To solve this problem, we need to calculate the loss in kinetic energy when the two discs are brought into contact with their axes of rotation coaxial.
Initially, the kinetic energies of the two discs are given by:
When the discs are combined, they rotate together with a common angular velocity \omega_f
The total angular momentum before contact is equal to the total angular momentum after contact:
I_1\omega_1 + I_2\omega_2 = (I_1 + I_2)\omega_fSolve for the final angular velocity:
\omega_f = \frac{I_1\omega_1 + I_2\omega_2}{I_1 + I_2}The kinetic energy of the system after combining is:
K_f = \frac{1}{2} (I_1 + I_2) \omega_f^2Substitute the expression for \omega_f:
K_f = \frac{1}{2} (I_1 + I_2) \left(\frac{I_1\omega_1 + I_2\omega_2}{I_1 + I_2}\right)^2The loss in kinetic energy is given by the difference between the initial and the final kinetic energies:
\Delta K = (K_1 + K_2) - K_fSubstitute the expressions for K_1, K_2, and K_f:
Simplify and calculate:
This gives us the final expression for the loss in kinetic energy. Therefore, the correct answer is:
The center of mass of a thin rectangular plate (fig - x) with sides of length \( a \) and \( b \), whose mass per unit area (\( \sigma \)) varies as \( \sigma = \sigma_0 \frac{x}{ab} \) (where \( \sigma_0 \) is a constant), would be 