Why Does the Skin Effect Not Reverse into a Core Effect in AC Conductors?

In summary, the "skin effect" is the phenomenon in which the magnetic field created by an alternating current in a conductor is strongest near the surface of the conductor. It is stronger for higher frequencies, and the frequency of current reversal versus speed of propagation of the eddies toward the core is a race that the eddies always win.
  • #1
Jackson Lee
77
1
Hey, guys. There is something interesting about the skin effect, which also made me curious:wink:. Could you please help to solve it?
The following is what I got from Wiki.

alternating current flowing through that conductor. The charge carriers constituting that current, usually electrons, are driven by an electric field due to the source of electrical energy. An alternating current in a conductor produces an alternating magnetic field in and around the conductor. When the intensity of current in a conductor changes, the magnetic field also changes. The change in the magnetic field, in turn, creates an electric field which opposes the change in current intensity. This opposing electric field is called “counter-electromotive force” (back EMF). The back EMF is strongest at the center of the conductor, and forces the conducting electrons to the outside of the conductor, as shown in the diagram on the right.[1]
275px-Skineffect_reason.svg.png
It is said that, according to theory of induction, induced current would oppose the change of magnetic field. Then when current increases in the upward direction, the outward induced current would be formed. However, when current decreases in the upward direction (you know this is AC current), then it seems induced current would change into inward direction so as to maintain magnetic field. If it is the case, the "skin effect" would change into "core effect". However, why does this never come true?
 
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  • #2
The speed of magnetic field propagation in a good conductor is very slow, not much better than walking speed. The magnetic field diffuses into the conductor, but does not get very far because the surface AC current reverses and quickly cancels the previous half cycle. The core ends up with an average of zero field.

Instead of EMF and a Back EMF, think of a Counter-Current, being the image of the surface current seen reversed in the reflective surface of the conductor. That is what keeps energy on the surface and limits diffusion into the conductor.

A surface current causes a magnetic field at 90°. That magnetic field causes another current at a further 90°. Turning left twice is equivalent to reversing direction.
 
  • #3
There is a fundamental difference between the electric field produced by electrostatic potential difference and the electric field produced due to dB/dt. The latter is non-conservative and circular in nature.It acts on the charge carriers perpendicular to the drift velocity in a clockwise direction or anticlockwise directions. Both ways the charge carriers get pushed away from the axis of the conductor to the periphery.
 
  • #4
I once saw a graphic here on PF illustrating @Baluncore 's point. But I can't find it today.

In the graphic in the OP, the red circles are eddy currents. Imagine them with much smaller radii near the surface.

1/120 second later: those eddies will move toward the core and be weakened by resistive losses, and a new set of eddies rotating the opposite way will be formed on the surface. The new and old eddies try to cancel each other.

Over several cycles we will have many layers of (alternate direction, but weakening) eddies moving toward the core.

Skin effect is stronger for higher frequencies. It is a race between the frequency of current reversal versus speed of propagation of the eddies toward the core.
 
  • #5
Let'sthink said:
There is a fundamental difference between the electric field produced by electrostatic potential difference and the electric field produced due to dB/dt. The latter is non-conservative and circular in nature.It acts on the charge carriers perpendicular to the drift velocity in a clockwise direction or anticlockwise directions. Both ways the charge carriers get pushed away from the axis of the conductor to the periphery.
Sorry, I was confused. What do you mean? In clockwise direction, the inner current seems to be propelled to outside. However, in anticlockwise direction, the condition is reversed. Why are charge carriers pushed away in both conditions? Could you please state it a little more clearly?
 
  • #6
I once saw a graphic here on PF illustrating @Baluncore 's point. But I can't find it today.

In the graphic in the OP, the red circles are eddy currents. Imagine them with much smaller radii near the surface.

1/120 second later: those eddies will move toward the core and be weakened by resistive losses, and a new set of eddies rotating the opposite way will be formed on the surface. The new and old eddies try to cancel each other.

Over several cycles we will have many layers of (alternate direction, but weakening) eddies moving toward the core.

Skin effect is stronger for higher frequencies. It is a race between the frequency of current reversal versus speed of propagation of the eddies toward the core.

I really hope I can see that graph. I am trying to imagine your described image and connect it with my question. If you can find it or come up with other possible explanations, please write it down here. I will feel very appreciative for it.
 
  • #7
Suppose a charge carrier is drifting parallel to axis at some distance from it suppose it gets acted upon by a circular electric field normal to the axis whether clockwise or anticlockwise will the distance from the axis will increase or not?
 
  • #9
Attached are a couple of good references to magnetic field diffusion.
 

Attachments

  • Diffusion Of Current Into Conductors, J.Edwards and T.K Saha, 2001.pdf
    61.1 KB · Views: 330
  • Magnetoquasistatic Relaxation and Diffusion Chapter 10 .pdf
    954.7 KB · Views: 272

1. What is the skin effect?

The skin effect is a phenomenon in which alternating current (AC) tends to flow on the surface of a conductor, rather than through its entire cross-section. This is due to the inductive reactance of the conductor, which increases with frequency, causing the current to be concentrated on the outer part of the conductor.

2. How does the skin effect affect electrical systems?

The skin effect can cause an increase in resistance and a decrease in effective cross-sectional area of the conductor, resulting in higher power losses and reduced efficiency in electrical systems. It is particularly important to consider in high-frequency applications, such as in radio and telecommunications.

3. What factors influence the skin effect?

The skin effect is influenced by the frequency of the AC, the conductivity and permeability of the conductor material, and the geometry of the conductor, including its shape, size, and surface roughness. It is also affected by the presence of nearby conductors and magnetic fields.

4. How can the skin effect be minimized?

The skin effect can be minimized by using larger conductors, as this reduces the effective resistance and increases the skin depth (the depth at which the current is concentrated). It can also be reduced by using conductors with higher conductivity, such as copper or silver, and by using insulated conductors to reduce the proximity effect (the tendency for current to be concentrated near the surface of a conductor due to the magnetic field of nearby conductors).

5. Why is the skin effect important in high-power transmission?

In high-power transmission, the skin effect can lead to significant power losses and reduced efficiency. This is why it is important to carefully design and select conductors for these applications, taking into account the frequency and other factors that can influence the skin effect. By minimizing the skin effect, we can improve the performance and reliability of high-power electrical systems.

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