The resistance \( R \) of a wire is given by the formula:
\[
R = \rho \frac{L}{A}
\]
where \( \rho \) is the resistivity, \( L \) is the length, and \( A \) is the cross-sectional area of the wire.
The area of the cross-section of the wire is:
\[
A = \pi R^2
\]
When the wire is stretched, the length \( L \) increases, and the radius \( R \) is halved. Let the new length be \( L' \) and the new radius be \( R' = \frac{R}{2} \).
Since the volume of the wire remains constant (because the wire is just stretched, not material added or removed), the volume before and after stretching is the same:
\[
\pi R^2 L = \pi (R/2)^2 L'
\]
Simplifying:
\[
R^2 L = \frac{R^2}{4} L'
\]
\[
L' = 4L
\]
So, the new resistance \( R' \) is:
\[
R' = \rho \frac{L'}{A'} = \rho \frac{4L}{\pi (R/2)^2} = \rho \frac{4L}{\pi \frac{R^2}{4}} = \rho \frac{16L}{\pi R^2} = 16R
\]