The drift velocity of electrons is given by:
\[
v_d = \frac{I}{nAe}
\]
where
\( v_d \) = drift velocity,
\( I \) = current,
\( n \) = number density of electrons,
\( A \) = cross-sectional area,
\( e \) = elementary charge.
(i) Series connection:
In a series circuit:
- The current \( I \) is the same through both wires.
- So, the drift velocities are:
\[
v_{d1} = \frac{I}{nA_1e}, \quad v_{d2} = \frac{I}{nA_2e}
\Rightarrow \frac{v_{d1}}{v_{d2}} = \frac{A_2}{A_1}
\]
(ii) Parallel connection:
In a parallel circuit:
- The voltage \( V \) across each wire is the same.
- Resistance \( R = \frac{\rho l}{A} \Rightarrow I \propto A \)
- Therefore,
\[
I_1 \propto A_1, \quad I_2 \propto A_2
\Rightarrow v_{d1} = \frac{I_1}{nA_1e} = \frac{A_1}{nA_1e} = \frac{1}{ne}
\]
\[
v_{d2} = \frac{I_2}{nA_2e} = \frac{A_2}{nA_2e} = \frac{1}{ne}
\Rightarrow \frac{v_{d1}}{v_{d2}} = 1
\]