Electrostatic charge or dieletric field?

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SUMMARY

The discussion centers on the distinction between dielectric fields and electric fields, referencing Steinmetz's critique of the outdated notion of electrostatic charge on conductors. Participants highlight the evolution of electromagnetic theory, emphasizing the integration of electric and magnetic fields into a unified electromagnetic field. Key concepts such as quantum electrodynamics and polarization fields are introduced, illustrating the complexity and historical context of these theories. The consensus is that modern electromagnetic theory provides a more accurate framework for understanding these phenomena than earlier models.

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  • Understanding of electromagnetic theory and its historical development
  • Familiarity with quantum electrodynamics and its implications
  • Knowledge of polarization fields and their relationship to dielectric materials
  • Basic grasp of the concepts of electric and magnetic fields
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  • Study the principles of quantum electrodynamics and its applications in modern physics
  • Research the historical evolution of electromagnetic theory from Maxwell to contemporary interpretations
  • Explore the concept of polarization fields and their significance in dielectric materials
  • Examine the differences between electric fields and dielectric fields in detail
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Electrical engineers, physicists, and students of electromagnetic theory seeking to deepen their understanding of the relationship between electric and magnetic fields, as well as the historical context of these concepts.

Deco56
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Hi,

I have a question on a quote I saw from Steinmetz regarding the two components of eletric field (magnetic and dielectric)

To quote, ''Unfortunately, to a large extent in dealing with dielectric fields the prehistoric conception of the electro- static charge (electron) on the conductor still exists, and by its use destroys the analogy between the two components of the electric field, the magnetic and the dielectric, and makes the consideration of dielectric fields unnecessarily complicated.''

Steinmetz continues, ''There is obviously no more sense in thinking of the capacity current as current which charges the conductor with a quantity of electricity, than there is of speaking of the inductance voltage as charging the conductor with a quantity of magnetism. But the latter conception, together with the notion of a quantity of magnetism, etc., has vanished since Faraday's representation of the magnetic field by lines of force."

Steinmetz is considered a legend in electrical engineering, yet he references a "prehistoric" notion of charge on conductor. Why do we still use charges on conductors? What made us abandon the dielectric field? Why have we strayed from lines of force? Thanks.
 
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There has been progress in physics and engineering since Steinmetz.
http://www.feynmanlectures.caltech.edu/I_02.html#Ch2-S2

Thus we have a new view of electromagnetic interaction. We have a new kind of particle to add to the electron, the proton, and the neutron. That new particle is called a photon. The new view of the interaction of electrons and photons that is electromagnetic theory, but with everything quantum-mechanically correct, is called quantum electrodynamics. This fundamental theory of the interaction of light and matter, or electric field and charges, is our greatest success so far in physics. In this one theory we have the basic rules for all ordinary phenomena except for gravitation and nuclear processes. For example, out of quantum electrodynamics come all known electrical, mechanical, and chemical laws: the laws for the collision of billiard balls, the motions of wires in magnetic fields, the specific heat of carbon monoxide, the color of neon signs, the density of salt, and the reactions of hydrogen and oxygen to make water are all consequences of this one law. All these details can be worked out if the situation is simple enough for us to make an approximation, which is almost never, but often we can understand more or less what is happening. At the present time no exceptions are found to the quantum-electrodynamic laws outside the nucleus, and there we do not know whether there is an exception because we simply do not know what is going on in the nucleus.
 
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Yes, we photons are the carriers of electromagnetic phenomenon but this is defined by the perpendicular crossing of dieletric and magnetic field lines (transverse waves). Steinmetz was aware of the electrical phenomenon preceding electromagnetism as well.

"At the present time no exceptions are found to the quantum-electrodynamic laws outside the nucleus, and there we do not know whether there is an exception because we simply do not know what is going on in the nucleus"

A little confusing, no?
 
