A point particle of charge \( Q \) is located at \( P \) along the axis of an electric dipole 1 at a distance \( r \) as shown in the figure. The point \( P \) is also on the equatorial plane of a second electric dipole 2 at a distance \( r \). The dipoles are made of opposite charge \( q \) separated by a distance \( 2a \). For the charge particle at \( P \) not to experience any net force, which of the following correctly describes the situation?
We are given the setup of two electric dipoles, and the task is to determine the value of \( \frac{a}{r} \) when the net force on the charge \( Q \) is zero.
Step 1: Force due to dipole 1 The electric field due to dipole 1 along its axis is given by: \[ E_1 = \frac{kq}{(r - a)^3} \] The force on the charge \( Q \) due to this field is: \[ F_1 = Q \cdot E_1 = Q \cdot \frac{kq}{(r - a)^3} \]
Step 2: Force due to dipole 2 The electric field due to dipole 2 in the equatorial plane is: \[ E_2 = \frac{kq}{(r + a)^3} \] The force on the charge \( Q \) due to this field is: \[ F_2 = Q \cdot E_2 = Q \cdot \frac{kq}{(r + a)^3} \]
Step 3: Condition for no net force For the net force to be zero, the forces from the two dipoles must cancel each other out: \[ F_1 = F_2 \] Substituting the expressions for the forces: \[ \frac{kq}{(r - a)^3} = \frac{kq}{(r + a)^3} \] Simplifying the equation: \[ (r + a)^3 = (r - a)^3 \]
Step 4: Solving for \( \frac{a}{r} \) Expanding both sides of the equation: \[ (r + a)^3 = r^3 + 3r^2a + 3ra^2 + a^3 \] \[ (r - a)^3 = r^3 - 3r^2a + 3ra^2 - a^3 \] Setting these equal to each other: \[ r^3 + 3r^2a + 3ra^2 + a^3 = r^3 - 3r^2a + 3ra^2 - a^3 \] Simplifying: \[ 6r^2a + 2a^3 = 0 \] Thus: \[ r^2a = - \frac{a^3}{3} \] \[ 4ra = 2a^3 \] Finally, solving for \( \frac{a}{r} \), we find: \[ \frac{a}{r} \sim 3 \] Thus, the correct answer is option (4).