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Question: A long circular tube of length \(10m\) and radius \(0.3m\) carries a current \(I\) along its curved ...

A long circular tube of length 10m10m and radius 0.3m0.3m carries a current II along its curved surface as shown. A loop created of wire of radius 0.1m0.1m and a resistance 0.05Ω0.05\Omega has been kept inside the tube with its axis coinciding with the axis of the tube. The current varies as I=I0cos(300t)I=I_0 cos(300t) where I0I_0 is constant. If the magnetic moment of the loop is Nμ0I0sin(300t)N\mu_0 I_0 sin(300t), then N'N' is
A.6 B.7 C.8 D.9 \begin{aligned} & A.6 \\\ & B.7 \\\ & C.8 \\\ & D.9 \\\ \end{aligned}

Explanation

Solution

The first step should be to find out the magnetic field inside the circular tube due to the current flowing along its curved surface. Then, from that value of magnetic field, we can calculate the flux linking the wire loop. With the flux, we can calculate the emf induced and then we will get the current induced in it by dividing the emf by the loop resistance. Then, by using the magnetic moment formula we will get the answer.
Formula used:
Magnetic field inside the tube,
B=μ0ILB=\dfrac{\mu_0 I}{L}
Flux linked in a wire loop,
ϕ=Bπr2\phi =B\pi r^2
Emf induced,
ε=dϕdt\varepsilon = \dfrac{d\phi}{dt}
Magnetic moment,
M=πIr2M=\pi I r^2

Complete answer:
We have been given that the length, LL and radius, RR of the circular tube is 10m10m and 0.3m0.3m respectively. The current flowing through its curved surface is II, which varies as I=I0cos(300t)I=I_0 cos(300t) with I0I_0 being a constant.
Now, using the Ampere’s circuital law, the magnetic field inside the tube can be written as
B=μ0ILB=\dfrac{\mu_0 I}{L},
And also, the flux linking the wire loop will be
ϕ=Bπr2\phi =B\pi r^2
Where rr be the radius of the wire loop placed inside the tube.
So,
ϕ=μ0ILπr2=μ0πr2I0cos300tL\phi = \dfrac{\mu_0 I}{L}\pi r^2=\dfrac{\mu_0 \pi r^2 I_0 cos300t}{L}
Since, induced emf in a loop is given by,
ε=dϕdt=ddt(μ0Lπr2I0cos300t)\varepsilon = \dfrac{d\phi}{dt}=-\dfrac{d}{dt}\left(\dfrac{\mu_0}{L}\pi r^2 I_0 cos300t\right)
    ε=μ0πr2I0300sin300tL\implies \varepsilon=\dfrac{\mu_0 \pi r^2 I_0 300sin300t}{L}
Therefore, current induced in the loop will be,
i=εri=\dfrac{\varepsilon }{r'}
Where r{r}' is the resistance of the loop.
i=μ0πr2I0300sin300tLr\therefore i=\dfrac{{{\mu }_{0}}\pi {{r}^{2}}{{I}_{0}}300sin300t}{Lr'}
Since, magnetic moment of the loop is given by,
M=πIr2M=\pi I r^2
M=300π2r4μ0I0sin300tLr\Rightarrow M=\dfrac{300{{\pi }^{2}}{{r}^{4}}{{\mu }_{0}}{{I}_{0}}sin300t}{Lr'}
Now, let us substitute the given values and taking
π2=10\pi^2 =10
M=300×10×(0.1)410×0.005μ0I0sin300t=6μ0I0sin300t\Rightarrow M=\dfrac{300\times 10\times (0.1)^4}{10\times 0.005}\mu_0 I_0 sin300t=6\mu_0 I_0 sin300t
Comparing this term with the one given in the question, we get
N=6N=6

So, the correct answer is “Option A”.

Note:
Initially, there is no current flowing in the wire loop. The magnetic field produced by the circular tube will induce an emf inside the loop and because of that, there will be current. The value of emf can vary with the position of the loop.