The resistance \( R \) of a wire is calculated using the formula:
\[R = \rho \frac{l}{A}\]
Where:
- \( \rho \) represents the resistivity of the material.
- \( l \) denotes the length of the wire.
- \( A \) is the cross-sectional area of the wire.
Initial conditions of the wire:
- Length \( l = 2 \, \text{m} \)
- Resistance \( R = 8 \, \Omega \)
Upon stretching the wire to twice its original length, the new length \( l' \) becomes:
\[l' = 2 \times 2 = 4 \, \text{m}\]
The volume of the wire remains constant during this process. Therefore, the initial volume equals the final volume:
\[V = A \cdot l = A' \cdot l'\]
Substituting the known lengths:
\[A \cdot 2 = A' \cdot 4\]
This yields the new cross-sectional area:
\[A' = \frac{A}{2}\]
The new cross-sectional area is half the original area.
The new resistance \( R' \) is determined by:
\[R' = \rho \frac{l'}{A'}\]
Substituting \( l' = 4 \, \text{m} \) and \( A' = \frac{A}{2} \):
\[R' = \rho \frac{4}{\frac{A}{2}} = \rho \frac{4 \cdot 2}{A} = \rho \frac{8}{A}\]
Given the original resistance \( R = \rho \frac{2}{A} = 8 \, \Omega \), we can express the new resistance in terms of the original resistance:
\[R' = \rho \frac{8}{A} = 4 \cdot \rho \frac{2}{A} = 4 \cdot R\]
Calculating the new resistance:
\[R' = 4 \cdot 8 = 32 \, \Omega\]
Alternatively, as resistance is directly proportional to \( \frac{l}{A} \), with \( l \) doubling and \( A \) halving, the resistance change is:
\[R' = R \cdot \frac{l'}{l} \cdot \frac{A}{A'} = 8 \cdot \frac{4}{2} \cdot \frac{A}{\frac{A}{2}} = 8 \cdot 2 \cdot 2 = 32 \, \Omega\]
The wire's new resistance is \( 32 \, \Omega \).