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Question: The long solenoid of diameter \(0.1m\) has \(2\times {{10}^{4}}\) turns per metre. At the centre of ...

The long solenoid of diameter 0.1m0.1m has 2×1042\times {{10}^{4}} turns per metre. At the centre of the solenoid, a coil of 100 turns and radius 0.01m0.01m is placed with its axis coinciding with the solenoid axis. The current in the solenoid reduces at a constant rate to 0 A from 4 A in 0.05s. If the resistance of the coil is 10π2Ω10{{\pi }^{2}}\Omega , the total charge flowing through the coil during this time is.
A. 32πμC32\pi \mu C
B. 16μC16\mu C
C. 32μC32\mu C
D. 16πμC16\pi \mu C

Explanation

Solution

Use the electro-magnetic concept that when the magnetic flux through a coil changes with time, an emf is induced in the coil. Find an expression for the emf. Then use ohm’s law and find an expression for the current in the coil. Later, find the charge flown through the coil in the given time.
Formula used:
B=μ0niB={{\mu }_{0}}ni
ϕ=NBA\phi =NBA
E=dϕdtE=\dfrac{d\phi }{dt}
E=iRE=i'R
i=ΔqΔti'=\dfrac{\Delta q}{\Delta t}

Complete step by step answer:
In this case, the current in the solenoid will produce a constant magnetic field at its centre which is equal to B=μ0niB={{\mu }_{0}}ni, where μ0{{\mu }_{0}} is permeability of free space, n is the number of turn per unit length of the solenoid and i is the current in the solenoid.
This magnetic field is passing through the coil which is located at the centre of the solenoid.
Therefore, there is some magnetic flux through this coil.
The flux through a coil due to a constant magnetic field is given as ϕ=NBA\phi =NBA, where N is number of turns of the coil, B is the magnetic field and A is the area enclosed by the coil.
In this case, B=μ0niB={{\mu }_{0}}ni and the area enclosed by the solenoid is A=πr2A=\pi {{r}^{2}}, where r is the radius of the small coil.
ϕ=Nμ0ni(πr2)=Nμ0πnr2i\Rightarrow \phi =N{{\mu }_{0}}ni(\pi {{r}^{2}})=N{{\mu }_{0}}\pi n{{r}^{2}}i …. (i)
When the current in the solenoid changes, the flux through the coil changes. As a result, an emf is induced in the coil.
The induced emf in the coil is equal to E=dϕdtE=\dfrac{d\phi }{dt}.
E=dϕdt=ddt(Nμ0πnr2i)\Rightarrow E=\dfrac{d\phi }{dt}=\dfrac{d}{dt}\left( N{{\mu }_{0}}\pi n{{r}^{2}}i \right)
Here, all the variables are constant except the current (i) in the solenoid.
E=Nμ0πnr2didt\Rightarrow E=N{{\mu }_{0}}\pi n{{r}^{2}}\dfrac{di}{dt} …. (ii).
It is given that the current in the solenoid reduces at a constant rate to 0 A from 4 A in 0.05s.
didt=40.05=80As1\Rightarrow \dfrac{di}{dt}=\dfrac{4}{0.05}=80A{{s}^{-1}}.
And according to the given data N=100N=100, n=2×104m1n=2\times {{10}^{4}}{{m}^{-1}}, r=0.01mr=0.01m.
The value of μ0=4π×107NA2{{\mu }_{0}}=4\pi \times {{10}^{-7}}N{{A}^{-2}}.
Substitute the values in (ii).
E=100(4π×107)π(2×104)(0.01)2(80)\Rightarrow E=100(4\pi \times {{10}^{-7}})\pi (2\times {{10}^{4}}){{(0.01)}^{2}}(80).
And from ohm’s law we know that E=iRE=i'R , where i’ is the current in the coil produced due to the emf and R is the resistance of the coil.
This means that i=ERi'=\dfrac{E}{R}. ….. (iii)
Since E is constant, i’ is constant.
Therefore, we can write i=ΔqΔti'=\dfrac{\Delta q}{\Delta t}, where Δq\Delta q is the flow of charge in time Δt\Delta t.
Substitute this value in (iii).
ΔqΔt=ER\Rightarrow \dfrac{\Delta q}{\Delta t}=\dfrac{E}{R}
Δq=ERΔt\Rightarrow \Delta q=\dfrac{E}{R}\Delta t
Here, Δt=0.05s\Delta t=0.05s and R=10π2ΩR=10{{\pi }^{2}}\Omega .
Substitute these values and the value of E in the above equation.
Δq=E=100(4π×107)π(2×104)(0.01)2(80)10π2(0.05)=32×106C=32μC\Rightarrow \Delta q=\dfrac{\Rightarrow E=100(4\pi \times {{10}^{-7}})\pi (2\times {{10}^{4}}){{(0.01)}^{2}}(80)}{10{{\pi }^{2}}}(0.05)=32\times {{10}^{-6}}C=32\mu C.
This means that the charge flown through the coil in the given time is 32μC32\mu C.
Hence, the correct option is C.

Note: You may have seen the emf induced in a coil due to the change in magnetic flux through the coil is given as E=dϕdtE=-\dfrac{d\phi }{dt}.
Here, the negative sign simply indicates that the emf induced opposes the change in current or magnetic flux. This means that the emf is induced in such that a way that it opposes the change in magnetic flux that occurs. We do not need to use the negative sign while solving problems as we are only interested in the magnitude of the emf.