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Question: Two similar coils of radius \(R\)are lying concentrically with their planes at right angles to each ...

Two similar coils of radius RRare lying concentrically with their planes at right angles to each other. The currents flowing in them are IIand 2I2Irespectively. The resultant magnetic field induction at the centre will be
A) μ0I2R\dfrac{{{\mu }_{0}}I}{2R}
B) μ0IR\dfrac{{{\mu }_{0}}I}{R}
C) 5μ0I2R\dfrac{\sqrt{5}{{\mu }_{0}}I}{2R}
D) 3μ0I2R\dfrac{3{{\mu }_{0}}I}{2R}

Explanation

Solution

Concentric circles have a common centre. Similarly, concentric coils have a common centre. Magnetic field induction refers to the production of electromotive force across a current carrying conductor in a changing magnetic field.

Complete step by step answer:
When current is passed through a coil, a magnetic field is created in the coil. This magnetic field restricts the current to flow through the coil. Here, in this question, two coils of the same radius RR are used. It is said that both the coils are concentric, but the planes of the coils are at right angles. This suggests that both the coils have a common centre, but the planes of the coils are perpendicular to each other. We are supposed to find the magnetic field induction at the common centre of both the coils.

From Biot-Savart law, we know that magnetic field induction at the centre of a current carrying coil is given by
Bcentre=μ0I2R{{B}_{centre}}=\dfrac{{{\mu }_{0}}I}{2R}
where
Bcentre{{B}_{centre}} is the magnetic field induction at the centre of a coil
μ0{{\mu }_{0}} is the magnetic constant of permeability in free space
II is the current flowing through the coil
RR is the radius of the coil
Let this be equation 1.
From the question, we are provided that currents flowing in both the coils of same radius RR are II and 2I2I respectively. Let the magnetic field induction at the centre due to the first coil be Bc1{{B}_{c1}} and the magnetic field induction at the centre due to the second coil be Bc2{{B}_{c2}}. Let the total magnetic field at the common centre due to both the coils be Btotal{{B}_{total}}. It is clear that the total magnetic induction at the common centre is nothing but the resultant magnetic field due to both the coils and is given by
Btotal=Bc12+Bc22{{B}_{total}}=\sqrt{{{B}_{c1}}^{2}+{{B}_{c2}}^{2}}
Let this be equation 2.
Applying equation 1 in both the coils, we have
Bc1=μ0I2R{{B}_{c1}}=\dfrac{{{\mu }_{0}}I}{2R}
where Bc1{{B}_{c1}} is the magnetic induction at the common centre due to the coil through which a current IIflows. Let this be equation 3.
Bc2=μ0(2I)2R{{B}_{c2}}=\dfrac{{{\mu }_{0}}(2I)}{2R}
where Bc2{{B}_{c2}} is the magnetic induction at the common centre due to the coil through which a current 2I2I flows. Let this be equation 4.
Observing both the equations above clearly, it is seen that
Bc2=2Bc1{{B}_{c2}}=2{{B}_{c1}}
Let this be equation 5.
Now, the resultant magnetic induction at the common centre due to both the coils (equation 1) can be expressed as
Btotal=Bc12+Bc22=(Bc1)2+(2Bc1)2=5Bc12=5Bc1{{B}_{total}}=\sqrt{{{B}_{c1}}^{2}+{{B}_{c2}}^{2}}=\sqrt{{{({{B}_{c1}})}^{2}}+{{(2{{B}_{c1}})}^{2}}}=\sqrt{5{{B}_{c1}}^{2}}=\sqrt{5}{{B}_{c1}}
Substituting the value of Bc1{{B}_{c1}} from equation 3 in the above equation, we have
Btotal=5Bc1=5μ0I2R{{B}_{total}}=\sqrt{5}{{B}_{c1}}=\sqrt{5}\dfrac{{{\mu }_{0}}I}{2R}
Therefore, the resultant magnetic field induction at the centre is given by
Btotal=5μ0I2R{{B}_{total}}=\sqrt{5}\dfrac{{{\mu }_{0}}I}{2R}

So, the correct answer is “Option C”.

Note:
The magnetic field induction at a point on the axis of a coil is different from the magnetic field induction at the centre of the coil. Magnetic field induction at a point on the axis of a coil is given by
Baxis=μ0IR22(R2+x2)32{{B}_{axis}}=\dfrac{{{\mu }_{0}}I{{R}^{2}}}{2{{({{R}^{2}}+{{x}^{2}})}^{\dfrac{3}{2}}}}
where xx is the distance of the point on the axis from the centre of coil.
Students can expect questions on this equation too. It is important to remember both the equations of magnetic field induction at the centre as well as a point on the axis to crack the questions on magnetic induction in a coil, easily.