The change in length of a wire due to an applied force is given by the formula: \[ \Delta L = \frac{F L}{A Y} \] where \( F \) is the applied force, \( L \) is the length of the wire, \( A \) is the cross-sectional area, and \( Y \) is the Young's modulus of the material.
Since both wires are made of the same material, \( Y \) is constant for both.
The cross-sectional area \( A \) of a wire is proportional to the square of the radius: \[ A = \pi r^2 \]
Let the radius of the first wire be \( r_1 \) and the radius of the second wire be \( r_2 \), with \( r_1 : r_2 = 2 : 1 \), so: \[ A_1 : A_2 = (2^2) : (1^2) = 4 : 1 \] Let the lengths of the wires be \( L_1 \) and \( L_2 \), with \( L_1 : L_2 = 1 : 2 \). Now, using the formula for change in length: \[ \Delta L_1 : \Delta L_2 = \frac{F L_1}{A_1} : \frac{F L_2}{A_2} = \frac{L_1}{A_1} : \frac{L_2}{A_2} \] Substitute the ratios: \[ \Delta L_1 : \Delta L_2 = \frac{1}{4} : \frac{2}{1} = 1 : 8 \]
Thus, the ratio of their change in length is \( 1 : 8 \).
If the given graph shows the load (W) attached to and the elongation ($\Delta l$) produced in a wire of length 1 meter and cross-sectional area 1 mm$^2$, then the Young's modulus of the material of the wire is
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: