Things That Repeat
80 min · LivePut a number on a bounce: period, frequency and angular frequency, timed the examiner’s way.
Dayo’s okada carries Hajia Ramatu’s eggs over the same row of drainage ridges every morning. At a crawl the
trays survive; at a brisk pace they survive; but at one in-between speed the back of the bike pumps up and down
until the crates leap off the carrier and crack. Time a bounce, pull a spring, swing a pendulum, measure
g in your own lab, and work out the exact speed Dayo must never ride.
This phone cannot draw the 3D lab, but every reading still works. Use the controls below.
Add load or change the spring, then tap Pull & release.
Every lesson in this unit closes one piece of the same case file, from a bouncing okada outside Ogbomoso to a pendulum on Mrs Okafor’s lab bench.
Outside Ogbomoso, Hajia Ramatu packs trays of eggs into crates every dawn, and Dayo rides them to the town market on his okada. Halfway there, the laterite road crosses a run of low concrete drainage ridges laid by the council, all about the same distance apart.
Her daughter Zainab, an SS2 student, keeps a notebook of the losses, and the pattern is strange: slow trips are fine, fast trips are fine, but trips at one middle speed end in broken eggs. Her classmate Tunde is sure that faster always means worse. Their physics teacher, Mrs Okafor, says the bike is behaving like a mass on a spring, and that physics can name the dangerous speed before another tray is lost.
Why does one in-between speed throw the crates off, and what must Dayo and Mallam Sule change?
Realism note: story numbers are a teaching model: chosen to be realistic and easy to work with, not measured on a real okada or road. (Teachers: 200 kg on the rear spring, a 2 Hz bounce, ridges 2.5 m apart; real suspensions and roads vary.)
a = −ω²x · T = 2π√(l/g) · resonance f = f₀
Each lesson takes about 80 minutes with a movement break, opens with a Do Now warm-up, and walks you through a 3D story, a virtual practical, a zoom, worked examples and a WAEC-style quiz.
Put a number on a bounce: period, frequency and angular frequency, timed the examiner’s way.
Restoring force, the SHM condition and the loaded spring: why extra crates slow the bounce.
When exactly do the crates leave the carrier? Displacement, velocity and acceleration, and the lift-off rule.
Does a heavier bob or a bigger swing change the timing? Fair tests, small angles and T = 2π√(l/g).
The Paper 3 pendulum, end to end: split cork, composite table, the T²–l graph and the precautions.
Where does the bounce energy go? Kinetic and potential energy, and what a shock absorber is for.
Solve the Ridge Road case: Barton’s pendulums, f = v/d, and the verdict for Dayo and Hajia Ramatu.
Built-in spaced retrieval: every lesson’s Do Now pulls cards from earlier lessons, and
every lesson hands Zainab one more clue. By Lesson 7 you have the period, the spring constant, the lift-off
rule, the local g and the damping story needed to name the dangerous speed.
Tap a tab, then slide along the graph. You will meet every one of these again in a lesson, with your own readings.
The graph needs Paper.js; the readings below still update.
Lesson 3 bench: A = 0.30 m, T = 2.0 s (the mud lump’s shadow)
Slide through one cycle. Wherever the amber x curve crosses zero, the teal v curve is at a peak: the body is fastest in the middle. At the ends v is zero but the dashed a curve is at its biggest, pointing back to the centre.
Every skill is practised on a virtual bench, seen up close in a zoom and tested with WAEC, NECO and JAMB-style questions.
Classify periodic and oscillatory motion and find T, f and ω from timing data.
Use Hooke’s law and a = −ω²x: acceleration proportional to displacement, always towards the centre.
Apply x = A sin ωt, v = ω√(A² − x²) and a_max = ω²A, and say where each peaks.
Solve ratio problems with T = 2π√(m/k) and T = 2π√(l/g).
Carry out the Paper 3 pendulum, plot T² against l and deduce g = 4π²/slope.
Use E = ½kA², explain damping, and predict a resonant speed with v = d f₀.
Almost every number question on simple harmonic motion in WAEC, NECO and JAMB is one of these six. Each step has a note under it.
a = −ω²xSHM conditionω = 2πfAngular frequencyv = ω√(A² − x²)Speed at xT = 2π√(m/k)Loaded springT = 2π√(l/g)Simple pendulumE = ½kA²Total energyf = f₀ResonanceTap each card to flip it and see the physics:
After a short Do Now warm-up, every lesson follows the same five-step inquiry loop, with a movement break at 45 minutes, so you test an idea before you memorise it.
Zainab, Tunde, Dayo, Hajia Ramatu, Mallam Sule and Mrs Okafor meet a real puzzle. Post your guess on the Wonder Wall.
Time oscillations, load a spring, swing a pendulum, ride the ridges, and plot the readings live.
See restoring forces, a circle’s shadow, a cut-away shock absorber and a resonance curve, then write the rules.
Step-by-step calculations, a case-solving challenge and 12 exam-style questions every lesson.
Rate each goal 1–4, do the blank-page recall, then try the 30-mark paper before opening the model answers.
Start with Lesson 1: count the okada’s bounces and put a number on its rhythm.