- #1
greypilgrim
- 548
- 38
Hi.
The derivation of the capacity of an ideal parallel-plate capacitor is inconsistent: On the one hand, the plates are assumed to be infinitely large to exploit symmetries to compute an expression for the electric field, on the other the area is finite to get a finite expression for the charge. Usually this is justified by the fact that the boundary only increases with the square root of the area and hence boundary effects can be neglected.
However, this can be tricky: An ideal, finite capacitor doesn't even agree with Maxwell's equation since the line integral of the electric field from one plate to the other is path-dependent (##E\cdot d## for paths between the plates, zero for paths outside). When it comes to voltage or work, boundary effects clearly cannot be neglected.
How can this subject be treated more rigorously than just what seems to me to pick and choose when to neglect boundary effects and when not to?
The derivation of the capacity of an ideal parallel-plate capacitor is inconsistent: On the one hand, the plates are assumed to be infinitely large to exploit symmetries to compute an expression for the electric field, on the other the area is finite to get a finite expression for the charge. Usually this is justified by the fact that the boundary only increases with the square root of the area and hence boundary effects can be neglected.
However, this can be tricky: An ideal, finite capacitor doesn't even agree with Maxwell's equation since the line integral of the electric field from one plate to the other is path-dependent (##E\cdot d## for paths between the plates, zero for paths outside). When it comes to voltage or work, boundary effects clearly cannot be neglected.
How can this subject be treated more rigorously than just what seems to me to pick and choose when to neglect boundary effects and when not to?