Practice portal › Laws of Motion › Friction: Blocks, Belts and Inclines
Asked in JEE Main 6th April 1st Shift 2026 · Friction on belts and accelerating surfaces
Idea: ride with the cube. In its frame each block feels a backward pseudo-force ma, and both blocks are in equilibrium.
Here a=g/2=5 m/s².
Block P, on the frictionless top. Horizontally it feels the thread's pull T towards the pulley and the pseudo-force backwards:
T=m_Pa=2×5=10 N.
Block Q, against the vertical side face. The pseudo-force presses it into that face, so it supplies the normal force:
N=m_Qa=1.5×5=7.5 N.
Q vertically. Its weight is m_Qg=1.5×10=15 N, the thread pulls up with T=10 N, and friction must make up the rest:
f=15-10=5 N, upward.
At the point of holding, f=μ N:
μ=5/(7.5)=2/3≈0.67.
Note where the normal force comes from: not from gravity, as on a table, but entirely from the cube's acceleration — stop the cube and Q falls.
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