RedX
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Drakkith said:Also, is that even accurate to what's really happening? For example, if one applied a positive voltage to one end of a wire, and a negative voltage to the other, the wire would develop an imbalance of charges on each end with a greater difference between the ends and a gradual fall off towards the middle correct?
This is correct, but for DC current, the difference between the imbalance at the ends and the imbalance at the middles will approach zero.
See this picture, figure 4-4 (c):
http://www.tpub.com/neets/book10/42.htm
In this picture you see a dramatic difference between the charge imbalance at the ends and the imbalance between the middles, but that is because the length of the wires are comparable to the wavelength of the frequency (the picture is of your typical center-fed half-wave antenna).
The difference in DC is less dramatic, and you'll just get something like a step function for your charge distribution.
addendum:
Note that saying the two wires are capacitors is perfectly reasonable. It's an unintended capacitance, which is why it's sometimes called parasitic capacitance. When studying transmission lines you usually give the wires a capacitance per unit length. In this case, the charge distribution on the wire follows the voltage distribution, since Q is proportional to V, i.e., Q=CV. Check out figure 3-20 here:
http://www.tpub.com/neets/book10/41f.htm
You can understand the physics of a real circuit using lumped elements: the capacitor represents the charges on the wire, and the inductance represents the magnetic fields of the wires. This is one of the reasons I believe that the Poynting view is not critical. The reason the voltage propagates slower if there is a dielectric is because it takes longer to fill each capacitor since the capacitance increases. Of course the Poynting view is correct and more aesthetically pleasing in my opinion, but for actual calculations, it's not necessary one has the Poynting view in mind.
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