21.6 CHAPTER 21. MOTION IN ONE DIMENSION
0
20
40
60
80
100
0 20 40 60 80 100
position
x
(m)
timet(s)
b
∆t
b ∆x
b
− 1
− 2
20 40 60 80 100
velocity
v
(m
−·s
1 )
timet(s)
b b b
0
1
2
0 20 40 60 80 100
acceleration
a
(m
−·s
2 )
timet(s)
b b b
Graphs for motion with a constant negative velocity. The area of the shaded portion in the
vvs.tgraph corresponds to the object’s displacement.
We see that the~vvs.tgraph is a horizontal line. If the velocity vs. time graph is a horizontal
line, it means that the velocity isconstant(not changing). Motion at a constant velocity is
known asuniform motion. We can use the~xvs.tto calculate the velocity by finding the
gradient of the line.
v=∆∆~xt
=~xtf−~xi
f−ti
=^0100 m−s^100 − 0 sm
=− 1 m·s−^1
Vivian has a velocity of− 1 m·s−^1 , or 1 m·s−^1 towards her house. You will notice that the
~vvs.tgraph is a horizontal line corresponding to a velocity of− 1 m·s−^1. The horizontal
line means that the velocity stays the same (remains constant) during the motion. This is
uniform velocity.
We can use the~vvs.tto calculate the acceleration by finding the gradient of the line.
a=∆∆~vt
=~vtf−~vi
f−ti
=^1 m·s
− (^1) − 1 m·s− 1
100 s− 0 s
= 0m·s−^2
Vivian has an acceleration of 0 m·s−^2. You will notice that the graph of~avs.tis a horizontal
line corresponding to an acceleration value of 0 m·s−^2. There is no acceleration during
the motion because his velocity does not change.
We can use the~vvs.tgraph to calculate the displacement by finding the area under the
graph.
410 Physics: Mechanics