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An electric dipole consists of charges +...

An electric dipole consists of charges `+ 2e and -2e` separated by 0.78mm. It is an electric field of strength `3.4xx10^(6) N//C`. Calculate the magnitude of the torque on the dipole when the dipole moment is (a) parallel to (b) perpendicular to, and (c) antiparallel to the electric field.

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To solve the problem, we need to calculate the torque on an electric dipole in an electric field for three different orientations: parallel, perpendicular, and antiparallel. The torque (\(\tau\)) on a dipole in an electric field is given by the formula: \[ \tau = \mathbf{p} \times \mathbf{E} = pE \sin \theta \] where: - \( \tau \) is the torque, - \( \mathbf{p} \) is the dipole moment, - \( \mathbf{E} \) is the electric field strength, - \( \theta \) is the angle between the dipole moment and the electric field. ### Step 1: Calculate the Dipole Moment (\( p \)) The dipole moment (\( p \)) is calculated using the formula: \[ p = Q \cdot d \] where: - \( Q \) is the magnitude of one of the charges, - \( d \) is the separation between the charges. Given: - \( Q = 2e = 2 \times 1.6 \times 10^{-19} \, \text{C} = 3.2 \times 10^{-19} \, \text{C} \) - \( d = 0.78 \, \text{mm} = 0.78 \times 10^{-3} \, \text{m} \) Calculating \( p \): \[ p = (3.2 \times 10^{-19} \, \text{C}) \times (0.78 \times 10^{-3} \, \text{m}) = 2.496 \times 10^{-22} \, \text{C m} \] ### Step 2: Calculate Torque for Each Case #### Case (a): Dipole Moment Parallel to Electric Field (\( \theta = 0^\circ \)) \[ \tau = pE \sin(0^\circ) = pE \cdot 0 = 0 \] **Torque when parallel = 0 Nm** #### Case (b): Dipole Moment Perpendicular to Electric Field (\( \theta = 90^\circ \)) \[ \tau = pE \sin(90^\circ) = pE \cdot 1 = pE \] Given \( E = 3.4 \times 10^6 \, \text{N/C} \): \[ \tau = (2.496 \times 10^{-22} \, \text{C m}) \times (3.4 \times 10^6 \, \text{N/C}) = 8.49 \times 10^{-16} \, \text{Nm} \] **Torque when perpendicular = \( 8.49 \times 10^{-16} \, \text{Nm} \)** #### Case (c): Dipole Moment Antiparallel to Electric Field (\( \theta = 180^\circ \)) \[ \tau = pE \sin(180^\circ) = pE \cdot 0 = 0 \] **Torque when antiparallel = 0 Nm** ### Final Results - Torque when parallel to electric field: **0 Nm** - Torque when perpendicular to electric field: **\( 8.49 \times 10^{-16} \, \text{Nm} \)** - Torque when antiparallel to electric field: **0 Nm**

To solve the problem, we need to calculate the torque on an electric dipole in an electric field for three different orientations: parallel, perpendicular, and antiparallel. The torque (\(\tau\)) on a dipole in an electric field is given by the formula: \[ \tau = \mathbf{p} \times \mathbf{E} = pE \sin \theta \] where: - \( \tau \) is the torque, ...
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