Magnetic Forces and Work: An Explanation

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Discussion Overview

The discussion revolves around the nature of magnetic forces and work, particularly in the context of parallel currents and the interaction between charged particles and magnetic fields. Participants explore theoretical implications, practical examples, and the underlying physics principles, including the roles of electric and magnetic fields.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • Some participants assert that the magnetic force on a moving charged particle does no work, as it is always perpendicular to the motion.
  • Others argue that while the magnetic field does not do work directly, it can induce an electric field that performs work on the charged particles or currents.
  • One participant explains that the attraction between two parallel currents is due to the magnetic field created by one current affecting the other, leading to a force that causes movement.
  • There is a discussion about the Lorentz force, with some participants emphasizing that it includes both electric and magnetic components, and only the electric component does work.
  • Some participants question the conditions under which work is done, particularly in relation to the movement of charges and the role of induced electric fields.
  • Concerns are raised about the definitions and implications of work done by magnetic fields, particularly in experimental contexts like the Stern-Gerlach experiment.

Areas of Agreement / Disagreement

Participants express differing views on the role of magnetic fields in doing work, with no consensus reached. Some maintain that magnetic fields do no work, while others suggest that induced electric fields are responsible for the work done in certain scenarios.

Contextual Notes

Participants highlight the complexity of the interactions between electric and magnetic fields, noting that definitions and assumptions about work and force may vary based on context. The discussion includes references to specific scenarios and theoretical constructs that may not be universally agreed upon.

Who May Find This Useful

This discussion may be of interest to those studying electromagnetism, particularly in understanding the nuances of magnetic forces, work, and the interplay between electric and magnetic fields in various physical contexts.

lugita15
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Since the magnetic force on a moving charged particle is qv X B, the work done by a static magnetic field is always zero.
But consider two parallel currents, both going from left to right. The second current will experience a magnetic force of attraction towards the first current. Therefore, it will move towards the first wire and work will be done on it by the magnetic field. But didn't we just say that it's impossible for a magnetic field to do work?

Any help would be greatly appreciated.
Thank You in Advance.
 
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lugita15 said:
But didn't we just say that it's impossible for a magnetic field to do work?
But you didn't say that. You said no work on a moving CHARGED PARTICLE.
That statement does not apply to currents.
 
The electric field does the work

The magnetic field itself does no work on the moving charges, it merely deflects them. This deflection induces an electric field in the wires, which acts on the wire's positively charged lattice, and does the work in moving the wires together.
 
The reason the first wire is attracted to the second wire is due to the moving charges inside the wire. When a current flows in the second wire, it creates a magnetic field that goes through the first wire perpenticular to the axis of the first wire, so a charge moving in the first wire with a certain velocity v and charge q will experience a force towards the second wire (if the currents are in the same direction) or away (if the currents are in opposite directions) from the second wire by qv x B. The same goes for the second wire, when a current flows in the first, a resultant force is created on the moving charges in the second wire, so essentially the two wires move together or apart depending on the current direction.
 
The question was not why there's a force between the two wires, but what is actually doing the work--since a magnetic field does no work on moving charges. To answer that requires looking below the surface at the induced electric field.
 
Meir Achuz said:
But you didn't say that. You said no work on a moving CHARGED PARTICLE.
That statement does not apply to currents.
Yes it does. The force on a current I in a magnetic field B is given by Il x B. The same argument can be applied.
 
Doc Al said:
The magnetic field itself does no work on the moving charges, it merely deflects them. This deflection induces an electric field in the wires, which acts on the wire's positively charged lattice, and does the work in moving the wires together.
It is my understanding that a magnetic field can only induce an electric field in a loop if there is a changing magnetic flux through the loop. What loop are you considering, and how is the magnetic flux changing through the loop?
 
No loop, no changing magnetic field. (Perhaps my use of the term "induced" was a bit sloppy.) There are charge carriers--electrons--moving in the wire. The magnetic field deflects them to one side of the wire, creating a charge separation and thus an electric field.
 
If you need a visual aid have a look at http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/hall.html" .
 
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  • #10
Here's my 2 cents:

The magnetic field of wire 1 deflects the current in wire 2 in the direction of wire 1, simply by the Lorentz force IxB. So now the velcoity of the electrons in the wire is no longer parallel to the orginal direction of the wire, but it acquires a component in the direction of wire 1! The Lorentz force thus acquires now both a component in the direction of wire 1, responsible for the attraction between the two wires, and a component in the direction opposing the current in wire 2.

Notice two points:

1) To sustain this situation and to get the two wires moving towards each other the Lorentz force in the direction opposing the current in wire 2 must be overcome. It is this force that pushes the electrons forward, overcoming the opposing Lorentz force, that eventually does the work in moving the two wires together. Notice that this is just the electric force driving the current, generated in a battery for example.

