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−^1
From 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)
b
b
b
0
1
2
3
4
5
6
7
8
9
0 1 2 3 4
acceleration
a
(m
−·s
2 )
timet(s)
bbb
Graphs for motion with a constant acceleration starting from rest.
414 Physics: Mechanics