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30.9 : Displacement Current

Ampère's law, in its usual form, does not work in places where the current changes with time and is not steady. Thus, Maxwell suggested including an additional contribution, called the displacement current, Id, to the real conduction current I.

Ampère's Law equation, ∮B·dℓ=μ₀I_enc+μ₀I_denc, integral form, electromagnetic theory.

where the displacement current is defined to be

Maxwell's displacement current equation; Id=ε0(dΦE/dt); theoretical electromagnetic analysis.

Here, εis the permittivity of free space, and ΦE is the electric flux.

The displacement current is an extra term in Maxwell's equations that is analogous to a real current in Ampère's law. However, it is produced by a changing electric field. It accounts for a changing electric field producing a magnetic field, just as a real current does, but the displacement current can produce a magnetic field even when no real current is present. When this extra term is included, the modified Ampère's law equation becomes

Ampère-Maxwell law equation, ∮B·dl=μ₀I_enc+ε₀μ₀dΦ_E/dt, illustrating electromagnetism.

In this way, Ampère's law can be modified so that it works in all situations, and it is independent of the surface through which the current I is measured.

Tags

Displacement CurrentAmp re s LawMaxwell s EquationsChanging Electric FieldMagnetic FieldPermittivity Of Free SpaceElectric FluxModified Amp re s LawReal Conduction CurrentTime varying Current

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30.9 : Displacement Current

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