1. Introduction
Ampere's circuital law relates the magnetic field around a closed path to the electric current enclosed by that path.
For a steady current, Ampere's law is written as:
However, this form creates a problem when the current is changing with time, especially during the charging of a capacitor.
2. The Problem with Ampere's Law
Consider a capacitor being charged by a battery. Current flows through the connecting wires, but there is no ordinary conduction current through the insulating gap between the capacitor plates.
The electric field between the capacitor plates changes with time. This changing electric field produces a magnetic field.
3. 🔄 Charging Capacitor Animation
Observe the changing electric field between the capacitor plates. This changing field is associated with displacement current.
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4. What is Displacement Current?
Displacement current is the current associated with a time-varying electric field.
It is not an actual flow of electric charges through the dielectric gap like conduction current.
Where:
Displacement current
Permittivity of free space
Electric flux
Rate of change of electric flux
5. Maxwell's Modification of Ampere's Law
Maxwell added the displacement current term to Ampere's law.
Therefore:
6. General Maxwell-Ampere Law
This equation shows that magnetic fields can be produced by:
🔌 Conduction Current
Produced by actual movement of electric charges.
⚡ Changing Electric Field
Produces displacement current and therefore contributes to the magnetic field.
7. Displacement Current in a Charging Capacitor
For a parallel plate capacitor:
Electric flux is:
Therefore:
Differentiating with respect to time:
Since:
We obtain:
During charging of an ideal capacitor, the displacement current between the plates is equal in magnitude to the conduction current in the wires.
8. Conduction Current vs Displacement Current
| Property | Conduction Current | Displacement Current |
|---|---|---|
| Origin | Movement of charges | Changing electric field |
| Symbol | I | Id |
| Expression | I = dQ/dt | Id = ε₀dΦE/dt |
| Capacitor gap | No conduction current | Displacement current exists |
| Produces magnetic field? | Yes | Yes |
9. ⭐ Key Concept
10. 📐 Important Formulae
For an ideal charging capacitor
11. 🧮 Worked Example
The electric flux through a surface changes at a rate of 2 × 106 N m²/C per second. Find the displacement current.
ε₀ = 8.85 × 10−12 C²/(N m²)
12. 🎯 Practice MCQs
Q1. Maxwell introduced displacement current to modify:
Q2. Displacement current is associated with:
Q3. The expression for displacement current is:
Q4. During charging of an ideal capacitor:
Q5. A changing electric field produces:
13. 🏆 One-Minute Revision
Relates magnetic field to current.
Added displacement current.
Id = ε₀dΦE/dt
Id = I