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Two short electric dipoles having dipole...

Two short electric dipoles having dipole moment `p_(1)" and "p_(2)` are placed co-axially and uni-directionally, at a distance r apart. Calculate nature and magnitude of force between them :

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To solve the problem of finding the nature and magnitude of the force between two short electric dipoles placed coaxially and unidirectionally at a distance \( r \) apart, we can follow these steps: ### Step-by-Step Solution: 1. **Understanding the Configuration**: - We have two dipoles, \( \mathbf{p_1} \) and \( \mathbf{p_2} \), placed along the same axis (coaxially) and pointing in the same direction (unidirectionally). - The distance between the two dipoles is \( r \). 2. **Potential Energy of the Dipoles**: - The potential energy \( U \) between two dipoles can be expressed as: \[ U = -\frac{1}{4 \pi \epsilon_0} \cdot \frac{2 \mathbf{p_1} \cdot \mathbf{p_2}}{r^3} \] - Since both dipoles are aligned in the same direction, the angle \( \theta \) between \( \mathbf{p} \) and the electric field \( \mathbf{E} \) is \( 0^\circ \), and thus \( \cos(0^\circ) = 1 \). 3. **Electric Field Due to a Dipole**: - The electric field \( \mathbf{E} \) at a distance \( r \) due to dipole \( \mathbf{p_2} \) acting on dipole \( \mathbf{p_1} \) is given by: \[ \mathbf{E} = \frac{1}{4 \pi \epsilon_0} \cdot \frac{2 \mathbf{p_2}}{r^3} \] 4. **Substituting Electric Field into Potential Energy**: - Substitute the expression for \( \mathbf{E} \) into the potential energy formula: \[ U = -\mathbf{p_1} \cdot \mathbf{E} = -\mathbf{p_1} \cdot \left( \frac{1}{4 \pi \epsilon_0} \cdot \frac{2 \mathbf{p_2}}{r^3} \right) \] - Thus, we have: \[ U = -\frac{1}{4 \pi \epsilon_0} \cdot \frac{2 \mathbf{p_1} \cdot \mathbf{p_2}}{r^3} \] 5. **Calculating the Force**: - The force \( \mathbf{F} \) between the dipoles can be found by taking the derivative of the potential energy with respect to the distance \( r \): \[ F = -\frac{dU}{dr} \] - Differentiating \( U \): \[ F = -\frac{d}{dr}\left(-\frac{1}{4 \pi \epsilon_0} \cdot \frac{2 \mathbf{p_1} \cdot \mathbf{p_2}}{r^3}\right) \] - This results in: \[ F = \frac{6 \mathbf{p_1} \cdot \mathbf{p_2}}{4 \pi \epsilon_0 r^4} \] 6. **Nature of the Force**: - The force is positive, indicating that the force is attractive since the potential energy is negative. Therefore, the nature of the force between the dipoles is attractive. ### Final Result: - The magnitude of the force between the two dipoles is: \[ F = \frac{6 \mathbf{p_1} \cdot \mathbf{p_2}}{4 \pi \epsilon_0 r^4} \] - The nature of the force is **attractive**.
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