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Question: The radius of a circular current carrying coil is \( R \) . At what distance from the centre of the ...

The radius of a circular current carrying coil is RR . At what distance from the centre of the coil on its axis, the intensity of the magnetic field will be 122\dfrac{1}{{2\sqrt 2 }} times at the centre?
A)2R \\\ B)\dfrac{{3R}}{2} \\\ C)R \\\ D)\dfrac{R}{2} \\\

Explanation

Solution

Hint : The magnetic effect on electric currents, moving electric charges and magnetic materials is defined by a magnetic field, which is a vector field. In a magnetic field, a moving charge encounters a force that is perpendicular to both its own velocity and the magnetic field.

Complete Step By Step Answer:
The magnetic field at the axis due to the circular current is given by,
Baxis=μ04π(2πNIR2(x2+R2)32){B_{axis}} = \dfrac{{{\mu _0}}}{{4\pi }}\left( {\dfrac{{2\pi NI{R^2}}}{{{{({x^2} + {R^2})}^{\dfrac{3}{2}}}}}} \right)
Where NN represents the number of turns in the coil,
II represents the current flowing in the coil,
RR represents the radius of the circular current carrying coil, and
xx represents the distance from the centre of the coil on its axis
We consider N=1N = 1 , and so we get,
Baxis=μ04π(2πIR2(x2+R2)32){B_{axis}} = \dfrac{{{\mu _0}}}{{4\pi }}\left( {\dfrac{{2\pi I{R^2}}}{{{{({x^2} + {R^2})}^{\dfrac{3}{2}}}}}} \right)
We can divide 2π2\pi by 4π4\pi , and then we get
B1=μ0IR22(R2+x2)32{B_1} = \dfrac{{{\mu _0}I{R^2}}}{{2{{({R^2} + {x^2})}^{\dfrac{3}{2}}}}}
B2=μ0I2R{B_2} = \dfrac{{{\mu _0}I}}{{2R}}
122B2=B1\dfrac{1}{{2\sqrt 2 }}{B_2} = {B_1}
Now we substitute the values of B1{B_1} and B2{B_2} in the above equation.
(122)(μ0I2R)=μ0IR22(R2+x2)32\left( {\dfrac{1}{{2\sqrt 2 }}} \right)\left( {\dfrac{{{\mu _0}I}}{{2R}}} \right) = \dfrac{{{\mu _0}I{R^2}}}{{2{{({R^2} + {x^2})}^{\dfrac{3}{2}}}}}
Since we have many terms same on both side, it gets cancelled out, and then we get,
122R3=1(R2+x2)32\dfrac{1}{{2\sqrt 2 {R^3}}} = \dfrac{1}{{{{\left( {{R^2} + {x^2}} \right)}^{\dfrac{3}{2}}}}}
Now we take the reciprocal on both sides, we get,
22R3=(R2+x2)322\sqrt 2 {R^3} = {\left( {{R^2} + {x^2}} \right)^{\dfrac{3}{2}}}
222\sqrt 2 can be written as 232{2^{\dfrac{3}{2}}} . Also, we multiply 23\dfrac{2}{3} on the exponent on both sides and we get,
2R2=R2+x2 2R2R2=x2 R2=x2  2{R^2} = {R^2} + {x^2} \\\ \Rightarrow 2{R^2} - {R^2} = {x^2} \\\ \Rightarrow {R^2} = {x^2} \\\
On taking square roots on both sides, we get,
x=Rx = R
The distance from the centre of the coil on its axis when the intensity of magnetic field will be 122\dfrac{1}{{2\sqrt 2 }} times at the centre is equal to RR .
Therefore, the correct option is C)RC)R .

Note :
Permanent magnetization exists in the Earth's crust, and the Earth's centre produces its own magnetic field, which sustains the majority of the field we calculate at the surface. As a result, the Earth can be defined as a "magnet."