To determine how the resistance of a conducting wire changes when its length is doubled, we need to use the formula for resistance in a wire, which is:
\[ R = \rho \frac{L}{A} \]
where:
- \( R \) is the resistance of the wire,
- \( \rho \) is the resistivity of the material (a constant for a given material at a given temperature),
- \( L \) is the length of the wire,
- \( A \) is the cross-sectional area of the wire.
### Initial Conditions
Let's denote the initial length of the wire as \( L_0 \) and its initial cross-sectional area as \( A_0 \). The initial resistance of the wire \( R_0 \) is:
\[ R_0 = \rho \frac{L_0}{A_0} \]
### When the Length is Doubled
When the wire is stretched so that its length becomes twice the original length, i.e., \( L = 2L_0 \), we need to determine how the cross-sectional area changes. Since the volume of the wire remains constant during stretching, we can use the fact that:
\[ L_0 A_0 = L A \]
Substituting \( L = 2L_0 \) into this equation:
\[ L_0 A_0 = 2L_0 A \]
Solving for \( A \):
\[ A = \frac{A_0}{2} \]
So, the cross-sectional area of the wire becomes half of its original area.
### New Resistance
Now, letβs calculate the new resistance \( R \) with the updated length and area:
\[ R = \rho \frac{L}{A} \]
Substituting \( L = 2L_0 \) and \( A = \frac{A_0}{2} \):
\[ R = \rho \frac{2L_0}{\frac{A_0}{2}} \]
Simplify the expression:
\[ R = \rho \frac{2L_0 \cdot 2}{A_0} = \rho \frac{4L_0}{A_0} \]
We know that \( R_0 = \rho \frac{L_0}{A_0} \). Therefore:
\[ R = 4R_0 \]
### Conclusion
The resistance of the wire increases by a factor of 4 when the length of the wire is doubled and its cross-sectional area is halved due to stretching.