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In the figure, a ladder of mass m is shown leaning against a wall. It is in static equilibrium making an angle θ with the horizontal floor. The coefficient of friction between the wall and the ladder is μ1 and that between the floor and the ladder is μ2. The normal reaction of the wall on the ladder is N1 and that of the floor is N2. If the ladder is about to slip, then

(A) μ1 = 0 μ2 ≠ 0 and Ntanθ = mg/2

(B) μ1  ≠ 0 μ= 0 and Ntanθ = mg/2

(C) μ1  ≠ 0 μ≠ 0 and N= mg/1+μ1μ2

(D)  μ1  = 0 μ2  ≠ 0 and N1 tan θ = mg/2

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(C) μ1  ≠ 0 μ≠ 0 and N= mg/1+μ1μ2

(D)  μ1  = 0 μ2  ≠ 0 and N1 tan θ = mg/2

Condition of translational equilibrium

Applying torque equation about corner (left) point on the floor

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