What are the fields produced around a current carrying conductor?

In summary, if the current is stationary, then there is only a magnetic field around the current carrying conductor.
  • #1
Godparicle
29
2
If we consider a current carrying conductor, every instant an electron enters the conductor, another electron will be leaving the conductor. Thus, the current carrying conductor will not be charged (i.e, it would not have any net positive or negative charge). Remember dipole has zero net charge, but it does have electric field around it. So, if net charge is zero, it doesn't mean there is no electric field.

It is important to notice that, if we assume only electrons to be moving, and kernels (positive nuclei) to be static, magnetic field will be produced only due to electrons.

Does it mean that electric field and magnetic field exists around the current carrying conductor?
Or
Does it mean that only magnetic field exists around the current carrying conductor?

The question is simple, but I have found varied answers until now.
 
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  • #2
Godparicle said:
So, if net charge is zero, it doesn't mean there is no electric field.
No, Gauss' Law ( http://en.wikipedia.org/wiki/Gauss's_law ) says that if there is no net charge inside a closed surface then the total electric flux through that surface is 0. There may still be an E field, but it will point inwards at some points and outwards at other points such that the total flux is 0.

Godparicle said:
Does it mean that electric field and magnetic field exists around the current carrying conductor?
Or
Does it mean that only magnetic field exists around the current carrying conductor?
A conductor with some finite resistivity will have a slight E-field as well as a B field. A superconductor carrying a steady current will have only a B field.
 
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  • #3
DaleSpam said:
No, Gauss' Law ( http://en.wikipedia.org/wiki/Gauss's_law ) says that if there is no net charge inside a closed surface then the total electric flux through that surface is 0. There may still be an E field, but it will point inwards at some points and outwards at other points such that the total flux is 0.

Yes, that is what I said before.

A conductor with some finite resistivity will have a slight E-field as well as a B field. A superconductor carrying a steady current will have only a B field.

Is there any source for this statement?
 
  • #4
Godparicle said:
Is there any source for this statement?
Which part of the statement? (There are two.)
If there is Resistance then there must be a Potential Drop so there will be an E field (Volts per Metre). That's normal textbook stuff.

If it's a superconductor then the charges will arrange themselves on the conductor to fit the minimal potential condition (same as if it were not carrying a current). Any net E field round the conductor will be due to its absolute potential (i.e. its place in the external circuit.
 
  • #5
sophiecentaur said:
Which part of the statement? (There are two.)
If there is Resistance then there must be a Potential Drop so there will be an E field (Volts per Metre). That's normal textbook stuff.
This is OK.

If it's a superconductor then the charges will arrange themselves on the conductor to fit the minimal potential condition (same as if it were not carrying a current).Any net E field round the conductor will be due to its absolute potential (i.e. its place in the external circuit.
Not clear for me.

Particularly, Dalespam stated that "A superconductor carrying a steady current will have only a B field." I wanted the source for this statement.
 
  • #6
The E field for a current carrying material is ##\sigma E=J##. The source of this is Ohm's law: http://en.wikipedia.org/wiki/Ohm's_law. Ohm's law is also covered in every textbook that covers EM physics or circuit analysis. This E field is small for ordinary conductors (large ##\sigma##) and 0 for superconductors (##\sigma = \infty##).

EDIT: corrected for mistake indicated by cabraham. See below.
 
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  • #7
Godparicle said:
Not clear for me.

Particularly, Dalespam stated that "A superconductor carrying a steady current will have only a B field." I wanted the source for this statement.
I don't think a "source" is necessary. Is it not just very basic? There will be no PD across a superconductor . There can be no fields parallel with the surface. What field can their be, apart from a field due to any net charge?
 
  • #8
It is OK, asking for sources is always appropriate here on PF. I provided a Wikipedia link, and Ohm's law is also in every textbook on basic EM physics and circuit analysis.
 
  • #9
Godparicle said:
Does it mean that electric field and magnetic field exists around the current carrying conductor?
Or
Does it mean that only magnetic field exists around the current carrying conductor?

The question is simple, but I have found varied answers until now.

