Consider two point charges, -q and +q, placed at a distance \(L\) apart. We need to find the electric field intensity at a point at a large distance \( R \) such that \( R \gg L \). The electric field due to a point charge is given by:
\[ E = \frac{k \cdot |q|}{r^2} \]
where \( k \) is Coulomb's constant, \( q \) is the charge, and \( r \) is the distance from the charge. For this system, we calculate the net electric field at a point at distance \( R \) from the midpoint between the charges. Since \( R \gg L \), the charges appear very close to each other relative to the distance \( R \). This system behaves like a dipole.
For a dipole, the electric field at a point along the perpendicular bisector at distance \( R \) is approximately given by:
\[ E_{\text{dipole}} = \frac{k \cdot p}{R^3} \]
where \( p = q \cdot L \) is the dipole moment. Thus, the electric field due to this configuration decreases with distance as:
\[ E \propto \frac{1}{R^3} \]
Therefore, the magnitude of the electric field intensity at a distance \( R \) varies as \(\frac{1}{R^3}\).