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Worked examples · Kinematics of Linear Motion

Kinematics of Linear Motion, Worked Examples (medium)

These medium Kinematics examples combine the core moves and ask you to read the motion: separating total distance from displacement when a particle reverses (split the interval at every v=0v=0), finding a minimum velocity by setting the acceleration a=0a=0, and integrating an acceleration twice while fixing each constant from a value given at t=1t=1. Try each on paper first, then check every line.

What these examples cover

These medium examples take the same three operations, differentiate, integrate, and solve v=0v=0, and ask you to combine them and read the motion carefully. You will separate total distance from displacement when the particle changes direction, find a minimum velocity using a=0a=0, and integrate an acceleration twice while fixing each constant from a value given at t=1t=1 rather than t=0t=0.

The arithmetic stays clean, but the thinking is a step up: you must decide where the velocity changes sign, and check whether a stationary value of velocity is a maximum or a minimum. Attempt each fully on paper first, then compare every line with the solution and pinpoint any step where your reasoning differed.

Worked examples

Work through all three. Each rewards a clear plan, find where the velocity is zero, decide the direction on each interval, and only then compute, so build that habit as you go.

Q1[5 marks]

A particle moves along a straight line and passes a fixed point OO at t=0t=0. Its velocity is v=3t212t+9v=3t^{2}-12t+9, in m s1\text{m s}^{-1}, at time tt s.

Find the total distance travelled in the first 33 seconds.

Show worked solution

Total distance differs from displacement whenever the particle changes direction, so first find where the velocity is zero.

3t212t+9=03t^{2}-12t+9=0

Divide by 33 and factorise.

t24t+3=0  (t1)(t3)=0t^{2}-4t+3=0\ \Rightarrow\ (t-1)(t-3)=0

So v=0v=0 at t=1t=1 and t=3t=3. Testing a value in each interval, v>0v>0 on 0t<10\le t<1 and v<0v<0 on 1<t<31<t<3, so the particle reverses direction at t=1t=1.

Find the displacement function by integrating, taking s=0s=0 at t=0t=0.

s=(3t212t+9)dt=t36t2+9ts=\int (3t^{2}-12t+9)\,dt=t^{3}-6t^{2}+9t

Evaluate the displacement at t=0t=0, t=1t=1 and t=3t=3.

s(0)=0,s(1)=16+9=4,s(3)=2754+27=0s(0)=0,\quad s(1)=1-6+9=4,\quad s(3)=27-54+27=0

The particle moves from 00 to 44 m in the first second, then back from 44 m to 00. Add the distance of each leg.

Total distance=40+04=4+4=8\text{Total distance}=|4-0|+|0-4|=4+4=8

Answer

The total distance travelled in the first 33 seconds is 88 m, even though the displacement over that interval is 00, the particle returns to OO.

Q2[5 marks]

A particle moves along a straight line. Its displacement from a fixed point OO is s=t39t2+24ts=t^{3}-9t^{2}+24t, in metres, at time tt s.

Find (a) the times when the particle is momentarily at rest, and (b) the minimum velocity of the particle.

Show worked solution

Differentiate the displacement to get the velocity.

v=dsdt=3t218t+24v=\frac{ds}{dt}=3t^{2}-18t+24

(a) The particle is at rest when v=0v=0. Divide by 33 and factorise.

t26t+8=0  (t2)(t4)=0t^{2}-6t+8=0\ \Rightarrow\ (t-2)(t-4)=0

So the particle is momentarily at rest at t=2t=2 s and t=4t=4 s.

(b) The velocity is least where its rate of change is zero, so set the acceleration to zero.

a=dvdt=6t18=0  t=3a=\frac{dv}{dt}=6t-18=0\ \Rightarrow\ t=3

Since a<0a<0 before t=3t=3 and a>0a>0 after it, the velocity has a minimum there. Substitute t=3t=3 into vv.

vt=3=3(3)218(3)+24=2754+24=3v|_{t=3}=3(3)^{2}-18(3)+24=27-54+24=-3

Answer

The particle is at rest at t=2t=2 s and t=4t=4 s, and its minimum velocity is 3 m s1-3\ \text{m s}^{-1}, moving in the negative direction at 3 m s13\ \text{m s}^{-1}.

Q3[6 marks]

A particle moves along a straight line with acceleration a=6t2a=6t-2, in m s2\text{m s}^{-2}, at time tt s. When t=1t=1 its velocity is 3 m s13\ \text{m s}^{-1} and its displacement from OO is 55 m.

Find (a) the initial velocity of the particle, and (b) its displacement from OO when t=2t=2.