It depends whether the current is stationary or it changes with time.
The stationary current produces stationary magnetic field around the wire: the field lines are concentric circles in planes perpendicular to the wire.
The time dependent current produces time dependent magnetic field. The time dependent magnetic field induces electric field.
Time dependent electric and magnetic field are inter-related, described by Maxwell's equations.

ehild
 
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  • #10
DaleSpam said:
The E field for a current carrying material is ##E=\sigma J##. The source of this is Ohm's law: http://en.wikipedia.org/wiki/Ohm's_law. Ohm's law is also covered in every textbook that covers EM physics or circuit analysis. This E field is small for ordinary conductors (small ##\sigma##) and 0 for superconductors (##\sigma = 0##).

I believe you have the right general idea, but you typed ##\sigma## where you should have typed ##\rho##. I recall Ohm's law in 3-D form as:

##J=\sigma E##, or ##E=J/\sigma##, or ##E=\rho J##. For a superconductor ##\sigma## is not zero, but infinite, whereas ##\rho## is zero. I assume you meant that. No big deal. Best regards. :)

Claude
 
  • #11
cabraham said:
I believe you have the right general idea, but you typed ##\sigma## where you should have typed ##\rho##. I recall Ohm's law in 3-D form as:

##J=\sigma E##, or ##E=J/\sigma##, or ##E=\rho J##. For a superconductor ##\sigma## is not zero, but infinite, whereas ##\rho## is zero. I assume you meant that.
Oops, you are 100% correct. I will go back and correct my post.

I make that mistake often because I think in terms of resistivity but I dislike the usual symbol for resistivity since it is the same as the usual symbol for charge density. I really should think in terms of conductivity.
 
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  • #12
DaleSpam said:
The E field for a current carrying material is ##\sigma E=J##. The source of this is Ohm's law: http://en.wikipedia.org/wiki/Ohm's_law. Ohm's law is also covered in every textbook that covers EM physics or circuit analysis. This E field is small for ordinary conductors (large ##\sigma##) and 0 for superconductors (##\sigma = \infty##).

J=E/ρ, if ρ=0, J=∞, i.e current per unit area is infinite, so infinite charge particles are moving per unit time per area. Do superconductors have infinite charge particles?

ehild said:
It depends whether the current is stationary or it changes with time.
The stationary current produces stationary magnetic field around the wire: the field lines are concentric circles in planes perpendicular to the wire.
The time dependent current produces time dependent magnetic field. The time dependent magnetic field induces electric field.
Time dependent electric and magnetic field are inter-related, described by Maxwell's equations.

Let's restrict our discussion to stationary currents for this time.
 
  • #13
"stationary current" is a contradiction

the word current by definition is something that flows

do you really mean a static charge ?
 
  • #14
ehild said:
It depends whether the current is stationary or it changes with time.
The stationary current produces stationary magnetic field around the wire: the field lines are concentric circles in planes perpendicular to the wire.
The time dependent current produces time dependent magnetic field. The time dependent magnetic field induces electric field.
Time dependent electric and magnetic field are inter-related, described by Maxwell's equations.
davenn said:
"stationary current" is a contradiction

the word current by definition is something that flows

do you really mean a static charge ?

I meant what echild meant above. To be explicit I didn't mean static charge.
 
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  • #15
davenn said:
"stationary current" is a contradiction

the word current by definition is something that flows
Stationary current means constant current.
It produces magnetic field.
Stationary current is maintained by potential difference between the end of the wire, that means electric field existing along the wire. The tangential component of the electric field is the same at both sides of the interface: both inside and outside of the wire. But I would not say that the electric field is produced by the current.

ehild
 
  • #16
ehild said:
Stationary current means constant current.
It produces magnetic field.

so you mean DC rather than AC ?
if so, why not just say DC ?
 
  • #17
Godparicle said:
J=E/ρ, if ρ=0, J=∞, i.e current per unit area is infinite, so infinite charge particles are moving per unit time per area. Do superconductors have infinite charge particles?
J is finite. E is 0.

There is a critical current density above which a superconductor becomes resistive.
 
