When a wire of resistance \( R \) is melted and stretched to \( N \) times its original length, its resistance changes due to both its increased length and decreased cross-sectional area.
### Step-by-step Explanation:
1. **Original Resistance**:
The resistance of a wire is given by the formula:
\[
R = \rho \frac{L}{A}
\]
Where:
- \( R \) is the resistance,
- \( \rho \) is the resistivity of the material,
- \( L \) is the length of the wire,
- \( A \) is the cross-sectional area of the wire.
2. **Stretching the Wire**:
When the wire is stretched to \( N \) times its original length, its volume remains constant. Since the volume of the wire is given by \( V = L \cdot A \), stretching it means the new length \( L' = N \cdot L \).
To conserve the volume, the new cross-sectional area \( A' \) will be reduced. Since volume is constant:
\[
L \cdot A = L' \cdot A' \quad \Rightarrow \quad A' = \frac{A}{N}
\]
3. **New Resistance**:
The resistance of the stretched wire is now:
\[
R' = \rho \frac{L'}{A'}
\]
Substituting \( L' = N \cdot L \) and \( A' = \frac{A}{N} \), we get:
\[
R' = \rho \frac{N \cdot L}{\frac{A}{N}} = \rho \cdot N^2 \cdot \frac{L}{A} = N^2 \cdot R
\]
### Final Result:
The new resistance \( R' \) after the wire is stretched to \( N \) times its original length is:
\[
R' = N^2 \cdot R
\]
So, the resistance increases by a factor of \( N^2 \) when the wire is stretched \( N \) times its original length.