Step 1: Relate resistance to resistivity: \(R = \frac{\rho l}{A}\).
For wires in parallel, \(\frac{1}{R_{eq}} = \frac{1}{R_1} + \frac{1}{R_2}\).
Step 2: Since the wires are combined in parallel, the effective length remains \(l\), but the total area becomes \(2A\).
\[ \frac{2A}{\rho_{eff} l} = \frac{A}{\rho_1 l} + \frac{A}{\rho_2 l} \implies \frac{2}{\rho_{eff}} = \frac{1}{\rho_1} + \frac{1}{\rho_2} \]
Step 3: Calculate \(\rho_{eff}\).
\[ \frac{2}{\rho_{eff}} = \frac{1}{6} + \frac{1}{3} = \frac{1+2}{6} = \frac{3}{6} = \frac{1}{2} \]
\[ \rho_{eff} = 4 \ \Omega \text{ cm} \]