Charged Massless Waves in Maxwells Equations?

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Discussion Overview

The discussion centers around the possibility of propagating waves in charge/current as described by Maxwell's equations. Participants explore whether these equations alone can support such waves, considering various theoretical implications and constraints.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions if Maxwell's equations allow for propagating waves in charge/current, suggesting that charge/current is a second derivative of potentials and may have waving solutions under fourth derivative constraints.
  • Another participant mentions that charge oscillations, such as plasma oscillations, can occur.
  • Concerns are raised about the implications of charges propagating at the speed of light, with one participant arguing that all known charged particles have mass, which would prevent actual charge from propagating at light speed.
  • It is noted that an electromagnetic wave in a conductor has exponentially decreasing amplitude due to free charge canceling the electric field, and that a gas of charge theoretically extinguishes an EM wave instantaneously.
  • Some participants clarify that EM waves do not necessarily travel at the speed of light and discuss the properties of plasmons, which can propagate interestingly despite not requiring particles to travel at light speed.
  • One participant expresses a desire to clarify their question regarding the existence of propagating waves of 4-currents within Maxwell's formalism, indicating that their initial presentation may have been unclear.
  • Suggestions are made to use differential forms for a clearer mathematical presentation of the problem.

Areas of Agreement / Disagreement

Participants express differing views on whether Maxwell's equations can support propagating waves in charge/current, with some arguing against it based on physical constraints while others propose that certain conditions or contexts may allow for such waves. The discussion remains unresolved with multiple competing views present.

Contextual Notes

Some participants highlight the limitations of the discussion, noting that the question may depend on specific definitions and assumptions about charge propagation and the nature of electromagnetic waves in various media.

Who May Find This Useful

This discussion may be of interest to those studying electromagnetic theory, plasma physics, or mathematical physics, particularly in the context of wave propagation and the implications of Maxwell's equations.

Phrak
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Hello. This is a first post for me.

Do Maxwell's equations alone allow for propagating waves in charge/current (\phi,s[/B]J)?

I was rather struck dumb by this question out of the blue. I've never seen it addressed, denyed or confirmed.

Schematically the electric and magnetic fields are first derivatives of the vector and electric potential, and can propagate as waves under first derivative constraints of the currents and charges.

Schematically the charge/current is a second derivative of the potentials. It seems it should have waving solutions under fourth derivative constrains of the potentials.

To make thing even better, there is no other velocity in maxwells equations other than c,
so should Maxwell's equations admit charged fields that propagate at the speed of light?
 
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there can be charge oscillations (waves). for example, plasma oscillations in a metal.
 
To make thing even better, there is no other velocity in maxwells equations other than c, so should Maxwell's equations admit charged fields that propagate at the speed of light?

All the charges we encounter are a property of matter, and I think all the charged particles we know have mass. This rules out actual charge propagating at light speed.
The electric field component of the EM wave doesn't have a source as such.

Another problem would be that a charge moving at light-speed would create an infinitely powerful magnetic field.
 
Phrak said:
Hello. This is a first post for me.

Do Maxwell's equations alone allow for propagating waves in charge/current (\phi,s[/B]J)?

I was rather struck dumb by this question out of the blue. I've never seen it addressed, denyed or confirmed.

Schematically the electric and magnetic fields are first derivatives of the vector and electric potential, and can propagate as waves under first derivative constraints of the currents and charges.

Schematically the charge/current is a second derivative of the potentials. It seems it should have waving solutions under fourth derivative constrains of the potentials.

To make thing even better, there is no other velocity in maxwells equations other than c,
so should Maxwell's equations admit charged fields that propagate at the speed of light?


I would say there is a flaw in your reasoning; it seems to me that you are referring to the wave-equation for electromagnetic waves in vacum, which does not accurately descripe an EM-wave in pressence of any charge or dielectric.

I think you will be able to compare the problem to that of an EM-wave in a conducter. Such wave propagetes with exponentially decreasing amplitude, because free carge tends to cancel off the electric field as it goes. This effect is dependent on the conductivity of the material. Now, since a gass of charge has infinite conductivity, an EM wave in such gas would in theory be extinguished instantaneous.

So I'd say the answer is no.
 
Mentz114 said:
The electric field component of the EM wave doesn't have a source as such.

Yes it does. An antenna is an obvious example.
 
Troels said:
I think you will be able to compare the problem to that of an EM-wave in a conducter. Such wave propagetes with exponentially decreasing amplitude, because free carge tends to cancel off the electric field as it goes. This effect is dependent on the conductivity of the material. Now, since a gass of charge has infinite conductivity, an EM wave in such gas would in theory be extinguished instantaneous.

First I agree the the OP has possibly missed the point that EM waves do not have to travel at c.

However, it's not as simple as you have implied. Firstly a plasma does not actually have infinite conductivity, so the EM wave is not fully extinguished: it does decay but it effectively tunnels to the other side.

Secondly (non-local) plasmons are longitudinal waves, meaning the charge oscillates in the direction of travel. The particles themselves do not have to travel at the speed of light (even for a transverse wave). Dispersion relations of plasmons show that in fact they can have very interesting properties, and can propagate at c.
 
mda said:
Yes it does. An antenna is an obvious example.

After the current in the antenna has stopped, the waves are still propagating. They now have no source.
 
Thank you all for your generous responses.

I'm afraid I stated the problem poorly, however. I mean to say: Ignoring all the rest of physics, and utilizing only Maxwell's formalism, are propagating waves of 4-currents existent in the formalism? Homogenious, nontrivial solutions to be more precise.

This would be so much easier to state in the language of differential forms, and maybe Laplace-De Rham operators and stuff. But the math can get pretty exotic. Is the Classical Physics category the right place to post this sort of question?
 
Phrak said:
Thank you all for your generous responses.

I'm afraid I stated the problem poorly, however. I mean to say: Ignoring all the rest of physics, and utilizing only Maxwell's formalism, are propagating waves of 4-currents existent in the formalism?
Homogenious, nontrivial solutions to be more precise.

look. it's not so clear what ur asking. the currents are typically given, and the fields solved for. what are you asking for?

This would be so much easier to state in the language of differential forms, and maybe Laplace-De Rham operators and stuff.

then do it.

But the math can get pretty exotic. Is the Classical Physics category the right place to post this sort of question?

yes. and you could post in the math forums too, i suppose.
 
  • #10
I shall try again in the Tensor Analysis & Differential Geometry section with better presentation.
 
  • #11
okay
 

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