Help in TEM wave propagation for a solenoid or magnetic dipole.

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SUMMARY

The discussion focuses on the propagation of Transverse Electromagnetic (TEM) waves generated by a solenoid or magnetic dipole, specifically under the influence of alternating current (AC). Participants clarify that the electric field (E) and magnetic field (B) lines behave differently under AC compared to direct current (DC), with AC creating closed loops of B as polarity changes. The conversation emphasizes the importance of the solenoid's size relative to the wavelength, noting that if the solenoid's circumference is significantly smaller than the wavelength, the behavior of the fields can be accurately described. The discussion also references Faraday's Law in relation to induced currents in loops with resistors.

PREREQUISITES
  • Understanding of Transverse Electromagnetic (TEM) waves
  • Knowledge of Faraday's Law of Electromagnetic Induction
  • Familiarity with alternating current (AC) and direct current (DC) concepts
  • Basic principles of electromagnetic field theory
NEXT STEPS
  • Research the behavior of electromagnetic fields in solenoids
  • Study the principles of Faraday's Law in detail
  • Explore the concept of phase retardation in electromagnetic waves
  • Investigate end-fire helical antennas and their applications
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Students and professionals in electrical engineering, physicists studying electromagnetic theory, and anyone interested in the practical applications of TEM wave propagation in solenoids and antennas.

yungman
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I am trying to figure out how the TEM wave looks like and how it propagate outward. Attached is a pdf of a drawing with only the solenoid and show the winding that the current is flowing in CCW and a reference. Also I draw a loop with one resistor and show the induced current and the polarity of the resistor for follow up question.

This is my thinking:

2tz7k.jpg


The magnetic flux line is shown in blue that loop from the top back to the bottom. I draw just two loops, but it is understand it is all around 360 deg around the z axis(symetric around the z axis or:

[tex]\hbox { Both }\frac {\partial \vec E}{\partial \phi} \;=\; \frac {\partial \vec B}{\partial \phi} \;=\; 0 \hbox { in cylindrical coordinates. }[/tex]

I think the associate electric field look like the red circle. The circles are parallel with the xy plane. The direction of propagation of each point move as shown in direction of the [itex]\hat n[/itex] at every point. The direction of [itex]\hat n[/itex] is:

[tex]\hat n \;=\; \vec E X \vec B[/tex]

basically, I think the propagation of the TEM is outward in direction of the [itex]\hat n[/itex] at all points. tell me whether I am correct.

Feel free to download the pdf and draw what you think is right and post it back.

Furthermore, I would like to see how the varying magnetic field induce current and voltage into the loop with resistor. I know we have Faraday's Law, I just want to see the machenism.

thanks for the help

Alan
 

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You're drawing looks pretty good to me; maybe that's why you have no replies, because there's nothing more to say! :-p

I just want to point out a few things because you didn't explicitly state them; although, I have a feeling that you know you've made certain assumptions.

First of all, you have assumed an AC current. If you were using a DC current, your picture would still be correct minus the fact that you would have no electric field. With an AC current, the common interpretation is that the lines of B will close in on themselves (form closed loops) as polarity changes. This is similar to the case of an oscillating electric dipole and its lines of E.

As for the lines of E in your picture, I like to think of them as lines of latitude on a sphere. Thus at the two poles, you would have lines of zero circumference. Each "change in polarity" can be pictured as the introduction of a new sphere, with lines of latitude (lines of E) pointed in the opposite direction as the preceding sphere. Thus radiation can be pictured by an increase in each sphere's radius. Note that no matter how big the sphere, you will always have loops of zero circumference at the poles, consistent with zero radiation along the z-axis.

Second point, everything you and I have said is strictly applicable only if the solenoid is small, i.e. if the circumference of the solenoid is much less than the wavelength. If this condition does not prevail, then you can have a much different picture arising from phase retardation, i.e. constructive and destructive interference due to fields being spatially separated throughout points on the solenoid. If this point interests you, then I'll refer you to the internet; look up end-fire helical antennas.
 
cmos said:
You're drawing looks pretty good to me; maybe that's why you have no replies, because there's nothing more to say! :-p

I just want to point out a few things because you didn't explicitly state them; although, I have a feeling that you know you've made certain assumptions.

First of all, you have assumed an AC current. If you were using a DC current, your picture would still be correct minus the fact that you would have no electric field. With an AC current, the common interpretation is that the lines of B will close in on themselves (form closed loops) as polarity changes. This is similar to the case of an oscillating electric dipole and its lines of E.

As for the lines of E in your picture, I like to think of them as lines of latitude on a sphere. Thus at the two poles, you would have lines of zero circumference. Each "change in polarity" can be pictured as the introduction of a new sphere, with lines of latitude (lines of E) pointed in the opposite direction as the preceding sphere. Thus radiation can be pictured by an increase in each sphere's radius. Note that no matter how big the sphere, you will always have loops of zero circumference at the poles, consistent with zero radiation along the z-axis.

Second point, everything you and I have said is strictly applicable only if the solenoid is small, i.e. if the circumference of the solenoid is much less than the wavelength. If this condition does not prevail, then you can have a much different picture arising from phase retardation, i.e. constructive and destructive interference due to fields being spatially separated throughout points on the solenoid. If this point interests you, then I'll refer you to the internet; look up end-fire helical antennas.

Thanks for you reply. Yes I am just based on a very simple model. Yes I under that when polarity of E change, it is like the circle is circulating in opposite direction. Thanks for all your help. This is kind of a spin off topic from the big MIT professor thread where we really going at it. Feel free to join in there.
 

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