For wires connected in series:
\[
I_1 = I_2
\]
Using
\[
I = neAv_d
\]
we get
\[
v_d \propto \frac{1}{A}
\]
and since
\[
A=\pi r^2,
\]
\[
v_d \propto \frac{1}{r^2}
\]
Therefore, drift velocity is inversely proportional to the square of the radius of the wire.