(a) Let us determine the projections of forces on the axis directed along the plane (x) and on the axis perpendicular to plane (y). If the angle between the plane and the horizontal is "\\alpha" and the block doesn't slip, then
"y: mg\\cos\\alpha-N = 0 \\;\\Rightarrow \\; N = mg\\cos\\alpha, \\\\\nx: mg\\sin\\alpha - F_{\\text{fr}} = 0."
For the greatest angle the friction force will be "F_{fr} = \\mu N = \\mu mg\\cos\\alpha." Therefore, "mg\\sin\\alpha = \\mu mg\\cos\\alpha\\; \\Rightarrow \\; \\tan\\alpha = \\mu, \\; \\alpha = \\arctan\\mu = \\arctan 0.30 \\approx 16.7^\\circ."
(b) Let us determine the projections of forces in this case.
"y: mg\\cos\\beta-N = 0 \\;\\Rightarrow \\; N = mg\\cos\\beta, \\\\\nx: mg\\sin\\beta - F_{\\text{fr}} - F = 0."
In this case "F_{fr} = \\mu N = \\mu m g\\cos\\beta," so "F = mg\\sin\\beta - \\mu m g \\cos\\alpha = mg(\\sin\\beta - \\mu\\cos\\alpha) = 0.150\\,\\mathrm{kg}\\cdot9.81\\,\\mathrm{N\/kg}\\cdot(\\sin30^\\circ- 0.30\\cos30^\\circ) = 0.35\\,\\mathrm{N}."
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