Let us describe the forces that are applied to the body. Let the x-axis be directed along the inclined plane and y-axis be perpendicular to the plane. Therefore, the projection of forces on the y-axis is
"y: -mg\\cos\\alpha + N = 0," (1)
and on the x-axis
"x: mg\\sin\\alpha - F_{fr} = ma." (2)
From (2) we get
"F_{fr} = mg\\sin\\alpha - ma = m(g\\sin\\alpha-a) = 18.0\\,\\mathrm{kg}(9.8\\,\\mathrm{m\/s^2} \\sin37^\\circ - 0.270\\,\\mathrm{m\/s^2})= 101.3\\,\\mathrm{N}."
We know that "F_{fr} = \\mu N = \\mu mg\\cos\\alpha," so
"\\mu = \\dfrac{F_{fr}}{mg\\cos\\alpha} = \\dfrac{101.3\\,\\mathrm{N}}{18.0\\,\\mathrm{kg}\\cdot9.8\\,\\mathrm{m\/s^2}\\cdot\\cos37^\\circ} = 0.719."
Comments
Leave a comment