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There is a small hole in a table. A stri...

There is a small hole in a table. A string of length lm passes through it. Two bodies of masses 70g and 100 g are attached at its ends. The lOOg mass hangs freely at a depth of 60 cm from the table. If this mass is to be in equilibrium, the other mass should rotate in a circle with a frequency equal to

A

`(4pi//140)` Hz

B

`pi//140 Hz`

C

`pi//sqrt(140)` Hz

D

`sqrt(140)/(4pi) Hz`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem step by step, we will analyze the forces acting on the two masses and apply the concepts of circular motion and equilibrium. ### Step 1: Identify the given values - Mass \( m_1 = 70 \, \text{g} = 0.07 \, \text{kg} \) - Mass \( m_2 = 100 \, \text{g} = 0.1 \, \text{kg} \) - Total length of the string \( L = 1 \, \text{m} \) - Length of the hanging part \( L_h = 60 \, \text{cm} = 0.6 \, \text{m} \) ### Step 2: Calculate the radius of the circular motion The length of the string that rotates in a circle is given by: \[ r = L - L_h = 1 \, \text{m} - 0.6 \, \text{m} = 0.4 \, \text{m} \] ### Step 3: Analyze the forces acting on the hanging mass \( m_2 \) The forces acting on mass \( m_2 \) are: - Weight \( W = m_2 g = 0.1 \, \text{kg} \times 10 \, \text{m/s}^2 = 1 \, \text{N} \) - Tension \( T \) in the string For the system to be in equilibrium: \[ T = m_2 g = 1 \, \text{N} \] ### Step 4: Analyze the forces acting on the rotating mass \( m_1 \) For mass \( m_1 \) which is rotating in a circle, the tension \( T \) also provides the centripetal force required for circular motion: \[ T = \frac{m_1 v^2}{r} \] Substituting \( T = 1 \, \text{N} \): \[ 1 = \frac{0.07 \, v^2}{0.4} \] ### Step 5: Solve for the velocity \( v \) Rearranging the equation gives: \[ v^2 = \frac{1 \times 0.4}{0.07} \] \[ v^2 = \frac{0.4}{0.07} \approx 5.7143 \] \[ v = \sqrt{5.7143} \approx 2.39 \, \text{m/s} \] ### Step 6: Relate linear velocity to angular frequency The relationship between linear velocity \( v \) and angular frequency \( \omega \) is given by: \[ v = r \omega \implies \omega = \frac{v}{r} \] Substituting the values: \[ \omega = \frac{2.39}{0.4} \approx 5.975 \, \text{rad/s} \] ### Step 7: Calculate the frequency \( f \) The frequency \( f \) is related to angular frequency \( \omega \) by: \[ f = \frac{\omega}{2\pi} \] Substituting the value of \( \omega \): \[ f = \frac{5.975}{2\pi} \approx \frac{5.975}{6.2832} \approx 0.951 \, \text{Hz} \] ### Final Answer The frequency of rotation of the smaller mass \( m_1 \) for the system to be in equilibrium is approximately \( 0.951 \, \text{Hz} \). ---
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