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JEE Main 2026 Preparation: Question Papers, Solutions, Mock Tests & Strategy Unacademy » JEE Study Material » Physics » Polarisation of a Dielectric Slab

Polarisation of a Dielectric Slab

Everything you must learn about dielectric categorisation can be summarised in this article. Find out everything you need to learn about dielectrics slab Polarisation. The best way to learn from experts is to get dielectric slab polarisation JEE notes.

Table of Content
  •  

Have you noticed how many insulation products are made of plastic, wood, or even glass? What is the reason for this scenario? Why aren’t we getting electric shocks when using plastic or wood? What is the reason that metal wires can only generate severe shocks? This chapter will look at dielectrics, the Polarisation of the dielectric constant, what dielectrics are and their many varieties, such as polar and nonpolar molecules, polarisation, polarizability, dielectric strength, and also dielectric slab polarisation questions. We will also examine some commonly used applications and examples of dielectric slab polarisation JEE notes.

What is Dielectric?

Dielectric is a material that has no electrical charge. It conducts electricity but does not conduct heat. Dielectric materials are used in appliances, electronic devices, and some other technical fields. They are also used in radio communication systems and medical equipment, such as pacemakers and defibrillators.

Dielectric slab polarisation is a technology for making electronic devices work in the presence of electric fields. It was invented by Joseph Henry, also known as the father of modern electronics. He used it to make telegraphs work in the presence of high voltage and later built a telephone network that could transmit over long distances without wires.

Classification of dielectric

Dielectrics are classified into two main categories: Polar Molecules and Nonpolar Molecules.

Polar Molecules: They are dielectrics where the chances of negative and positive molecules interfering are minimal or not even possible. This is because they all have an asymmetrical shape. Examples include CO2, H2O NO2, as well as other gases.

If there isn’t an electric field, the molecules’ dipole moment is altered unexpectedly. This means that the dipole moment on average is zero. If an electric field from outside is in place and the molecules can assemble in the same direction in the direction of an electric field.

Nonpolar Molecules: Unlike nonpolar molecules, the negative and negative charge centres of nonpolar molecules don’t match, i.e., they are not equal. The molecule can no longer sustain any permanent (or inherently) dipole moments.

Constant of Dielectric

If a dielectric slab is placed between parallel plates, there is a dielectric constant. The dielectric Constant represents the proportion of force of the electric field to the lower value of the electric field capacitor. This is the formula:

εr = E0 / E

where E0 represents the electric field applied, E is an electric field net of which εr is the dielectric constant

Polarizability

In the presence of an electric field, positively charged electrons and positively charged nuclei of atoms are exposed to opposing forces and go through charge separation. Polarizability measures a material’s dielectric constant and refractive index at a higher (optical) frequency.

The field applied is independent of temperature and proportional to the induced dipole moment. Its direction for the induced dipole force (x) for one polar atom is in line with the field of electricity E. The polarisability of a bound system influences its dynamical response to external forces.

It also gives information about how internal structures are formed in the molecule. A solid’s polarizability can be measured as dipole moments per volume of crystal cell:

P = ε0 α E

which denotes the atomic polarizability, and E is the electric field

Dielectric Polarisation

If an electric field from outside is applied to a dielectric material, the material’s behaviour can be detected; this is known by the term Dielectric Polarisation. Dielectric slab Polarisation is understood through the shifting in charge (positive or negative) if the electric field has been applied.

The polarisation process is triggered due to an electric field or external forces, like mechanical strain in the case of piezoelectric crystals (piezoelectric crystals are solid materials that accumulate electrical charge in their crystals). Dielectric Polarisation can happen spontaneously in pyroelectric crystals, particularly ferroelectrics (Ferroelectricity is a characteristic of certain substances that display an electric polarisation that is spontaneous and is reversed through using an electrical field).

Conclusion

Dielectric slab Polarisation is an electromagnetic field created when charged particles are an element’s response depending on its geometry. Brought into proximity with an electric field. In this type of field, the electric polarity is usually reversed. This can be seen by bringing a small piece of metal to touch a hand-held LED (light-emitting diode). In this case, the electricity coming out is positive and that coming in is negative. Learn more about Dielectric polarisation questions.

faq

Frequently Asked Questions

Get answers to the most common queries related to the JEE Examination Preparation.

What is the position of the external field at the surface of a metallic conductor?

Ans: As stated in the case of solid charged sphere examples, the external field at the surface of a metallic ...Read full

Give the formula of the electric field of a point charge using electric flux and Gauss’ law.

Ans: The electric flux Φ =EA where E is electric field, A is area...Read full

What does a uniformly charged surface consist of?

Ans: A uniformly charged surface consists of a constant charge per unit area over that surface. The electric ...Read full

Write the applications of Gauss’ law in everyday life.

Ans: As given in the case of solid charged sphere examples, the Gauss’ law is applied in everyday life in v...Read full

Ans: As stated in the case of solid charged sphere examples, the external field at the surface of a metallic conductor is perpendicular to the surface. The electric field lines are normal to their surface. The lines start and end on charges on the surface. But the electric field inside the conductor is zero.

Ans: The electric flux Φ =EA where E is electric field, A is area

On substituting the area:

Flux Φ =E × 4πr2..(1) where r is radius

According to Gauss’ law:

Electric flux Φ = Q ⁄ ε0….(2) where Q is charge and ε0 is electric constant

From equations (1) and (2):

Electric flux   E × 4πr2 =Q ⁄ ε0

Then the electric field of a point charge is: E= Q ⁄ 4πr2ε0 

Ans: A uniformly charged surface consists of a constant charge per unit area over that surface. The electric field inside a uniformly charged sphere is zero. In the case of two-dimensional surfaces, the amount of charge per unit area is called uniform surface charge density.

Ans: As given in the case of solid charged sphere examples, the Gauss’ law is applied in everyday life in various electrostatic problems.

  •   It is used to solve problems relating to spherical, planar, and cylindrical symmetries.
  •   It uses a simple method to calculate the electric field.
  •  It can be used to calculate the electric field of an infinite wire, infinite plane sheet, thin spherical shell, etc.

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