To understand how the resistance of a conducting wire changes when its length is increased, we can use the formula for resistance in terms of its physical properties:
\[
R = \rho \frac{L}{A}
\]
where:
- \( R \) is the resistance,
- \( \rho \) is the resistivity of the material (which remains constant for a given material),
- \( L \) is the length of the wire,
- \( A \) is the cross-sectional area of the wire.
### Initial Resistance
Letβs assume the initial length of the wire is \( L \) and its cross-sectional area is \( A \). The initial resistance \( R_1 \) can be expressed as:
\[
R_1 = \rho \frac{L}{A}
\]
### Stretching the Wire
When the wire is stretched to twice its original length, the new length \( L' \) is:
\[
L' = 2L
\]
Now, let's consider the change in cross-sectional area. When a wire is stretched, its volume remains constant (assuming no material is added or removed). The initial volume \( V \) of the wire can be expressed as:
\[
V = L \times A
\]
After stretching, the volume \( V' \) remains the same, but the length has changed to \( L' \) and the new cross-sectional area \( A' \) will be different. We can express this as:
\[
V' = L' \times A' = 2L \times A'
\]
Setting the initial volume equal to the final volume gives:
\[
L \times A = 2L \times A'
\]
From this, we can solve for the new cross-sectional area \( A' \):
\[
A' = \frac{A}{2}
\]
### New Resistance
Now we can find the new resistance \( R_2 \) using the new length and new area:
\[
R_2 = \rho \frac{L'}{A'} = \rho \frac{2L}{\frac{A}{2}} = \rho \frac{2L \cdot 2}{A} = \rho \frac{4L}{A}
\]
### Ratio of Resistances
Now we can find the ratio of the new resistance \( R_2 \) to the original resistance \( R_1 \):
\[
\frac{R_2}{R_1} = \frac{\rho \frac{4L}{A}}{\rho \frac{L}{A}} = \frac{4L}{L} = 4
\]
### Conclusion
Thus, when the length of the conducting wire is stretched to twice its original length, its resistance will increase by a factor of **4**.