Show worked solution

Integrate the acceleration to get the velocity, keeping a constant c1c_{1}.

v=(6t2)dt=3t22t+c1v=\int (6t-2)\,dt=3t^{2}-2t+c_{1}

Use v=3v=3 when t=1t=1.

3=3(1)22(1)+c1=1+c1  c1=23=3(1)^{2}-2(1)+c_{1}=1+c_{1}\ \Rightarrow\ c_{1}=2

So v=3t22t+2v=3t^{2}-2t+2. The initial velocity is its value at t=0t=0.

vt=0=3(0)22(0)+2=2v|_{t=0}=3(0)^{2}-2(0)+2=2

(b) Integrate the velocity to get the displacement, keeping a constant c2c_{2}.

s=(3t22t+2)dt=t3t2+2t+c2s=\int (3t^{2}-2t+2)\,dt=t^{3}-t^{2}+2t+c_{2}

Use s=5s=5 when t=1t=1.

5=11+2+c2=2+c2  c2=35=1-1+2+c_{2}=2+c_{2}\ \Rightarrow\ c_{2}=3

So s=t3t2+2t+3s=t^{3}-t^{2}+2t+3. Substitute t=2t=2.

st=2=(2)3(2)2+2(2)+3=84+4+3=11s|_{t=2}=(2)^{3}-(2)^{2}+2(2)+3=8-4+4+3=11

Answer

The initial velocity is 2 m s12\ \text{m s}^{-1}, and the displacement from OO when t=2t=2 is 1111 m.

Q4[3 marks]

A particle passes through a fixed point OO at time t=0t=0 with velocity v=84tv=8-4t, in m s1\text{m s}^{-1}, at time tt s. Find the maximum displacement of the particle from OO.

Show worked solution

The particle is furthest from OO at the instant it turns back, so first find where the velocity is zero.

84t=0  t=28-4t=0\ \Rightarrow\ t=2

Integrate the velocity to get the displacement function, taking s=0s=0 at t=0t=0.

s=(84t)dt=8t2t2s=\int (8-4t)\,dt=8t-2t^{2}

Since v>0v>0 for 0t<20\le t<2 and v<0v<0 for t>2t>2, the particle moves away from OO then returns, so t=2t=2 gives the furthest point. Substitute t=2t=2.

st=2=8(2)2(2)2=168=8s|_{t=2}=8(2)-2(2)^{2}=16-8=8

Answer

The maximum displacement of the particle from OO is 88 m, reached at t=2t=2 s; after this the particle turns back towards OO.

Q5[4 marks]

A particle passes through a fixed point OO at time t=0t=0. Its displacement from OO is s=t36t2+8ts=t^{3}-6t^{2}+8t, in metres, at time tt s.

Find (a) the other two times, t>0t>0, at which the particle passes through OO, and (b) the direction of motion of the particle at the later of these two times.

Show worked solution

The particle passes through OO whenever s=0s=0, so factorise the displacement.

s=t(t26t+8)=t(t2)(t4)s=t(t^{2}-6t+8)=t(t-2)(t-4)

So s=0s=0 when t=0t=0, t=2t=2 or t=4t=4. The particle passes through OO again at t=2t=2 s and t=4t=4 s.

(b) Differentiate to get the velocity, then evaluate it at the later time, t=4t=4.

v=dsdt=3t212t+8v=\frac{ds}{dt}=3t^{2}-12t+8
vt=4=3(4)212(4)+8=4848+8=8v|_{t=4}=3(4)^{2}-12(4)+8=48-48+8=8

Answer

The particle passes through OO again at t=2t=2 s and t=4t=4 s. At t=4t=4 s its velocity is 8 m s18\ \text{m s}^{-1}, which is positive, so it is moving in the positive direction.

Q6[4 marks]

A particle passes through a fixed point OO at time t=0t=0 and moves with velocity v=2t6v=2t-6, in m s1\text{m s}^{-1}, at time tt s. Find the total distance travelled by the particle between t=1t=1 s and t=4t=4 s.

Show worked solution

First find the displacement function by integrating the velocity, taking s=0s=0 at t=0t=0.

s=(2t6)dt=t26ts=\int (2t-6)\,dt=t^{2}-6t

Check whether the particle changes direction inside [1,4][1,4] by solving v=0v=0.

2t6=0  t=32t-6=0\ \Rightarrow\ t=3

Since t=3t=3 lies inside the interval, split it there and evaluate ss at t=1t=1, t=3t=3 and t=4t=4.

s(1)=16=5,s(3)=918=9,s(4)=1624=8s(1)=1-6=-5,\quad s(3)=9-18=-9,\quad s(4)=16-24=-8
Total distance=9(5)+8(9)=4+1=5\text{Total distance}=|{-9}-({-5})|+|{-8}-({-9})|=4+1=5

Answer

The total distance travelled between t=1t=1 s and t=4t=4 s is 55 m, the particle keeps moving in the negative direction until t=3t=3 s, then reverses.

