Jeff Rosenbury
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Gerry Rzeppa said:Yeah, I'm not buying that one. Looking around in books and on the web the consensus appears to be that the dielectric constant for conductors is infinity. Here, for example, is a clip from a book called, Comprehensive Physics:
You are looking at the case of a perfect electric conductor (PEC) like a superconductor. In a PEC there is no electric field. The entire field is canceled by eddy currents since there is no resistance. Yet in normal metals there is some limited resistance. That resistance slows eddy currents and allows a field to form. So the logic of "No field, no ε" doesn't hold.
Gerry Rzeppa said:And here's a similar argument from a paper on the web (bold highlight mine):
"In E&M, we learned the famous formula for dielectric materials: D(r) = ε E(r). D is the electrical displacement, which is related to the electric field caused by the free moving charge (the externally added charge). E is the electric field caused by the total charge, which includes the free moving and the bound charge (the internally induced charge). ε is the dielectric constant, also called permittivity, which relates the D to E. ε is infinite for metals in the limit where the applied field is spatially uniform. In this case, the electrons inside the metal are free to arrange themselves until their own electric field exactly counters the externally applied field D. Thus, the total field E becomes 0."
From above: "in the limit where the applied field is spatially uniform". Your applied field is not uniform. You have somewhat artificially set up a case where the underlying assumptions don't apply. Now you are using arguments based on those assumptions.
Capacitance is a defined quantity. It is defined as the charge divided by the voltage. You are arguing that this isn't the case. Well there's nothing wrong with that argument. As Lewis Carol wrote: "'When I use a word,' Humpty Dumpty said in a rather scornful tone, 'it means just what I choose it to mean -- neither more nor less.'" But don't expect others to agree with you or even understand you.
The answer to why a smaller circuit requires more electrons is because the electric field falls off with distance. Remember those electrons have paired protons somewhere. When the proton is near, it partially cancels the effects of the electron. When it's far, not so much.
You are correct that the capacitive approach may not be the best to solve this problem. I feel the lack of reliable ε measurements for metals make it problematic. Experimental data should be obtained. The test set up I envision would want a PEC to count the electrons across the small (differentialish) elements. Also, the value of ε might depend on the geometry (and temperature). (Remember ε is also a defined value. It relates the electric displacement with the electric field -- very similar to capacitance. There is no requirement that the number be a simple real value.)
For what it's worth, this would make a great science project/thesis (if it hasn't been done yet).