Why is the magnetic field of a wire circular?

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Discussion Overview

The discussion revolves around the nature of the magnetic field generated by a current-carrying wire, specifically addressing why the field is circular and exploring the underlying principles such as the Biot-Savart Law and symmetry arguments. Participants also delve into the interaction between a moving charge and the magnetic field, questioning the perpendicular nature of the force experienced by the charge.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that the magnetic field of a moving charge can be visualized using the right-hand thumb rule, likening it to Saturn's rings.
  • Others argue that the circular nature of the magnetic field around a straight wire can be deduced from the Biot-Savart Law, which involves vector calculations to show that the magnetic field is orthogonal to the radius vector from the wire.
  • Some participants suggest that symmetry plays a role in determining the shape of the magnetic field, questioning what other shapes could arise from a long straight wire.
  • There are claims that the magnetic field could theoretically have an outward component, but this must be proven through laws like Ampere's Law or the Biot-Savart Law.
  • Several participants express uncertainty about the necessity of symmetry in explaining the magnetic field's behavior and whether spontaneous symmetry breaking could occur.
  • Participants seek clarification on why the magnetic field is not dipolar and emphasize the need for a precise definition of the magnetic field in this context.
  • Questions arise regarding the nature of the force on a moving charge in a magnetic field, specifically why it is perpendicular to both the magnetic field and the velocity of the charge, beyond the explanation of the cross product.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the reasons for the circular nature of the magnetic field or the role of symmetry. Multiple competing views remain regarding the explanations and interpretations of the magnetic field's characteristics.

Contextual Notes

Some discussions highlight the limitations of symmetry arguments without the support of established laws like the Biot-Savart Law. There is also mention of the complexity involved in understanding the interactions between charges and magnetic fields.

Mr Virtual
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Hi
First of all, since magnetic field in a wire carrying current is due to the movement of electrons, I assume that the magnetic field of a single isolated moving electron, or any other charged particle, can also be deduced by the right hand thumb rule i.e. the field will be much like Saturn's ring around it, where we assume saturn to be a charged particle, and its ring as its field.

Now my question is: How is this field deduced. Why is it circular? Is it the result of superposition, if any?

Secondly, I know that magnetic force exerted on a moving charge consists of a cross product of B and v. But I think that this force is the result of interaction between the charge's own magnetic field and the applied field, B.
My question is: How does this interaction exactly happen? How does it result in this force? Most importantly, what causes this force to be perp to both B and v (I need an explanation other than that it is just the result of cross product)? I raised a similar question elsewhere but didn't get much help.
I'd be grateful if somebody explains.

Thanks
Mr V
 
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Mr Virtual said:
Hi
First of all, since magnetic field in a wire carrying current is due to the movement of electrons, I assume that the magnetic field of a single isolated moving electron, or any other charged particle, can also be deduced by the right hand thumb rule i.e. the field will be much like Saturn's ring around it, where we assume saturn to be a charged particle, and its ring as its field.

Now my question is: How is this field deduced. Why is it circular?
The proof that magnetic field lines due to a straight, infinitely long, constant current are circular is based on the Biot-Savart Law.
The Biot Savart Law states that the magnetic field dB produced by an infinitesimal segment of wire ds which carries a current I through it is given by
Biot-Savart.gif

The proof itself involves quite messy vector calculations, but amounts to this: proving that at any point P, B is orthogonal to a radius vector r, drawn perpendicular to the wire with initial point on the wire and terminal point at P.
 
Mr Virtual said:
Hi
First of all, since magnetic field in a wire carrying current is due to the movement of electrons, I assume that the magnetic field of a single isolated moving electron, or any other charged particle, can also be deduced by the right hand thumb rule i.e. the field will be much like Saturn's ring around it, where we assume saturn to be a charged particle, and its ring as its field.

Now my question is: How is this field deduced. Why is it circular? Is it the result of superposition, if any?

