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Numericals · Q44

Q.A 2 m long ladder of mass 10 kg is kept against a wall such that its base is 1.2 m away from the wall. The wall is smooth but the ground is rough. The roughness of the ground is such that it offers a maximum horizontal resistive force (for sliding motion) equal to half the normal reaction at the point of contact. A monkey of mass 20 kg starts climbing the ladder. How far can it climb along the ladder? How much is the horizontal reaction at the wall?

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Ladder length 2 m, base 1.2 m from the wall, so by Pythagoras the height reached at the wall is 22−1.22=4−1.44=2.56=1.6\sqrt{2^2-1.2^2}=\sqrt{4-1.44}=\sqrt{2.56}=1.6 m. Working in kg-weight (kgf) units throughout, so that g need not be introduced separately: ground normal reaction Ng=10+20=30N_g=10+20=30 kgf (ladder 10 kg + monkey 20 kg), and the maximum available friction at the ground is fmax=12Ng=15f_{max}=\frac{1}{2}N_g=15 kgf. The wall is smooth, so it supplies only a horizontal reaction NwN_w (no vertical, no friction there); horizontal equilibrium requires Nw=fN_w=f (the ground friction must exactly balance the wall's push).

Let s be the distance the monkey has climbed along the 2 m ladder (from the base); its horizontal position from the base is s2×1.2=0.6s\frac{s}{2}\times1.2=0.6s, and the ladder's own weight (10 kgf) acts at its midpoint, horizontal position 1.22=0.6\frac{1.2}{2}=0.6 m. Taking torques about the BASE of the ladder (where NgN_g and f both act, contributing zero torque about that point) balances the two downward weight-torques against the wall reaction's torque: Nw(1.6)=10(0.6)+20(0.6s)=6+12sN_w(1.6)=10(0.6)+20(0.6s)=6+12s, giving Nw=3.75+7.5sN_w=3.75+7.5s kgf. The monkey can climb further as long as the required NwN_w (equivalently, the required friction f, since f=Nwf=N_w) stays below fmax=15f_{max}=15 kgf; setting Nw=15N_w=15: 3.75+7.5s=15⇒7.5s=11.25⇒s=1.53.75+7.5s=15\Rightarrow 7.5s=11.25\Rightarrow s=1.5 m, at which point Nw=15N_w=15 kgf. …

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