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Displacement currents play a central role in the propagation of electromagnetic radiation, such as light and radio waves, through empty space.
In particular for low-frequencies where the displacement currents are often disregarded [13, 14].
We can reasonably invoke the quasistatic approximation and neglect displacement currents in Maxwell's equations.
Using radio wave frequencies for testing, the effect of displacement currents cannot be neglected anymore.
Our formulation of Maxwell's equations discards displacement currents, which are negligible in the frequency range considered here.
Electric source impressed upon at its edges produces alternating electric and magnetic fields causing eddy as well as displacement currents to flow through the surrounding materials.
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Alternating current will pass readily, however, and is called a displacement current.
Displacement current, in electromagnetism, a phenomenon analogous to an ordinary electric current, posited to explain magnetic fields that are produced by changing electric fields.
Maxwell's insight on displacement current, therefore, made it possible to understand electromagnetic waves as being propagated through space completely detached from electric currents in conductors.
He found that the model gave rise to a corresponding "displacement current" in the dielectric medium, which could then be the seat of transverse waves.
Maxwell gave it the name displacement current, which was proportional to the rate of change of the electric field that kept cropping up naturally in his theoretical formulations.
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