Step 1: Read the pulley arrangement.
The block carries a small movable pulley bolted to it, and the string runs from a fixed point, around this movable pulley, over the large fixed pulley at the top, and down to the hanging mass \(M\). Because the block's pulley is a movable pulley, two string segments pull the block toward the top of the incline, so the net pulling force on the block is \(2T\), where \(T\) is the tension in the string.
Step 2: Relate T to the hanging mass.
The string is massless and the pulleys are frictionless, so the tension is the same throughout the string. At the point of impending motion the hanging mass is in equilibrium, giving \(T = Mg\).
Step 3: Write the force balance on the block along the incline.
At the verge of sliding up, friction acts down the incline at its full static value. Along the incline: \(2T = mg\sin\theta + \mu mg\cos\theta\), where \(m = 50\) kg, \(\theta = 30^{\circ}\), and \(\mu = 0.3\).
Step 4: Substitute T = Mg and solve for M.
\[ 2Mg = mg(\sin\theta + \mu\cos\theta) \implies M = \frac{m(\sin\theta+\mu\cos\theta)}{2} \]
With \(\sin30^{\circ}=0.5\) and \(\cos30^{\circ}=0.866\): \(M = \dfrac{50(0.5 + 0.3\times0.866)}{2} = \dfrac{50(0.5+0.2598)}{2} = \dfrac{50\times0.7598}{2} = \dfrac{37.99}{2} = 19.0\) kg.
Final Answer:
The movable pulley doubles the pulling force for a given string tension, so the required hanging mass works out to about 19.0 kg.
\[ \boxed{M \approx 19.0\ \text{kg}} \]