Cambridge A-Level Physics 9702 – Equations of Motion
Equations of Motion
Objective
Determine the instantaneous velocity of an object by analysing the gradient (slope) of its displacement–time graph.
Key Concepts
Displacement ($s$) is the position of an object relative to a chosen origin.
Time ($t$) is measured uniformly and increases in the forward direction.
The gradient of a straight line on a graph is given by the ratio of the vertical change to the horizontal change.
For a displacement–time graph, the gradient represents velocity.
Mathematical Relationship
The average velocity over a time interval $\Delta t$ is
$$v_{\text{avg}} = \frac{\Delta s}{\Delta t}$$
In the limit as $\Delta t \to 0$, the average velocity becomes the instantaneous velocity:
$$v = \frac{ds}{dt}$$
Procedure to Find \cdot elocity from a Displacement–Time Graph
Identify the portion of the graph for which the velocity is required.
If the graph is a straight line, the velocity is constant. Calculate the gradient directly:
Choose two points $(t_1, s_1)$ and $(t_2, s_2)$ on the line.
Compute $\Delta s = s_2 - s_1$ and $\Delta t = t_2 - t_1$.
Use $v = \dfrac{\Delta s}{\Delta t}$.
If the graph is curved, the velocity at a particular instant is the gradient of the tangent to the curve at that point.
Draw a tangent line at the point of interest.
Measure the rise and run of the tangent (use a ruler or grid).
Calculate the gradient as above.
Record the sign of the gradient:
Positive gradient → motion in the positive direction.
Negative gradient → motion in the opposite direction.
Check units: displacement in metres (m), time in seconds (s), so velocity in metres per second (m s⁻¹).
Worked Example
A car moves along a straight road. The displacement–time graph for the interval $0 \le t \le 8\ \text{s}$ is a straight line passing through the points $(0\ \text{s},\ 0\ \text{m})$ and $(8\ \text{s},\ 40\ \text{m})$.
Find the velocity of the car.
Identify two points: $(t_1, s_1) = (0,\ 0)$ and $(t_2, s_2) = (8,\ 40)$.
The positive sign indicates motion in the positive direction.
Common Pitfalls
Mixing up displacement with distance travelled – displacement can be negative, distance cannot.
Reading the gradient from a curved segment without drawing a proper tangent.
Forgetting to keep consistent units when calculating $\Delta s$ and $\Delta t$.
Interpreting the area under a velocity–time graph as displacement, not the gradient of a displacement–time graph.
Summary Table
Graph Type
Shape of $s$–$t$ Curve
Velocity
Interpretation
Straight line (positive slope)
Linear increase
Constant $v = \dfrac{\Delta s}{\Delta t} > 0$
Uniform motion in positive direction
Straight line (negative slope)
Linear decrease
Constant $v = \dfrac{\Delta s}{\Delta t} < 0$
Uniform motion in negative direction
Horizontal line
Zero slope
$v = 0$
Object at rest
Curved line
Changing slope
Variable $v$ (gradient of tangent)
Accelerated motion
Suggested diagram: A displacement–time graph showing a straight‑line segment, a curved segment, and a horizontal segment with tangents drawn to illustrate gradient calculation.
Practice Questions
From a displacement–time graph, a particle moves from $s = 2\ \text{m}$ at $t = 1\ \text{s}$ to $s = 14\ \text{m}$ at $t = 5\ \text{s}$. Calculate its average velocity.
A graph shows a curved $s$–$t$ relationship. At $t = 3\ \text{s}$ the tangent to the curve has a rise of $6\ \text{m}$ for a run of $2\ \text{s}$. Determine the instantaneous velocity at that instant.
Explain why the gradient of a horizontal segment of a displacement–time graph is zero, and what physical situation this represents.