Additionl field proportional to magnetisation?

In summary, magnetisation of a sample is the net dipole moment per unit volume, which can be represented as M = m(net) / V. It has been observed that the magnetic field due to the material is proportional to the magnetisation, meaning B = μM. This relationship can be explained by the fact that B = µo(M + H) = µH, where M and H are measured in electric units and B is measured in magnetic units. The conversion factor between these units is µo, represented in units of Wb.A-1m-1 or T.m.A-1. The use of µ as a conversion factor is simply a convenience to make it appear as if B is proportional to H alone.
  • #1
jd12345
256
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Magnetisation of a sample is net dipole moment per unit volume i.e. M = m(net) / V

It turns out that magnetic field due to the material is proportional to magnetisation
i.e. B(magnetic field due to material) = μM
Any explanation to this? It should be proportional but any proof for this or is it just experimental
 
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  • #2
hi jd12345! :smile:
jd12345 said:
Magnetisation of a sample is net dipole moment per unit volume i.e. M = m(net) / V

It turns out that magnetic field due to the material is proportional to magnetisation
i.e. B(magnetic field due to material) = μM
Any explanation to this? It should be proportional but any proof for this or is it just experimental

isn't it B = µo(M + H) = µH ?

M and H are measured in electric units, as electric current/distance (Am-1),

(magnetic dipole moment is charge times distance/time, = distance times charge/time = distance times electric current, in A.m)

but B is measured in magnetic units, as magnetic flux/area (Wb.m-2)

there's no fundamental reason for this … they're all the same thing! :rolleyes: … it's just more convenient in practice! :biggrin:

so to convert between these different species of units, we must have a universal conversion factor, and that's µo (in Wb.A-1m-1 or T.m.A-1) :wink:

µ (as opposed to µo) is just a trick to make it look as if B is proportional to H on its own
 

1. What is "Additional field proportional to magnetisation"?

Additional field proportional to magnetisation is a term used in magnetism, specifically in the study of magnetic materials. It refers to an external magnetic field that is applied to a material and is proportional to the magnetisation of the material. This additional field is used to manipulate or measure the magnetisation of the material.

2. How is the additional field proportional to magnetisation calculated?

The additional field proportional to magnetisation is calculated by multiplying the magnetisation of the material by a proportionality constant, known as the magnetic susceptibility. This constant depends on the properties of the material and can be experimentally determined.

3. What is the significance of the additional field proportional to magnetisation?

The additional field proportional to magnetisation is significant because it allows us to understand and control the properties of magnetic materials. It is a crucial aspect in the study of magnetism and is used in various applications, such as in magnetic storage devices and medical imaging.

4. How does the additional field affect the magnetisation of a material?

The additional field has a direct effect on the magnetisation of a material. If the field is in the same direction as the material's magnetisation, it can enhance or strengthen it. On the other hand, if the field is in the opposite direction, it can weaken or even reverse the material's magnetisation.

5. Can the additional field proportional to magnetisation be measured?

Yes, the additional field proportional to magnetisation can be measured using various techniques such as vibrating sample magnetometry, SQUID magnetometry, or magnetic resonance imaging. These methods allow us to determine the strength and direction of the additional field and the resulting change in magnetisation of the material.

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