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Electric Polarisation of Dielectrics

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Estimated time: 12 minutes
CISCE: Class 12

Introduction

A dielectric is an insulating material that does not conduct electricity but can be polarised by an external electric field. Unlike conductors, dielectrics have no free charge carriers — their response to a field comes from the alignment of existing molecular dipoles.

Think of a dielectric like a box of tiny compass needles (molecular dipoles). Normally, they point in random directions. When you bring a magnet (external field) near, all needles rotate to align with it — this is exactly how molecules align inside a dielectric under an electric field.

CISCE: Class 12

Definition: Electric Polarisation

Electric Polarisation is the phenomenon in which an external electric field induces or aligns molecular dipoles within a dielectric, producing equal and opposite bound surface charges on its faces.

CISCE: Class 12

Definition: Dielectric Constant (K)

Dielectric Constant (K) is the ratio of the applied field to the net field inside the dielectric, indicating how much the material reduces the electric field.

CISCE: Class 12

Definition: Dielectric Strength

Dielectric Strength is the maximum electric field a dielectric can withstand without electrical breakdown (i.e., before it starts conducting).

CISCE: Class 12

Formula: Dielectric Constant

K = \[\frac {E_0}{E}\]

K = \[\frac {\sigma}{\sigma-\sigma_i}\]

where σ = surface charge density on plates, σi​ = induced (bound) charge density.

CISCE: Class 12

Formula: Dielectric Strength

Eds​ = \[\frac {V_{max}}{d}\]​​

SI unit: V/m

CISCE: Class 12

Electric Polarisation

  • The induced charges are called bound charges (not free charges) — they cannot move through the material.
  • Polarisation opposes the applied field partially, but never cancels it completely inside a dielectric.
CISCE: Class 12

Behaviour in a Parallel Plate Capacitor

When a dielectric slab is placed between charged parallel plates:

  • The dipoles align with the applied field E0.
  • Torque acts on each dipole, given by:
    τ = pE0 sin⁡ θ

where p = dipole moment, E0​ = applied field, θ = angle between dipole and field.

  • Induced bound charges create an internal opposing field E′.
  • The net field inside the dielectric is reduced but never zero:
    E = E0 − E′
CISCE: Class 12

Dielectric Strength of Common Materials

Material Dielectric Strength (approx) Common Use
Air ~ 3 × 106 V/m Capacitors, insulation
Paper ~ 1.6 × 107 V/m Paper capacitors
Glass ~ 9 × 106 V/m Insulators, capacitors
Mica ~ 1.6 × 108 V/m High-voltage capacitors
Teflon ~ 6 × 107 V/m Wire insulation
CISCE: Class 12

Polarisation Vector, Susceptibility & Displacement Vector

Quantity Formula Unit Meaning
Polarisation Vector \[\vec P\] = n\[\vec p\] C/m2 Dipole moment per unit volume
Electric Susceptibility \[\vec P\] = ε0χe\[\vec E\] Dimensionless Measures ease of polarisation
Electric Displacement \[\vec D\] = ε0\[\vec E\] + \[\vec P\] C/m2 Total field response in dielectric
Displacement (simplified) \[\vec D\] = ε\[\vec E\] C/m2 Alternate form using permittivity
K–Susceptibility Relation K = 1 + χe Dimensionless Links constant and susceptibility
CISCE: Class 12

Applications of Dielectrics

  • Capacitors — dielectrics increase capacitance and charge storage.
  • Piezoelectric crystals — generate voltage under mechanical stress.
  • Electrets — permanently polarised dielectrics (analogous to permanent magnets).
  • LCDs — rely on controlled polarisation of liquid crystal dielectrics.

Video Tutorials

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