  • #18
davenn said:
so you mean DC rather than AC ?
if so, why not just say DC ?
I mean stationary current which is not the same as DC. DC - direct current - means current flowing in the same direction all time. But it can change with time.
AC - alternating current - alternates its direction so the time average of the current is zero.

ehild
 
  • #19
Godparicle said:
J=E/ρ, if ρ=0, J=∞, i.e current per unit area is infinite, so infinite charge particles are moving per unit time per area. Do superconductors have infinite charge particles?

DaleSpam said:
J is finite. E is 0. There is a critical current density above which a superconductor becomes resistive.

Not the correct answer mathematically.

The equation suggests J to be ∞ . Your explanation should match with the equation results.
 
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  • #20
Godparicle said:
Not the correct answer mathematically.

The equation suggests J to be ∞ .
The math is correct. Your claim here is not right. Your statement would only be correct if E were nonzero.

The observed facts are 0 E and finite J. What value of ##\sigma## in ##J=\sigma E## do you think matches those observed facts? If not ##\sigma=\infty## then there must be some finite ##\sigma## which satisfies it. What do you think is that value?
 
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  • #21
@DaleSpam:

Considering your claims to be true, (i.e J=finite value, ρ=0, E=0), we have

J ≠ E/ρ

Finite value ≠ 0 / 0, your values are not agreeing with the equation.

Your claim here is not right.
 
  • #22
Godparicle said:
@DaleSpam:

Considering your claims to be true, (i.e J=finite value, ρ=0, E=0), we have

J ≠ E/ρ

Finite value ≠ 0 / 0, your values are not agreeing with the equation.

Your claim here is not right.
Dale's claim is quite right. ##E## = ##\rho####J##. Do you agree? If ##J## is finite and ##\rho## is zero, would you expect ##E## to be anything other than zero? As far as the "0/0" thing goes, that ratio can be finite. In a superconductor, ##E## & ##\rho## are both zero while ##J## is finite. No conflict, because a ratio of 2 quantities can be finite when the numerator & denominator both vanish. Again, "0/0" could be finite, or zero, or infinite. In calculus, there is a rule known as "l'Hopital's rule". If you've studies calculus, you already know that a ratio where top & bottom both vanish can be zero, infinite, or finite. I suggest you review the rule of l'Hopital. Best regards.

Claude
 
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  • #23
Godparicle said:
Finite value ≠ 0 / 0, your values are not agreeing with the equation..
0/0 is undefined as is ##\infty ~ 0##. It certainly may be finite. It only tells you that you need a different method to find the value. In this case J and E are measured experimentally. J is finite E is 0. Those are known values. The unknown is ##\sigma## and there is no finite value of ##\sigma## for which ##J=\sigma E## holds. Therefore, we say ##\sigma=\infty##.
 
  • #24
Godparicle said:
@DaleSpam:

Considering your claims to be true, (i.e J=finite value, ρ=0, E=0), we have

J ≠ E/ρ

Finite value ≠ 0 / 0, your values are not agreeing with the equation.

Your claim here is not right.

To illustrate this issue using a mechanical example, consider the equation ##F = ma##. If an object of mass ##m## is at rest, then the net force acting on it must be zero. The acceleration is zero as well. If we tried to ascertain the mass from this information we get ##m = F/a = 0/0##, which is indeterminate. The mass is non-zero, non-infinite, but force (summation) and acceleration are both zero. With any "##y=mx##" type of equation this is applicable. Does this help? :-)

Claude
 
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  • #25
Read the article from Arvix.org: http://arxiv.org/pdf/1202.1851v1.pdf

Here is a passage from that article:

"For a spherical geometry, infinite cylinder and infinite
plane, no electric fields exist outside the superconductor.
For other geometries however electric field lines do exist
outside the superconductor, implying that the surface is
not equipotential"

So, I am under impression that electric field may exist around a superconductor.
 
  • #26
cabraham said:
To illustrate this issue using a mechanical example, consider the equation ##F = ma##. If an object of mass ##m## is at rest, then the net force acting on it must be zero. The acceleration is zero as well. If we tried to ascertain the mass from this information we get ##m = F/a = 0/0##, which is indeterminate. The mass is non-zero, non-infinite, but force (summation) and acceleration are both zero. With any "##y=mx##" type of equation this is applicable. Does this help?

