Skin depth of zero thickness in DC circuits

In summary, the skin depth formula is inversely proportional to conductivity and frequency omega. There are three cases where the skin depth of a metal is zero: 1) for an EM wave of any frequency incident on a perfect metal wall with infinite conductivity, resulting in a surface current; 2) for an AC battery connected to a load with finite resistivity, with the current only on the periphery of the conductor; and 3) for a DC battery connected to a load via ideal wires, with the current flowing on the skin of the conductor. In the case of DC current, the electric and magnetic fields push and pull the current, while resistance plays a role in creating an electric field along the wire. For an ideal conductor,
  • #1
fisico30
374
0
Hello Forum,

the formula for skin depth is both inversely proportional to conductivity and frequency omega.
There seem to be 3 cases when the skin depth of a metal is exactly (or tends to) zero:

1) if an EM wave of frequency f (any frequency) is incident on a perfect metal wall (infinite conductivity sigma). The current is a surface current that exists only on the surface of the ideal conductor;

2) If a AC battery is connected to a load via wires with finite resistivity. The AC current only distributes itself on the periphery of the conductor with the current density being largest near the surface of the conductor;

3) In the case of a DC battery connected to a load via ideal wires (sigma=infinity). We read in books that DC current flows uniformly across the cross-section of the conductor. However if the wires are perfect conductors the electric field E inside is equal to zero! How is that DC current generated then if E=0 and there is no F=q*E force to push charges and make a current...
I read that even in the DC case, if the wires have infinity conductivity (as postulated in intro book) ,the current ends up flowing only on the skin a not inside the conductor as most book say...
What is the true story as far as 3) goes?

I thought that in the DC case there was no skin effect...

thanks
fisico30
 
Physics news on Phys.org
  • #2
For 3), when you close the circuit there is a wave of electric and magnetic fields that starts going down the wire (in the space around the wire.) The current is pushed by the inductance of the wire behind the wavefront and pulled by the natural capacitance just ahead of the wavefront. Resistance of the wire is zero and has nothing to do with the current flowing.

Finite resistance *leads to* an electric field along the wire. It's not the cause of the current but an effect of it.
 
  • #3
Hi Antiphon,
so you say that "...The current is pushed by the inductance of the wire behind the wavefront and pulled by the natural capacitance just ahead of the wavefront. Resistance of the wire is zero and has nothing to do with the current flowing..."

That seems to be equivalent (correct me if I am wrong) to say that there are surface charges on the conductors caused by battery...They causes the capacitance and their motion the inductance that then cause the current.

"...Finite resistance *leads to* an electric field along the wire. It's not the cause of the current but an effect of it..."

Not sure I understand or agree with it: charges move if there is a force on them. The electric force is F=q*E. If there is finite resistance a force is needed and that is caused by an electric field being present. So I don't see how the E field is an effect and not the cause...

In the theoretical case 3) do you agree that a DC current flows uniformly across an ideal conductor or do you believe it flows on the skin instead?

thanks
fisico30
 
  • #4
Yes to your first remark about the motion along the wire.

For the second remark, F=qE + qvXB. The electric term is not the only one. Think of an ideal conducting ring with a current flowing in it. Now if you introduce a finite but small resistance in the ring, a tangential electric field will appear suddenly which was not there before. No battery. The electric field is created by forcing current through the resistance. If you quickly take away the resistance, it's the voltage that drops to zero with it, not the current.

For an ideal conductor, the current flows in an infinitely thin sheet at the surface if it is AC current. To answer the DC question you must know the history of the fields. It is possible to cause DC currents to circulate indefinitely inside a perfect conductor.
 
  • #5


Hello fisico30,

Thank you for bringing up this interesting topic. I can provide some insights into the concept of skin depth in DC circuits.

Firstly, it is important to understand that skin depth is a concept that applies to AC circuits and not DC circuits. In DC circuits, the current flows uniformly throughout the cross-section of the conductor, as you mentioned. This is because in DC circuits, the electric field is constant and there is no change in frequency. Therefore, the concept of skin depth is not relevant in this case.

In the case of an ideal conductor with infinite conductivity, the electric field inside the conductor is indeed zero. However, this does not mean that there is no current flowing. In fact, the current is still present and flows uniformly throughout the conductor. This is because in DC circuits, the current is driven by the potential difference between the two ends of the conductor, not by the electric field.

It is also important to note that in real-world scenarios, there is no such thing as a perfect conductor with infinite conductivity. Therefore, the concept of skin depth can be applied to AC circuits where the conductivity is finite and the current tends to flow on the surface of the conductor. This is due to the skin effect, where the higher frequency components of the AC current tend to flow closer to the surface of the conductor, while the lower frequency components penetrate deeper into the conductor.

In summary, skin depth is a concept that applies to AC circuits and not DC circuits. In DC circuits, the current flows uniformly throughout the conductor regardless of its thickness. I hope this helps clarify any confusion about the concept of skin depth in DC circuits.
 

FAQ: Skin depth of zero thickness in DC circuits

What is the concept of skin depth in DC circuits?

The skin depth in DC circuits refers to the distance from the surface of a conductor to the point where the current density has decreased to 37% of its value at the surface. It is a measure of how far the current can penetrate into a conductor.

How is the skin depth calculated?

The skin depth is calculated using the formula δ = √(2ρ/πμf), where δ is the skin depth, ρ is the resistivity of the conductor, μ is the permeability of the material, and f is the frequency of the current.

What is the significance of skin depth in DC circuits?

Skin depth is significant in DC circuits because it affects the resistance of the conductor, which in turn affects the flow of current. It is also important in determining the distribution of current within a conductor.

How does the skin depth vary with different materials?

The skin depth varies with different materials based on their resistivity and permeability. Materials with higher resistivity and lower permeability will have a larger skin depth, meaning the current can penetrate deeper into the material.

Can skin depth be ignored in DC circuits?

No, skin depth cannot be ignored in DC circuits as it plays a crucial role in determining the behavior of the circuit. It affects the resistance and current distribution, which can ultimately impact the performance of the circuit.

Back
Top