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Physics Circle Motn
Physics Autumn Y13
| Question | Answer |
|---|---|
| Angular velocity measured in | Radians per second Symbol is lower case omega, not w |
| Frequency of rotations measured in | Hz |
| Velocities of all points on string when rotation | w same for all, but linear velocity different. |
| Why is there centrapetal acceleration | Velocity changing so must be an a towards centre of circle always at 90 degrees to v. |
| N2L requirements | F = ma only true with constant mass and SI units |
| Why is there a centrapetal force | N2L applies so there must be a centrapetal force as there is a centrapetal acceleration |
| Normal driving effect of friction | Friction on road from wheel backwards, so friction forwards on wheel from road - doesnt oppose car motion. There is a max to the frictional force, so as v increases eventually r must increase |
| Skidding wheels | Friction on road from wheel forwards so from road backwards on wheel - opposes car motion |
| Car wheels turning | Friction gains a perpendicular component as friction in new wheel direction, which is the centrapetal force. |
| Loop de loop physics at the top | N and mg both acting downwards. Falls when it loses contact, which is when N = 0, making mg + N the lowest force it can be (so with such a low v r must decrease to give minimum force of mg) As v up, N increases for enough centripetal |
| Loop de loop calculating height fallen for energy | h = 0 at the top of the loop where we do our calculations |
| Work done in circular motion | Zero as no displacement in direction of force (orbits last forever) |
| 'Apparent weight' | NCF |
| Centripetal force | Not a real force. Provided by a real force. Is the resultant of all real forces acting on body. |
| How to solve circular motion Qs | Free body diagram. Resolve forces towards centre of circle with resultant = CF If needed resolve forces at 90 degrees to CF where resultant = 0 NOT statics problems |
| Why a wider radius turn faster | Higher r when turning so higher v possible before max frictional force (as m is fixed) |
| Banking aircraft | Normal circle but with lift force at angle. Lift always at 90 degrees to wings. Also need to speed up when turning so vertical component still balances weight once some component horizontal. |
| Why angle theta increases when angular velocity of conical pendulum increases | So vertical equilibrium maintained as Tcostheta = mg so costheta must decrease so theta increases |
| What happens if too fast over road bump | Max centripetal force is when N=0 so mg. If too fast, will 'jump' the car as radius increases |
| Why normal reaction force is significantly reduced | Ultimately is just trying to limit centrapetal force, but can also see as weight being 'used up' as centripetal so less going into surface. |
| Radius of a diagonal swing spinning | The radius of the actual 2D circle it takes, not the swing rope |
| Actually evaluate answer don't just write the variables | |
| Read through the practical skills booklet before exam |