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Question: Two identical loops \(P\) and \(Q\) each of radius \(5cm\) are lying in perpendicular planes such th...

Two identical loops PP and QQ each of radius 5cm5cm are lying in perpendicular planes such that they have a common centre as shown in the figure. Find the magnitude and direction of the net magnetic field at the common center of the two coils, if they carry currents equal to 3A3A and 4A4A respectively.

Explanation

Solution

Hint We are given here with two similar loops with some amount of current flowing through it. We are asked to calculate the magnitude and direction of the net magnetic field on their common centre. Thus, we will use the formula for magnetic field due to a current carrying loop.
Formulae Used
B=μoI2RB = \dfrac{{{\mu _o}I}}{{2R}}
Where, BB is the magnetic field on the point, II is the current flowing through the loop and RR is the radius of the loop.

Complete Step By Step Solution
Here,
We redraw the diagram taking into account the flow of the current in the two.

Now,
We use the right hand thumb rule and then find the magnetic field on the centre due to the individual loops.
Thus,
The diagram turns out to be

BP{B_P} is the magnetic field on the centre due to loopPP.
BQ{B_Q} is the magnetic field due to loopQQ.
And, Bnet{B_{net}} is the net magnetic field on the common centre.
θ\theta is the direction of the net magnetic field. Basically, the angle of the net magnetic field with the horizontal.
Now,
As per the formula,
Bp=μo(3)2(5×102){B_p} = \dfrac{{{\mu _o}(3)}}{{2(5 \times {{10}^{ - 2}})}}
BQ=μo(4)2(5×102){B_Q} = \dfrac{{{\mu _o}(4)}}{{2\left( {5 \times {{10}^{ - 2}}} \right)}}
Thus,
Bnet=BP2+BQ2{B_{net}} = \sqrt {{B_P}^2 + {B_Q}^2}
Thus, substituting the values in the formula, we get
Bnet=μo2(5×102)32+42{B_{net}} = \dfrac{{{\mu _o}}}{{2\left( {5 \times {{10}^{ - 2}}} \right)}}\sqrt {{3^2} + {4^2}}
Thus, we get
Bnet=μo2×102{B_{net}} = \dfrac{{{\mu _o}}}{{2 \times {{10}^{ - 2}}}}
We know,
μo=4π×107{\mu _o} = 4\pi \times {10^{ - 7}}
Thus, we get
Bnet=2π×107×102{B_{net}} = 2\pi \times {10^{ - 7}} \times {10^2}
Thus, we get the magnitude as
Bnet=2π×105T{B_{net}} = 2\pi \times {10^{ - 5}}T
Now,
For finding the direction, we proceed with
tanθ=BPBQ\tan \theta = \dfrac{{{B_P}}}{{{B_Q}}}
Substituting the values of BP{B_P} andBQ{B_Q}, we get
tanθ=34\tan \theta = \dfrac{3}{4}
Thus, we get
θ=tan1(34)\theta = {\tan ^{ - 1}}\left( {\dfrac{3}{4}} \right)

Note Here we have considered the direction of the flow of current as per the diagram above. But if the directions were something different from our direction, though the methodology remained the same. The magnitude would be calculated to be the same but the direction will differ by a general branch value of tan1(0){\tan ^{ - 1}}\left( 0 \right).