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Question: Two circular coils \( 1 \) and \( 2 \) are made from the same wire but the radius of \( 1st \) coil ...

Two circular coils 11 and 22 are made from the same wire but the radius of 1st1st coil is twice that of the 2nd2nd coil. What potential difference in volts should be applied across them so that the magnetic field at the centres is the same.
(A) 44 times of first coil
(B) 66 times of first coil
(C) 33 times of first coil
(D) 22 times of first coil

Explanation

Solution

Hint : Use the formula for magnetic field at the centre of a coil by Biot- Savart law and equate the magnetic fields to find the relationship between the currents. Then use ohm’s law to deduce the voltage relation. The magnetic field of a circular at the centre is given by, B=μ0i2rB = \dfrac{{{\mu _0}i}}{{2r}} where, rr is the radius of the coil , μ0{\mu _0} is the absolute magnetic permeability , ii is the current flowing through it.

Complete Step By Step Answer:
we know that the magnetic field at the centre of a coil by Biot –Savart law is B=μ0i2rB = \dfrac{{{\mu _0}i}}{{2r}} ,where, rr is the radius of the coil , μ0{\mu _0} is the absolute magnetic permeability , ii is the current flowing through it.
We have given here two coils with the radius of the first coil twice of that second.
So, magnetic field at the centre field is, B1=μ0i12r1{B_1} = \dfrac{{{\mu _0}{i_1}}}{{2{r_1}}} and of the second is, B2=μ0i22r2{B_2} = \dfrac{{{\mu _0}{i_2}}}{{2{r_2}}}
This magnetic field for both the coils is the same. Hence we can write, B1=B2{B_1} = {B_2}
Therefore, μ0i12r1=μ0i22r2\dfrac{{{\mu _0}{i_1}}}{{2{r_1}}} = \dfrac{{{\mu _0}{i_2}}}{{2{r_2}}}
Or, i1r1=i2r2\dfrac{{{i_1}}}{{{r_1}}} = \dfrac{{{i_2}}}{{{r_2}}}
Now, we have, r1=2r2{r_1} = 2{r_2}
Putting the value in the equation we get,
i12r2=i2r2\dfrac{{{i_1}}}{{2{r_2}}} = \dfrac{{{i_2}}}{{{r_2}}}
Or, i1=2i2{i_1} = 2{i_2}
Now, we know, resistance of a wire of length ll with cross section AA of resistivity ρ\rho is given by,
R=ρlAR = \dfrac{{\rho l}}{A} . Here we have coils made of the same materials. Hence, resistivity and cross section is the same. So, Resistance of the first coil is, R1=ρl1A{R_1} = \dfrac{{\rho {l_1}}}{A} . Now, length of the first coil l1=2πr1=2π(2r2){l_1} = 2\pi {r_1} = 2\pi (2{r_2})
So, R1=ρ2π(2r2)A{R_1} = \dfrac{{\rho 2\pi (2{r_2})}}{A}
Resistance of the second coil is, R2=ρl2A{R_2} = \dfrac{{\rho {l_2}}}{A} . length of the second coil l1=2πr2{l_1} = 2\pi {r_2} .
So, R2=ρ2πr2A{R_2} = \dfrac{{\rho 2\pi {r_2}}}{A}
Therefore, by Ohm's law we can find the voltage across the first coil, V1=i1R1{V_1} = {i_1}{R_1} . Putting the values,
V1=2i2ρ2π(2r2)A{V_1} = 2{i_2}\dfrac{{\rho 2\pi (2{r_2})}}{A} .
voltage across secondary coil, V2=i2R2{V_2} = {i_2}{R_2} . Putting the values, V2=i2ρ2πr2A{V_2} = {i_2}\dfrac{{\rho 2\pi {r_2}}}{A}
Hence, ratios of their voltages is, V1V2=2i2ρ2π(2r2)Ai2ρ2πr2A\dfrac{{{V_1}}}{{{V_2}}} = \dfrac{{2{i_2}\dfrac{{\rho 2\pi (2{r_2})}}{A}}}{{{i_2}\dfrac{{\rho 2\pi {r_2}}}{A}}}
Or, V1V2=2i2ρ2π(2r2)i2ρ2πr2\dfrac{{{V_1}}}{{{V_2}}} = \dfrac{{2{i_2}\rho 2\pi (2{r_2})}}{{{i_2}\rho 2\pi {r_2}}}
Or, V1V2=2i2(2r2)i2r2\dfrac{{{V_1}}}{{{V_2}}} = \dfrac{{2{i_2}(2{r_2})}}{{{i_2}{r_2}}}
So, it becomes,
V1V2=41\dfrac{{{V_1}}}{{{V_2}}} = \dfrac{4}{1}
Therefore, V1=4V2{V_1} = 4{V_2} .
So, we have to apply a voltage across the first coil that should be four times of the second coil for the magnetic field to be the same.
Hence, option (A) is correct.

Note :
Magnetic field due to any circular coil at its centre depends on the current flowing through it and the radius of the coil. The more the current the more the intensity of the magnetic coil is, less the radius more the magnetic field at the centre of the coil.
Helmholtz coils is an arrangement of similar coils of the same radius to produce a homogeneous magnetic field . Difference is only that we calculate the magnetic field on the axis of it to get a homogenous magnetic field along that region.