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Chapter · Kinematics

Kinematics: the maths of motion

Kinematics in Add Math treats displacement, velocity and acceleration as three functions of time linked by differentiation and integration: velocity is the rate of change of displacement, v=dsdtv=\frac{ds}{dt}, and acceleration is the rate of change of velocity, a=dvdta=\frac{dv}{dt}. Moving the other way, integrating acceleration gives velocity, and integrating velocity gives displacement.

Three quantities, linked by one operation

Kinematics in Add Math is really an application chapter, nearly everything in it reuses differentiation and integration from earlier chapters, applied to a particle moving along a straight line. The whole topic rests on one relationship: displacement, velocity, and acceleration are three functions of time, and each one is found from the one before it by differentiating, or the one after it by integrating.

v=dsdt,a=dvdtv = \frac{ds}{dt}, \qquad a = \frac{dv}{dt}

Read left to right, differentiating displacement ss with respect to time gives velocity vv; differentiating velocity gives acceleration aa. Read the other way, integrating acceleration gives velocity (plus a constant, found from given conditions), and integrating velocity gives displacement (plus another constant).

Once this chain is comfortable, most kinematics questions become a matter of deciding which direction along the chain the question requires, rather than learning a new technique for each one.

  • Displacement ss: position relative to a fixed starting point, measured with direction, it can be negative.
  • Velocity vv: rate of change of displacement, also signed, since direction still matters.
  • Acceleration aa: rate of change of velocity, positive acceleration does not always mean speeding up, if velocity is negative.

Why the signs matter more than the size

The single idea that separates confident kinematics answers from shaky ones is treating displacement, velocity, and acceleration as signed quantities along a line, not as plain sizes. A particle can have negative velocity while moving in the direction defined as negative, and a negative acceleration can mean speeding up if the velocity is also negative, the object is moving faster in the negative direction, not slowing down.

Three moments worth naming precisely

The particle is momentarily at rest when v=0v=0. The particle is instantaneously not accelerating when a=0a=0, which for many functions is also where velocity is at a maximum or minimum.

The particle returns to its starting point when s=0s=0 again after starting at s=0s=0, these are three different conditions, and a question usually asks about only one of them.

A common early confusion is assuming "the particle stops" and "the particle changes direction" are the same statement. They usually coincide, but not always, checking the sign of velocity just before and just after v=0v=0 is the reliable way to tell whether the particle actually reverses or merely slows to zero and continues the same way, which happens, for example, at a point of inflexion in velocity.

Total distance is not the same as displacement

This distinction accounts for a large share of the marks lost in kinematics, and it is worth treating as its own skill rather than an afterthought. Displacement over an interval is simply the difference between the final and initial position, direction and any doubling-back cancel out.

Total distance travelled adds up every bit of movement, regardless of direction, so any time the particle reverses direction within the interval, distance and displacement give different numbers.

The reliable method is to find every value of tt within the interval where v=0v=0, since those are the only points where a reversal can happen. Splitting the interval at each of those points, working out the displacement over each smaller piece separately, and adding the absolute value of each piece gives total distance, while simply adding the pieces without the absolute value, letting negative displacements cancel positive ones, gives net displacement.

Do not skip the split

Integrating velocity over the whole interval in one step, without checking for a sign change first, only ever gives displacement, never total distance, whenever a direction reversal happens partway through.

A worked example, start to finish

A particle moves in a straight line so that its velocity, in m s1\text{m s}^{-1}, at time tt seconds is given by v=3t212t+9v=3t^{2}-12t+9, for t0t\geq0, starting from s=0s=0 when t=0t=0.

  1. Find when the particle is momentarily at rest, by setting v=0v=0: 3t212t+9=03t^{2}-12t+9=0, which factorises to 3(t1)(t3)=03(t-1)(t-3)=0, giving t=1t=1 and t=3t=3.
  2. Find acceleration by differentiating velocity: a=dvdt=6t12a=\frac{dv}{dt}=6t-12.
  3. Find displacement by integrating velocity: s=t36t2+9t+cs=t^{3}-6t^{2}+9t+c; since s=0s=0 when t=0t=0, c=0c=0, giving s=t36t2+9ts=t^{3}-6t^{2}+9t.
s=t36t2+9ts = t^{3} - 6t^{2} + 9t

At t=1t=1, s=16+9=4s=1-6+9=4; at t=3t=3, s=2754+27=0s=27-54+27=0. Between t=0t=0 and t=1t=1 the particle moves 4 m in the positive direction; between t=1t=1 and t=3t=3 it reverses and returns 4 m back to s=0s=0.

