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A jet must reach 80 m/s to lift off and the runway is only 1500 m long. You know the engine's acceleration and the takeoff speed — but nobody handed you the time. Can you still prove the plane gets airborne in time?
A jet must reach 80 m/s to lift off and the runway is only 1500 m long. You know the engine's acceleration and the takeoff speed — but nobody handed you the time. Can you still prove the plane gets airborne in time?
When acceleration is constant, four equations link u, v, a, s and t — and each one skips a different quantity. Pick the equation missing the variable you don't have, and any constant-acceleration problem cracks open.
When acceleration is constant, five quantities describe the motion: initial velocity u, final velocity v, acceleration a, displacement s, and time t. Four 'SUVAT' equations connect them, and each equation leaves out exactly one quantity. To solve any problem, list what you know, spot the one variable you neither have nor want, and choose the equation that omits it.
The trick is matching equation to unknowns. No time given? Use + 2as. Don't know the final velocity yet? Use s = ut + ½at². The equation is just average velocity ½(u+v) multiplied by time — handy when a isn't given. Watch signs: pick a positive direction and keep u, v, a and s consistent with it; a deceleration is simply a negative a. For vertical motion under gravity, (the topic of the next lesson, Free Fall). **Limiting case:** set and all three equations collapse to ; set and they simplify to , — sanity-check every answer against these. **Connect it:** all three live inside the v–t graph: is the straight line itself, is the area under it, and is what remains when you eliminate between them. One picture, three equations.
Grabbing a SUVAT equation at random — first list which of u, v, a, s, t you know and want, then pick the equation that omits the variable you don't have.