The resistance \( R \) of a wire is given by the formula:
\[
R = \rho \frac{L}{A}
\]
where:
- \( \rho \) is the resistivity of the material,
- \( L \) is the length of the wire,
- \( A \) is the cross-sectional area of the wire.
When the wire is stretched, its length changes, but the volume of the wire remains constant. Since the volume \( V = A \times L \), if the wire is stretched to double the original length, the new length \( L' \) is 48 cm, and the original length \( L = 24 \) cm.
The volume remains constant, so:
\[
A_1 L_1 = A_2 L_2 \quad \Rightarrow \quad A_2 = \frac{A_1 L_1}{L_2}
\]
Thus, the new area \( A_2 \) is half the original are(A)
Since resistance is directly proportional to the length and inversely proportional to the area, the new resistance will be:
\[
R' = R \times \left( \frac{L'}{L} \right) \times \left( \frac{A}{A'} \right)
\]
Substitute the values:
\[
R' = 8 \times \frac{48}{24} \times 2 = 8 \times 2 \times 2 = 32 \, \Omega
\]
Thus, the new resistance of the stretched wire is \( 32 \, \Omega \).