Two discs of moment of inertia \( I_1 = 4 \, kg \, m^2 \) and \( I_2 = 2 \, kg \, m^2 \) about their central axes and normal to their planes, rotating with angular speeds \( 10 \, rad/s \) and \( 4 \, rad/s \) respectively are brought into contact face to face with their axes of rotation coincident. The loss in kinetic energy of the system in the process is __________ J.
The kinetic energy of a rotating body is given by the formula:
\( KE = \frac{1}{2} I \omega^2 \),
where \( I \) is the moment of inertia and \( \omega \) is the angular velocity.
Kinetic Energy of Each Disc Before Contact: For disc 1:
\( KE_1 = \frac{1}{2} I_1 \omega_1^2 = \frac{1}{2} (4 \, \text{kg m}^2)(10 \, \text{rad/s})^2 = \frac{1}{2} \times 4 \times 100 = 200 \, \text{J} \).
For disc 2:
\( KE_2 = \frac{1}{2} I_2 \omega_2^2 = \frac{1}{2} (2 \, \text{kg m}^2)(4 \, \text{rad/s})^2 = \frac{1}{2} \times 2 \times 16 = 16 \, \text{J} \).
Total Kinetic Energy Before Contact:
\( KE_{\text{total initial}} = KE_1 + KE_2 = 200 \, \text{J} + 16 \, \text{J} = 216 \, \text{J} \).
Finding Final Angular Velocity After Contact: When the discs come into contact, they will rotate together, and we can use the principle of conservation of angular momentum. Initial angular momentum \( L_{\text{initial}} \):
\( L_{\text{initial}} = I_1 \omega_1 + I_2 \omega_2 = (4 \, \text{kg m}^2)(10 \, \text{rad/s}) + (2 \, \text{kg m}^2)(4 \, \text{rad/s}) = 40 + 8 = 48 \, \text{kg m}^2/\text{s} \).
The total moment of inertia after they are in contact:
\( I_{\text{total}} = I_1 + I_2 = 4 \, \text{kg m}^2 + 2 \, \text{kg m}^2 = 6 \, \text{kg m}^2 \).
Final angular velocity \( \omega_f \):
\( L_{\text{final}} = I_{\text{total}} \omega_f \implies 48 = 6 \omega_f \implies \omega_f = 8 \, \text{rad/s} \).
Final Kinetic Energy After Contact:
\( KE_{\text{final}} = \frac{1}{2} I_{\text{total}} \omega_f^2 = \frac{1}{2} (6 \, \text{kg m}^2)(8 \, \text{rad/s})^2 = \frac{1}{2} \times 6 \times 64 = 192 \, \text{J} \).
Calculating Loss in Kinetic Energy:
\( \text{Loss in KE} = KE_{\text{total initial}} - KE_{\text{final}} = 216 \, \text{J} - 192 \, \text{J} = 24 \, \text{J} \).
A uniform circular disc of radius \( R \) and mass \( M \) is rotating about an axis perpendicular to its plane and passing through its center. A small circular part of radius \( R/2 \) is removed from the original disc as shown in the figure. Find the moment of inertia of the remaining part of the original disc about the axis as given above.
Choose the correct nuclear process from the below options:
\( [ p : \text{proton}, n : \text{neutron}, e^- : \text{electron}, e^+ : \text{positron}, \nu : \text{neutrino}, \bar{\nu} : \text{antineutrino} ] \)