21.6 CHAPTER 21. MOTION IN ONE DIMENSION
~v 2 s=∆∆~xt=~xtf−~xi
f−ti
= 215 , 5 ms−− 15 , 5 ms= 10m·s−^1~v 3 s=∆∆~xt=~xtf−~xi
f−ti
= 330 , 5 ms−− 215 , 5 ms= 15m·s−^1From these velocities, we can draw the velocity-time graph which forms a straight line.
The acceleration is the gradient of thevvs.tgraph and can be calculated as follows:
a=∆∆~vt=~vtf−~vi
f−ti
=^15 m·s− (^1) − 5 m·s− 1
3 s− 1 s
= 5m·s−^2
The acceleration does not change during the motion (the gradient stays constant). This is
motion at constant or uniform acceleration.
The graphs for this situation are shown below:
0
5
10
15
20
0 1 2 3 4
position
x
(m)
timet(s)
b
b
b
0
5
10
15
0 1 2 3 4
velocity
v
(m
−·s
1 )
timet(s)bbb01234567890 1 2 3 4accelerationa(m−·s2 )
timet(s)bbbGraphs for motion with a constant acceleration starting from rest.414 Physics: Mechanics