Kinematics graphs: displacement, velocity and acceleration
Kinematics graphs describe how motion changes with time. The central ideas are:
For straight line motion, the gradient of a displacement time graph is velocity, the gradient of a velocity time graph is acceleration, and the signed area under a velocity time graph is displacement.
Prerequisites
Section titled “Prerequisites”You should be able to:
- distinguish displacement from distance, and velocity from speed, using kinematics language;
- calculate the gradient of a straight line;
- find areas of rectangles, triangles and trapezia;
- interpret negative coordinates and choose a positive direction;
- use SI units from quantities and units in mechanics.
This lesson concerns motion along a straight line. Time is plotted horizontally and cannot run backwards.
The three graph types
Section titled “The three graph types”Let , and denote displacement, velocity and acceleration. Their connections are:
| Graph | Gradient represents | Signed area between and represents |
|---|---|---|
| displacement time | velocity, | no standard kinematic quantity |
| velocity time | acceleration, | displacement, |
| acceleration time | rate of change of acceleration | change in velocity, |
In compact form,
and
You do not need calculus to use straight line segments: gradient and elementary area are enough. The notation explains why those methods work and prepares you for calculus in kinematics.
Displacement time graphs
Section titled “Displacement time graphs”A point gives the particle’s displacement from the chosen origin at time . The sign of tells you which side of the origin the particle occupies. It does not tell you its direction of travel.
The gradient gives velocity:
Therefore:
- a positive gradient means motion in the positive direction;
- a negative gradient means motion in the negative direction;
- a horizontal section means the particle is stationary;
- a steeper graph means a greater speed;
- a changing gradient means the velocity is changing.
A straight line has constant velocity. A curve that becomes steeper has increasing speed, but the sign of its gradient still determines the direction.
Worked example 1: reading piecewise displacement
Section titled “Worked example 1: reading piecewise displacement”A particle’s displacement time graph joins the points
with straight line segments. Distances are in metres and times in seconds. Describe the motion and find the velocity on each interval.
From ,
The particle moves in the positive direction from to .
From , the graph is horizontal, so
The particle remains at for seconds.
From ,
It moves in the negative direction, passes the origin, and finishes at . The negative displacement at the end describes position, not distance travelled.
Its total distance is
Curvature and acceleration
Section titled “Curvature and acceleration”On a smooth displacement time curve, acceleration describes how the gradient changes:
- increasing gradient means ;
- decreasing gradient means ;
- constant gradient means .
For example, a graph can slope downwards while becoming less steep. Then but , so the particle moves in the negative direction while slowing down.
Self-check 1
Section titled “Self-check 1”A displacement time graph is a straight line from to . Find the velocity and the time at which the particle crosses the origin.
Answer
The velocity is the gradient:
Starting at when , the displacement is . Set :
Velocity time graphs
Section titled “Velocity time graphs”A point gives the instantaneous velocity. The graph’s height gives velocity, while its distance from the time axis gives speed:
Above the time axis, and motion is in the positive direction. Below it, and motion is in the negative direction. Crossing the axis usually indicates a change of direction.
The gradient gives acceleration:
A horizontal velocity time segment means constant velocity and zero acceleration. It does not mean the particle is stationary unless the segment lies on .
Signed area and displacement
Section titled “Signed area and displacement”Area above the time axis counts positively and area below counts negatively:
Total distance counts both positively:
More precisely, distance is the area between the graph and the time axis. Split the interval wherever .
Worked example 2: acceleration, displacement and distance
Section titled “Worked example 2: acceleration, displacement and distance”A particle has a velocity time graph made of straight lines joining
Find the acceleration on each stage, the time at which the particle reverses, its displacement, and its total distance during the seconds.
The gradients give the accelerations:
and
On the last stage, velocity falls from at each second. It reaches zero after seconds, at
The particle reverses there. Calculate signed areas:
The third trapezium formula already includes the negative portion, so the displacement is
For distance, split the final stage at . Its positive triangular area is
and its negative triangular area has magnitude
Hence
The distance, about m, is greater than the displacement because the particle reverses.