The net displacement over the first 3 seconds is 00 m, but the total distance travelled is 4+4=84+4=8 m, a direct illustration of why the two are not interchangeable.

Q1[6 marks]

A particle moves in a straight line with acceleration a=6t6 m s2a=6t-6\ \text{m s}^{-2}, starting with velocity v=3 m s1v=-3\ \text{m s}^{-1} when t=0t=0. Find the velocity when t=2t=2, and state whether the particle is speeding up or slowing down at that instant.

Show worked solution

Integrate acceleration: v=3t26t+cv=3t^{2}-6t+c. Since v=3v=-3 when t=0t=0, c=3c=-3, giving v=3t26t3v=3t^{2}-6t-3.

At t=2t=2: v=3(4)123=3 m s1v=3(4)-12-3=-3\ \text{m s}^{-1}. At t=2t=2, acceleration is a=6(2)6=6 m s2a=6(2)-6=6\ \text{m s}^{-2}, which is positive, while velocity is negative, since acceleration and velocity have opposite signs, the particle is slowing down at that instant.

Where marks usually slip

Kinematics leans heavily on calculus skills learned earlier, so slips here are often carried over from those chapters rather than new to this one.

  • Forgetting the constant of integration when moving from acceleration to velocity, or velocity to displacement, kinematics questions almost always give a starting condition specifically to fix that constant.
  • Reading a negative velocity as "the particle has stopped" rather than "the particle is moving in the negative direction."
  • Calculating displacement over an interval and reporting it as total distance, without checking for a direction reversal first.
  • Assuming maximum velocity happens where acceleration is zero without confirming it is a maximum rather than a minimum.

Kinematics questions can appear in Paper 2 (2 hours 30 minutes, 100 marks), and marking is analytic. Writing the constant of integration explicitly, and stating clearly which quantity, displacement, velocity, or distance, each line of working refers to, protects marks even when a later step goes wrong.

How one-to-one teaching can help

Kinematics sits at the intersection of several earlier chapters, differentiation, integration, and quadratic equations all show up inside a single question, so a shaky patch in any one of them can surface here even when the kinematics idea itself is understood. A teacher working with you one-to-one can trace a wrong answer back to which underlying skill actually needs attention, rather than re-teaching the whole chapter from scratch.

Our teachers are experienced; lessons run online and are taught in English, while SPM papers themselves are set bilingually in Bahasa Melayu and English.

If kinematics, or the calculus chapters it draws on, is a sticking point, a one-hour paid trial class at the teacher's own rate (from RM50 per hour, depending on experience) is a reasonable place to start.

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Frequently asked questions

What is the difference between velocity and speed in kinematics?

Velocity is signed and includes direction, it can be negative. Speed is the size of velocity only, always given as a positive value, found by taking the absolute value of velocity at that instant.

How do I find total distance travelled, not just displacement?

Find every value of tt in the interval where v=0v=0, since those are the only points where the particle can reverse direction. Split the interval at each one, find the displacement over each piece, and add the absolute value of each piece together.

Does a = 0 always mean the particle has stopped?

No. a=0a=0 means velocity is momentarily not changing, which often (though not always) corresponds to a maximum or minimum velocity, it says nothing directly about whether the particle itself is at rest, which is instead found from v=0v=0.

Why do kinematics questions give a starting velocity or displacement?

Integrating acceleration or velocity introduces a constant of integration that calculus alone cannot determine. A given starting condition, such as the value of ss or vv at t=0t=0, is what fixes that constant to a specific number.

Source:SRC-FORMAT

Written by the spmaddmath.com.my editorial team.· Last updated 5 September 2026

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