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(i) When a conductor is stretched, its resistance changes because resistance is proportional to the length of the conductor. The resistance is given by:
\[
R = \rho \frac{l}{A}
\]
where \( l \) is the length and \( A \) is the cross-sectional area. When the length is doubled, the resistance also doubles:
\[
R' = 2R
\]
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(ii) The drift velocity is inversely proportional to the length of the conductor (as the potential difference and electric field remain the same):
\[
v_d' = \frac{v_d}{2}
\]
Thus, the relations are:
\[
R' = 2R \quad \text{and} \quad v_d' = \frac{v_d}{2}
\]
Thus, the final resistance is twice the initial resistance, and the final drift velocity is half the initial drift velocity.