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Two discs of moments of inertia I1 and I...

Two discs of moments of inertia `I_1` and `I_2` about their respective axes (normal to the disc and passing through the centre), and rotating with angular speed `omega_1` and `omega_2` are brought into contact face to face with their axes of rotation coincident. What is the loss in kinetic energy of the system in the process?

A

`I_(1)I_(2)(omega_1 - omega_2)^(2)/2(I_1 + I_2)`

B

`I_(1)I_(2)(omega_1 - omega_2)^(2)/(2(I_1 + I_2))`

C

`I_(1)I_(2)(omega_1 + omega_2)^(2)/(I_1 - I_2)`

D

`I_(1)I_(2)(omega_1 + omega_2)^(2)/2(I_1 - I_2)`

Text Solution

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The correct Answer is:
To find the loss in kinetic energy when two discs are brought into contact, we can follow these steps: ### Step 1: Calculate Initial Kinetic Energy The initial kinetic energy of the system is the sum of the kinetic energies of both discs. The formula for rotational kinetic energy is given by: \[ KE = \frac{1}{2} I \omega^2 \] Thus, the initial kinetic energy \( KE_{initial} \) can be expressed as: \[ KE_{initial} = \frac{1}{2} I_1 \omega_1^2 + \frac{1}{2} I_2 \omega_2^2 \] ### Step 2: Determine Final Angular Velocity When the discs are brought into contact, they will rotate together with a common angular velocity \( \omega \). To find this angular velocity, we use the conservation of angular momentum: \[ L_{initial} = L_{final} \] The initial angular momentum is: \[ L_{initial} = I_1 \omega_1 + I_2 \omega_2 \] The final angular momentum when both discs are rotating together is: \[ L_{final} = (I_1 + I_2) \omega \] Setting these equal gives: \[ I_1 \omega_1 + I_2 \omega_2 = (I_1 + I_2) \omega \] From this, we can solve for \( \omega \): \[ \omega = \frac{I_1 \omega_1 + I_2 \omega_2}{I_1 + I_2} \] ### Step 3: Calculate Final Kinetic Energy The final kinetic energy \( KE_{final} \) of the system when both discs are rotating together is: \[ KE_{final} = \frac{1}{2} (I_1 + I_2) \omega^2 \] Substituting the expression for \( \omega \): \[ KE_{final} = \frac{1}{2} (I_1 + I_2) \left( \frac{I_1 \omega_1 + I_2 \omega_2}{I_1 + I_2} \right)^2 \] This simplifies to: \[ KE_{final} = \frac{1}{2} \frac{(I_1 \omega_1 + I_2 \omega_2)^2}{I_1 + I_2} \] ### Step 4: Calculate Loss in Kinetic Energy The loss in kinetic energy \( \Delta KE \) is given by: \[ \Delta KE = KE_{initial} - KE_{final} \] Substituting the expressions we derived: \[ \Delta KE = \left( \frac{1}{2} I_1 \omega_1^2 + \frac{1}{2} I_2 \omega_2^2 \right) - \frac{1}{2} \frac{(I_1 \omega_1 + I_2 \omega_2)^2}{I_1 + I_2} \] ### Step 5: Simplify the Expression To simplify, we can factor out \( \frac{1}{2} \): \[ \Delta KE = \frac{1}{2} \left( I_1 \omega_1^2 + I_2 \omega_2^2 - \frac{(I_1 \omega_1 + I_2 \omega_2)^2}{I_1 + I_2} \right) \] This can be further simplified to: \[ \Delta KE = \frac{1}{2} \frac{I_1 I_2 (\omega_1 - \omega_2)^2}{I_1 + I_2} \] ### Final Result Thus, the loss in kinetic energy when the two discs come into contact is: \[ \Delta KE = \frac{I_1 I_2 (\omega_1 - \omega_2)^2}{2(I_1 + I_2)} \]
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