(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: \[ R' = 2R \] (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.
In the given reaction sequence, the structure of Y would be: