If the coefficient of friction between A and B is μ, the maximum acceleration of the wedge A for which B will remain at rest with respect to wedge is
A
μg
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B
g[1+μ1−μ]
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C
g[1−μ1+μ]
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D
gμ
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Solution
The correct option is Bg[1+μ1−μ] By placing the frame of reference on block A, FBD of B is
Let, N be the normal force acting. Now taking components of all the forces perpendicular to the plane N−mgcosθ−masinθ=0 N=mg+ma√2 As, f=μN f=μm(g+a)√2 Taking mg and ma along f mgsinθ+f=macosθ mg√2+μm(g+a)√2=ma√2 a=g[1+μ1−μ]