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A thin circular ring of mass m and radiu...

A thin circular ring of mass m and radius R is rotating about its axis perpendicular to the plane of the ring with a constant angular velocity `omega`. Two point particleseach of mass M are attached gently to the opposite end of a diameter of the ring. The ring now rotates, with an angular velocity` (omega)/2`. Then the ratio`m/M` is

A

1

B

2

C

`1/2`

D

`sqrt(2)`

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The correct Answer is:
To solve the problem, we will use the principle of conservation of angular momentum. Here are the steps to find the ratio \( \frac{m}{M} \): ### Step 1: Understand the Initial Conditions Initially, we have a thin circular ring of mass \( m \) and radius \( R \) rotating with an angular velocity \( \omega \). The moment of inertia \( I \) of the ring about its axis is given by: \[ I_{\text{ring}} = mR^2 \] ### Step 2: Calculate Initial Angular Momentum The initial angular momentum \( L_i \) of the system can be calculated using the formula: \[ L_i = I_{\text{ring}} \cdot \omega = mR^2 \cdot \omega \] ### Step 3: Understand the Final Conditions After attaching two point masses \( M \) at opposite ends of a diameter of the ring, the system now rotates with an angular velocity of \( \frac{\omega}{2} \). ### Step 4: Calculate Final Moment of Inertia The final moment of inertia \( I_f \) of the entire system (ring + two point masses) is: \[ I_f = I_{\text{ring}} + 2 \cdot I_{\text{particle}} \] Where \( I_{\text{particle}} = M R^2 \) (moment of inertia of each point mass about the axis). Thus: \[ I_f = mR^2 + 2 \cdot (M R^2) = mR^2 + 2MR^2 \] ### Step 5: Calculate Final Angular Momentum The final angular momentum \( L_f \) of the system is given by: \[ L_f = I_f \cdot \omega_f = (mR^2 + 2MR^2) \cdot \frac{\omega}{2} \] ### Step 6: Set Initial and Final Angular Momentum Equal By conservation of angular momentum, we have: \[ L_i = L_f \] Substituting the expressions we derived: \[ mR^2 \cdot \omega = \left(mR^2 + 2MR^2\right) \cdot \frac{\omega}{2} \] ### Step 7: Cancel Common Factors We can cancel \( R^2 \) and \( \omega \) from both sides (assuming \( R \neq 0 \) and \( \omega \neq 0 \)): \[ m = \left(m + 2M\right) \cdot \frac{1}{2} \] ### Step 8: Rearrange the Equation Multiplying both sides by 2 gives: \[ 2m = m + 2M \] Rearranging this, we get: \[ 2m - m = 2M \] Thus: \[ m = 2M \] ### Step 9: Find the Ratio \( \frac{m}{M} \) Now we can find the ratio: \[ \frac{m}{M} = \frac{2M}{M} = 2 \] ### Final Answer The ratio \( \frac{m}{M} \) is: \[ \frac{m}{M} = 2 \]
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