A 3 kg block is connected as shown in the figure. Spring constants of two springs \( K_1 \) and \( K_2 \) are 50 Nm\(^{-1}\) and 150 Nm\(^{-1}\) respectively. The block is released from rest with the springs unstretched. The acceleration of the block in its lowest position is ( \( g = 10 \) ms\(^{-2}\) )
When the block is released from rest, all of its gravitational potential energy is converted into spring potential energy at its lowest point. Let both springs stretch by \( x \) meters (since they are symmetrically placed and the block moves straight down).
Total spring potential energy: \[ PE_{\text{spring}} = \frac{1}{2}K_1 x^2 + \frac{1}{2}K_2 x^2 = \frac{1}{2}(K_1 + K_2)x^2 = \frac{1}{2}(50 + 150)x^2 = 100x^2 \] Gravitational potential energy lost: \[ PE_{\text{gravity}} = m g x = 3 \cdot 10 \cdot x = 30x \]
\[ 30x = 100x^2 \quad \Rightarrow \quad 3x = 10x^2 \quad \Rightarrow \quad x = 0.3 \, \text{m} \]
At the lowest point, net force acting on the block: \[ F = mg - (K_1 + K_2)x = 30 - (50 + 150)\cdot 0.3 = 30 - 200 \cdot 0.3 = 30 - 60 = -30 \, \text{N} \] The negative sign indicates the net force is upward (restoring direction).
\[ a = \frac{F}{m} = \frac{-30}{3} = -10 \, \text{m/s}^2 \] Taking magnitude (as the question asks for acceleration, not direction): \[ \boxed{a = 10 \, \text{m/s}^2} \]
The acceleration of the block at its lowest point is \( \boxed{10 \, \text{m/s}^2} \).
A 4 kg mass is suspended as shown in the figure. All pulleys are frictionless and spring constant \( K \) is \( 8 \times 10^3 \) Nm\(^{-1}\). The extension in spring is ( \( g = 10 \) ms\(^{-2}\) )