The resistance of a wire is given by the formula: \[ R = \rho \frac{L}{A} \] Where:
- \( R \) is the resistance, - \( \rho \) is the resistivity of the material (which remains constant),
- \( L \) is the length of the wire,
- \( A \) is the cross-sectional area of the wire.
When the wire is stretched, the length increases by 25%, meaning the new length \( L' \) is: \[ L' = L(1 + 0.25) = 1.25L \] Since the volume of the wire is conserved (it’s just being stretched), the volume \( V = A \times L \) remains constant. The new area \( A' \) after stretching is related to the initial area by: \[ A' = \frac{A}{1.25} \]
Thus, the new resistance \( R' \) is given by: \[ R' = \rho \frac{L'}{A'} = \rho \frac{1.25L}{A/1.25} = R \times \left( \frac{1.25}{\frac{1}{1.25}} \right) = R \times 1.25^2 = 10 \times 1.25^2 = 10 \times 1.5625 = 15.6 \, \Omega \] Therefore, the new resistance is \( 15.6 \, \Omega \).
The graph between variation of resistance of a wire as a function of its diameter keeping other parameters like length and temperature constant is
If the ratio of lengths, radii and Young's Moduli of steel and brass wires in the figure are $ a $, $ b $, and $ c $ respectively, then the corresponding ratio of increase in their lengths would be: