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If the current in a primary circuit is I...

If the current in a primary circuit is `I=I_(0)` Sin `omegat` and the mutual inductance is M, then the value of induced voltage in secondary circuit will be :-

A

`e=MI_(0) omega Cos omega t`

B

`e=MI_(0) omega Cost omega t`

C

`e=[M omega Cos omegat] //I_(0)`

D

`e=(M omega Cos omega t)//I_(0)`

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The correct Answer is:
To find the induced voltage in the secondary circuit when the current in the primary circuit is given by \( I = I_0 \sin(\omega t) \) and the mutual inductance is \( M \), we can follow these steps: ### Step 1: Understand the relationship between current and induced voltage The induced voltage (or electromotive force, EMF) in the secondary circuit due to a changing current in the primary circuit is given by the formula: \[ E = M \frac{dI}{dt} \] where \( E \) is the induced voltage, \( M \) is the mutual inductance, and \( \frac{dI}{dt} \) is the rate of change of current in the primary circuit. ### Step 2: Differentiate the current function The current in the primary circuit is given by: \[ I = I_0 \sin(\omega t) \] To find \( \frac{dI}{dt} \), we differentiate \( I \) with respect to \( t \): \[ \frac{dI}{dt} = I_0 \frac{d}{dt}(\sin(\omega t)) = I_0 \omega \cos(\omega t) \] Here, we used the chain rule where the derivative of \( \sin(x) \) is \( \cos(x) \) and multiplied by the derivative of \( \omega t \) which is \( \omega \). ### Step 3: Substitute \( \frac{dI}{dt} \) into the induced voltage formula Now, we substitute \( \frac{dI}{dt} \) back into the formula for induced voltage: \[ E = M \frac{dI}{dt} = M \left(I_0 \omega \cos(\omega t)\right) \] This simplifies to: \[ E = M I_0 \omega \cos(\omega t) \] ### Step 4: Final expression for the induced voltage Thus, the induced voltage in the secondary circuit is: \[ E = M I_0 \omega \cos(\omega t) \] ### Conclusion The value of the induced voltage in the secondary circuit is \( M I_0 \omega \cos(\omega t) \). ---
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