The resistance 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.
Initially, the wire has:
- Length \( l = 2 \, \text{m} \),
- Resistance \( R = 8 \, \Omega \).
When the wire is stretched to double its original length, the new length is:
\[
l' = 2 \times 2 = 4 \, \text{m}
\]
Since the volume of the wire remains constant during stretching, the volume before and after stretching is equal:
\[
V = A \cdot l = A' \cdot l'
\]
\[
A \cdot 2 = A' \cdot 4
\]
\[
A' = \frac{A}{2}
\]
The new cross-sectional area is half the original area.
The new resistance \( R' \) is given by:
\[
R' = \rho \frac{l'}{A'}
\]
Substitute \( l' = 4 \, \text{m} \) and \( A' = \frac{A}{2} \):
\[
R' = \rho \frac{4}{\frac{A}{2}} = \rho \frac{4 \cdot 2}{A} = \rho \frac{8}{A}
\]
Since the original resistance is \( R = \rho \frac{2}{A} = 8 \, \Omega \), we can express the new resistance in terms of the original resistance:
\[
R' = \rho \frac{8}{A} = 4 \cdot \rho \frac{2}{A} = 4 \cdot R
\]
\[
R' = 4 \cdot 8 = 32 \, \Omega
\]
Alternatively, since resistance is proportional to \( \frac{l}{A} \), and \( l \) doubles while \( A \) halves, the resistance changes by:
\[
R' = R \cdot \frac{l'}{l} \cdot \frac{A}{A'} = 8 \cdot \frac{4}{2} \cdot \frac{A}{\frac{A}{2}} = 8 \cdot 2 \cdot 2 = 32 \, \Omega
\]
Thus, the new resistance of the wire is \( 32 \, \Omega \).