Note: the direction of 'extra' force "{\\vec F}" is not specified in the problem so we shall assume it is directed along the slope
Let "Ox" axis be along the inclined plane (positive direction in direction of possible sliding) and "Oy" axis is perpendicular to the inclined plane. There are 4 power actiong on the box: gravitational force "m\\vec g" , force of friction "{{\\vec F}_{{\\rm{frict}}}}" , normal force "{\\vec N}" and the 'extra' force "{\\vec F}" we need to find.
Let's write down the Newton's second law assume there's no sliding
Assume that the force "{\\vec F}" has component only along the "Ox" - axis let's project this equations to the "Oy" axis. The componenst of vectors are "\\vec g = g(\\cos \\alpha ,\\sin \\alpha )" , "\\vec N = (0,N)" , "{{\\vec F}_{{\\rm{frict}}}} = ( - {F_{{\\rm{frict}}}},0)" and "F = ( - F,0)" (whe choose minus sign for x-component of extra force because it should be directed against the direction of possible sliding). Then the equation for the "Oy" axis is
thus
"N = mg\\cos \\alpha"Now we use "{F_{{\\rm{frict}}}} = \\mu N" (Amontons-Coulomb friction law) and write down the equation for the "Ox" axis
thus
"{F_x} \\approx 5{\\rm{[kg}}] \\cdot 9.8[{{\\rm{m}} \\over {{{\\rm{s}}^{\\rm{2}}}}}] \\cdot (\\sin {\\pi \\over 6} - 0.3\\cos {\\pi \\over 6}) \\approx 11.8[{\\rm{N}}]"
So "\\left| {\\vec F} \\right| \\approx 11.8[{\\rm{N}}]"
This is the answer.
Comments
Leave a comment