Secondly, I know that magnetic force exerted on a moving charge consists of a cross product of B and v. But I think that this force is the result of interaction between the charge's own magnetic field and the applied field, B.
My question is: How does this interaction exactly happen? How does it result in this force? Most importantly, what causes this force to be perp to both B and v (I need an explanation other than that it is just the result of cross product)? I raised a similar question elsewhere but didn't get much help.
I'd be grateful if somebody explains.

Thanks
Mr V

It's not always circular.

I don't know if there's a particular answer to 'why' it happens. Physics examines 'what' happens. When a charge moves, it creates a magnetic field, and the magnetic field is always arranged perpendicular to the direction of motion of the charged particle and perpendicular to the Electric field, following the right-hand rule as you mentioned.

Given those rules, a line charge moving in a direction along the length of itself will generate a circular magnetic field. There are cases where a straight field can be generated too (like inside a coil).

I suppose you could see it as a superposition of the induced field from all the point charges that make up the distributed line charge (the wire), but point charges in electrodynamics are more complicated than distributed charges.
 
Another way of looking at it is just symmetry, if you have a field from a long straight wire what other shape could it be?
If it was square - where would the information come from to specify where the corners should be? This also explains why the field from a point charge should be spherical.
 
mgb_phys said:
Another way of looking at it is just symmetry, if you have a field from a long straight wire what other shape could it be?
If it was square - where would the information come from to specify where the corners should be?
Well, the magnetic field lines, in principle at least, could be going outward from the wire. The actual proof the magnetic field line are circular must be derived from Ampere's Law or the Biot-Savart Law. Symmetry arguments alone aren't enough.
 
Pythagorean said:
It's not always circular.

I don't know if there's a particular answer to 'why' it happens. Physics examines 'what' happens. When a charge moves, it creates a magnetic field, and the magnetic field is always arranged perpendicular to the direction of motion of the charged particle and perpendicular to the Electric field, following the right-hand rule as you mentioned.
The observation that the magnetic field created by a moving charge is perpendicular to the direction of motion is a consequence of the Biot-Savart Law, and is what the OP wanted proved.
 
lugita15 said:
Well, the magnetic field lines, in principle at least, could be going outward from the wire. The actual proof the magnetic field line are circular must be derived from Ampere's Law or the Biot-Savart Law. Symmetry arguments alone aren't enough.

Symmetry is enough. Since reversing the current in a loop is no different from looking at it from the other side, the magnetic field cannot symmetrically have any outward component.

Then again, plenty of students would have asked "but why does it have to be symmetric?". Can you say there are no cases of spontaneous symmetry breaking in physics?
 
cesiumfrog said:
Symmetry is enough. Since reversing the current in a loop is no different from looking at it from the other side, the magnetic field cannot symmetrically have any outward component.

Then again, plenty of students would have asked "but why does it have to be symmetric?". Can you say there are no cases of spontaneous symmetry breaking in physics?

well symmetry arguments are helpful and indeed too good but are useless(here for other components) without bioy-savart law.
this example may be stupid but anyway-suppose i newly discovered the field due to wire and suppose i say the field due to wire at any point depends on say how i look at it ,or depends on the sorce that produces the current.:biggrin:..which kill symmetry arguments then u can't decide.
well what i am supporting is well cooperated operation of biot savart and symmetry and in general physical laws(through observations) and symmetry
 
And why it is not dipole? I think it is not circular, it is not correct.
 
  • #10
Thanks for your answers.

Can I now get an answer to: how the force felt by a moving charge in a magnetic field is perpendicular to both B and v. I mean any explanation besides that cross product rule is involved here?

Eagerly awaiting your answers...

Mr V
 
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  • #11
Can you tell me why it is not dipole, please?
 
  • #12
stmartin said:
Can you tell me why it is not dipole, please?

who said that and what is "it"?
 
