Where the SUVAT Equations Come From
Where the SUVAT Equations Come From
- When the acceleration is constant, the v-t graph is one straight line, and everything about the motion can be read from that line.
- The four equations of motion (the SUVAT equations) are only the gradient and the area of that line, written in symbols.
One line, four equations
Build the four equations from that one line, one at a time. Each is just a small step from the line or from the equation before it.
Equation 1 — from the gradient
- The line goes up from at the start to at time .
- Gradient is the acceleration: .
- Multiply both sides by : .
- Add to both sides: .
Equation 2 — area as a trapezium
- The displacement is the area under the line.
- That area is a trapezium: the two upright sides are and , and the width is .
- Area of a trapezium = average of the two sides × width.
- The average of and is , so .
Equation 3 — split the same area
- Cut the same area into a rectangle with a triangle on top.
- Rectangle: height , width , so its area is .
- Triangle: width , height , which is from Equation 1.
- Triangle area .
- Add the two parts: .
Equation 4 — remove t
- From Equation 1, make the subject: .
- Put this into Equation 2: .
- The top becomes , so .
- Rearrange: .
Symbols
- = displacement (m)
- = initial velocity (m s⁻¹)
- = final velocity (m s⁻¹)
- = acceleration (constant) (m s⁻²)
- = time taken (s)
- Each equation uses four of the five letters and leaves one out. That fact becomes the method on the next page.
- Only and are printed on the exam data sheet. Know the other two from memory.
- A show-that question can ask you to build any of these from the graph, so learn the gradient-and-area reasoning, not just the four results.
Common mistake
These equations need constant acceleration in a straight line. If the acceleration changes (for example, when air resistance becomes important), they no longer apply; go back to the graph.