A uniform cube of side a and mass m rests on a rough horizontal table. A horizontal force F is applied normal to one of the faces at a point directly above the centre of the face, at a height 3a/4 above the base. The minimum value of F for which the cube begins to topple on an edge is (assume the cube does not slide):
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For toppling problems, always take moments about the edge of rotation.
Step 1: At the point of toppling, torque about the edge is balanced.
Step 2: Torque due to applied force,
F × (3a)/(4)
Step 3: Torque due to weight,
mg × (a)/(2)
Step 4: Equating torques,
F · (3a)/(4) = mg · (a)/(2)
Step 5: Solving,
F = (mg)/(2)