Worked example 3: reconstructing a velocity graph
Section titled “Worked example 3: reconstructing a velocity graph”A car starts from rest, accelerates uniformly at for seconds, travels at constant velocity for seconds, then decelerates uniformly to rest in seconds. Find its maximum velocity and total distance.
After seconds,
The velocity time graph joins
The total distance is the area under the graph:
This is also a derivation of the constant acceleration result that displacement equals average velocity multiplied by time. See constant acceleration and SUVAT equations.
Self-check 2
Section titled “Self-check 2”A velocity time graph joins to with a straight line. Find the acceleration, when the particle changes direction, the displacement, and the distance travelled.
Answer
The acceleration is
Since , the velocity is zero at seconds. The signed trapezium area is
For distance, split at :
Acceleration time graphs
Section titled “Acceleration time graphs”The height of an acceleration time graph gives acceleration. Its signed area gives change in velocity:
Area does not give the final velocity unless the initial velocity is known:
An acceleration graph below the axis means . Whether the particle speeds up or slows down still depends on the sign of .
Worked example 4: change in velocity
Section titled “Worked example 4: change in velocity”A particle has initial velocity . Its acceleration is for , then for . Find its velocity at and .
During the first stage,
so
During the second stage,
so
Although acceleration is negative for the last seconds, velocity remains positive. The particle slows down but does not reverse.
Self-check 3
Section titled “Self-check 3”A particle begins with velocity . Its acceleration increases linearly from at to at . Find its velocity at .
Answer
The change in velocity is the triangular area:
Therefore
Moving between graphs
Section titled “Moving between graphs”To sketch a velocity graph from a displacement graph, track the displacement graph’s gradient, not its height. To sketch an acceleration graph from a velocity graph, track the velocity graph’s gradient.
For example, if a velocity time graph is:
- a straight line rising from to , acceleration is a positive constant throughout, including when ;
- horizontal at , acceleration is zero;
- a straight line falling, acceleration is a negative constant.
At a sharp corner, the gradient changes instantaneously. In an idealised piecewise model, acceleration jumps and is not defined at that single instant. Do not invent a sloping transition unless the question supplies one.
Conversely, moving from an acceleration graph to a velocity graph requires an initial velocity. Moving from velocity to displacement requires an initial displacement. Area gives change, so without an initial value there are infinitely many vertically shifted graphs.
Common misconceptions
Section titled “Common misconceptions”Position is not direction
Section titled “Position is not direction”A particle can have and . It is then left of the origin but moving in the positive direction.
Negative velocity is not negative speed
Section titled “Negative velocity is not negative speed”Velocity may be negative, but speed is and is never negative.
Negative acceleration is not always deceleration
Section titled “Negative acceleration is not always deceleration”If and , velocity becomes more negative and speed increases. Speed decreases only when and have opposite signs.
Zero velocity is not zero acceleration
Section titled “Zero velocity is not zero acceleration”At a reversal, may be zero while the velocity graph has a nonzero gradient, so .
Area must carry units
Section titled “Area must carry units”Under a velocity time graph,
Under an acceleration time graph,
These unit products help identify what an area means.
Exam method
Section titled “Exam method”- Read both axes, scales and units.
- Mark any axis crossings and stage boundaries.
- For a gradient, use two points on the relevant straight line or a tangent to a curve.
- For displacement, use signed area.
- For distance, split wherever velocity changes sign and add magnitudes.
- State signs and units, then interpret negative answers in context.
Mixed self-check
Section titled “Mixed self-check”A particle starts at displacement m with velocity . Its velocity increases linearly to at , then decreases linearly to at .
- Find the acceleration on each stage.
- Find when the particle changes direction.
- Find its displacement from the origin at .
- Find the total distance travelled.
Answer
On the first stage,
On the second,
Starting from at , velocity reaches zero seconds later, so the particle reverses at .
The signed area under the velocity graph is
Therefore its displacement from the origin is
For distance, split the second stage at :
Next steps
Section titled “Next steps”- Use straight line velocity graphs to understand and derive the constant acceleration equations.
- Extend gradients and areas to functions and curves in calculus in kinematics.
- Apply the same sign discipline to vertical and horizontal components in two dimensional motion and projectiles.