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How do you describe motion in a straight line using the constant-acceleration equations, motion graphs and calculus?

Displacement, velocity and acceleration, the constant-acceleration (suvat) equations, motion under gravity, displacement-time and velocity-time graphs, and using calculus when acceleration varies.

A focused answer to the OCR A-Level Mathematics A kinematics content, covering displacement, velocity and acceleration, the constant-acceleration suvat equations, motion under gravity, interpreting displacement-time and velocity-time graphs, and using differentiation and integration when acceleration varies with time.

Generated by Claude Opus 4.812 min answer

Reviewed by: AI editorial process; not yet individually human-reviewed

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  1. What this dot point is asking
  2. The answer
  3. Examples in context
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What this dot point is asking

OCR wants you to define displacement, velocity and acceleration, use the constant-acceleration (suvat) equations including for vertical motion under gravity, interpret displacement-time and velocity-time graphs (gradients and areas), and use calculus (differentiation and integration) to handle motion where the acceleration is not constant.

The answer

Displacement, velocity and acceleration

Displacement is position relative to a fixed point (a vector). Velocity is the rate of change of displacement, and acceleration is the rate of change of velocity. In a straight line we treat them as signed quantities, with one direction chosen as positive.

The suvat equations

When acceleration is constant, the five quantities ss (displacement), uu (initial velocity), vv (final velocity), aa (acceleration) and tt (time) are linked by the standard equations.

Motion under gravity

A body moving freely under gravity has constant acceleration g=9.8g = 9.8 m s−2^{-2} downwards. Choose a positive direction and keep signs consistent: if up is positive then a=−9.8a = -9.8, and at the highest point v=0v = 0.

Motion graphs

On a displacement-time graph the gradient is velocity. On a velocity-time graph the gradient is acceleration and the area under the graph is the displacement. Reading gradients and areas turns a graph into the motion.

Examples in context

Choosing the right suvat equation

The skill is matching the equation to the four quantities involved. List s,u,v,a,ts, u, v, a, t, mark what you know and what you want, and pick the equation missing the one variable you neither know nor need.

Variable acceleration and calculus

When acceleration varies with time the suvat equations do not apply; instead, differentiate to go from displacement to velocity to acceleration, and integrate to go back. To find total distance (not displacement) when the direction changes, split the motion at the times when v=0v = 0 and add the magnitudes.

Try this

Q1. A car travels from rest at a=2a = 2 m s−2^{-2} for 55 s. Find its final speed and the distance covered. [3 marks]

  • Cue. v=0+2(5)=10v = 0 + 2(5) = 10 m s−1^{-1}; s=12(2)(52)=25s = \tfrac{1}{2}(2)(5^2) = 25 m.

Q2. A particle has displacement s=2t3−9t2s = 2t^3 - 9t^2. Find its acceleration at t=2t = 2. [3 marks]

  • Cue. v=6t2−18tv = 6t^2 - 18t, a=12t−18a = 12t - 18, so at t=2t = 2, a=6a = 6 m s−2^{-2}.

Exam-style practice questions

Practice questions written in the style of OCR exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

OCR 20196 marksA ball is projected vertically upwards from ground level with speed 2121 m s−1^{-1}. Taking g=9.8g = 9.8 m s−2^{-2} and ignoring air resistance, find the greatest height reached and the total time before it returns to the ground.
Show worked answer →

Take upwards as positive, so a=−9.8a = -9.8, u=21u = 21. At the greatest height v=0v = 0 (M1).

Use v2=u2+2asv^2 = u^2 + 2as: 0=212+2(−9.8)s0 = 21^2 + 2(-9.8)s, so 19.6s=44119.6s = 441 and s=22.5s = 22.5 m (M1, A1).

For the total time, the ball returns to s=0s = 0. Use s=ut+12at2s = ut + \tfrac{1}{2}at^2 with s=0s = 0 (M1): 0=21t−4.9t2=t(21−4.9t)0 = 21t - 4.9t^2 = t(21 - 4.9t).

So t=0t = 0 (start) or t=214.9≈4.29t = \dfrac{21}{4.9} \approx 4.29 s (A1, A1).

Markers reward v=0v = 0 at the top, the correct suvat equation for the height, setting s=0s = 0 for the return, and the total time.

OCR 20216 marksA particle moves in a straight line so that its velocity at time tt seconds is v=3t2−12t+9v = 3t^2 - 12t + 9 m s−1^{-1}. Find the times when the particle is instantaneously at rest, and the total distance travelled in the first 44 seconds.
Show worked answer →

At rest when v=0v = 0 (M1): 3t2−12t+9=3(t2−4t+3)=3(t−1)(t−3)=03t^2 - 12t + 9 = 3(t^2 - 4t + 3) = 3(t - 1)(t - 3) = 0, so t=1t = 1 and t=3t = 3 (A1).

Displacement is ∫v dt=t3−6t2+9t\int v\,dt = t^3 - 6t^2 + 9t (M1). The velocity changes sign at t=1t = 1 and t=3t = 3, so compute each leg separately.

From 00 to 11: s(1)−s(0)=(1−6+9)−0=4s(1) - s(0) = (1 - 6 + 9) - 0 = 4 m. From 11 to 33: s(3)−s(1)=(27−54+27)−4=−4s(3) - s(1) = (27 - 54 + 27) - 4 = -4 m (so 44 m back). From 33 to 44: s(4)−s(3)=(64−96+36)−0=4s(4) - s(3) = (64 - 96 + 36) - 0 = 4 m (A1).

Total distance =4+4+4=12= 4 + 4 + 4 = 12 m (M1, A1).

Markers reward solving v=0v = 0, integrating for displacement, splitting at the direction changes, and summing the distances.

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