Correct Answer - Option 3 : -38 V
Faraday’s Laws of Electromagnetic Induction:
First Law: It tells us about the condition under which an EMF is induced in a conductor or coil and may be stated as under:
When the magnetic flux linking a conductor or coil changes, an EMF is induced in it.
Second Law: It gives the magnitude of the induced EMF in a conductor or coil and may be stated as under:
The magnitude of the EMF induced in a conductor or coil is directly proportional to the rate of change of flux linkages i.e.
Induced EMF (E) ∝ \(\frac{Nϕ_1-Nϕ_2}{t}\)
In differential form, we have,
E = \(N\frac{dϕ}{dt}\)
The direction of induced EMF is given by Lenz’s law.
The magnitude and direction of induced EMF should be written as:
E = - \(N\frac{dϕ}{dt}\) .... (1)
Consider a magnetic circuit having 'N; numbers of turns, 'A' cross-sectional area, 'L' is the length and current 'I'
We know that,
MMF = NI = ϕS
or, ϕ = \(\frac{NI}{S}\)
Where S is reluctance and given by,
S = \(\frac{L}{μ_oμ_rA}\)
From equation (1),
E = - \(N\frac{d(NI/S)}{dt}\)
or, E = - \(\frac{N^2}{S}\frac{dI}{dt}\) = - \(L\frac{dI}{dt}\)
Application:
Given,
d = 100 mm ⇒ L = πd = 100π mm
N = 600
μr = 4000
A = 500 mm2
Hence,
S = \(\frac{L}{μ_oμ_rA}\) = \(\frac{100\pi\ mm}{4\pi \times 10^{-7}\times 4000\times 500\ mm^2}\)
or, S = \(\frac{L}{μ_oμ_rA}\) = \(\frac{100}{4 \times 10^{-7}\times 4000\times 500\ mm}\)
or, S = \(\frac{L}{μ_oμ_rA}\) = \(\frac{10^{12}}{8 \times10^6}=\frac{10^6}{8}\ H^{-1}\)
Hence, L = \(\frac{N^2}{S}= \frac{600\times 600\times 8}{10^6}=\frac{72}{25}\ H\)
Since, the current is reduced to zero in 60 ms.
Hence, \(\frac{dI}{dt}=\frac{0.8}{60}\times 1000=\frac{80}{6}\)
Hence, E = - \(L\frac{dI}{dt}\) = \(-\frac{72}{25}\times \frac{80}{6}=-\frac{960}{25}=-38.4\ V\)