Energy transfer in electromagnetic induction

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Discussion Overview

The discussion revolves around the concept of energy transfer in electromagnetic induction, specifically focusing on the interaction between a moving magnet and a coil. Participants explore the timing of induced currents and the resulting forces experienced by the magnet, considering both theoretical implications and practical scenarios.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants propose that the magnet experiences resistance to its motion only after a delay of time 2t, where t is the time taken for light to travel from the magnet to the coil and back.
  • Others argue that the magnetic field around the magnet exists continuously, and as the magnet approaches the coil, the induced current begins to flow immediately upon encountering the field lines.
  • A participant questions when the change in magnetic flux starts to increase, suggesting that there must be a delay before the coil feels the effect of the changing magnetic field.
  • Some contributions reference Feynman's studies on field interactions, indicating that the reaction force experienced by the magnet may not necessarily involve a delay, depending on the nature of the interaction.
  • There is a discussion about the implications of the speed of light as a limit for information transmission, with some participants suggesting that the magnet may feel the reaction force immediately after it is nudged, despite the time taken for the induced current to develop.

Areas of Agreement / Disagreement

Participants express differing views on whether the magnet experiences resistance immediately or after a delay. There is no consensus on the timing of the induced current's effect on the magnet's motion, with multiple competing perspectives remaining unresolved.

Contextual Notes

Participants highlight the complexity of the interaction between the magnet and the coil, noting that assumptions about the instantaneous nature of the magnetic field and the timing of induced currents may not hold under scrutiny. The discussion also touches on the implications of causality and the limits imposed by the speed of light.

Who May Find This Useful

This discussion may be of interest to those studying electromagnetic induction, physics students exploring concepts of energy transfer, and individuals curious about the theoretical implications of field interactions in electromagnetism.

  • #61
entropy15 said:
The energy in the radiation should be coming from the source driving the electromagnet.
Assume that the electromagnet is powered by a power source - a battery or a charged capacitor.
The energy in the radiation also comes from the KE of the source. When a capacitor is discharged to power the magnet then by E=mc² that capacitor has less mass. So in a frame where it is moving it also has less KE. So not only is the electrical potential energy in the capacitor decreased, but also the KE of the capacitor is decreased. That additional energy goes into the radiation.*

Note that this is a very small effect for ordinary speeds. It is only significant at large fractions of c.

*this explanation is a little sloppy, a better explanation would be in terms of the four-momentum. If you are interested, please open a new thread in the relativity sub-forum.
 
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  • #62
DaleSpam said:
Note that this is a very small effect for ordinary speeds. It is only significant at large fractions of c.

So for smaller velocities (compared to c) there should be no noticeable increase in the amount of energy being emitted by the electromagnet whether it is stationary or moving.

So assume that the velocity of the electromagnet involved in the experiment I mentioned earlier (post 56) is small compared to c.
But it is moving so as to cause a significant change in the flux linking the coil. Then how do we we explain it?
 
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  • #63
Doppler. The total energy is not significantly affected for v<<c, but it is still concentrated in the forward direction. As I said in 59 above, the total energy is not terribly important in this scenario, only the energy at the loop.
 
  • #64
DaleSpam said:
Doppler. The total energy is not significantly affected for v<<c, but it is still concentrated in the forward direction. As I said in 59 above, the total energy is not terribly important in this scenario, only the energy at the loop.

What if we increase the number of turns in the coil? Would that not mean the coil acquiring more energy?
 
  • #65
entropy15 said:
What if we increase the number of turns in the coil? Would that not mean the coil acquiring more energy?
What do you think? Try to reason this from what you know of Maxwell's equations, especially the fact that energy is conserved in them and the fact that they are linear (superposition).
 
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  • #66
DaleSpam said:
What do you think? Try to reason this from what you know of Maxwell's equations, especially the fact that energy is conserved in them and the fact that they are linear (superposition).

