Worked examples · Kinematics of Linear Motion
Kinematics of Linear Motion, Worked Examples (KBAT)
These hard Kinematics examples chain the whole method together and ask you to interpret the motion: building velocity from an acceleration and an initial value before adding the legs for a total distance, comparing two particles that leave the same point to find when they meet again by setting , and integrating twice to locate a maximum velocity (where ) and the displacement at that instant. Try each on paper first, then check every line.
What these examples cover
These hard examples ask you to run the whole machinery at once and interpret the motion, not just compute it. You will build a velocity from an acceleration and an initial value, decide where it changes sign, and add the legs to get a total distance; compare two particles that leave the same point and find when they meet again; and integrate an acceleration twice to locate a maximum velocity and the displacement at that instant.
Nothing here needs heavy arithmetic, the numbers stay small, but each part depends on the one before it, so a single sign slip carries through. Attempt each in full, then check line by line, paying close attention to direction and to the meaning of every value you find.
Worked examples
Work through all three. Each is several small steps in a chain, so keep the steps in order, fix the constant, analyse the sign of the velocity, then compute, and the marks follow.
A particle moves along a straight line and passes a fixed point with velocity at . Its acceleration is , in , at time s.
Find the total distance travelled in the first seconds.
Show worked solution
First build the velocity by integrating the acceleration, using the initial velocity to fix the constant.
Since when , we get , so . Find where the particle is at rest.
So at and . Checking signs, on and on ; the particle reverses at .
Integrate again for the displacement, with at .
Evaluate the displacement at the key times and .
Add the distance of each leg as the absolute change in displacement.
Answer
The total distance travelled in the first seconds is m. The particle first moves forward m, then back m.
Two particles and leave a fixed point at the same instant and move along the same straight line. At time s, has velocity , in , and moves with constant velocity .
Find (a) the time after when and meet again, and their distance from then, and (b) the total distance has travelled up to that instant.
Show worked solution
Find the displacement of each particle from by integrating, using at for both.
(a) They meet where their displacements are equal.
Factorise, taking out .
The relevant root is , rejecting (the start) and . Their common displacement is:
(b) To get ’s total distance, find where is at rest, since changes sign.
on and on , so reverses at . Evaluate .
Add the two legs.
Answer
and meet again at s, m from . By then has travelled m in total, having first gone m in the negative direction before turning back.
A particle moves along a straight line and passes a fixed point with velocity at . Its acceleration is , in , at time s.
Find (a) the maximum velocity of the particle, and (b) its displacement from at the instant the velocity is maximum.
Show worked solution
Integrate the acceleration for the velocity, fixing the constant from at .
So . The velocity is greatest where its rate of change, the acceleration, is zero.
Because before and after it, this is a maximum. Substitute into .
(b) Integrate the velocity for the displacement, with at .
Substitute .
Answer
The maximum velocity is , reached at s, and the displacement from at that instant is m.
A particle moves along a straight line such that its displacement from a fixed point is given by , in m, at time s, where . Find (a) the two instants at which the particle is instantaneously at rest, and (b) the maximum displacement of the particle from .
Show worked solution
Differentiate the displacement to get the velocity, since the particle is given here as a function of rather than of .
(a) The particle is instantaneously at rest where .
So the particle is at rest at and . (b) To decide which instant gives the maximum displacement, differentiate again to get the acceleration and check its sign at each instant.
A negative acceleration at means is at a maximum there (turning from increasing to decreasing); a positive acceleration at means is at a minimum. Evaluate at .
Answer
The particle is instantaneously at rest at s and s. Its maximum displacement from is m, reached at s (checking : , which is only a local minimum, matching there).
A particle moves along a straight line and passes through a fixed point with velocity at . Its acceleration is , in , at time s.
Find (a) the total distance travelled by the particle in the first seconds, and (b) its average velocity over this time. Explain why your two answers are different.
Show worked solution
Integrate the acceleration to get the velocity, using the given initial velocity to fix the constant.
So . The particle is at rest at and , both inside the first seconds, so it reverses direction twice.
Integrate again for the displacement, with at .
Evaluate the displacement at the start, at each rest instant, and at the end of the interval.
(a) Add the distance of each leg.
(b) The average velocity uses only the net displacement over the time taken, not the distance covered.