Q7[4 marks]

A particle moves along a straight line with velocity v=t22t3v=t^{2}-2t-3, in m s1\text{m s}^{-1}, at time tt s, t0t\ge 0. Find the value of tt at which the speed of the particle is 5 m s15\ \text{m s}^{-1}.

Show worked solution

Speed is the magnitude of velocity, so the speed is 55 when v=5v=5 or v=5v=-5. Try v=5v=5 first.

t22t3=5  t22t8=0  (t4)(t+2)=0t^{2}-2t-3=5\ \Rightarrow\ t^{2}-2t-8=0\ \Rightarrow\ (t-4)(t+2)=0

This gives t=4t=4 or t=2t=-2; reject t=2t=-2 since t0t\ge 0. Now try v=5v=-5.

t22t3=5  t22t+2=0t^{2}-2t-3=-5\ \Rightarrow\ t^{2}-2t+2=0

The discriminant of this equation is (2)24(1)(2)=4(-2)^{2}-4(1)(2)=-4, which is negative, so there is no real value of tt for this case.

Answer

The speed of the particle is 5 m s15\ \text{m s}^{-1} only at t=4t=4 s; the case v=5v=-5 has no real solution.

Q8[3 marks]

A particle moves along a straight line such that its displacement from a fixed point OO is s=t34t2+2s=t^{3}-4t^{2}+2, in metres, at time tt s. Determine whether the particle is moving with increasing or decreasing speed at t=1t=1 s.

Show worked solution

The particle speeds up when its velocity and acceleration have the same sign, and slows down when they have opposite signs. Differentiate to get the velocity.

v=dsdt=3t28tv=\frac{ds}{dt}=3t^{2}-8t

Differentiate again to get the acceleration, then evaluate both at t=1t=1.

a=dvdt=6t8a=\frac{dv}{dt}=6t-8
vt=1=3(1)28(1)=5,at=1=6(1)8=2v|_{t=1}=3(1)^{2}-8(1)=-5,\qquad a|_{t=1}=6(1)-8=-2

Answer

At t=1t=1 s, v=5 m s1v=-5\ \text{m s}^{-1} and a=2 m s2a=-2\ \text{m s}^{-2}; since both are negative, the particle is moving with increasing speed.

Key method points

These three examples show how the basic moves combine once you have to interpret the motion, not just compute it. Keep these points to hand.

  • Total distance adds the length of each leg of the motion; split the interval at every time where v=0v=0 and sum the absolute changes in displacement.
  • Displacement over an interval can be zero while the total distance is not, the particle may return to where it started.
  • A velocity is greatest or least where its rate of change is zero, i.e. where a=dvdt=0a=\frac{dv}{dt}=0; check the sign of aa on either side to tell a maximum from a minimum.
  • When you integrate twice, you get two separate constants, fix each one from its own given condition before substituting.
  • An initial condition need not be given at t=0t=0; use whatever time is stated to find the constant, then read the value you actually want.

How a teacher helps

Medium Kinematics questions reward a clear plan, and that is exactly what a good lesson builds. The usual lost mark is treating displacement as distance, or stopping at a=0a=0 without checking whether the velocity is a maximum or a minimum.

Our teacher makes the reversal points visible, a quick sign line for vv, so the method becomes automatic. Because our teachers are experienced, you learn the reasoning, not a recipe.

Lessons are taught in English, while SPM papers are set in both Malay and English, so the notation stays familiar.

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Frequently asked questions

What is the difference between distance and displacement here?

Displacement is the change in position from start to finish and can be negative or zero. Total distance adds up how far the particle actually travels on each leg, so you split the time interval wherever v=0v=0 and sum the absolute changes.

How do I know a stationary velocity is a minimum, not a maximum?

Look at the acceleration a=dvdta=\frac{dv}{dt} on either side of the point. If aa changes from negative to positive, the velocity has a minimum; from positive to negative, a maximum.

Why are there two constants when I integrate twice?

Each integration introduces its own constant. Integrating acceleration gives a velocity constant; integrating that velocity gives a displacement constant.

Find each from its own stated condition before you evaluate anything.

The initial value is given at t=1t=1, not t=0t=0. Does that matter?

Not for the method, substitute t=1t=1 with the given value to find the constant. Only after the function is complete do you put in t=0t=0 to read the initial velocity or displacement.

Source:SRC-DSKP-EN

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

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