To determine the distance from dipole \( A \) at which both dipoles \( A \) and \( B \) produce the same potential, we need to use the formula for the electric potential \( V \) due to a dipole at a point along its axial line:
V = \frac{1}{4\pi \varepsilon_0} \cdot \frac{\vec{d} \cdot \hat{r}}{r^2}
Since dipoles \( A \) and \( B \) are aligned along the x-axis with dipole moments \( \vec{d}_A = - 4 \,qa \,\hat{i}\) and \( \vec{d}_B = - 2 \,qa\, \hat{i} \), consider a point \( P \) at a distance \( x \) from dipole \( A \) where x \lt R (as both dipoles produce equal potential at that point).
Step 1: Calculate the potential at point \( P \) due to dipole \( A \)
Electric potential at distance \( x \) due to dipole \( A \):
V_A = \frac{-4 \,qa}{4\pi \varepsilon_0 \, x^2}
Step 2: Calculate the potential at point \( P \) due to dipole \( B \)
The distance from dipole \( B \) is \( R - x \).
Electric potential at distance \( R - x \) due to dipole \( B \):
V_B = \frac{-2 \,qa}{4\pi \varepsilon_0 \, (R - x)^2}
Step 3: Set the potentials equal
For the potential due to both dipoles to be equal at point \( P \), equate \( V_A \) and \( V_B \):
\frac{-4 \,qa}{x^2} = \frac{-2 \,qa}{(R - x)^2}
Canceling the common terms and simplifying:
\frac{4}{x^2} = \frac{2}{(R-x)^2}
\frac{2}{x^2} = \frac{1}{(R-x)^2}
Taking reciprocal and square roots gives:
x = \frac{R-x}{\sqrt{2}}
Solving for \( x \):
\sqrt{2}x = R - x
x(\sqrt{2} + 1) = R
x = \frac{R}{\sqrt{2} + 1}
We apply the property of surds for simplicity:
x = \frac{R}{\sqrt{2} + 1} \cdot \frac{\sqrt{2} - 1}{\sqrt{2} - 1}
x = \frac{R(\sqrt{2} - 1)}{1}
x = \frac{\sqrt{2}R}{\sqrt{2} - 1}
Therefore, the correct answer is:
\frac{\sqrt{2}R}{\sqrt{2} - 1}