Step 1: Understanding the Concept:
When the mass is released, it falls under gravity, and the spring stretches. The mass will momentarily come to rest at the maximum extension $x_{\max}$. At this point, the loss in gravitational potential energy is completely converted into the elastic potential energy of the spring.
Step 2: Key Formula or Approach:
Using the Work-Energy Theorem or Conservation of Mechanical Energy: \[ \Delta K + \Delta U_g + \Delta U_s = 0 \] Since the initial and final velocities are zero, $\Delta K = 0$.
Step 3: Detailed Explanation:
Let the maximum extension be $x_{\max}$. The loss in gravitational potential energy of the mass is: \[ \Delta U_g = -Mg x_{\max} \] The gain in elastic potential energy of the spring is: \[ \Delta U_s = \frac{1}{2} k x_{\max}^2 \] Equating the magnitudes (or setting the sum to zero): \[ Mg x_{\max} = \frac{1}{2} k x_{\max}^2 \] Since $x_{\max} \neq 0$: \[ Mg = \frac{1}{2} k x_{\max} \] \[ x_{\max} = \frac{2Mg}{k} \] Step 4: Final Answer:
The maximum extension in the spring is $2Mg/k$.
Five identical springs are used in the three configurations as shown in figure. The time periods of vertical oscillations in configurations (a), (b) and (c) are in the ratio. 