Concept:
The resistance of a wire is given by the relation
\[
R = \rho \frac{L}{A}
\]
where
• \( \rho \) = resistivity of the material (constant for a given material),
• \( L \) = length of the wire,
• \( A \) = cross-sectional area.
When a wire is stretched, its volume remains constant (assuming uniform stretching). Since
\[
\text{Volume} = A \times L
\]
if the length increases, the cross-sectional area must decrease proportionally.
Step 1: Apply the constant volume condition.
Let the original length be \(L\) and the original area be \(A\).
If the wire is stretched to double its length, then
\[
L' = 2L
\]
Since the volume remains constant,
\[
AL = A' L'
\]
\[
AL = A'(2L)
\]
\[
A' = \frac{A}{2}
\]
Thus, the new cross-sectional area becomes half.
Step 2: Substitute into the resistance formula.
The new resistance is
\[
R' = \rho \frac{L'}{A'}
\]
Substituting \(L' = 2L\) and \(A' = \frac{A}{2}\):
\[
R' = \rho \frac{2L}{A/2}
\]
\[
R' = \rho \times \frac{2L \times 2}{A}
\]
\[
R' = 4\rho \frac{L}{A}
\]
\[
R' = 4R
\]
Thus, the new resistance becomes
\[
\boxed{4R}
\]