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What is the acceleration in $\\mathrm{ms^{-2}}$ of the particle as it slides down the plane if the plane is smooth? 

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What is the acceleration in $\\mathrm{ms^{-2}}$ of the particle as it slides down the plane if the coefficient of friction is $\\var{mu}$?

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Finding the acceleration of a particle on an inclined plane which is at an angle to the horizontal. Smooth then with value for coefficient of friction.

"}, "name": "Simon's copy of inclined plane 1", "advice": "

You can draw a diagram of the forces acting upon the particle.

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(a)

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When the plane is smooth we have that the coefficient of friction $\\mu = 0$. 

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We then resolve $F=ma$ in the direction down the slope. 

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\\begin{align} F &= ma, \\\\
                    mg \\cos ((90 - \\theta)^{\\circ}) & = ma, \\\\
                  \\var{mass} \\times 9.8 \\times \\cos (\\var{90 - theta}^{\\circ}) & = \\var{mass} \\times a, \\\\
                                             9.8 \\cos (\\var{90 - theta}^{\\circ}) & = a, \\\\
                                            \\var{precround(9.8*cos(radians(90-theta)),3)} \\mathrm{ms^{-2}} & = a. \\end{align}

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So the acceleration of the particle when the slope is smooth is $ \\var{precround(9.8*cos(radians(90-theta)),3)} \\mathrm{ms^{-2}}$.

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(b)

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If the plane is rough and the coefficient of friction is $\\mu = \\var{mu}$ then we first resolve the forces perpendicular to the plane to find $R$.

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\\begin{align} F & = ma, \\\\
                   R - mg \\cos \\theta & = 0, \\\\
                           R &= mg \\cos \\theta, \\\\
                              & = \\var{mass} \\times 9.8 \\cos( \\var{theta}^{\\circ})=\\var{precround(mass*9.8*cos((pi/180)*theta),3)}.
                             \\end{align}

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We then resolve $F=ma$ in the direction down the slope, using the value we have for $R$.

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\\begin{align} F & = ma, \\\\
                 mg \\sin \\theta - \\mu R & = ma, \\\\
                  mg \\sin \\theta - \\mu mg \\cos \\theta & = ma, \\\\
                     g \\sin \\theta - \\mu g \\cos \\theta & = a, \\\\
                     \\left(9.8\\sin(\\var{theta}^{\\circ})\\right) - \\left(\\var{mu}\\times 9.8 \\cos(\\var{theta}^{\\circ})\\right)& = a, \\\\
                     \\var{precround(9.8*sin(radians(theta))-mu*9.8*cos(radians(theta)),3)} \\mathrm{ms^{-2}} & = a. \\end{align}

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So the acceleration of the acceleration of the particle is $\\var{precround(9.8*sin(radians(theta))-mu*9.8*cos(radians(theta)),3)} \\mathrm{ms^{-2}}$ when the coefficient of friction is $mu=\\var{mu}$.

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Suppose that there is a plane which is inclined to the horizontal at an angle of $\\var{theta}^{\\circ}$. A particle of mass $\\var{mass}\\mathrm{kg}$ is placed upon the plane. 

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All parts should be answered to 3d.p and the acceleration due to gravity should be taken as $g = 9.8 \\mathrm{ms^{-2}}$.

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