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# Magnetization and magnetic intensity - magnetic susceptibility and permeability, practice problems, FAQs

You might have heard that different materials possess different magnetic properties. They find their applications depending upon the requirement. But have you ever wondered why do they possess different properties or why don’t they all behave the same? To go to depth of this question, you should first be aware of magnetization.

• Magnetization of materials
• Magnetization Vector ($\stackrel{\to }{I}$)
• Magnetic intensity ($\stackrel{\to }{H}$)
• Magnetic Susceptibility
• Magnetic Permeability
• Relative Permeability
• Practice problems
• FAQs

## MAGNETIZATION OF MATERIALS

We know that if there exists unpaired electrons giving a net magnetic moment to an atom and the atoms are randomly distributed in the materials, the net magnetic moment of the material becomes zero.

If the same material is placed in an external magnetic field produced by a permanent magnet, then unpaired electrons behaving as magnetic dipoles will try to align themselves along the direction of the external magnetic field, as shown in the figure. Thus, the material now can show the magnetic properties.

Magnetization Vector ($\stackrel{\to }{\mathbit{I}}$)

• Also known as intensity of Magnetization, the magnetization vector is defined as net magnetic moment per unit volume.

$\stackrel{\to }{I}=\frac{{\stackrel{\to }{M}}_{net}}{V}$

• As the temperature increases the randomness of motion of electrons in a material increases. The increase in randomness suggests the randomness in their alignment also.The orientation of unpaired electrons can lead to zero net magnetic moment. Thus, increase in temperature of magnetic material decreases magnetism of the material.
• $\stackrel{\to }{\mathbit{I}}$ depends on the nature of the material and temperature.
• The direction of intensity of magnetization is the same as that of induced dipole moment.
• SI unit of magnetization vector:

Consider a bar magnet having pole strength 𝑚, length 𝑙 and the cross-section 𝐴,

The magnetic moment is defined as $M=m×l$

Therefore, intensity of magnetization, $\stackrel{\to }{I}=\frac{{\stackrel{\to }{M}}_{net}}{V}$

$⇒I=\frac{m×l}{Al}=\frac{m}{A}$

Thus intensity of magnetization can also be defined as pole strength per unit cross sectional area.

## Magnetic intensity ($\stackrel{\to }{\mathbit{H}}$)

• It is the ability of an external magnetic field to magnetise a material medium.

• $\stackrel{\to }{\mathbit{H}}$ is also known as Magnetising Field Intensity
• Magnetic intensity can also be defined as the ratio of magnetising field and permeability of free space.

• For an air core solenoid, ${B}_{o}={\mu }_{o}nI$

$⇒H=\frac{{\mu }_{o}nI}{{\mu }_{o}}=nI$

Thus material of the core of solenoid does not influence its magnetic intensity.

• SI unit:

To magnetise a material, we apply an external magnetic field to the material. Under influence of the external magnetic field, most of the atomic dipoles align themselves along the direction of and creates their own magnetic field inside the material.

Net magnetic field inside matter:

Internal factor: Due to alignment of dipoles (I), (Magnetization) $={\mu }_{o}\stackrel{\to }{I}$

External factor: Magnetising field intensity ${=\mu }_{o}\stackrel{\to }{H}$

Net magnetic field,

• is independent of nature of the medium as it measures the ability of an external magnetic field to magnetise a material medium.
• If no material is present (vacuum),

## Magnetic Susceptibility

• Magnetic susceptibility is defined as the ratio of magnitude of intensity of magnetization and that of magnetic intensity.
• Experimental results show that intensity of magnetization is proportional to the magnetic intensity

𝜒 is used to represent magnetic susceptibility.

• Higher the value of 𝜒, more easily the material can be magnetised.
• No magnetization in vacuum, and hence 𝜒=0
• 𝜒 depends on the nature of material and temperature.
• Magnetic susceptibility is a dimensionless and unitless, scalar quantity.

Magnetic Permeability

It is the ratio of magnitudes of magnetic field and magnetic intensity inside a material.

• Units of magnetic permeability: Wb/Am
• Dimensions of magnetic permeability: [MLT-2A-2]
• It is a scalar quantity.
• Measures the extent of penetration of a magnetising field inside a given material.

Consider a material being placed in the influence of an external magnetic field as shown.

The net magnetic field is given by,

Since, magnetization

Where is Permeability of the material

If there is no material, is the permeability of the vacuum.

Relative permeability: The relative permeability of a material is a factor by which magnetic field increases when a material is introduced.

• It can also be defined as the ratio of permeability of medium to the permeability of free space.
• It is a dimensionless and unitless quantity.

