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Question: A circular coil carrying a current I has radius R and number of turns N . If all the three, i.e., th...

A circular coil carrying a current I has radius R and number of turns N . If all the three, i.e., the current I, radius R and number of turns N are doubled, then magnetic field at its centre becomes
(A) Double
(B) Half
(C) Four times
(D) One fourth

Explanation

Solution

When the current I is flowing in the circular coil of radius R and number of turns N then first we use Biot savart law to derive the relation between magnetic field, radius, current and number of turns i.e., B=μ0NIR22(R2+x2)3/2B = \dfrac{{{\mu _0}NI{R^2}}}{{2{{({R^2} + {x^2})}^{3/2}}}} and use above expression for centre point.

Complete step by step answer:
We know that at the axis of a current carrying coil at distance x from the centre, magnetic field B is given by
B=μ0NIR22(R2+x2)3/2B = \dfrac{{{\mu _0}NI{R^2}}}{{2{{({R^2} + {x^2})}^{3/2}}}}
At centre x=0x = 0
So, BC=μ0NIR22(R2)3/2{B_C} = \dfrac{{{\mu _0}NI{R^2}}}{{2{{({R^2})}^{3/2}}}}
BC=μ0NIR22R3{B_C} = \dfrac{{{\mu _0}NI{R^2}}}{{2{R^3}}}
    BC=μ0IN2R\implies {B_C} = \dfrac{{{\mu _0}IN}}{{2R}} …..(1)
If I, R & N are doubled then magnetic field at centre will be
BC{B_C}’ = μ0(2I)(2N)2(2R)\dfrac{{{\mu _0}(2I)(2N)}}{{2(2R)}}
    BC\implies {B_C}’ = 2(μ0NI2R)2\left( {\dfrac{{{\mu _0}NI}}{{2R}}} \right)
From equation (1)
BC{B_C}’ = 2BC2{B_C}
Hence, the magnetic field at the centre will also become doubled.

So, option A is the correct answer Double.

Note:
If any point which is situated at any distance from centre on axial line, then we can also calculate the magnetic field by above formula which is
B=μ0NIR22(R2+x2)3/2B = \dfrac{{{\mu _0}NI{R^2}}}{{2{{({R^2} + {x^2})}^{3/2}}}}.