MathsMechanics › Kinematics with constant acceleration

Kinematics with constant acceleration

When acceleration holds steady, five quantities lock together and any three determine the rest. The suvat equations are the bookkeeping, the velocity-time graph is the reason they work, and gravity is the standard example.

Year 12-13EDEXCEL 9MA0 M7

Builds on Modelling, quantities and units.

IN THIS TOPIC

  • Read displacement and acceleration from velocity-time graphs.
  • Select and use the suvat equations for constant acceleration.
  • Model vertical motion under gravity, using the symmetry of up-and-down flight.

WHAT YOU PROBABLY THINK

At the top of its flight a thrown ball has zero acceleration.

The graph behind the formulas

A velocity time graph from 4 up to 10 metres per second over 3 seconds: the gradient is the acceleration 2 and the area 21 is the displacementarea = s = 21 mgradient = a = 243
FIG. 1One trapezium holds the whole theory: gradient a, area s.

Plot velocity against time and constant acceleration is a straight line: gradient is the acceleration, area underneath is the displacement. Every suvat equation is this trapezium described in symbols:

v = u + at,     s = (u + v)2tIN THE FORMULAE BOOKLET
s = ut + 12at2,     v2 = u2 + 2asIN THE FORMULAE BOOKLET

Each equation omits exactly one of the five letters. The working method is clerical and reliable: list s, u, v, a, t; fill in the three you know; pick the equation missing the one you do not care about.

WORKED EXAMPLE

A braking train

A train slows from 24 m s⁻¹ to 12 m s⁻¹ over 300 m. Find the deceleration.

Known: u = 24, v = 12, s = 300; wanted: a; time not involved, so use v² = u² + 2as.

144 = 576 + 600a, so a = −432/600 = −0.72 m s⁻²: a deceleration of 0.72.

The sign did the physics: negative because the train slows while moving in the positive direction.

Gravity: the standard constant

Height against time for a ball thrown up at 14.7 metres per second: peak of about 11 metres at 1.5 seconds, symmetric either side1.5 s11.0 mv = 0 at the top
FIG. 2Thrown at 14.7, back in your hand 3 seconds later: the flight is symmetric about its silent peak.

Free flight near the ground is constant acceleration g = 9.8 m s⁻² downwards, air resistance modelled away. Taking up as positive, a = −9.8 for the whole flight, on the way up, at the top, and on the way down. At the peak the velocity is zero; the acceleration never is.

A ball thrown up at 14.7 m s⁻¹ reaches v = 0 when t = 14.7/9.8 = 1.5 s, at height 14.7 × 1.5 − 4.9 × 1.5² = 11.0 m, and lands with speed 14.7 again: the flight is symmetric, and the symmetry is a free answer-checker.

THE EXAM BIT

  • Write the suvat list and fill it in before choosing an equation; the selection is then automatic.
  • suvat applies only while acceleration is constant: split the motion at the moment the acceleration changes.
  • In vertical motion, declare the positive direction and keep g's sign consistent with it.
  • Graph questions pay for areas and gradients, not for formulas: say which you are using.

CHECK YOURSELF

A stone is dropped from rest down a well and hits the water after 2 s. Taking g = 9.8 m s⁻², find the depth and the speed at impact.

Show a hint

u = 0 makes two suvat equations very short.

Show the answer

Depth: s = ½ × 9.8 × 2² = 19.6 m.

Impact speed: v = 9.8 × 2 = 19.6 m s⁻¹.

List s, u, v, a, t; pick the equation missing the letter you do not need.

Gravity is a constant −9.8 with up positive, all flight long, peak included.

WORKBOOK

Printable practice for this topic: original exam-style questions with room to work, and a fully worked answer book. Free to use; please do not redistribute or sell.

CHECK YOUR PROGRESS

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  • Read displacement and acceleration from velocity-time graphs.
  • Select and use the suvat equations for constant acceleration.
  • Model vertical motion under gravity, using the symmetry of up-and-down flight.

No animated video for this topic yet; these notes stand alone.