## Practice problems

Q. A solenoid has a material of relative permeability 400. If solenoid has 1000 turns per metre and carries a current of 2 𝐴. Find

1) Magnetic intensity(𝐻)

2) Net magnetic field(𝐵𝑛𝑒𝑡)

3) Intensity of magnetization(I)

⇒H=nI

$⇒{B}_{net}=400×4\pi ×{10}^{-7}×2×{10}^{3}$

I=𝜒H

${\mu }_{r}=1+\chi ⇒\chi =400-1=399$

$⇒I=399×2×{10}^{3}=7.98×{10}^{5}\frac{A}{m}$

Q. A 2 A current is flowing in the winding of a toroid. There are 950 turns and the mean circumferential length is . If the magnetic field inside the toroid is 4 T, then find the magnetic susceptibility of the core.

Given:

Magnetic field inside a toroid,

$B=\frac{\mu NI}{2\pi r}$

Here, the mean circumferential length is,

Substituting values in equation (1),

$\mu =\frac{4×19\pi ×{10}^{-2}}{950×2}$

The relative permeability will be

${\mu }_{r}=\frac{{\mu }_{m}}{{\mu }_{o}}=\frac{4×19\pi ×{10}^{-2}}{950×2}×\frac{1}{4\pi ×{10}^{-7}}$

${⇒\mu }_{r}=1000$

Using formula, ${\mu }_{r}=1+\chi$

$\chi ={\mu }_{r}-1=1000-1=999$

Q. Find the magnitude of magnetic field B at the centre of a bar magnet having pole strength 3.6 Am, magnetic length 12 cm and cross-sectional area 0.9 cm2.

A.

Given:

Pole strength of magnet, m=3.6 Am

Magnetic length, 2l=12 cm

Cross-sectional area, A=0.9 cm2

At the centre of the magnet, magnetic field can be written as

$\stackrel{\to }{B}=|{1}_{o}\stackrel{\to }{H}+o$

Here,

Magnetization of bar magnet can be calculated as,

Due to north pole magnetic intensity at the centre,

${H}_{N}=\frac{1}{4\pi }\frac{m}{{l}^{2}}=\frac{1}{4\pi }\frac{3.6}{\left(6×{10}^{-2}{\right)}^{2}}=\frac{1000}{4\pi }\frac{A}{m}$

Similarly, magnetic intensity due to south pole at the centre is,

${H}_{S}=\frac{1000}{4\pi }\frac{A}{m}$

Resultant magnetic intensity,

$H={H}_{N}+{H}_{S}=\frac{2000}{4\pi }=159.2\frac{A}{m}$ [Towards the south pole]

Net magnitude of magnetic field at the centre, using the equation (1) can be obtained as:

$⇒B={\mu }_{o}\left(I+H\right)$

$B=4\pi ×{10}^{-7}\left(4×{10}^{4}+159.2\right)$

towards North pole

Q. If the space inside a current carrying toroid is filled with aluminium, then find the increase in magnetic field in terms of percentage. The susceptibility of aluminium is $2.1×{10}^{-5}$.

A.

Given,

Susceptibility of aluminium,

Magnetic field in the absence of aluminium,

${B}_{o}={\mu }_{o}H$

The magnetic field when the space within the toroid is filled with aluminium,

The increase in the field is,

$B-{B}_{o}={\mu }_{o}\chi H$

The percent increase is,

$\frac{B-{B}_{o}}{{B}_{o}}×100=\frac{{\mu }_{o}\chi H}{{\mu }_{o}H}×100=\chi ×100$

$⇒\frac{B-{B}_{o}}{{B}_{o}}×100=2.1×{10}^{-5}×100=2.1×{10}^{-3}$

## FAQs

Q1. What is the relative permeability of a diamagnetic material?
The relative permeability of a diamagnetic material is less than 1 since diamagnetic materials repel the external magnetic field lines. Magnetic field lines inside these materials are comparatively lesser than the free space.

Q2. What is the physical significance of magnetic susceptibility?
The ease with which the material can be magnetised when subjected to external magnetic fields is represented by magnetic susceptibility.

Q3. A steel rod is located at the north magnetic pole of the earth. It is partially embedded into the ground. The rod acquires magnetic properties after a long time, then -

1. End of the steel rod embedded inside the ground will become the North Pole
2. End of the steel rod embedded inside the ground will become the South Pole
3. Cannot be predicted
4. None of the above

A. (b)

Consider the magnetic field lines around the Earth.

These lines will enter the rod through the end embedded into the ground and exit through its other end, which is above the ground.

Therefore, the upper end of the rod which is outside the ground becomes the North pole and the part of rod inside the ground acquires the South pole.

Hence, option B is correct.

Q4. A plane parallel to the magnetic axis of a bar magnet cuts it into two equal halves. What happens to the intensity of magnetization?
$I=\frac{M}{V}$
Here, magnetic moment, $M\to \frac{M}{2}$(since pole strength becomes half) and volume, $V\to \frac{V}{2}$