Consider the arrangement shown in the figure. Assuming friction-less contacts, then the magnitude of external horizontal force P applied at the lower end for an equilibrium of the rod will be: (The rod is uniform and its mass is ′m′)
A
mg2
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B
mg2cotθ
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C
mg2tanθ
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D
mg2secθ
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Solution
The correct option is Bmg2cotθ Let length of the rod=l from ∑fx=0 P=R2 from ∑fy=0 R1=mg taking moment at A R2×BC=mg×AM R2×Lsinθ=mg×12cosθ R2=mg2lcosθsinθ R2=P=mg2cotθ