// Numbas version: finer_feedback_settings {"name": "SUVAT equations question 10", "extensions": [], "custom_part_types": [], "resources": [["question-resources/ball_image.png", "/srv/numbas/media/question-resources/ball_image.png"]], "navigation": {"allowregen": true, "showfrontpage": false, "preventleave": false, "typeendtoleave": false}, "question_groups": [{"pickingStrategy": "all-ordered", "questions": [{"functions": {}, "ungrouped_variables": ["u", "a", "t", "s"], "name": "SUVAT equations question 10", "tags": [], "advice": "

First it is best to sketch an image of what is happening. The ball rolls through $A$ with constant deceleration and a positive velocity. As it is decelerating it will eventually stop (have velocity $0 \\mathrm{ms^{-1}}$) at some unknown point, say $B$. However the ball will continue to decelerate and therefore will change direction and return to the point $A$.

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a) We have $u=\\var{u}$ and $a = \\var{a}$, where $a$ is negative as the ball is decelerating. We are asked to find the time, $t$, that the ball returns to point $A$, which means the balls displacement from $A$ will be zero. Therefore $s=0$. We use the formula $s = ut+\\frac{1}{2}at^2$ and solve for $t$. As this is a quadratic in $t$ there will be two solutions, however we know that the ball is at point $A$ when $t=0$ so we are trying to find the other value of $t$ which is when the ball returns to point $A$.

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Therefore \\begin{align} s &= ut+ \\frac{1}{2}at^2, \\\\
                                     \\frac{1}{2}at^2 + ut &= 0, \\\\
                                     t\\left(\\frac{1}{2}at+u\\right) &= 0.\\end{align}

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We discard the solution $t=0$ so \\begin{align}
                                        \\frac{1}{2}at + u &=0, \\\\
                                          t & = -\\frac{2u}{a}, \\\\
                                            & = \\var{precround(-(2*u)/a,3)} \\mathrm{s}.
\\end{align} 
Therefore the ball returns to point $A$ after $\\var{precround(-(2*u)/a,3)}$ seconds.

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b) We have $u=\\var{u}$ and $a=\\var{a}$. At the point labelled $B$ in the diagram the velocity of the ball is $v=0$ for an instant as it has reached its furthest point from $A$ and will change direction. We want to find the distance between point $A$ and $B$ and then double it, to calculate the total distance the ball travels as it goes from $A$ to $B$ and back. Therefore we use the equation $v^2 = u^2+2as$, rearranged for $s$.
\\begin{align} v^2 & = u^2 + 2as, \\\\
                    2as & = v^2 - u^2, \\\\
                       s & = \\frac{v^2 - u^2}{2a}, \\\\
                          & = \\frac{ 0 - \\var{u}^2}{2 \\times \\var{a}}, \\\\
                          & = \\var{precround((-u^2)/(2*a),3)} \\mathrm{m}. \\end{align}
So we have the distance from point $A$ to point $B$, $s=\\var{precround((-u^2)/(2*a),3)}$ metres. Therefore the total distance travelled by the ball in $\\var{precround(-(2*u)/a,3)}$ seconds is $2 \\times s=\\var{precround(2*((-u^2)/(2*a)),3)}$ metres.

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Find the time in $\\mathrm{s}$ (to 3d.p.) between when the ball first passes through point $A$ and when it returns to point $A$.

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The total distance in $\\mathrm{m}$ travelled by the ball in this time.

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At time $t=0$ a ball rolls through a point $A$ in the positive direction with a speed $\\var{u} \\mathrm{ms^{-1}}$. The ball rolls with constant deceleration $\\var{-a} \\mathrm{ms^{-2}}$.

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acceleration - negative as decelerating

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initial velocity of the ball

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