A parallel plate capacitor made of circular plates is being charged such that the surface charge density on its plates is increasing at a constant rate with time. The magnetic field arising due to displacement current is:
- A
zero at all places
- B
constant between the plates and zero outside the plates
- C
non-zero everywhere with maximum at the imaginary cylindrical surface connecting peripheries of the plates
- D
zero between the plates and non-zero outside
Displacement current density: . Since , we get , which is constant in time and uniformly distributed across the area between the plates.
Applying Ampere–Maxwell law on circular loops of radius between the plates: for $r < R$ (plate radius), the enclosed displacement current grows as $r^2$, giving $B\propto r$. For $r > RB\propto 1/r$.
So is non-zero both inside and outside the imaginary cylinder, peaking exactly at — the cylindrical surface connecting the plate edges.
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