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Question: Two smooth blocks of masses $m$ and $m'$ connected by a light inextensible strings are moving on a s...

Two smooth blocks of masses mm and mm' connected by a light inextensible strings are moving on a smooth wedge of mass MM. If a force FF acts on the wedge the blocks do not slide relative to the wedge. Find the (a) acceleration of the wedge and (b) value of FF.

Answer

(a) Acceleration of the wedge: a=mgma = \frac{m'g}{m}

(b) Value of FF: F=mgm(M+m+m)F = \frac{m'g}{m}(M + m + m')

Explanation

Solution

The problem asks us to find the acceleration of the wedge and the applied force FF under the condition that the blocks do not slide relative to the wedge.

Understanding the Constraint:

The crucial condition "the blocks do not slide relative to the wedge" implies that all three bodies (block mm, block mm', and wedge MM) move together as a single system in the horizontal direction. Let their common horizontal acceleration be aa.

Part (a): Acceleration of the wedge

  1. Free Body Diagram for block mm:

    Block mm is on the horizontal surface of the wedge. The only horizontal force acting on it is the tension TT from the string. Applying Newton's second law in the horizontal direction for block mm: T=ma(Equation 1)T = m a \quad \text{(Equation 1)}

  2. Free Body Diagram for block mm':

    Block mm' is hanging vertically. The forces acting on it are the tension TT in the string (upwards) and its weight mgm'g (downwards). Since block mm' does not slide relative to the wedge, its vertical acceleration must be zero (as the wedge itself has no vertical acceleration). Applying Newton's second law in the vertical direction for block mm': Tmg=0T - m'g = 0 T=mg(Equation 2)T = m'g \quad \text{(Equation 2)}

  3. Solving for acceleration aa:

    Equating the expressions for tension TT from Equation 1 and Equation 2: ma=mgma = m'g Therefore, the acceleration of the wedge (and the blocks) is: a=mgma = \frac{m'g}{m}

Part (b): Value of Force FF

  1. Consider the entire system:

    The external horizontal force acting on the combined system (wedge MM + block mm + block mm') is FF. The total mass of this combined system is (M+m+m)(M + m + m'). Applying Newton's second law to the entire system in the horizontal direction: F=(M+m+m)aF = (M + m + m') a

  2. Substitute the value of aa:

    Substitute the expression for aa found in Part (a) into this equation: F=(M+m+m)(mgm)F = (M + m + m') \left(\frac{m'g}{m}\right) F=mgm(M+m+m)F = \frac{m'g}{m}(M + m + m')

The condition that blocks do not slide relative to the wedge implies a common horizontal acceleration aa for all three masses. By analyzing the forces on block mm horizontally (T=maT=ma) and on block mm' vertically (T=mgT=m'g), we find a=mg/ma = m'g/m. Then, considering the entire system, the net external force FF causes this common acceleration, so F=(M+m+m)aF = (M+m+m')a. Substituting aa gives the value of FF.