In electricity and magnetism, we usually learn that a magnetic field is produced by moving electric charges (current). But there are some situations, like in a charging or discharging capacitor, where a magnetic field exists even though no actual charges move between the plates. To explain this, James Clerk Maxwell introduced the idea of displacement current and improved Ampère’s Law. This new form is called the Maxwell–Ampere Law. It tells us that a magnetic field can be produced not only by real electric current but also by a changing electric field. This concept helps us understand how electric and magnetic fields are connected. In this article, displacement current, its formula, the problem with Ampère’s Law, and the Maxwell–Ampere Law are explained in very simple words for students.
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A displacement current is a current that occurs when an electric field changes in time, for example in a capacitor that is charging or discharging. It doesn’t actually involve any flow of charges at all, but it causes an electromagnetic field to change smoothly, like a current. This concept has an explanation for how electric and magnetic fields interact when there are no moving charges.
The displacement current was introduced by James Clerk Maxwell to explain the continuity of current in a circuit, especially between the plates of a capacitor.
$
I_d=\varepsilon_0 \frac{d \Phi_E}{d t}
$
where
For a Capacitor
$
I_d=\varepsilon_0 A \frac{d E}{d t}
$
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The Maxwell-Ampere Law is an extension of Ampere's circuital law given by James Clerk Maxwell. It explains how a magnetic field is produced not only by an electric current but also by a changing electric field.
Statement
The magnetic field around a closed loop is produced by conduction current as well as displacement current passing through the surface bounded by the loop.
In the Ampère-Maxwell law, the magnetic field $\vec{B}$ around a closed loop is related to the current passing through that loop. The law is expressed as:
$
\oint \vec{B} \cdot d \vec{s}=\mu_0 I
$
where:
Ampère’s Law works well for steady (unchanging) currents, but it has a limitation when applied to circuits with changing electric fields, such as those with a condenser (capacitor).
Example with a Capacitor (Condenser)
Consider a capacitor connected to a voltage source, with:
As the capacitor gets charged, an electric current will flow in the circuit, but no current actually flows between the plates of the capacitor because they are separated by an insulating gap. If we try to apply Ampère’s Law in this case to a loop between the capacitor plates, we run into a problem because we do not have any current there.
Frequently Asked Questions (FAQs)
Yes, along the closed path, the amount of travel and travel current is constant.
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Under Faraday's electromagnetic induction legislation, an emf is induced by a fluctuating magnetic field, According to Maxwell, a current and therefore a magnetic field is created in an electric field. Such a current is called the current of displacement. A time-changing electric field therefore produces a magnetic field and vice versa. The electrical and magnetic field behaviour is hence symmetrical.
Ampere is the SI current shifting unit (A)
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The current is called displacement current due to the changing electric field.