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A square loop of side 10 cm and resistan...

A square loop of side 10 cm and resistance 0.5 `Omega` is placed vertically in the East-West plane. A uniform magnetic field of 0.10 T is set-up across the plane in the North-East direction. The magnetic field is decreased to zero in 0.70 sat a steady rate. The magnitudes of induced emf and current during this time interval are

A

0.1mV,2V

B

1mV,2mV

C

1V,2A

D

1mV,0.2A

Text Solution

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The correct Answer is:
To solve the problem, we will follow these steps: ### Step 1: Understand the parameters given in the problem - Side of the square loop, \( a = 10 \, \text{cm} = 0.1 \, \text{m} \) - Resistance of the loop, \( R = 0.5 \, \Omega \) - Initial magnetic field, \( B_i = 0.1 \, \text{T} \) - Final magnetic field, \( B_f = 0 \, \text{T} \) - Time interval for the change in magnetic field, \( \Delta t = 0.7 \, \text{s} \) ### Step 2: Calculate the area of the square loop The area \( A \) of the square loop is given by: \[ A = a^2 = (0.1 \, \text{m})^2 = 0.01 \, \text{m}^2 \] ### Step 3: Calculate the initial magnetic flux The magnetic flux \( \Phi \) through the loop is given by: \[ \Phi = B \cdot A \cdot \cos(\theta) \] Since the magnetic field is in the North-East direction and the loop is in the East-West plane, the angle \( \theta \) between the magnetic field and the area vector is \( 45^\circ \). Thus, \( \cos(45^\circ) = \frac{1}{\sqrt{2}} \). Calculating the initial flux: \[ \Phi_i = B_i \cdot A \cdot \cos(45^\circ) = 0.1 \, \text{T} \cdot 0.01 \, \text{m}^2 \cdot \frac{1}{\sqrt{2}} = 0.000707 \, \text{Wb} \, (\text{Weber}) \] ### Step 4: Calculate the final magnetic flux Since the final magnetic field \( B_f = 0 \, \text{T} \), the final flux is: \[ \Phi_f = B_f \cdot A \cdot \cos(45^\circ) = 0 \cdot 0.01 \cdot \frac{1}{\sqrt{2}} = 0 \, \text{Wb} \] ### Step 5: Calculate the change in magnetic flux The change in magnetic flux \( \Delta \Phi \) is given by: \[ \Delta \Phi = \Phi_f - \Phi_i = 0 - 0.000707 \, \text{Wb} = -0.000707 \, \text{Wb} \] ### Step 6: Calculate the induced EMF According to Faraday's law of electromagnetic induction, the induced EMF \( \mathcal{E} \) is given by: \[ \mathcal{E} = -\frac{\Delta \Phi}{\Delta t} \] Substituting the values: \[ \mathcal{E} = -\frac{-0.000707 \, \text{Wb}}{0.7 \, \text{s}} = \frac{0.000707}{0.7} \approx 0.00101 \, \text{V} \, (\text{or } 1.01 \, \text{mV}) \] ### Step 7: Calculate the induced current Using Ohm's law, the induced current \( I \) can be calculated as: \[ I = \frac{\mathcal{E}}{R} \] Substituting the values: \[ I = \frac{0.00101 \, \text{V}}{0.5 \, \Omega} \approx 0.00202 \, \text{A} \, (\text{or } 2.02 \, \text{mA}) \] ### Final Results - Induced EMF: \( \mathcal{E} \approx 1.01 \, \text{mV} \) - Induced Current: \( I \approx 2.02 \, \text{mA} \)
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