Suppose an object is moving along a one-dimensional position axis. The object starts its motion at _t_ = 0 at the position _x_ = 0 and with velocity _v_ = 0. It has an acceleration of +2.0 m/s ^2^. After 4.0 seconds, the object's acceleration instantaneously changes to - 2.0 m/s ^2^. Plot velocity and position versus time graphs for the first 8.0 seconds of the object's motion.
System: The object will be treated as a point particle.
Model: [One-Dimensional Motion with Constant Acceleration|1-D Motion (Constant Acceleration)].
Approach: We will use the model twice. Once to describe the motion from _t_ = 0 seconds to _t_ = 4.0 seconds, and once more to describe the motion from _t_ = 4.0 seconds to _t_ = 8.0 seconds.
For the first part of the motion, our givens are:
{panel:title=givens}{latex}\begin{large}\[ t_{\rm i} = \mbox{0 s} \]\[t = \mbox{4.0 s} \]\[x_{\rm i} = \mbox{0 m} \] \[ v_{\rm i} = \mbox{0 m/s} \] \[ a = \mbox{2.0 m/s}^{2} \] \end{large}{latex}{panel}
We begin by finding the velocity. The simplest Law of Change appropriate to our givens is:
{latex}\begin{large}\[ v = v_{\rm i} + a (t-t_{\rm i}) \]\end{large}{latex}
which, after substituting the givens, tells us:
{latex}\begin{large} \[ v = (\mbox{2.0 m/s}^{2}) t \] \end{large}{latex}
This is the equation for a line with slope 2 and intercept 0, giving the graph:
VELPLOT 1
We then find the position. The most direct Law of Change is:
{latex}\begin{large} \[ x = x_{\rm i} + v_{\rm i} (t-t_{\rm i}) + \frac{1}{2} a (t-t_{\rm i})^{2} = \frac{1}{2}(\mbox{2.0 m/s}^{2})t^{2}\] \end{large}{latex}
which yields the parabolic graph:
POSPLOT1
We now wish to analyze the second part of the motion. In this part of the motion, we must change our givens. We now have _t_~i~ = 4.0 s, _t_ = 8.0 s, and _a_ = -- 2.0 m/s ^2^. Unfortunately, this is *not* enough. We do not know _x_~i~, x, _v_~i~ or _v_. We have too few givens to proceed.
The answer to this dilemma is simple. We have just derived expressions that give _x_ and _v_ for any time between 0 s and 4.0 s. We would like to know _x_ and _v_ at 4.0 s. Thus, we can use the _final_ time of the first part of the problem to obtain the _initial_ conditions for the second part. From our graphs or from the equations, we can complete our list of givens for the second part:
{panel:title=givens (second part)}{latex}\begin{large}\[ t_{\rm i} = \mbox{4.0 s}\]\[t = \mbox{8.0 s} \] \[ x_{\rm i} = \mbox{16 m} \] \[ v_{\rm i} = \mbox{8 m/s} \] \[ a = \mbox{-2.0 m/s}^{2}\] \end{large}{latex}{panel}
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