Solveeit Logo

Question

Question: A current of \[0.24\,A\] flows through a circular coil of 72 turns, the average diameter of the coil...

A current of 0.24A0.24\,A flows through a circular coil of 72 turns, the average diameter of the coil being 20 cm. What is the strength of the field produced at the centre of the coil?
A. 1.09×104T1.09 \times {10^{ - 4}}\,T
B. 1.09×103T1.09 \times {10^{ - 3}}\,T
C. 1.09×102T1.09 \times {10^{ - 2}}\,T
D. 1.5×104T1.5 \times {10^{ - 4}}\,T

Explanation

Solution

Use Biot Savart’s law to determine the magnetic field at the center of the coil.
B=μ0nI2aB = \dfrac{{{\mu _0}nI}}{{2a}}
Here, μ0{\mu _0} is the permeability of the vacuum, n is the number of turns, I is the current and a is the radius of the coil.

Complete step by step answer:
According to Biot Savart’s law, the magnetic field produced at the center of the coil of radius aa, due to the current II flowing through the coil is expressed as,
B=μ0nI2aB = \dfrac{{{\mu _0}nI}}{{2a}}

Here, μ0{\mu _0} is the permeability of the vacuum, n is the number of turns of the coil, I is the current flowing through the coil and a is the radius of the coil.

The vacuum permeability is the constant and it has value 4π×107H/m4\pi \times {10^{ - 7}}\,H/m.

The diameter of the coil is twice the radius of the coil. Therefore, substitute d for 2a in the above equation.
B=μ0nIdB = \dfrac{{{\mu _0}nI}}{d}

Substitute 4π×107H/m4\pi \times {10^{ - 7}}\,H/m for μ0{\mu _0}, 72 for n, 0.24A0.24\,A for I, and 20 cm for d in the above equation.
B=(4π×107H/m)(72)(0.24A)(20cm)(102m1cm)B = \dfrac{{\left( {4\pi \times {{10}^{ - 7}}\,H/m} \right)\left( {72} \right)\left( {0.24\,A} \right)}}{{\left( {20\,cm} \right)\left( {\dfrac{{{{10}^{ - 2}}\,m}}{{1\,cm}}} \right)}}
B=2.17×10520×102\Rightarrow B = \dfrac{{2.17 \times {{10}^{ - 5}}}}{{20 \times {{10}^{ - 2}}}}
B=1.09×104T\therefore B = 1.09 \times {10^{ - 4}}\,T

So, the correct answer is “Option A”.

Note:
The modified form of the Biot Savart’s law, B=μ0nIdB = \dfrac{{{\mu _0}nI}}{d} is used to calculate the field only at the centre of the coil. To calculate the magnetic field at other places, you need to use ideal Biot Savart’s law, B=μ0I4πdl×ra2B = \dfrac{{{\mu _0}I}}{{4\pi }}\int {\dfrac{{d\vec l \times \vec r}}{{{a^2}}}} .