Sorry I am unable to think of any reason here. Could you please explain
 
  • #67
Superposition means that if you have two sources then the total field is the sum of the field from each of the two individual sources. Think how that might apply to increasing the number of turns.
 
  • #68
DaleSpam said:
Superposition means that if you have two sources then the total field is the sum of the field from each of the two individual sources. Think how that might apply to increasing the number of turns..

I was referring to the turns in the absorbing coil placed at a distance x from the electromagnet.
 
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  • #69
Me too. Think about the field generated by the induced current in the first turn. How does that affect the total field seen by the second turn.
 
  • #70
DaleSpam said:
Doppler. The total energy is not significantly affected for v<<c, but it is still concentrated in the forward direction. As I said in 59 above, the total energy is not terribly important in this scenario, only the energy at the loop.

The point I was trying to make was that the initail energy due to the current induced in the coil is entirely due to the electromagnetic wave.
The kinetic energy of the electromagnet cannot contribute to the induced current, as it does not decrease initailly.

Lets consider the time interval between x/c and when the coil begins to feel resistance due to mutaul induction. It will be less than 2x/c since the electromagnet is moving towards the coil.
The energy due to the current in the coil during this time cannot be greater than the energy in the electromagnetic wave intially radiated.

But if we increase the value of v, the energy in the coil increases because of a larger change in flux. But there is no noticeable increase in the radiation energy. (v<<c)

If we consider the frame of the moving electromagnet there is no Doppler effect.
All the electromagnet sees is the coil moving towards it.
Here again we can see that the energy in the coil (between x/c and 2x/c) increases with increase in the relative velocity.
 
  • #71
But there is no noticeable increase in the radiation energy. (v<<c)

If the electromagnet radiates isotropically in its frame (if it has symmetric shape), the energy radiated into all directions per unit time is Lorentz invariant; it is the same in all frames. Let's say the electromagnet radiated 1 J in one second, in its own frame of reference.

What is important, is that in the frame of the coil, the electromagnet is moving towards it. When a source of isotropic radiation moves in some direction, the radiation is released preferentially to that direction. Check

https://en.wikipedia.org/wiki/Synchrotron_radiation

The bunches of charged particles circling in synchrotron move so fast that the radiation is needle-like, similar to laser, only much brighter and not monochromatic.

With the electromagnet, it is similar; even if it moves slowly, there is more radiation going to the coil than in the other directions.

As the velocity is increased, coil receives greater and greater power. However, there is a limit: when v approaches c, the coil receives almost all the radiated power 1 J/s and this is the maximum. Of course, as the processes in the source are slowed down (dilatation) , it will receive it for a long time and thus the net amount of energy received in the end can be much greater than 1 J.

Where did the extra energy came from? From the total energy of the electromagnet; as the net energy of the electromagnet decreases by radiation, in the frame of the coil the electromagnet loses also momentum via loss of its mas (the velocity is unaffected).
 
  • #72
entropy15 said:
The point I was trying to make was that the initail energy due to the current induced in the coil is entirely due to the electromagnetic wave.
The kinetic energy of the electromagnet cannot contribute to the induced current, as it does not decrease initailly.
The EM wave is what carries the KE away. The KE of the magnet does decrease as soon as the electromagnet radiates. Remember, the KE decreases due to the loss of mass from radiating energy, even if the velocity remains constant.

entropy15 said:
Lets consider the time interval between x/c and when the coil begins to feel resistance due to mutaul induction. It will be less than 2x/c since the electromagnet is moving towards the coil.
The energy due to the current in the coil during this time cannot be greater than the energy in the electromagnetic wave intially radiated.
Yes, that is not in doubt at all. The point is that the energy in the EM wave depends on the reference frame. In reference frames where the magnet was initially moving the energy in the EM wave is greater than in the frame where it was stationary. Energy is frame variant.

