics
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Michael Lin
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Hi All,

From electromagnetic theories, with the Lorentz gauge condition for the magnetic vector potential, I get the following wave equation:
1/csquared * d2A/dt2 + del2 A= u0 j.
in some literatures, they ignored the d2A/dt2 term and I don't know why they can do that. Is it becasue they assumed some quasi-stationary condition on the E field created by the magnetic field?
This simplication leads to a big simplification in which they can solve it as a Poisson Equation. I just want to know why they can ignore that term.

Thanks,
Micahel
 
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Yes, it is typically called the quasistatic approximation. You keep the Faraday term [tex]\partial B/ \partial t[/tex] in Maxwell's equations, but drop the Maxwell term [tex]\partial E/ \partial t[/tex]. This is an approximation which is valid in some limited circumstances where the displacement current (Maxwell term) is small compared to the real current. A typical scenario might be a wire loop in a magnetic field and the like.

More properly, by leaving out the Maxwell term you ignore the possibility of electromagnetic waves. To justify this approximation, the frequencies of interest in your system must correspond to electromagnetic waves of wavelength much larger than your system of interest. In other words, everything should be slowly varying or "quasistatic".
 
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