When a wire of resistance \( R \) is melted and then stretched to \( N \) times its original length, its resistance changes. Here’s how to understand it:
1. Understanding Resistance:
The resistance \( R \) of a wire is given by the formula:
\[
R = \rho \frac{L}{A}
\]
Where:
- \( \rho \) is the resistivity of the material (a constant for a given material),
- \( L \) is the length of the wire,
- \( A \) is the cross-sectional area of the wire.
2. Melting and Stretching the Wire:
When the wire is melted and stretched, the total volume of the wire stays constant. The volume before and after stretching remains the same because the material isn't lost—just reshaped.
- Initially, the volume of the wire is \( V_{\text{initial}} = A_{\text{initial}} \times L_{\text{initial}} \).
- After stretching, the volume remains the same, so:
\[
A_{\text{final}} \times L_{\text{final}} = A_{\text{initial}} \times L_{\text{initial}}
\]
If the length is stretched by a factor of \( N \) (i.e., \( L_{\text{final}} = N \times L_{\text{initial}} \)), the cross-sectional area will decrease by a factor of \( N^2 \) because volume is length × area. Thus, we have:
\[
A_{\text{final}} = \frac{A_{\text{initial}}}{N^2}
\]
3. New Resistance:
Now, using the formula for resistance, the new resistance \( R_{\text{new}} \) after the wire is stretched is:
\[
R_{\text{new}} = \rho \frac{L_{\text{final}}}{A_{\text{final}}}
\]
Substitute the values:
\[
R_{\text{new}} = \rho \frac{N \times L_{\text{initial}}}{\frac{A_{\text{initial}}}{N^2}} = \rho \times \frac{N^3 \times L_{\text{initial}}}{A_{\text{initial}}}
\]
Since the original resistance \( R \) is \( \rho \frac{L_{\text{initial}}}{A_{\text{initial}}} \), we can write:
\[
R_{\text{new}} = N^3 \times R
\]
Final Answer:
The new resistance \( R_{\text{new}} \) is \( N^3 \) times the original resistance \( R \).