What is the origin of displacement current?
Origin of Displacement Current
Displacement current was first proposed by James Clerk Maxwell in 1861, as a necessary addition to Ampere's law in order to maintain consistency with the conservation of charge and to explain the behavior of electromagnetic waves.
Explanation
Displacement current arises from the changing electric field in a region of space, and is represented by the term ε(dE/dt) in Ampere's law, where ε is the permittivity of the medium and dE/dt is the rate of change of the electric field. This term accounts for the flow of electric charge that is not carried by the movement of electrons, but rather by the changing electric field itself.
Significance
The concept of displacement current is important in the study of electromagnetic waves, which are composed of oscillating electric and magnetic fields that propagate through space. These waves can only exist if the electric field is able to change over time, which creates a displacement current that generates a magnetic field. This magnetic field in turn creates an electric field, and the cycle repeats itself, resulting in the propagation of the electromagnetic wave.
Conclusion
In conclusion, displacement current is a fundamental concept in the study of electromagnetism, and is necessary to explain the behavior of electromagnetic waves. It arises from the changing electric field in a region of space, and is represented by a term in Ampere's law. The concept of displacement current has many practical applications, including in the design of antennas, microwave circuits, and other electronic devices.
What is the origin of displacement current?
According to Faraday's law of electromagnetic induction, a time varying magnetic field produces an induced EMF. According to Maxwell, a time varying electric field sets up a current and hence a magnetic field. Such a current is called displacement current. It follows that a time varying electric field produces a magnetic field and vice -versa. Hence the behaviours of electric and magnetic fields are symmetrical.