2)In the entire process the Lorentz force is prependicular to the current, and thus does no work! Griffiths has a nice intuitive analogy: when you push a block up an inclined plane by exerting a horziontal force, it is you who does the work. The normal force no plays the role of the magnetic field in this analogy. It is always perpendicular to the ramp and the motion, so does no work. It has however a component in the horizontal direction that you have to overcome to move the block. It has also a vertical component that is responsible for the vertical movement of the block. But it is actually your horizontal force, merely deflected by the normal force in the vertical direction. The role of the normal force (and the magnetic force in your question) is one of redirecting a horizontal force in the vertical direction.
 
  • #11
Careful da_willem, the Lorentz force includes the electric force, which definitely does do work in this case. However, under no circumstances does the magnetic force do work; by definition the magnetic force is always perpendicular to motion and hence does no work.
 
  • #12
Hootenanny said:
Careful da_willem, the Lorentz force includes the electric force, which definitely does do work in this case. However, under no circumstances does the magnetic force do work; by definition the magnetic force is always perpendicular to motion and hence does no work.

Sorry, I always, probably faulty, call only the magnetic part the 'Lorentz force'.
 
  • #13
da_willem said:
Sorry, I always, probably faulty, call only the magnetic part the 'Lorentz force'.
No problem, I just wanted to avoid confusion for the OP :smile:
 
  • #14
Doc Al said:
No loop, no changing magnetic field. (Perhaps my use of the term "induced" was a bit sloppy.) There are charge carriers--electrons--moving in the wire. The magnetic field deflects them to one side of the wire, creating a charge separation and thus an electric field.
I understand your explanation. But consider two positive charges q moving parallel to each other, each with speed v. Due to the magnetic field of the first charge, the second charge is attracted to it. What is the source of the work done on each of the charges, if it is not the magnetic field?
 
  • #15
lugita15 said:
I understand your explanation. But consider two positive charges q moving parallel to each other, each with speed v. Due to the magnetic field of the first charge, the second charge is attracted to it. What is the source of the work done on each of the charges, if it is not the magnetic field?
Indeed there will be a magnetic force, but there will also be an electric force. Are the charges going to move towards one another or away from one another? Consider the relative strengths of the electric and magnetic fields; http://academic.mu.edu/phys/matthysd/web004/l0220.htm. Can the magnetic force ever be greater than (or even equal to) the electric force? And recall the definition of work...:wink:
 
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  • #16
Parallel current attracts/antiparallel current repels...

Are you people sure that only Electric field in Lorentz force law expression takes the responsibility?

I am thinking of the source driving the current.
 
  • #17
This has been an interesting thread. I found it intuitively difficult to reconsile my experience of interaction between permanent magnets with the assertion that the magnetic field does no work. One question:

Does the magnetic field in the Stern-Gerlach experiment do work on an electron?
 
  • #18
neelakash said:
Parallel current attracts/antiparallel current repels...

Are you people sure that only Electric field in Lorentz force law expression takes the responsibility?

I am thinking of the source driving the current.

Which is an electric field...
 
  • #19
cesiumfrog said:
This has been an interesting thread. I found it intuitively difficult to reconsile my experience of interaction between permanent magnets with the assertion that the magnetic field does no work. One question:

Does the magnetic field in the Stern-Gerlach experiment do work on an electron?

Hmm, that's a very interesting question. Classically the energy of a magnetic dipole in an magnetic field is -\vec{m} \cdot \vec{B} so in an inhomogeneous magnetic field the force is given by

\vec{F}=\nabla (\vec{m} \cdot \vec{B})

The magnetic moment will move and it seems as though it is the magnetic field is responsible. But actually what I think will happen is that the current that produces the magnetic moment will decrease, or if it is sustained the force responsible does the work.

But now arises a problem, in case of a fundamental magnetic moment, spin, what happens? A particle carrying spin also has an energy -mB in a magnetic field. What force is now responsible for the work?

I think a that here we should change our language and no longer speak of a force, as there is no such thing in quantum mechanics. But still, what is responsible for the energy of a particle with spin in a magnetic field? I once saw a quantum mechanical derivation of this energy formula, I will look into it some further, it is indeed a very interesting subject...
 
  • #20
I am being more and more convinced about it.However,I am saying for a current carrying wire.You cannot blame me questioning about what is going to happen if we consider only two point charges...They constitute non-steady current ---nonsteady magnetic field and the force is a bizarre one...

Come to the problem.It's a fact that magnetic force attracts a wire towards another.Consider a moment when one wire is approaching another (horizontally) with speed u (w.r.t. my inertial frame).Let the current in this wire flow as usual with speed w (vertically).Now,EACH charge is moving as v= sqrt[w^2 +u^2] in my inertial frame.Magnetic force is not along horizontal.It tilts down.

The horizontal component is responsible for vertical motion of charges and only that...It can never influence any motion in the horizontal direction.Similarly,the downward force component is sustained by the horizontal movement of the wire.You also cannot say that this acts on the vertical motion of charges along the wire...Magnetic force never influence charges moving along its direction...

