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Question: The correct relation between B and M for a small current carrying coil is: A) \(B = \dfrac{{{\mu _...

The correct relation between B and M for a small current carrying coil is:
A) B=μ0M2x3B = \dfrac{{{\mu _0}M}}{{2{x^3}}}
B) B=μ0Mx3B = \dfrac{{{\mu _0}M}}{{{x^3}}}
C) B=μ0Mπx3B = \dfrac{{{\mu _0}M}}{{\pi {x^3}}}
D) B=μ0M2πx3B = \dfrac{{{\mu _0}M}}{{2\pi {x^3}}}

Explanation

Solution

Hint A small amount of current is flowing in a coil. We have to derive a relation between B and M. We will use definitions of B and M to find which one is a correct formula satisfying the relation.

Complete step by step solution
Both B and M are vector quantities.
B - It is magnetic flux density. The amount of magnetic field lines crossing a unit area normally from a magnetic material. Strength of the magnetic field is given by this quantity.
It's S.I. unit is kgs2/A\dfrac{{kg}}{{{s^2}}}/A or Tesla.
B=μ0I2xB = \dfrac{{{\mu _0}I}}{{2x}} …(1)
Here x= radius of circle and μ0{\mu _0} is magnetic susceptibility.
Value of μ0{\mu _0} is 4π×107TmA4\pi \times {10^{ - 7}}\dfrac{{Tm}}{A} .
M -It is a magnetization field. It is also known as magnetic polarization. When current is passed from all the dipoles aligns itself in a particular direction. This sets up magnetic moments which get induced in the substance. The response of a magnet on the application of magnetic field gives resultant magnetization. Hence it is also explained as magnetic moment per unit volume.
M=mV=IAM = \dfrac{m}{V} = IA …(2)

I=MA A=πx2  I = \dfrac{M}{A} \\\ A = \pi {x^2} \\\

Using value of equation (2) in (1)
B=μ0M2πx3B = \dfrac{{{\mu _0}M}}{{2\pi {x^3}}}

Hence the correct option is (D).

Note
If B=μ0IxB = \dfrac{{{\mu _0}I}}{x} is used then we get B=μ0Mπx3B = \dfrac{{{\mu _0}M}}{{\pi {x^3}}} I.e. option (C) as our solution. But this is not the correct option. If we have used M=mVM = \dfrac{m}{V} then we might not reach the solution. So, we cannot use this value. Option A and B are also wrong. Therefore, we are left with only one option I.e. D which is correct.