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 \( 15.6 \, \Omega \).
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: