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A current I=20sin(100pit)A is passed in ...

A current `I=20sin(100pit)A` is passed in the first coil, which induces a maximum emf of `10piV` in the second coil. The mutual inductance for the pair of coils is

A

(a)10 mH

B

(b)15 mH

C

(c)25 mH

D

(d)5 mH

Text Solution

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The correct Answer is:
To find the mutual inductance \( M \) between the two coils, we start with the information given in the problem: 1. The current in the first coil is given by: \[ I = 20 \sin(100 \pi t) \, \text{A} \] Here, we can identify: - \( I_0 = 20 \) A (the maximum current) - \( \omega = 100 \pi \) rad/s (the angular frequency) 2. The maximum induced EMF in the second coil is given as: \[ E_{\text{max}} = 10 \pi \, \text{V} \] ### Step 1: Use the formula for induced EMF The induced EMF \( E \) in the second coil due to the changing current in the first coil can be expressed as: \[ E_{\text{max}} = M \frac{dI}{dt} \] where \( M \) is the mutual inductance. ### Step 2: Differentiate the current To find \( \frac{dI}{dt} \), we differentiate the expression for current \( I \): \[ I = 20 \sin(100 \pi t) \] Differentiating with respect to time \( t \): \[ \frac{dI}{dt} = 20 \cdot 100 \pi \cos(100 \pi t) = 2000 \pi \cos(100 \pi t) \] The maximum value of \( \frac{dI}{dt} \) occurs when \( \cos(100 \pi t) = 1 \): \[ \left(\frac{dI}{dt}\right)_{\text{max}} = 2000 \pi \, \text{A/s} \] ### Step 3: Substitute into the EMF formula Now we can substitute this maximum rate of change of current into the EMF formula: \[ E_{\text{max}} = M \cdot (2000 \pi) \] Given that \( E_{\text{max}} = 10 \pi \): \[ 10 \pi = M \cdot (2000 \pi) \] ### Step 4: Solve for mutual inductance \( M \) Dividing both sides by \( \pi \): \[ 10 = M \cdot 2000 \] Now, solving for \( M \): \[ M = \frac{10}{2000} = \frac{1}{200} = 0.005 \, \text{H} = 5 \, \text{mH} \] ### Conclusion Thus, the mutual inductance for the pair of coils is: \[ \boxed{5 \, \text{mH}} \]
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