When the wire is stretched, its length is halved. The resistance \( R \) of a wire is given by:
\[
R = \rho \frac{L}{A},
\]
where \( \rho \) is the resistivity, \( L \) is the length, and \( A \) is the cross-sectional area of the wire.
- When the wire is stretched, the volume remains constant, so \( L_1 A_1 = L_2 A_2 \), where the subscript 1 and 2 represent the initial and final conditions.
The final resistance is given by:
\[
R_2 = R_1 \left( \frac{L_2}{L_1} \right)^2.
\]
Since the length is halved, the final resistance will be:
\[
R_2 = 16 \left( \frac{1}{2} \right)^2 = 16 \times \frac{1}{4} = 4 \, \Omega.
\]