Upon contact and subsequent separation of two charged metallic spheres with radii \(R_1\) and \(R_2\), charge redistribution occurs, resulting in equal potentials on both spheres. The potential \(V\) for a sphere with charge \(Q\) and radius \(R\) is defined as:
\(V=\frac{Q}{R}\)
Let \(Q_1\) and \(Q_2\) denote the charges on spheres with radii \(R_1\) and \(R_2\), respectively, after contact. Equating their potentials yields:
\(\frac{Q_1}{R_1}=\frac{Q_2}{R_2}\)
Rearranging this equation provides the ratio of the charges:
\(\frac{Q_2}{Q_1}=\frac{R_2}{R_1}\)
The derived relationship is:
\(\frac{Q_2}{Q_1}=\frac{R_2}{R_1}\)