When a wire is stretched, its resistance changes due to changes in both its length and its cross-sectional area. To understand the new resistance after stretching, letβs go through the process step by step.
### Initial Situation
- **Initial Length (L):** \( L \)
- **Initial Cross-Sectional Area (A):** \( A \)
- **Initial Resistance (R):** \( R \)
The resistance \( R \) of the wire is given by the formula:
\[ R = \rho \frac{L}{A} \]
where \( \rho \) is the resistivity of the material.
### After Stretching
When the wire is stretched to \( N \) times its original length:
- **New Length (L'):** \( N \times L \)
Since the volume of the wire remains constant during stretching, we can express the relationship between the original and new cross-sectional area. The volume \( V \) of the wire is given by:
\[ V = L \times A \]
After stretching, the volume remains the same:
\[ V' = L' \times A' = (N \times L) \times A' \]
Setting the volumes equal:
\[ L \times A = (N \times L) \times A' \]
\[ A' = \frac{A}{N} \]
### New Resistance
The new resistance \( R' \) can be calculated using the new length and new cross-sectional area:
\[ R' = \rho \frac{L'}{A'} \]
Substitute \( L' = N \times L \) and \( A' = \frac{A}{N} \):
\[ R' = \rho \frac{N \times L}{\frac{A}{N}} \]
\[ R' = \rho \frac{N^2 \times L}{A} \]
Since the original resistance \( R \) was \( \rho \frac{L}{A} \):
\[ R' = N^2 \times R \]
### Conclusion
After stretching the wire to \( N \) times its original length, the new resistance of the wire will be \( N^2 \) times the original resistance. So, if the initial resistance was \( R \), the new resistance \( R' \) is \( N^2 \times R \).