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Question: A long solenoid of diameter \(0.1m\) has \(2 \times {10^4}\)turns per meter. At the center of the so...

A long solenoid of diameter 0.1m0.1m has 2×1042 \times {10^4}turns per meter. At the center of the solenoid, a coil of 100100 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 0A0A from 4A4A in0.05s0.05s. If the resistance of the coil is 10π2Ω10{\pi ^2}\Omega , the total charge flowing through the coil during this time is:
(a)\left( a \right) 26πμC26\pi \mu C
(b)\left( b \right) 22μC22\mu C
(c)\left( c \right) 16πμC16\pi \mu C
(d)\left( d \right) 32πμC32\pi \mu C

Explanation

Solution

Hint So in this question, the concept of faraday law will be used to solve it. By using the formulaε=Ndϕdt\varepsilon = - N\dfrac{{d\phi }}{{dt}}, and then formatting the formula to get the change in the charge, we will get the total charge flowing through the coil.
Formula used:
According to faraday law
ε=Ndϕdt\varepsilon = - N\dfrac{{d\phi }}{{dt}}
Here,
NN, will be the number of turns

Complete Step By Step Solution In this question, we have the diameter and the number of turns is also given. We have to find the total charge flowing in the coil at that time.
As we know,
ε=Ndϕdt\varepsilon = - N\dfrac{{d\phi }}{{dt}}
Now dividing the above equation withRR, we get
εR=NRdϕdt\Rightarrow \dfrac{\varepsilon }{R} = - \dfrac{N}{R}\dfrac{{d\phi }}{{dt}}
So it can also be written as,
I=NRdϕdt\Rightarrow \vartriangle I = - \dfrac{N}{R}\dfrac{{d\phi }}{{dt}}
And here, the change in current can be written as
qt=NRdϕdt\Rightarrow \dfrac{{\vartriangle q}}{{\vartriangle t}} = - \dfrac{N}{R}\dfrac{{d\phi }}{{dt}}
Now, taking the change in time to the right side, we get
q=[NR(ϕt)]t\Rightarrow \vartriangle q = - \left[ {\dfrac{N}{R}\left( {\dfrac{{\vartriangle \phi }}{{\vartriangle t}}} \right)} \right]\vartriangle t
Here, the negative sign shows us that the change in the flux is opposed by the induced emf.
So from here,
q=μ0niπr2R\Rightarrow \vartriangle q = \dfrac{{{\mu _0}ni\pi {r^2}}}{R}
So, now on substituting the values given in the question, we get
q=4π×107×100×4×π×(0.01)210π2\Rightarrow \vartriangle q = \dfrac{{4\pi \times {{10}^{ - 7}} \times 100 \times 4 \times \pi \times {{\left( {0.01} \right)}^2}}}{{10{\pi ^2}}}
So on simplifying the equation, we get
q=32μC\Rightarrow \vartriangle q = 32\mu C
Therefore, 32μC32\mu C a charge is required through the coil during this time.

Hence the option DD will be the correct choice.

Note When there is a change in attractive transition going through a curl, a prompted emf is delivered which contradicts the reason because of which it is created. That is if motion builds, at that point, there would be an electromotive power delivered in the framework which consistently contradicts the change in attractive flux. The same is genuine when the attractive motion is diminished. Continuously there is a restrict of change (Actually this is the law of nature)