← Mechanical Systems
4b Vertical circular motion and apparent weight
A recurring context every year: a loop, a roundabout, or an orbit, where gravity does not always point the same way relative to the centripetal direction — this changes which forces combine to supply F_c at different points.At the top vs the bottom of a vertical loop
- At the TOP: gravity and the normal force both point toward the centre (downward), so N + mg = mv²/r.
- At the BOTTOM: gravity points away from the centre (down) while the normal force points toward it (up), so N − mg = mv²/r.
- MINIMUM speed at the top is when N = 0 and gravity alone supplies the centripetal force: mg = mv²/r, giving v_min = √(gr).
- Below v_min, the object cannot maintain contact with the track at the top — it falls away from the circular path.
Over a bump and through a dip
- On TOP of a bump the centre is below the object: gravity points towards it and the reaction force away, so mg − N = mv²/r. The faster it goes, the smaller N gets.
- It leaves the surface when N = 0, so the MAXIMUM speed over the top is v = √(gr). (At the top of a loop the same √(gr) is a minimum: there N points towards the centre.)
- At the bottom of a dip the centre is above: N − mg = mv²/r, so N is bigger than the weight, as at the bottom of a loop.