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Courant de déplacement
La loi d'Ampère, dans sa forme habituelle, ne fonctionne pas dans les endroits où le courant change avec le temps et n'est pas constant. Ainsi, Maxwel…
Ampere's law states that the line integral of a magnetic field along a closed curve equals the permeability of free space times the net current passing through the loop.
Consider a parallel plate capacitor connected with a battery in a charging condition.
Applying Ampere's law to the shown Amperian loop with two surfaces gives two different magnetic field values, which is impossible.
As the capacitor is charging, the electric field, and hence the electric flux, increases through the bulging surface. The value of electric flux can be obtained in terms of the charge.
In 1865, James Clerk Maxwell, predicted that due to this time-varying electric field, a non-zero magnetic field is produced between the plates of the capacitor through a fictitious current called displacement current.
The expression for displacement current is given in terms of electric flux.
Thus, Ampere's law is modified with the inclusion of an additional term for displacement current. It is known as the Ampere-Maxwell law or generalized Ampere's law.
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Q1: Why does Ampere's law fail for a charging capacitor?
Ampere's law produces inconsistent magnetic field values when applied to different surfaces of an Amperian loop around a charging capacitor because current does not pass through all surfaces equally. The law assumes steady current, but a capacitor's charging creates a time-varying electric field that Ampere's law in its original form cannot account for, revealing a fundamental limitation in the classical formulation.
Q2: What is displacement current and how is it defined?
Displacement current is a fictitious current introduced by Maxwell to account for changing electric fields. It is defined as the product of the permittivity of free space and the time rate of change of electric flux through a surface. Unlike real conduction current, displacement current produces a magnetic field even when no actual charge movement occurs, enabling Ampere's law to work in all situations.
Q3: How does the electric flux change during capacitor charging?
As a capacitor charges, the electric field between its plates increases, causing the electric flux through the bulging surface of an Amperian loop to increase with time. The value of electric flux can be expressed in terms of the charge accumulating on the capacitor plates, directly linking the time-varying charge to the changing electromagnetic field.
Q4: What is the Ampere-Maxwell law and how does it modify Ampere's law?
The Ampere-Maxwell law, also called the generalized Ampere's law, modifies the original Ampere's law by adding a displacement current term to the real conduction current. This modification ensures the law works independently of the surface chosen for measurement and accounts for magnetic fields produced by changing electric fields, making it valid in all electromagnetic situations.
Q5: Why did Maxwell introduce displacement current in 1865?
Maxwell introduced displacement current to resolve the inconsistency in Ampere's law when applied to time-varying electric fields. He predicted that a changing electric field produces a non-zero magnetic field between capacitor plates through this fictitious current, providing a unified framework that explains how magnetic fields arise from both real currents and changing electric fields.
Q6: How does displacement current differ from real conduction current?
Real conduction current involves actual charge movement through a conductor, while displacement current arises from a time-varying electric field with no charge motion. Displacement current is analogous to real current in Ampere's law and produces magnetic fields identically, but it can generate magnetic fields even when no real current is present, making it essential for understanding electromagnetic phenomena.
Q7: What makes the modified Ampere's law independent of the surface choice?
By including the displacement current term, the modified Ampere's law accounts for all sources of magnetic fields—both real currents and changing electric fields. This ensures that regardless of which surface bounds an Amperian loop, the total contribution from conduction and displacement currents remains constant, making the law surface-independent and universally applicable.