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A horizontal rod of mass 10g and length ...

A horizontal rod of mass `10g` and length `10cm` is placed on a smooth plane inclined at an angle of `60^@` with the horizontal with the length of the rod parallel to the edge of the inclined plane. A uniform magnetic field induction B is applied vertically downwards. If the current through the rod is `1*73ampere`, the value of B for which the rod remains stationary on the inclined plane is

A

`1.73` T

B

`(1)/(1.73)`T

C

1.T

D

None of the above

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to find the value of the magnetic field induction \( B \) that keeps the rod stationary on the inclined plane. We will use the balance of forces acting on the rod. ### Step-by-Step Solution: 1. **Identify the Forces Acting on the Rod:** - The weight of the rod \( W = mg \) acts vertically downwards. - The magnetic force \( F_B \) acts perpendicular to the direction of the current and the magnetic field. 2. **Resolve the Weight of the Rod:** - The weight of the rod can be resolved into two components: - Perpendicular to the inclined plane: \( W_{\perp} = mg \cos(60^\circ) \) - Parallel to the inclined plane: \( W_{\parallel} = mg \sin(60^\circ) \) 3. **Magnetic Force on the Rod:** - The magnetic force acting on the rod is given by: \[ F_B = I \cdot L \cdot B \cdot \sin(90^\circ) = I \cdot L \cdot B \] - Since the rod is horizontal and the magnetic field is vertical, the angle between the current direction and the magnetic field is \( 90^\circ \). 4. **Set Up the Equation for Equilibrium:** - For the rod to remain stationary, the magnetic force must balance the component of the weight acting down the incline: \[ F_B = W_{\parallel} \] - Therefore, we have: \[ I \cdot L \cdot B = mg \sin(60^\circ) \] 5. **Substitute Known Values:** - Given: - Mass \( m = 10 \, \text{g} = 10 \times 10^{-3} \, \text{kg} \) - Length \( L = 10 \, \text{cm} = 10 \times 10^{-2} \, \text{m} \) - Current \( I = 1.73 \, \text{A} \) - \( g \approx 10 \, \text{m/s}^2 \) - \( \sin(60^\circ) = \frac{\sqrt{3}}{2} \) - Plugging in the values: \[ 1.73 \cdot (10 \times 10^{-2}) \cdot B = (10 \times 10^{-3}) \cdot 10 \cdot \frac{\sqrt{3}}{2} \] 6. **Simplify the Equation:** - This simplifies to: \[ 1.73 \cdot 10^{-1} \cdot B = 5 \sqrt{3} \times 10^{-3} \] - Rearranging gives: \[ B = \frac{5 \sqrt{3} \times 10^{-3}}{1.73 \times 10^{-1}} \] 7. **Calculate the Value of B:** - Calculating the right-hand side: \[ B = \frac{5 \sqrt{3}}{1.73} \times 10^{-2} \] - Approximating \( \sqrt{3} \approx 1.732 \): \[ B \approx \frac{5 \times 1.732}{1.73} \times 10^{-2} \approx 5 \times 10^{-2} \approx 0.05 \, \text{T} \] 8. **Final Result:** - Thus, the value of \( B \) for which the rod remains stationary on the inclined plane is approximately \( 1 \, \text{T} \).
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