Answer:
Explanation:
Let the board length be L
Let the board mass be m
Let the reaction force of the wall on the board be R
Let the normal force of the floor on the board be F
Let the angle from floor to board be θ
Sum vertical forces to zero
F - mg = 0
F = mg
Sum horizontal forces to zero
μF - R = 0
μF = R
Sum moments about the floor contact point to zero
R[Lsinθ] - mg[½Lcosθ] = 0
R[Lsinθ] = mg[½Lcosθ]
Rsinθ = mg½cosθ
μFsinθ = F½cosθ
μsinθ = ½cosθ
sinθ/cosθ = 1/(2μ)
tanθ = 1/(2(0.584))
θ = 40.5689606...
θ = 40.6°