Then,who does the work?If you stop and think about it,you can see easily unless the battery would do work on the charges moving up the wire,the "attraction" what we see would not be there.Since the battery is out of the scene,it takes a time to conceive this.But note that if battery does this,you do not have to blame any unjust thing on any force (What about the electric force?That leads to repulsion!).All we need is to have a means to redirect the verical force of the battery into horizontal motion of the wire.The role of magnetic force is precisely this-simply to "redirect" the vertical force of the battery to horizontal motion of the wire.And this workdone is F_horizontal*dr.Since there is no apparently visible horizontal force apart from magnetic one,one may first think (wrongly) that magnetic force is doing the work...

How can I justify the concept of "redirecting"?I found it said by Griffiths in a similar example shown by him.He says that magnetic force redirects the efffort and leads to the physical reality.
 
  • #21
What is said by da_willem may be true...but that does not answer the actual question.
Let me be true to you.I did not understand how he got to the concept of magnetic dipole moment where we do not have a loop at all.
Since I do not know QM,I cannot say anything regarding this but this much I know that all sorts of magnetism do not arise out of QM.Only diamagnetism and ferromagnetism is a rigorous QM phenomenon.
 
  • #22
neelakash said:
What is said by da_willem may be true...but that does not answer the actual question.
Let me be true to you.I did not understand how he got to the concept of magnetic dipole moment where we do not have a loop at all.
Since I do not know QM,I cannot say anything regarding this but this much I know that all sorts of magnetism do not arise out of QM.Only diamagnetism and ferromagnetism is a rigorous QM phenomenon.

Elementary particles have a property called spin, which follows from relativistic quantum mechanics (Dirac equation). Spin, acts in the presence of a magnetic field in the same way a current loop would.
 
  • #23
neelakash said:
How can I justify the concept of "redirecting"?I found it said by Griffiths in a similar example shown by him.He says that magnetic force redirects the efffort and leads to the physical reality.

The electrons in the wire are deflected towards the other wire. They are however confined to the wire by electric forces (positive nuclei). What happens is that the entire wire moves towards the other wire, this movement however goes at the expense of the kinetic energy of the electrons. To maintain this energy the battery driving the electric current will have to do work to maintain the electron velocity and thereby the velcoity of the wire in total.
 
  • #24
That is good.So,everything OK?
 
  • #25
Hootenanny said:
Indeed there will be a magnetic force, but there will also be an electric force. Are the charges going to move towards one another or away from one another? Consider the relative strengths of the electric and magnetic fields; http://academic.mu.edu/phys/matthysd/web004/l0220.htm. Can the magnetic force ever be greater than (or even equal to) the electric force? And recall the definition of work...:wink:
The definition of work is integral of F.dr. If the magnetic force on an object is either parallel of antiparallel to the direction of motion, as it is in this case, there should be a nonzero work done by the magnetic force, and thus by the magnetic field. What is the explanation here?
 
  • #26
magnetic forces never do work.
 
  • #27
lugita15 said:
The definition of work is integral of F.dr. If the magnetic force on an object is either parallel of antiparallel to the direction of motion, as it is in this case, there should be a nonzero work done by the magnetic force, and thus by the magnetic field. What is the explanation here?

The equally charged particles will be repulsed by the electric force, which does the work that supplies this kinetic energy. This can most easily be seen in an inertial frame moving along with the particles, where the situation is the extremely simple one of two equally charged particles repulsing each other by the normal Coulomb force.

When you switch to the 'nonmoving' frame, relative to which the particles move with a certain velocity a magnetic field 'arises' in our description. Note that for velocities smaller than c, this attraction force is always smaller than the electric repulsion force.

In this stationary frame the repulsion force is thus diminished by the magnetic field, but should ofcourse yield the same acceleration. I think this has something to do with time dilation, if anyone knows I'm quite interested.
 
  • #28
Originally Posted by lugita15
The definition of work is integral of F.dr. If the magnetic force on an object is either parallel of antiparallel to the direction of motion, as it is in this case, there should be a nonzero work done by the magnetic force, and thus by the magnetic field. What is the explanation here?

F_mag=q(vxB)
and F.dl=q(vxB).(v dt)
 
  • #29
I didn't have time to read past the first few threads but I think that the answer is obvious:
Let's say that one wire has a current going through it and the other one doesn't, in this case there will be no force. Only when the current is switched on in the second wire do they move towards each other. This means that the source of the work is whatever is "pumping" the electrons around in the wires. Since that wasn't very clear I'll explain a different way:
Lets say we have a satellite orbiting around Earth, it's spinning around and around but the only force acting on it is gravity which is perpendicular to the motion so it isn't doing any work! How can that be? Well in this case the easy answer is that since the satellite's energy stays constant throughout the orbit no work has to be done on it by Earth.
The same thing applies here. In order to find the source of the work done on the wires we have to look at the energy source of the system; who looses energy by the force moving the wires? The source of the current (batteries..) of course.
Am I missing something?
 
  • #30
Good!That is a direct proof that the battery does the work.
Here the wire gains a sidewise motion that calls for a KE.This is suppiled by the battery.

I do not understand the relevance of the analogy of the planetary motion.
 

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