Considering the case of a parallel plate capacitor being charged, show how one is required to generalize Ampere's circuital law to include the term due to displacement current.
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Using Gauss’ law, the electric flux ΦE of a parallel plate capacitor having an area A, and a total charge Q is Where electric field is As the charge Q on the capacitor plates changes with time, so current is given by i = dQ/dt This is the missing term in Ampere’s circuital law. So the total current through the conductor is
i = Conduction current (ic) + Displacement current (id) As Ampere’s circuital law is given by After modification we have Ampere−Maxwell law is given as The total current passing through any surface, of which the closed loop is the perimeter, is the sum of the conduction and displacement current.
i = Conduction current (ic) + Displacement current (id) As Ampere’s circuital law is given by After modification we have Ampere−Maxwell law is given as The total current passing through any surface, of which the closed loop is the perimeter, is the sum of the conduction and displacement current.
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The space between the capacitor consists of an insulator. Hence, no actual transfer of charge occurs in this region. Current flows in the circuit during the charging of a capacitor. This demands the need of the presence of a displacement current in the capacitor resulting in a magnetic field.
∫B.dl=μo I
Here I is the sum of conduction and displacement currents.
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