Part of ME-02 — Kinematics

Feynman Note — Kinematics Simply Explained

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Analogy: The Car Journey

Imagine you're on a road trip. Kinematics is the GPS log — it records where you went and how fast, but doesn't care why (the engine, the road — that's dynamics/forces).

Displacement vs Distance: If you drive 10 km east then 10 km west, your distance is 20 km (total odometer reading) but your displacement is 0 km (you're back where you started). Distance never lies backwards; displacement can.

SUVAT equations: Think of a recipe with five ingredients: initial speed (u), final speed (v), acceleration (a), displacement (s), and time (t). Every recipe (equation) uses four of the five. If three are known, the recipe gives you the fourth. The "missing" ingredient tells you which recipe to pick.

Projectile motion: Imagine a bullet fired horizontally from a cliff while another is dropped straight down at the same instant. Both hit the ground at the same time — because they share identical vertical motion (s=12gt2s = \frac{1}{2}gt^2, independent of horizontal speed). The fired bullet just travels farther sideways. This is why a cannon aimed horizontally and one aimed at 0° hit the ground simultaneously.

Centripetal acceleration: A stone on a string spun in a circle moves at constant speed. But it's always accelerating — toward your hand. Speed says how fast; velocity says which way. The string continuously yanks the stone's direction without speeding it up. Remove the string and it flies off tangentially — proof that the acceleration was centripetal (toward centre) all along.

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