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

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µ2N2 = N1
µ1N1 + N2 = mg
mg = N1L sin θ + µ1N1 cos θ
if µ1 = 0, N2 = mg
N1 =
if µ2 = 0, N1 = 0
N2 = mg
⇒ not possible
N2 =