Your posts helped me. Thank you.
 
  • #27
I hop this is not too off topic.

DaleSpam said:
A conductor with some finite resistivity will have a slight E-field as well as a B field. A superconductor carrying a steady current will have only a B field.

On the same day I read the above quote, I listened to Leonard Susskind's lecture 6 on Special Relativity and Fields (available on YouTube and iTunes). He said that electric and magnetic fields are frame dependent. What I see as electric/magnetic, another frame will see as magnetic/electric. E becomes B and B becomes E.

DaleSpam, is your statement about superconductors frame dependent?
 
  • #28
anorlunda said:
He said that electric and magnetic fields are frame dependent. What I see as electric/magnetic, another frame will see as magnetic/electric. E becomes B and B becomes E.

DaleSpam, is your statement about superconductors frame dependent?
Yes, all statements about E, B, and J are inherently frame dependent for the reason mentioned by Susskind.
 
  • #29
Godparicle said:
Read the article from Arvix.org: http://arxiv.org/pdf/1202.1851v1.pdf
As the authors explicitly state, they are deliberately going against the established mainstream theory. Time and experiments will decide, but my comments above are (I believe) consistent with the consensus theory and therefore not consistent with challenging theories.
 
  • #30
DaleSpam said:
The E field for a current carrying material is σE=J\sigma E=J. The source of this is Ohm's law: http://en.wikipedia.org/wiki/Ohm's_law. Ohm's law is also covered in every textbook that covers EM physics or circuit analysis. This E field is small for ordinary conductors (large σ\sigma) and 0 for superconductors (σ=∞\sigma = \infty).

My actual question is regarding the fields produced "around" the conductor.

The E in your equation is the electric field set up across the ends of the conductor (If I am not wrong).

Sorry for not noticing this point before.
 
  • #31
The E is the field within the superconductor, not just at the ends, but at any point within.

For the fields outside the conductor you would need to solve Maxwell's equations. I believe that there would also be no E-field outside of a superconducting wire, unless imposed externally, but I cannot justify that at the moment.
 
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  • #32
DaleSpam said:
For the fields outside the conductor you would need to solve Maxwell's equations. I believe that there would also be no E-field outside of a superconducting wire, unless imposed externally, but I cannot justify that at the moment.

Anyway, thank you for the info on the fields within the current carrying conductors.

I look forward if anyone wants to reply for the actual question. I quote it once again:

Godparicle said:
If we consider a current carrying conductor, every instant an electron enters the conductor, another electron will be leaving the conductor. Thus, the current carrying conductor will not be charged (i.e, it would not have any net positive or negative charge). Remember dipole has zero net charge, but it does have electric field around it. So, if net charge is zero, it doesn't mean there is no electric field.

It is important to notice that, if we assume only electrons to be moving, and kernels (positive nuclei) to be static, magnetic field will be produced only due to electrons.

Does it mean that electric field and magnetic field exists around the current carrying conductor?
Or
Does it mean that only magnetic field exists around the current carrying conductor?

The question is simple, but I have found varied answers until now.
 
  • #35
Yes, I was intrigued by some of the results, particularly the Poynting vector. It seems that in a very reasonable sense power doesn't flow through a wire.
 

1. What are the fields produced around a current carrying conductor?

The fields produced around a current carrying conductor are electric and magnetic fields.

2. How are the fields around a current carrying conductor affected by the direction of the current?

The direction of the current determines the direction of the magnetic field, while the electric field is always perpendicular to the magnetic field.

3. How does the strength of the current affect the fields around a conductor?

The strength of the current directly affects the strength of the magnetic field, while the electric field is dependent on the distance from the conductor and the amount of charge.

4. Are the fields around a current carrying conductor uniform?

No, the fields around a current carrying conductor are not uniform. The strength of the fields decreases as the distance from the conductor increases.

5. How do the fields around a current carrying conductor change when the current is increased or decreased?

When the current is increased, the strength of the fields also increases. Conversely, when the current is decreased, the strength of the fields decreases as well.

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