Are Maxwell's Equations More Complex Than We Thought?

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SUMMARY

This discussion centers on the complexities of Maxwell's equations, particularly the equations involving curl operations and their implications. The equations curl E = -dB/dt and curl E(r,t) = j*omega*u0*H(r,t) are analyzed, where j represents the imaginary unit, omega is angular frequency, and u0 is the permeability of free space. The discussion highlights the assumptions made in solving Maxwell's equations, specifically the separation of spatial and temporal components and the representation of the temporal part as T(t) = Ae^{i omega t}. These insights clarify the relationship between the electric field E and magnetic field H, as well as the role of the dielectric tensor in these equations.

PREREQUISITES
  • Understanding of Maxwell's equations
  • Familiarity with vector calculus, specifically curl operations
  • Knowledge of complex numbers and their application in electrical engineering
  • Basic concepts of electromagnetic fields, including permeability and permittivity
NEXT STEPS
  • Study the derivation and implications of curl operations in vector calculus
  • Explore the relationship between electric fields (E) and magnetic fields (H) in depth
  • Learn about the role of the dielectric tensor in electromagnetic theory
  • Investigate the separation of variables technique in solving differential equations
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Students and professionals in electrical engineering, physicists studying electromagnetism, and anyone seeking a deeper understanding of Maxwell's equations and their applications in electromagnetic theory.

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Easy question for those who know, I expect. It would help me understand though.

Generally, wherever I look for information the equation

curl E = - dB/dt

is given, but in some areas I see the equation

curl E(r,t) = j*omega*u0*H(r,t)

where j is the imaginary unit, omega is angular freq., u0 is permeability of free space.

B=u0*H so that's ok, but does this imply that dB/dt = -j*omega*B ?

Also, curl H(r,t) = -j*omega*e0*e*E(r,t) is given where e0 is permittivity of free space, e is a dielectric tensor. I assume this can be explained in the same way.

I'm missing a chunk of understanding as you probably notice ;)
 
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Usually, when trying to write down solutions to Mawell's equations, people assume two things about the field:

1) The spatial part and the temporal part can be separated: E(r,t) = R(r)T(t).
2) The temporal part can be written as T(t) = Ae[itex]^{i \omega t}[/itex].

The first assumption is fairly basic to solving differential equations, and separable functions are a very important class of solutions- I can't give a consise reason why, but for now, it makes it possible to analytically solve the equations.

The second assumption just means that the temperal part oscillates like a sine wave. It's written that way to be more general (and actually, the full expression is T(t) = Ae[itex]^{i \omega t}[/itex] + BAe[itex]^{-i \omega t}[/itex] ). There's good reasons for this assumption as well, which I don't need to get into now.

Anyhow, hopefully you can see where the j[itex]\omega[/itex] comes from now- electrical engineers use 'j' instead of 'i' becasue 'i' is current density.

The other part is the conversion of E to D, and B to H. But you seem to have a handle on that part.
 
Ah, yes I see now.

Thanks very much!
 

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