entropy15 said:
But if we increase the value of v, the energy in the coil increases because of a larger change in flux. But there is no noticeable increase in the radiation energy. (v<<c)
No noticeable increase in the TOTAL radiation energy, but there is a noticeable increase in the energy through the coil. Doppler.

entropy15 said:
If we consider the frame of the moving electromagnet there is no Doppler effect.
This is incorrect, the Doppler effect depends only on the relative velocity. In any frame there is the exact same amount of Doppler effect. In the magnet's frame, of course, the Doppler effect is due entirely to the movement of the loop.

entropy15 said:
All the electromagnet sees is the coil moving towards it.
Here again we can see that the energy in the coil (between x/c and 2x/c) increases with increase in the relative velocity.
Doppler.
 
  • #73
Jano L. said:
As the velocity is increased, coil receives greater and greater power. However, there is a limit: when v approaches c, the coil receives almost all the radiated power 1 J/s and this is the maximum..

You mean to say that there is limit to the energy that can be transferred to the coil between the interval x/c and 2x/c.

Can we not increase the energy transferred initially by increasing the number of turns in the coil. More turns mean more current flowing in the coil.
 
  • #74
This goes back to the point before. I think DaleSpam's answer was: "Think about the field generated by the induced current in the first turn. How does that affect the total field seen by the second turn. My hint is that the equation:
\displaystyle{\varepsilon}=-N \frac{d \Phi}{dt}
Uses a lot of assumptions, and if you break those assumptions, you cannot expect the equation to give correct results.

Edit: actually, it doesn't use a lot of assumptions, but the simple case of increasing number of turns to increase the current through the coil does introduce assumptions.

Another Edit: and generally, it is assumptions used along with this equation that have caused the problems in this thread. For example, the assumption "that the magnetic field at the magnet and at the coil is approximately the same" is often used with this equation, but this assumption becomes false when the magnet and coil are far away from each other.
 
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  • #75
entropy15 said:
You mean to say that there is limit to the energy that can be transferred to the coil between the interval x/c and 2x/c.

Can we not increase the energy transferred initially by increasing the number of turns in the coil.
In addition to BruceW's point above, I would like to point out that the two statements are not mutually exclusive. Specifically, it is possible that the statements "there is a limit to the energy that can be transferred" and "we can increase the energy transferred by increasing the number of turns" can both be true.
 
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  • #76
DaleSpam said:
In addition to BruceW's point above, I would like to point out that the two statements are not mutually exclusive. Specifically, it is possible that the statements "there is a limit to the energy that can be transferred" and "we can increase the energy transferred by increasing the number of turns" can both be true.

How is that possible?
 
  • #77
entropy15 said:
How is that possible?
Like this (ignore the scale and units of the vertical axis, this is just to give a general idea of the concept of a monotonically increasing function with a horizontal asymptote)
1-s2.0-S0022509608001993-gr8.jpg

If each dot represents the energy extracted by a coil with i turns then it is both true that "there is a limit to the energy that can be transferred" and "we can increase the energy transferred by increasing the number of turns".
 
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  • #78
DaleSpam said:
Like this (ignore the scale and units of the vertical axis, this is just to give a general idea of the concept of a monotonically increasing function with a horizontal asymptote)

Thanks for clarifying. This seems to indicate that the amount of energy transferred converges to a fixed value as N (no. of turns) tends to infinity.

Is this because the successive turns in the coil are linked to lesser magnetic flux?
 
  • #79
Yes, it is because each turn reduces the flux seen by the other turns. This can be seen through the superposition principle.

Suppose that you have two turns, consider them to be two separate loops. There is a current in loop A which creates a field which opposes the change in the external field. By superposition the field seen by loop B is the sum of the field from loop A and the external field, which is less than the change in the external field. So the current induced in B is a function of the external field and the current induced in A where current in A reduces the induced current in B.

Then, to consider the loops as separate turns in a single coil simply equate the current in A to the current in B.
 
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