  • #13
Why it is circular, why not dipole? On all of the posts, no one exactly said what is it. Please let's define it correctly. Thank you.
 
  • #14
stmartin said:
Why it is circular, why not dipole? On all of the posts, no one exactly said what is it. Please let's define it correctly. Thank you.
I can't understand what you're saying. Are you asking why the magnetic field lines are circular? The Biot-Savart Law, like I said before. I'm not sure what you mean by "why not dipole". Why aren't the magnetic field lines of an infinitely long, straight current the same as those of a magnetic dipole? There's no a priori reason they should be.
 
  • #15
lugita15 said:
I can't understand what you're saying. Are you asking why the magnetic field lines are circular? The Biot-Savart Law, like I said before. I'm not sure what you mean by "why not dipole". Why aren't the magnetic field lines of an infinitely long, straight current the same as those of a magnetic dipole? There's no a priori reason they should be.

And why there is prior that, the field should be circular?
 
  • #16
Assume the following -- interactions occur because of fields, and do a simple experiment: set up two long wires with currents, and observe that they attract for parallel currents, and repel for antiparallel ones, and also that the force is purely perpendicular to the wires. Assume that this is a reasonable model for infinitely long wires.

By symmetry, you'll deduce that the field is circular about the wire. And you'll also deduce, by symmetry, that the force on a current is perpendicular to the current and the field. Try thinking up of the arguments yourself -- I'll post the full logical steps in a few days.
 
  • #17
Why magnetic field has the shape it has is a small problem compared to the question what magnetic field itself is. This is not a mere philosophical issue, the question "what magnetic field is" has some answers that come from special relativity. Mr Virtual, do you understand what I say in the post #9 in this thread https://www.physicsforums.com/showthread.php?t=175438 It could be true that I start the post too provocatively. It's best to ignore it, I agree mostly what pervect says later in the thread.

Mr Virtual said:
But I think that this force is the result of interaction between the charge's own magnetic field and the applied field, B.

I don't think that's correct. It is in fact the charge that interacts with the fields.

Can I now get an answer to: how the force felt by a moving charge in a magnetic field is perpendicular to both B and v.

You could get, but the answer is technical, so I'm not starting this with LaTex right away. I can start typing more details of the calculation if you are with me in my post #9 of the thread linked above.
 
  • #18
are these 2 fields equal?
this one: http://img54.imageshack.us/img54/2199/untitled12jd5.jpg
with
this one: http://www.peter-thomson.co.uk/tornado/fusion/images/magneticfieldcurrent.gif
 
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  • #19
The first is a magnetic dipole field. The second is the field produced by a long straight wire (current). If by "equal" you mean "same configuration", the answer is "no". The two configurations of currents are different, so the fields are different.
 
  • #20
jtbell said:
The first is a magnetic dipole field. The second is the field produced by a long straight wire (current). If by "equal" you mean "same configuration", the answer is "no". The two configurations of currents are different, so the fields are different.
And what is the difference? In the both cases the electrons are moving.
 
  • #21
I should say that they are in deed opposite.

1 case, the earth:
the current is circular around the latitude of the earth.

2 case, the current:
the current is straight inducing a magnetic field in the 'latitude' of the wire.
 
  • #22
ArielGenesis said:
I should say that they are in deed opposite.

1 case, the earth:
the current is circular around the latitude of the earth.

2 case, the current:
the current is straight inducing a magnetic field in the 'latitude' of the wire.
Yes, that is the difference. And how will you explain what happens when the electron is moving circular, when its in orbital? Why the field lines are spread like on the first picture?
 
  • #24
Can you help me?
Here is one more picture when the charge is moving http://img54.imageshack.us/img54/2199/untitled12jd5.jpg
 
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  • #25
stmartin: they're that way because of the equations. Why are the equations that way? Because that's what experimental evidence + reasonable assumptions about the non-perversity of the universe demands. To work out what the logical steps are, try what I suggested in my last post to this thread.
 

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