Why does a resistive wire heat up from current flow?

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Discussion Overview

The discussion centers around the phenomenon of resistive heating in wires due to current flow, exploring the underlying mechanisms and energy transformations involved. Participants examine the relationship between electron kinetic energy, electric fields, and thermal energy within conductors, touching on theoretical models and analogies.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants note that the kinetic energy from the drift velocity of electrons is insufficient to explain the heating, questioning the source of heat energy.
  • Others argue that the energy carried by electric fields, as described by Poynting's Theorem, is a crucial factor in understanding resistive heating.
  • A participant suggests that while electric energy is carried outside the conductor, resistive heating occurs within it due to collisions between electrons and atomic cores.
  • One participant introduces the idea that a significant friction force must exist for the electron-gas to lose kinetic energy rapidly, contributing to heating.
  • Another participant discusses the mechanical analogy of fluid dynamics to explain energy loss in electrical systems, emphasizing the role of resistance in opposing electron motion.
  • Concerns are raised about the oversimplification of concepts in educational contexts, with a participant reflecting on their own learning experience and the inadequacy of high school explanations.

Areas of Agreement / Disagreement

Participants express a range of views on the mechanisms of resistive heating, with no consensus reached on the primary factors involved. Multiple competing explanations and analogies are presented, indicating an ongoing debate.

Contextual Notes

Some discussions highlight the limitations of high school physics education in conveying complex concepts related to electricity and resistance, suggesting a need for deeper exploration of the topic.

Who May Find This Useful

This discussion may be of interest to students and educators in physics, as well as individuals seeking a deeper understanding of electrical conduction and resistive heating mechanisms.

cosmik debris
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The kinetic energy of electrons in a conductor is roughly 9 orders of magnitude greater than the kinetic energy from the drift velocity of the electrons. It seems that the kinetic energy from the drift velocity is not enough to account for the heating, where does the heat energy come from?

Cheers
 
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Charged particles create fields. The fields of each particle interact with all the other charged particles simultaneously. That makes them behave very differently than uncharged particles. The energy of an electric current is carried in the fields. See Poynting's Theorem. Therefore you should not equate mechanical kinetic and potential energies with electric energy; they are very different.

If you are really interested in the fine details of conduction and resistance and electric energy read these articles
https://en.wikipedia.org/wiki/Drude_model
https://en.wikipedia.org/wiki/Poynting's_theorem.
 
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cosmik debris said:
It seems that the kinetic energy from the drift velocity is not enough to account for the heating, where does the heat energy come from?
Yes the KE is largely irrelevant. The energy comes from the fields. This is what Poynting’s theorem describes

In an analogy, although a bicycle chain is moving, the KE in the chain is largely irrelevant to the amount of energy transferred along the chain.
 
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On second thought, it is a bit more nuanced. While electric energy is carried outside the conductor (Poynting Vector), resistive heating losses occur within the conductor.

A pop sci type of explanation comes from this image from The Drude Model Wikipedia article. As electrons accelerate in the field and collide with atoms from all directions, they convey thermal energy to the atoms.

Electrona_in_crystallo_fluentia.svg
 
cosmik debris said:
The kinetic energy of electrons in a conductor is roughly 9 orders of magnitude greater than the kinetic energy from the drift velocity of the electrons. It seems that the kinetic energy from the drift velocity is not enough to account for the heating, where does the heat energy come from?

Cheers

Well, if the electron-gas has a very small amount of kinetic energy, then it must lose that kinetic energy very quickly, in order to provide a significant amount of heating energy. So there must be a large friction force.

Now as we know that the electron-gas does not stop despite of the huge friction, we conclude that there is a large force F pushing the electron-gas.

Heating power = drift velocity * F
or:
Heating power = drift velocity * friction force
 
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jartsa said:
it must lose that kinetic energy very quickly,
A 'mechanical' reason for losing KE and never gaining much is the interaction of the electrons with the positive ion cores of the conductor.
If you allow electrons and unobstructed path through a vacuum, they gain loads of KE. In fact each electron gains eV Joules and electrons can easily reach speeds where Special Relativity starts to have an effect. A beam of electrons can be considered as having a Resistance which is equal to the PD / the beam current
 
cosmik debris said:
The kinetic energy of electrons in a conductor is roughly 9 orders of magnitude greater than the kinetic energy from the drift velocity of the electrons. It seems that the kinetic energy from the drift velocity is not enough to account for the heating, where does the heat energy come from?
Even if you could compare this to fluids where the energy was mechanical and not electrical, it still wouldn't be kinetic energy that is lost. Conservation of mass (continuity) demands that the velocity and therefore kinetic energy of a fluid in a pipe be constant, since otherwise mass would have to be lost somewhere. A fluid in a pipe works similar to sliding a block across the floor: the loss is work due to friction; simple force times distance in the case of the block.

Switching back to electricity, the principle is basically the same. You have a resistance to the motion of the electrons that applies a force against their motion. The nuts and bolts of what causes the force is different in the three cases, so the loss is a different function of flow rate for each (linear, square and cube function), but the idea is otherwise similar.

So maybe the next question is on a nuts and bolts level what causes resistance? Googling (or reading @anorlunda's post) gives me high school class notes that talk about electrons bouncing off of ions when traveling through the matrix, but that feels overly mechanical to me (even if it is electromagnetic "bouncing"). Maybe someone else can provide a deeper dive if indeed there is more to it...
 
russ_watters said:
high school class notes
I think that says it all. What a high school teacher / textbook tells a student about something as sophisticated at this topic is guaranteed to be far too simple.
I am so pleased that, when I was at School, they rapped our knuckles if we asked for the 'electron' description of electricity. It was not until my first year at Uni, in a solid state Physics intro course that the transfer of energy by electrons was actually presented to us. (decades later) The utter nonsense that my teacher friends were expected to teach about 'Modern Physics' to kids at school (up to 16 years) was positively embarrassing. It made it all far too simple.
 
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thanks for all your answers, I should have remembered the Drude model.

Cheers
 

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