
\(\frac{1}{5}\) ms–2
\(\frac{4}{5}\) ms–2
\(\frac{8}{11}\) ms–2
To find the acceleration of the block, we need to analyze the forces acting on both the 40 kg block on the surface and the 4 kg block hanging from the pulley.
Let's denote:
For the 40 kg block on the surface, the forces are:
The net force equation for the 40 kg block is:
T - \mu \cdot M \cdot g = M \cdot a
For the 4 kg hanging block, the forces are:
The net force equation for the 4 kg block is:
m \cdot g - T = m \cdot a
Substituting the known values:
Simplifying the equations:
Solving these two equations simultaneously:
40 - 8 = 44 a \Rightarrow 32 = 44a \Rightarrow a = \frac{32}{44} = \frac{8}{11} \, \text{ms}^{-2}
Therefore, the acceleration of the block is \frac{8}{11} \, \text{ms}^{-2}.