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A magnet of moment 4Am^(2) is kept suspe...

A magnet of moment `4Am^(2)` is kept suspended in a magnetic field of induction `5xx10^(-5)T`. The workdone in rotating it through `180^(@)` is

A

`4xx10^(-4) J`

B

`5xx10^(-4) J`

C

`2xx10^(-4) J`

D

`10^(-4) J`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem of calculating the work done in rotating a magnet of moment \( M = 4 \, \text{Am}^2 \) through an angle of \( 180^\circ \) in a magnetic field of induction \( B = 5 \times 10^{-5} \, \text{T} \), we can follow these steps: ### Step-by-Step Solution: 1. **Understanding the Torque**: The torque \( \tau \) experienced by a magnetic dipole in a magnetic field is given by: \[ \tau = M \cdot B \cdot \sin(\theta) \] where \( M \) is the magnetic moment, \( B \) is the magnetic field induction, and \( \theta \) is the angle between the magnetic moment and the magnetic field. 2. **Setting Up the Work Done**: The work done \( W \) in rotating the magnet from an angle \( \theta_1 \) to \( \theta_2 \) is given by: \[ W = \int_{\theta_1}^{\theta_2} \tau \, d\theta \] For our case, we are rotating from \( \theta = 0^\circ \) to \( \theta = 180^\circ \) (which is \( \pi \) radians). 3. **Substituting the Torque Expression**: Substitute the expression for torque into the work done formula: \[ W = \int_{0}^{\pi} M \cdot B \cdot \sin(\theta) \, d\theta \] 4. **Calculating the Integral**: The integral of \( \sin(\theta) \) is: \[ \int \sin(\theta) \, d\theta = -\cos(\theta) \] Therefore, we have: \[ W = M \cdot B \left[-\cos(\theta)\right]_{0}^{\pi} \] Evaluating this from \( 0 \) to \( \pi \): \[ W = M \cdot B \left[-\cos(\pi) + \cos(0)\right] \] Since \( \cos(\pi) = -1 \) and \( \cos(0) = 1 \): \[ W = M \cdot B \left[-(-1) + 1\right] = M \cdot B \left[1 + 1\right] = 2MB \] 5. **Substituting the Values**: Now substitute the values of \( M \) and \( B \): \[ W = 2 \cdot 4 \, \text{Am}^2 \cdot 5 \times 10^{-5} \, \text{T} \] \[ W = 40 \times 10^{-5} \, \text{J} \] \[ W = 4 \times 10^{-4} \, \text{J} \] ### Final Answer: The work done in rotating the magnet through \( 180^\circ \) is: \[ W = 4 \times 10^{-4} \, \text{J} \]
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