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 \$(t1, s1)\$ and \$(t2, s2)\$ on the line.
Compute \$\Delta s = s2 - s1\$ and \$\Delta t = t2 - t1\$.
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: \$(t1, s1) = (0,\ 0)\$ and \$(t2, s2) = (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.