The resistance \( R \) of a conductor is given by:
\[
R = \rho \frac{l}{A}
\]
where \( \rho \) is the resistivity of the material, \( l \) is the length of the conductor, and \( A \) is the cross-sectional area.
When the length is increased to \( 2l \), the new resistance \( R' \) is given by:
\[
R' = \rho \frac{2l}{A'}
\]
Since the volume of the conductor remains constant while stretching, the volume before and after stretching must be equal:
\[
lA = 2lA'
\]
\[
A' = \frac{A}{2}
\]
Thus, the final resistance \( R' \) becomes:
\[
R' = \rho \frac{2l}{A/2} = 4 \times \rho \frac{l}{A} = 4R
\]
Therefore, the relation between \( R' \) and \( R \) is:
\[
R' = 4R
\]
For drift velocity, the drift velocity \( v_d \) is related to the current and the electric field by:
\[
J = nq v_d
\]
where \( n \) is the number of charge carriers per unit volume, \( q \) is the charge of an electron, and \( v_d \) is the drift velocity.
When the length of the conductor is stretched, the electric field \( E \) remains the same, but the cross-sectional area decreases. Since the current is conserved, the drift velocity must increase, as the current density remains the same. Therefore, the final drift velocity \( v'_d \) is related to the initial drift velocity \( v_d \) by:
\[
v'_d = 2v_d
\]