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A ball of mass m kg hangs from a spring...

A ball of mass `m kg` hangs from a spring of spring constant `k`. The ball oscillates with a period of `T` seconds if the ball is removed, the spring is shortened(`w.r.t.` length in mean position) by

A

`(gT^(2))/((2pi)^(2))` metre

B

`(3T^(2)g)/((2pi)^(2))` metre

C

`(Tm)/(k,)` metre

D

`(Tk)/(m)` metre

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem of how much the spring will be shortened when the ball is removed, we can follow these steps: ### Step 1: Understand the relationship between period, mass, and spring constant The period \( T \) of a mass-spring system is given by the formula: \[ T = 2\pi \sqrt{\frac{m}{k}} \] where \( m \) is the mass and \( k \) is the spring constant. ### Step 2: Rearrange the formula to find the spring constant \( k \) We can rearrange the formula to express \( k \) in terms of \( T \) and \( m \): \[ T^2 = 4\pi^2 \frac{m}{k} \] This leads to: \[ k = \frac{4\pi^2 m}{T^2} \] ### Step 3: Determine the forces acting on the spring when the ball is attached When the ball of mass \( m \) is hanging from the spring, the force exerted by the ball due to gravity is: \[ F_{\text{initial}} = mg \] where \( g \) is the acceleration due to gravity. ### Step 4: Calculate the change in force when the ball is removed When the ball is removed, the final force \( F_{\text{final}} \) acting on the spring becomes zero. The change in force \( \Delta F \) is given by: \[ \Delta F = F_{\text{final}} - F_{\text{initial}} = 0 - mg = -mg \] ### Step 5: Relate the change in force to the change in displacement Using Hooke's law, the change in displacement \( \Delta x \) can be expressed as: \[ \Delta x = \frac{\Delta F}{-k} \] Substituting for \( \Delta F \): \[ \Delta x = \frac{-mg}{-k} = \frac{mg}{k} \] ### Step 6: Substitute the expression for \( k \) into the displacement equation Now, we can substitute the expression for \( k \) that we derived earlier: \[ \Delta x = \frac{mg}{\frac{4\pi^2 m}{T^2}} = \frac{mg T^2}{4\pi^2 m} \] The mass \( m \) cancels out: \[ \Delta x = \frac{g T^2}{4\pi^2} \] ### Final Answer Thus, the spring will be shortened by: \[ \Delta x = \frac{g T^2}{4\pi^2} \] ---
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