Answer
The particle covers a total distance of m, but its average velocity is only , because it doubles back on itself: after s it has ended up only m from , even though it walked m of straight line to get there.
Particle passes through a fixed point with zero velocity at time and has acceleration , in , at time s. At the same instant, particle is m from on the same straight line and travels directly towards at a constant speed of .
Find (a) the time at which and meet, and their distance from then, and (b) the velocity of each particle at that instant, stating whether they are then moving in the same or in opposite directions.
Show worked solution
Find 's velocity and displacement from by integrating twice, using and at .
Since starts m from and moves towards at a constant , its displacement from decreases steadily.
(a) and meet where their displacements from are equal.
Test small integer values: gives , so is a root. Factorise it out.
The quadratic factor has discriminant , so it has no real roots; is the only solution.
(b) Find each particle's velocity at .
Answer
and meet at s, m from . At that instant moves at away from while still moves at towards , opposite directions, so is overtaking at the meeting point rather than the two coming to rest together.
A particle travels along a straight line such that its velocity is given by , in , at time s, for . Find (a) the values of at which the particle is instantaneously at rest, (b) the minimum velocity of the particle in this interval, and (c) the minimum speed of the particle in this interval.
Show worked solution
(a) The particle is at rest where .
(b) The minimum velocity occurs where the acceleration is zero, since is an upward-opening quadratic in .
So the minimum velocity is at . (c) Speed is , not itself, so check its value at the rest instants found in (a) as well.
Answer
The particle is at rest at s and s. Its minimum velocity is , at s, but its minimum speed is , reached at s and s, since the particle is momentarily stationary there.
The most negative velocity is not the slowest the particle ever moves.
A particle moves along a straight line and passes through a fixed point with velocity at time . Its acceleration is , in , at time s, where is a constant.
Given that the particle is instantaneously at rest when s, find (a) the value of and the other instant at which the particle is at rest, and (b) the range of values of during which the particle is moving in the negative direction.
Show worked solution
Integrate the acceleration to get the velocity, using the given initial velocity to fix the constant of integration.
(a) Use the fact that at to find .
So . Factorise to find the other instant at which the particle is at rest.
(b) Since the coefficient of is positive, is negative between its two roots. Test a value in between, say , to confirm.
Outside the factors and have the same sign, so there, matching the given .
Answer
, and the particle is also at rest at s. It moves in the negative direction for , having set off in the positive direction, reversed at s, and turned forward again at s.
Key method points
These three examples show what a full-mark solution to a hard Kinematics question looks like, an ordered chain of small, correct steps. Keep these to hand.
- Build the motion in order: integrate acceleration for velocity, then velocity for displacement, fixing each constant from a given value before using the function.
- For a total distance, always locate the times where , test the sign of in each interval, and add the absolute change in displacement over each leg.
- Two bodies meet when their displacements from the same origin are equal; set and solve, then reject times that are not physically relevant.
- A maximum or minimum velocity occurs where ; confirm which by checking the sign of on either side.
- Keep exact fractions through the working and simplify only at the end, the messy-looking values often combine to a clean total, such as .
How a teacher helps
Hard Kinematics questions are really several small steps chained together, and the marks are won by keeping the chain in order. The common slip is a lost sign or a rejected root kept by mistake, which then travels through the rest of the answer.
In a lesson our teacher slows the first two lines right down, the constant of integration and the sign analysis, because getting those right makes everything after them follow. Our teachers are experienced, so you learn to plan a multi-step solution with confidence.
Lessons are taught in English, while SPM papers are set in both Malay and English.
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Book a Trial ClassFrequently asked questions
How do I find when two particles meet?
Write each displacement from the same starting point as a function of , set them equal, and solve. Discard any root that is not physically relevant, such as the starting instant or a negative time.
Do I add distances or displacements for total distance?
Distances. Find every time where , work out the displacement at those times and at the endpoints, and add the absolute change over each leg.
Adding displacements directly would let a backward leg cancel a forward one.
How do I know the velocity is at a maximum?
Set the acceleration to find the candidate time, then check the sign of on either side. Positive changing to negative is a maximum; negative to positive is a minimum.
The working has fractions like . Have I gone wrong?
Not necessarily, kinematics answers are often exact fractions. Keep them exact through the calculation; here the two legs and add to a clean m.
Source:SRC-DSKP-EN