A paradox about Drift Velocity

In summary, the conversation discusses the concept of drift speed, which is the speed at which electrons move in a circuit. Despite having a low drift velocity, the current in a circuit can move at close to the speed of light due to the near-instantaneous response of electrons to changes in the electric field. Analogies, such as the sweets in a tube or pushing a pencil, are used to explain this concept, but it is important to understand that these analogies have their limitations.
  • #36
To get an approximate idea of the order of drift velocity without much math,

charge of electron is roughly 10^-19C, so a one amp current in a wire corresponds to an exchange of 10^19 electrons per second, since these are the charge carriers.

A piece of matter that you hold in your hand has roughly 10^23 atoms, (via avogradro).

so you figure you have roughly 10^23 valence electrons (via atoms), but you only need to move 10^19 of them every second.

So they must move on average 10^-4 m/s.

Quick approximation, you'll do better by knowing the current, current density, & concentration of valance electrons.Specifically, the drift velocity doesn't mean that's how fast the signal propagates. If I move an electron on one side of the wire, that coulomb field (disturbance) propagates at the speed of light. In practice the electron at one end of a wire never reaches the other end (according to this classical drift velocity idea), it would take an awfully long time. However the signal particularly in Ac propagates at "near" (see last line) the speed of light.

Even with :slowed: light in a medium, the light still travels at C, its just the light gets absorbed and re -emitted and this takes a certain amount of time which delays the light.

the light however always travels at C, but we speak of the speed of the light in the medium to include these absorption and emission times.

Another thing to keep in mind, the coulomb disturbance mentioned above is mediated by light itself, so it will feel the effects of the delay time, all relative to permittivity and permeability.
 
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  • #37
Per Oni said:
Just reading some wiki pages I found this: http://en.wikipedia.org/wiki/Poynting_vector:

So it looks like there’s still some controversy.

There’s another aspect of electrical conduction theory I like to mention, namely: energy leaves the source at near light speed towards the surrounding dielectric. Therefore it follows that the source should receive a kickback in the opposite direction. Has anyone ever seen a paper dealing with that fact, or anyone any thoughts?

But a so-called "DC current" is not time-invariant. At the molecular level the electrons are making short hops as they jump from place to place. There is a constant exchange of convection current, where the electrons carry the current, and displacement current where the "medium" carries the current or energy.
 
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  • #38
Repainted said:
The electrons themselves move at a low average drift velocity, but the current in the wire moves at close to the speed of light.
This is incorrect. The current is nothing but the flow of electrons, and is in fact quite directly related to the drift velocity. It is the electric field that propagates along the wire at the speed of light.

Matterwave said:
Imagine electrons traveling in a circuit like when I push a very long pencil. I push on one side of the pencil, and the other side moves (almost instantaneously)! The current, then, is not determined by how fast I can push the pencil, but by how much of the pencil moves past a certain point within a certain amount of time.

All of the electrons within the wire start moving almost instantly after the circuit is switched on. This is very much like how all of my pencil starts moving almost instantly after I push it.

DrMik said:
Imagine a cardboard tube full of sweets. If you push in another sweet at one end another drops out of the opposite end, no matter how long the tube is. That shows that the sweet put in only travels a couple of millimetres yet its action can be seen instantly at the other end of the tube which could be a metre away! How is that?
I hate these analogies, not because they miss little details about propagation speeds and "instantaneous" effects, but because they fundamentally mislead in terms of explaining the effect. One would gather from these analogies, that the current is driven primarily by electron-electron interactions (or collisions), but that couldn't be further from the truth. The current is generated as a response of all* the free electrons in the wire to the applied field, and any analogy ought to make some attempt at conveying that basic idea.

It is the fault of this poor shock-wave analogy that, I believe, leads to statements about current traveling at close to c. Or statements like the following, extracted from above: "The current, then, is not determined by how fast I can push the pencil, but by how much of the pencil moves past a certain point within a certain amount of time." How fast I can push a pencil is exactly the same thing as how much of the pencil moves past a fixed point over some time - that is essentially the definition of "fast" (or speed). But by restricting oneself to the failing analogy, one has to use rather weird definitions.

A better analogy might be holding a string of beads by one end and letting go. All the beads travel downwards in response to the same external field (gravitational, in this case), but occasionally feel weak tugs from other beads (electron-electron interactions) and from the air around them (electron-phonon and electron-impurity interactions).

*Ignoring Fermi distributions - I'm using "all" to mean throughout the length of the wire.
 
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  • #39
Gokul43201 said:
A better analogy might be holding a string of beads by one end and letting go. All the beads travel downwards in response to the same external field (gravitational, in this case), but occasionally feel weak tugs from other beads (electron-electron interactions) and from the air around them (electron-phonon and electron-impurity interactions).
Yes, yes, that's a much better analogy, thanks. I think it still misses slightly in that, unlike a gravitation field and beads, the availability of the conduction band electrons influence the degree to which the EM field propagates (though having ~no influence on the speed of the EM). Sound right?
 
  • #40
Yes, it misses what I think are (relatively) smaller details (like the dielectric function that you mention), but that's inevitable with any analogy. Still, I like it a lot better than the analogy using the pencil (or the horizontal line of balls/sweets) which serves little or no pedagogical value, and IMO, is more likely to propagate misconceptions than clarify them.
 

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