I've never even heard of a dielectric field. It sounds like something used back before we knew what the EM field was. Since then, the electric field has been combined with the magnetic field to form the electromagnetic field. This combination is able to explain all classical electrical or magnetic phenomena.
 
Drakkith said:
I've never even heard of a dielectric field. It sounds like something used back before we knew what the EM field was. Since then, the electric field has been combined with the magnetic field to form the electromagnetic field. This combination is able to explain all classical electrical or magnetic phenomena.

Steinmetz is like Tesla and Edison era electromagnetic theory. Personally, Stratton and Chew are as far back as I'm willing to go for study material although Sommerfeld is interesting from a historical standpoint.

I seem to recall that the dielectric field may be an older term for the polarization field.

We've progressed leaps and bounds in electromagnetic theory since the first strong experimental results of Maxwell's theory in the 1880's. While the underlying theory has basically been complete since Maxwell put it down, there has been a lot of progress in simplifying and interpreting the theory. We just find better ways of representing the stuff. For example, Stratton uses Hertzian potentials but I much prefer the exponential potentials that Kong used in his work 30 years later. Both of them are correct, but I much prefer to work with the latter.
 
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The dieletric field is simply the electric field, and has similar field lines and electric flux just like the magnetic field. Except the electron has destroyed this analogy. The electron is just one end of the dieletric field...dielectric field is the same as magnetic field except magnetic fields form circles around wire while dieletric lines shoot out radially from a conductor
 
Okay. So your question is why we abandoned the dielectric field? Because modern EM theory works using the electromagnetic field and explains practically all observed phenomena better than alternatives.
 
Deco56 said:
The dieletric field is simply the electric field, and has similar field lines and electric flux just like the magnetic field. Except the electron has destroyed this analogy. The electron is just one end of the dieletric field...dielectric field is the same as magnetic field except magnetic fields form circles around wire while dieletric lines shoot out radially from a conductor

Saying that the dielectric field has similar field lines as the magnetic field only increases my suspicions that the dielectric field is an analogy of the Polarization field. Electric charges are monopoles while all magnetic fields are produced by at least a dipole. The Polarization field is the result of the the induced dipole moments in a dielectric due to an applied electric field. So the lowest multipole represented in the Polarization field is the dipole, like the magnetic field.

Perhaps the concept of dielectric, bound charges, and its polarization were not well known, developed or understood when Steinmetz made his statements. That would account for his frustration at a complex theory for dielectric fields. For example, Debye relaxation was posed around 1910 I think.
 
Born2bwire said:
Saying that the dielectric field has similar field lines as the magnetic field only increases my suspicions that the dielectric field is an analogy of the Polarization field. Electric charges are monopoles while all magnetic fields are produced by at least a dipole. The Polarization field is the result of the the induced dipole moments in a dielectric due to an applied electric field. So the lowest multipole represented in the Polarization field is the dipole, like the magnetic field.

Perhaps the concept of dielectric, bound charges, and its polarization were not well known, developed or understood when Steinmetz made his statements. That would account for his frustration at a complex theory for dielectric fields. For example, Debye relaxation was posed around 1910 I think.

Steinmetz had an excellent grasp of electromagnetic and electrical phenomenon. He invent complex versor algebra to describe AC phenomenon and was. What eminates out of a charge? An E-field...
Dielectric-and-Magnetic-Flux-Lines-2.png


This picture is familiar, applies to all conductors and explains the dieletric/magnetic field directions and their orthogonality.
 
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Then what do you purport to be the difference between the dielectric and the electric field?
 
  • #11
Well, for one an electric field is thought only to exist after a charge exists and propagates with c. Second, dieletric fields must end on conductors or themselves, electric fields do not need to end on conductors, but can formed closed loops.

It mostly is semantics, they represent the same idea but the electric field is more difficult to understand because of how it ties in the electrical charge, electron. As steinmetz said, there is no more sense in thinking that current charges a space with an amount of magnetism as there is of conduction current or voltage charge a plate with a certain amount of electrification, as described above.
 

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