The drift velocity of electrons is defined as:\[v_d = \frac{I}{nAe}\]with the following parameters: \( v_d \) representing drift velocity, \( I \) representing current, \( n \) representing the number density of electrons, \( A \) representing cross-sectional area, and \( e \) representing the elementary charge.(i) Series Connection:In a series circuit, the current \( I \) remains constant across all components.Consequently, the drift velocities are expressed as:\[v_{d1} = \frac{I}{nA_1e}, \quad v_{d2} = \frac{I}{nA_2e}This leads to the ratio:\[\Rightarrow \frac{v_{d1}}{v_{d2}} = \frac{A_2}{A_1}\](ii) Parallel Connection:In a parallel circuit, the voltage \( V \) is identical across each branch.Given the resistance formula \( R = \frac{\rho l}{A} \), current is directly proportional to the cross-sectional area (\( I \propto A \)).Therefore:\[I_1 \propto A_1, \quad I_2 \propto A_2\]The drift velocities are calculated as:\[v_{d1} = \frac{I_1}{nA_1e} = \frac{A_1}{nA_1e} = \frac{1}{ne}\]\[v_{d2} = \frac{I_2}{nA_2e} = \frac{A_2}{nA_2e} = \frac{1}{ne}Resulting in the ratio:\[\Rightarrow \frac{v_{d1}}{v_{d2}} = 1\]