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A coil of 100 turns and area 2 xx 10^(-2...

A coil of `100` turns and area `2 xx 10^(-2) m^(2)`, pivoted about a vertical diameter in a uniform magnetic field carries a current of `5A`. When the coil is held with its plane in North-South direction, it experiences a torque of `0.3 N//m`. When the plane is in East-West direction the torque is `0.4 Nm`. The value of magnetic induction is (Neglect earth's magnetic field)

A

`0.12T`

B

`0.03T`

C

`0.14T`

D

None of these

Text Solution

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The correct Answer is:
To solve the problem, we need to find the value of the magnetic induction (B) given the torque experienced by a coil in two different orientations in a magnetic field. ### Step-by-Step Solution: 1. **Understanding the Torque Formula**: The torque (\( \tau \)) experienced by a coil in a magnetic field is given by the formula: \[ \tau = N \cdot I \cdot A \cdot B \cdot \sin(\theta) \] where: - \( N \) = number of turns in the coil - \( I \) = current through the coil - \( A \) = area of the coil - \( B \) = magnetic induction - \( \theta \) = angle between the magnetic field and the normal to the coil's plane 2. **Torque in North-South Direction**: When the coil is in the North-South direction, the angle \( \theta \) is \( 90^\circ \) (since the area vector is perpendicular to the magnetic field). Therefore, \( \sin(90^\circ) = 1 \): \[ \tau_1 = N \cdot I \cdot A \cdot B_1 \] Given \( \tau_1 = 0.3 \, \text{Nm} \), \( N = 100 \), \( I = 5 \, \text{A} \), and \( A = 2 \times 10^{-2} \, \text{m}^2 \): \[ 0.3 = 100 \cdot 5 \cdot (2 \times 10^{-2}) \cdot B_1 \] Simplifying this: \[ 0.3 = 1000 \cdot (2 \times 10^{-2}) \cdot B_1 \] \[ 0.3 = 20 \cdot B_1 \] \[ B_1 = \frac{0.3}{20} = 0.015 \, \text{T} \] 3. **Torque in East-West Direction**: When the coil is in the East-West direction, the angle \( \theta \) is \( 0^\circ \) (the area vector is parallel to the magnetic field). Therefore, \( \sin(0^\circ) = 0 \): \[ \tau_2 = N \cdot I \cdot A \cdot B_2 \cdot \sin(0^\circ) \] Given \( \tau_2 = 0.4 \, \text{Nm} \): \[ 0.4 = N \cdot I \cdot A \cdot B_2 \] Here, \( \tau_2 = 0.4 \): \[ 0.4 = 100 \cdot 5 \cdot (2 \times 10^{-2}) \cdot B_2 \] Simplifying this: \[ 0.4 = 1000 \cdot (2 \times 10^{-2}) \cdot B_2 \] \[ 0.4 = 20 \cdot B_2 \] \[ B_2 = \frac{0.4}{20} = 0.02 \, \text{T} \] 4. **Finding the Resultant Magnetic Field**: Since the two magnetic fields \( B_1 \) and \( B_2 \) are perpendicular to each other, we can find the resultant magnetic induction \( B \) using the Pythagorean theorem: \[ B = \sqrt{B_1^2 + B_2^2} \] Substituting the values: \[ B = \sqrt{(0.015)^2 + (0.02)^2} \] \[ B = \sqrt{0.000225 + 0.0004} \] \[ B = \sqrt{0.000625} = 0.025 \, \text{T} \] ### Final Answer: The value of magnetic induction \( B \) is \( 0.025 \, \text{T} \).
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