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Published byHector Eugene Bradford Modified over 9 years ago
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Force and Momentum Chapter 1
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Reminders from GCSE Momentum is a measure of how easy or difficult it is to change the motion of a body –The greater the momentum, the bigger the force needed to change it Momentum (p) = mass x velocity kg ms –1 or Nm kg ms –1 Momentum is a vector Momentum is conserved
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Newton’s Laws and momentum N1: An object remains at rest or travelling at a constant velocity unless acted on by a force –ie a force is needed to change a body’s momentum N2: the rate of change of momentum is proportional to the force acting We define the Newton as the unit of force which gives a mass of 1 kg an acceleration of 1 ms –2
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More on Newton’s 2 nd law More generally: –If m is constant: –If m changes at a constant rate: e.g., a rocket ejecting hot exhaust gases
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Impulse impulse (Ns) So impulse is equal to the change of momentum of a body This idea is used a lot in road safety –Collisions often involve large changes of momentum –If you can extend the time over which this happens, you can reduce the force (and so serious injuries)
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Road safety All the devices shown below are designed to increase the time of the momentum change during an accident. How?
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Impulse example A golf ball of mass 0.05 kg is hit off a tee at a speed of 40 ms –1. What is its momentum? p = mv = 0.05 × 40 = 2 kg ms –1 The club was in contact with the ball for 0.5 ms. What force did it exert on the ball? ∆p = force × time, F = ∆p/t = 2/0.0005 F = 4000 N –Golf club animationGolf club animation
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Duck and airliner Estimate the impact force of a duck hitting an airliner. –Mass of duck = 0.5kg –Length of duck = 0.3m –Velocity of airliner = 250ms -1 Equivalent to ~10.6 tonnes!
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Force-time graphs Force x time = change in momentum So area under graph = impulse
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Rebound impacts +u -v
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Rebound impacts For rebounds at an angle, need to consider normal components of velocity If u=v, 1 = 2 Before collision u normal =ucos after collision v normal =-ucos So p=-2mucos F=-2mucos /t u v
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Conservation of momentum The principle states: for a system of interacting objects, the total momentum remains constant, provided no external force acts. Derived by Newton from N3, but in fact more fundamental.
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Conservation of momentum Force F 1 on ball A: Force on ball B: But F 1 =-F 2, so uAuA uBuB vAvA vBvB Total momentum afterTotal momentum before A A A B B B
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Conservation of momentum Now make sure you can do the questions on p. 13… by doing them …and q.4 on p. 20 – do it too.
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Newton’s Cradle Flash animation More than you ever wanted to know herehere
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Elastic collisions An elastic collision is one where there is no loss of kinetic energy –If a ball bounces perfectly elastically, it will reach the same initial height In (macroscopic) real life there are no perfectly elastic collisions –but some gas particles and sub-atomic particles get pretty close So Elastic means p and KE are conserved –Newton’s cradle is a good exampleNewton’s cradle
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Head-on elastic collisions Objects bounce off each other
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Conservation of momentum Conservation of kinetic energy To obtain expressions for the velocities after the collision, rewrite the above as: which may be substituted into equation (2) above to obtain: Dividing these relationships gives
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Inelastic collisions In an inelastic collision, some KE is converted to other forms of energy –Heat, sound, light etc… A totally inelastic collision is one where the colliding objects stick together –Loss of KE is a maximum (but generally not complete) A partially inelastic collision is where the colliding objects move apart and have less KE after the collision than before.
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Inelastic collisions Check you can do the calculations on page 15
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Elastic collisions
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Inelastic collisions
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Centre of mass In all closed systems, the motion of the centre of mass is unchanged during a collision In an elastic collision there is motion relative to the centre of mass afterwards In a completely inelastic collision there is no motion relative to the centre of mass afterwards Adjustable applet Billiard balls animation Physclips
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Explosions Momentum is conserved (as usual) Momentum before = momentum after = 0 Make sure you can do qs on p. 17…
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