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Question: A Rowland ring of mean radius 15 cm has 3500 turns of wire wound on a ferromagnetic core of relative...

A Rowland ring of mean radius 15 cm has 3500 turns of wire wound on a ferromagnetic core of relative permeability 800. What is the magnetic field B in the core for a magnetising current of 1.2 A?

Explanation

Solution

A Rowland ring is just a toroid which produces magnetic fields. For calculating the magnetic field produced by a toroid, we need permeability of the material of the core, number of turns per unit length of the toroid and the amount of current flowing through the toroid.
Formula used:
The magnetic field produced by a toroid is given as
B=μnI ...(i)B = \mu nI{\text{ }}...\left( i \right)
Here B represents the magnetic field produced by the toroid, μ\mu is the permeability of the material of the core of the toroid, n represents the number of turns in the toroid per unit length while I is the current flowing through the coils of the toroid.

Detailed step by step solution:
We are given a Rowland ring which is a toroid whose core is made of magnetic material. We are given the radius of the ring whose value is
r=15cm=0.15mr = 15cm = 0.15m
The number of turns in the coil is given as
N=3500N = 3500
But we need no. of turns per unit length of the toroid which can be obtained as follows:
n=N2πr=35002π×0.15n = \dfrac{N}{{2\pi r}} = \dfrac{{3500}}{{2\pi \times 0.15}}

We are given the relative permeability of the ferromagnetic core of the toroid.
μr=800{\mu _r} = 800
Now we can calculate the permeability of the core as follows:
μ=μ0μr=800μ0\mu = {\mu _0}{\mu _r} = 800{\mu _0}
Here μ0=4π×107{\mu _0} = 4\pi \times {10^{ - 7}}
The current flowing through the core is given as
I=1.2AI = 1.2A
Now we can calculate the magnetic field produced in the toroid by using equation (i) in the following way.
B=μnI=800×4π×107×35002π×0.15×1.2=4.48TB = \mu nI = 800 \times 4\pi \times {10^{ - 7}} \times \dfrac{{3500}}{{2\pi \times 0.15}} \times 1.2 = 4.48T
This is the required answer.

Note: A toroid is basically a solenoid which has been folded in a circular shape. The magnetic flux is produced in a toroid by the phenomenon of magnetic induction. The direction of the produced field can be determined by using the right hand rule.