When a wire is stretched to double its original length without a loss of mass, its **resistivity** remains the same. However, the **resistance** of the wire changes. Let's break it down:
### Resistivity (ρ):
Resistivity is an intrinsic property of the material and does not depend on the wire's dimensions (length or cross-sectional area). It only depends on the material itself, temperature, and other intrinsic factors. Hence, when the wire is stretched to double its length, the **resistivity (ρ)** remains constant.
### Resistance (R):
The resistance of the 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.
If the wire is stretched to **double its length**:
1. **Length (L):** The new length becomes \( 2L \).
2. **Cross-sectional area (A):** The volume of the wire remains constant (since there is no loss of mass). The volume \( V \) is given by \( V = A \times L \). When the length doubles, the cross-sectional area decreases to maintain the same volume. The new cross-sectional area \( A' \) becomes \( \frac{A}{2} \).
Now, substituting these into the resistance formula:
\[
R' = \rho \frac{2L}{A/2} = 4 \times \left( \rho \frac{L}{A} \right) = 4R
\]
### Conclusion:
- **Resistivity** of the wire remains unchanged.
- **Resistance** of the wire increases by a factor of 4.