\(\def \u#1{\,\mathrm{#1}}\) \(\def \abs#1{\left|#1\right|}\) \(\def \ast{*}\) \(\def \deg{^{\circ}}\) \(\def \tau{\uptau}\) \(\def \ten#1{\times 10^{#1}}\) \(\def \redcancel#1{{\color{red}\cancel{#1}}}\) \(\def \BLUE#1{{\color{blue} #1}}\) \(\def \RED#1{{\color{red} #1}}\) \(\def \PURPLE#1{{\color{purple} #1}}\) \(\def \th#1,#2{#1,\!#2}\) \(\def \lshift#1#2{\underset{\Leftarrow\atop{#2}}#1}}\) \(\def \rshift#1#2{\underset{\Rightarrow\atop{#2}}#1}}\) \(\def \dotspot{{\color{lightgray}{\circ}}}\) \(\def \ccw{\circlearrowleft}\) \(\def \cw{\circlearrowright}\)
Chapter 3: Linear Motion
16.

Constant Acceleration

When the acceleration of an object is constant, there are a set of equations we can use to predict how that object will move. Consider the motion of the object between some initial moment i and some final moment f. There are five variables we need to completely describe its motion:

(no alternate text)

$$a={\Delta v\over\Delta t}={v_f-v_i\over\Delta t}$$

We already know two equations we can use to solve for these five variables. The first is the definition of acceleration (right), which can be rewritten without fractions as

$$v_f=v_i+a\Delta t$$

The second is the definition of average velocity $\bar v={\Delta x\over \Delta t}$, with the fact (here unproved) that when the acceleration is constant, the average velocity is the average of $v_i$ and $v_f$, giving us

$$\Delta x=\frac12(v_i+v_f)\Delta t$$

Two equations allow us to solve for two unknowns, which means that we need to be given three of the five variables above to solve for the rest. That's worth repeating:

In a one-dimensional constant-acceleration problem,
we must be given three of the five variables
in order to solve for the rest.