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The potential energy of a particle in a ...

The potential energy of a particle in a force field is:
`U = (A)/(r^(2)) - (B)/(r )`,. Where `A` and `B` are positive
constants and `r` is the distance of particle from the centre of the field. For stable equilibrium the distance of the particle is

A

B/2A

B

2A/B

C

A/B

D

B/A

Text Solution

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The correct Answer is:
To find the distance of the particle from the center of the force field for stable equilibrium, we start with the given potential energy function: \[ U = \frac{A}{r^2} - \frac{B}{r} \] where \( A \) and \( B \) are positive constants, and \( r \) is the distance from the center of the field. ### Step 1: Find the force from the potential energy The force \( F \) associated with a potential energy \( U \) is given by: \[ F = -\frac{dU}{dr} \] ### Step 2: Differentiate the potential energy We need to differentiate \( U \) with respect to \( r \): \[ U = \frac{A}{r^2} - \frac{B}{r} \] Differentiating \( U \): \[ \frac{dU}{dr} = \frac{d}{dr}\left(\frac{A}{r^2}\right) - \frac{d}{dr}\left(\frac{B}{r}\right) \] Using the power rule for differentiation: \[ \frac{d}{dr}\left(\frac{A}{r^2}\right) = -2A \cdot r^{-3} = -\frac{2A}{r^3} \] \[ \frac{d}{dr}\left(\frac{B}{r}\right) = -B \cdot r^{-2} = -\frac{B}{r^2} \] Thus, \[ \frac{dU}{dr} = -\frac{2A}{r^3} + \frac{B}{r^2} \] ### Step 3: Set the force to zero for stable equilibrium For stable equilibrium, the net force must be zero: \[ -\frac{dU}{dr} = 0 \] This leads to: \[ -\left(-\frac{2A}{r^3} + \frac{B}{r^2}\right) = 0 \] So we have: \[ \frac{2A}{r^3} = \frac{B}{r^2} \] ### Step 4: Solve for \( r \) Cross-multiplying gives: \[ 2A = Br \] Now, solving for \( r \): \[ r = \frac{2A}{B} \] ### Conclusion The distance of the particle from the center of the force field for stable equilibrium is: \[ r = \frac{2A}{B} \]
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