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Question: The magnetic susceptibility of a material of a rod is 499. Permeability of vacuum ​is \(4\pi \times ...

The magnetic susceptibility of a material of a rod is 499. Permeability of vacuum ​is 4π×107Hm14\pi \times {10^{ - 7}}H{m^{ - 1}} Absolute permeability of the material of the rod is:
A π×104\pi \times {10^4}
B 2π×1042\pi \times {10^4}
C 3π×1043\pi \times {10^{ - 4}}
D 4π×1044\pi \times {10^{ - 4}}

Explanation

Solution

Hint
As the magnetic susceptibility is given and permeability is also given then we find the value of absolute permeability by using the formula μ=μo(1+χm)\mu = {\mu _o}\left( {1 + {\chi _m}} \right)

Complete step-by-step answer:
Magnetic susceptibility is the measure of how much a material can be magnetised in the presence of a magnetic field.
Here, it is given that the susceptibility of a material of a rod χm=499{\chi _m} = 499
Permeability of the vacuum μo=4π×107Hm1{\mu _o} = 4\pi \times {10^{ - 7}}H{m^{ - 1}}
We have to find the value of absolute permeability of the material of the rod
As, we know the relation between the magnetic susceptibility and permeability is
μ=μo(1+χm)\mu = {\mu _o}\left( {1 + {\chi _m}} \right)
Where, μ is the absolute permeability of the material.
μo{\mu _o} is the permeability of the vacuum
χm{\chi _m} is the magnetic susceptibility of the material.
Now, put the given values in the above equation, we get
μ=4π×107(1+499)\mu = 4\pi \times {10^{ - 7}}\left( {1 + 499} \right)
μ=2π×104Hm1\mu = 2\pi \times {10^{ - 4}}H{m^{ - 1}}
Hence, the value of absolute permeability is μ=2π×104Hm1\mu = 2\pi \times {10^{ - 4}}H{m^{ - 1}}
Therefore, (B) option is correct.

Additional information
Magnetic susceptibility is the measure of how much the material is magnetized in the presence of a magnetic field. It is the ratio of the magnetization to the applied magnetic field.

Note
Magnetic permeability helps us measure a material's resistance to the magnetic field or measure of the degree to which the magnetic field can penetrate through a material. It is the ratio of the magnetic induction to the magnetic intensity.