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the angle between of the electric dipole...

the angle between of the electric dipolemoment `p` and the electric field `E` when the dipole is in stable equilibrium

A

`0`

B

`pi//4`

C

`pi//2`

D

`pi`

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The correct Answer is:
To determine the angle between the electric dipole moment \( \mathbf{p} \) and the electric field \( \mathbf{E} \) when the dipole is in stable equilibrium, we can follow these steps: ### Step-by-Step Solution: 1. **Understanding Electric Dipole and Torque**: - An electric dipole consists of two equal and opposite charges separated by a distance. The dipole moment \( \mathbf{p} \) is a vector quantity that points from the negative charge to the positive charge. - When placed in an electric field \( \mathbf{E} \), the dipole experiences a torque \( \tau \) given by the equation: \[ \tau = \mathbf{p} \times \mathbf{E} = pE \sin \theta \] where \( \theta \) is the angle between \( \mathbf{p} \) and \( \mathbf{E} \). 2. **Condition for Equilibrium**: - For the dipole to be in equilibrium, the net torque acting on it must be zero. This occurs when the dipole moment \( \mathbf{p} \) is aligned with the electric field \( \mathbf{E} \) or directly opposite to it. 3. **Analyzing Angles**: - The torque is zero when \( \theta = 0^\circ \) (dipole aligned with the field) or \( \theta = 180^\circ \) (dipole anti-aligned with the field). However, we need to determine which of these positions corresponds to stable equilibrium. 4. **Stable vs. Unstable Equilibrium**: - **Stable Equilibrium**: If the dipole is slightly displaced from its equilibrium position and experiences a restoring torque that brings it back to equilibrium, it is in stable equilibrium. This occurs at \( \theta = 0^\circ \). - **Unstable Equilibrium**: If the dipole is slightly displaced and experiences a torque that moves it further away from equilibrium, it is in unstable equilibrium. This occurs at \( \theta = 180^\circ \). 5. **Conclusion**: - Therefore, the angle between the electric dipole moment \( \mathbf{p} \) and the electric field \( \mathbf{E} \) when the dipole is in stable equilibrium is: \[ \theta = 0^\circ \]
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