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CBSE Class 12th Physics Notes: Magnetism and Matter (Part ‒ III)

Get Chapter wise revision notes on Chapter 5: Magnetism and Matter (Part III) for CBSE class 12 physics board exam 2017. These notes are useful for quick revision of important concepts before exams.

Dec 14, 2016 16:30 IST
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Get Chapter wise revision notes on Chapter 5: Magnetism and Matter (Part III) for CBSE class 12 physics board exam 2017. These notes are useful for quick revision of important concepts before exams.

Chapter wise revision notes for class 12 Physics on chapter 5 Magnetism and Matter (Part III) are available in this article. Important concepts of this chapter are already covered in Part I and Part II.

In this part, we will study the concepts given below:

Atom as Magnetic Dipole

Relative Magnetic Permeability

Magnetic Intensity

Intensity of Magnetisation

Magnetic Susceptibility

Relation between Magnetic Susceptibility and Magnetic Permeability

Classification of Magnetic Material

Diamagnetic Material

Paramagnetic Material

Ferromagnetic Material

Curie’s Law in Magnetism

Hysteresis Curve

The notes are as follow:

Atom as Magnetic Dipole

In an atom, an electron revolves around the nucleus. The orbit of electron behaves like a current loop of current which has a definite magnetic dipole moment associated with it.

Magnetic dipole moment of an orbit of radius r having electron moving with velocity ω, is given by,

Expression for Magnetic Dipole of atom

CBSE Class 12 Physics Syllabus 2017

Important terms used in Magnetism

Relative Magnetic Permeability

It is the ability of a material to permit magnetic lines of force to pass through it. It is given by,

μR = (B/Bo) = (μ/μo)

Where Bo is number of magnetic lines per unit area in vacuum, B is number of magnetic lines of force per unit area in the given material medium. μ is magnetic permeability of a material and μo is magnetic permeability of free space.

μR ha no dimension and its value for vacuum is one.

Magnetic Intensity

Degree to which a magnetic field can magnetise a material is represented in terms of magnetic intensity.

It is given by, H = n i or H = B/ μ, where, n is number turns per unit length of a toroidal solenoid carrying a current i. It is a vector quantity and its SI unit is Am‒1.

Intensity of Magnetisation

Intensity of Magnetisation of a magnetic material is defined as magnetic moment per unit volume of the material.

Intensity of Magnetisation

Magnetic Susceptibility

Susceptibility of a magnetic material is defined as the ratio of the intensity of magnetisation (I) induced in the material to the magnetizing force (H) applied to it.

It is given by,

Magnetic Susceptibility

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Relation between Magnetic Susceptibility and Magnetic Permeability

A magnetic material placed in a magnetising field of magnetising intensity H, the material gets magnetised. Total magnetic induction B in the material is the sum of the magnetic induction Bo in vacuum produced by the magnetic intensity and magnetic induction Bm, due to magnetisation of the material, therefore, B = Bo + Bm

Now, Bo = μo H and Bm = μo I, where I is the intensity of magnetistion induced in the magnetic material. So, B = μo (H + I)

We know that, B = μ H and I = χm H

Relation between Magnetic Susceptibility and Magnetic Permeability

Classification of Magnetic Material

Different types of material behave differently in presence of external magnetic field and are categorised into following types:

(i) Diamagnetic Material (ii) Paramagnetic Material and (iii) Ferromagnetic Material

Diamagnetic Material

Diamagnetic substances are those which have tendency to move from stronger to the weaker part of the external magnetic field. Materials in whose atoms (molecules) or ions do not possess any net magnetic moment of their own.

Some diamagnetic materials are bismuth, copper, lead, silicon, nitrogen (at STP), water and sodium chloride.

Paramagnetic Material

Paramagnetic materials are those which get weakly magnetised when placed in an external magnetic field. They have tendency to move from a region of weak magnetic field to strong magnetic field, i.e., they get weakly attracted to a magnet.

The individual atoms (or ions or molecules) of a paramagnetic material possess a permanent magnetic dipole moment of their own.

Ferromagnetic Material

Ferromagnetic substances are those which gets strongly magnetised when placed in an external magnetic field. They have strong tendency to move from a region of weak magnetic field to strong magnetic field, i.e., they get strongly attracted to a magnet.

The individual atoms (or ions or molecules) in a ferromagnetic material possess a dipole moment as in a paramagnetic material but in a more cooperative way.

Properties of Diamagnetic Material, Paramagnetic Material, Ferromagnetic Material

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Curie’s Law in Magnetism

According to this law, the intensity of magnetization (I) of magnetic material is directly proportional to the magnetic field (H), and inversely proportional to the absolute temperature (T) of the material.

Where, C is a constant known as Curie’s constant.

Hysteresis Curve:

Hysteresis curve is the relation between magnetic induction or intensity of magnetization of a ferromagnetic material with magnetizing force or magnetic intensity.

 Hysteresis Curve for a ferromagnetic materials

The graph given above shows hysteresis loop for ferromagnetic materials taken through one cycle of magnetisation.

Chapter Wise Revision Notes on Chapter 5: Magnetism and Matter (Part I)

Chapter Wise Revision Notes on Chapter 5: Magnetism and Matter (Part II)

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