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Collisions © D Hoult 2010.

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Presentation on theme: "Collisions © D Hoult 2010."— Presentation transcript:

1 Collisions © D Hoult 2010

2 Elastic Collisions © D Hoult 2010

3 1 dimensional collision
Elastic Collisions 1 dimensional collision © D Hoult 2010

4 1 dimensional collision: bodies of equal mass
Elastic Collisions 1 dimensional collision: bodies of equal mass © D Hoult 2010

5 1 dimensional collision: bodies of equal mass
Elastic Collisions 1 dimensional collision: bodies of equal mass (one body initially stationary) © D Hoult 2010

6 1 dimensional collision: bodies of equal mass
Elastic Collisions 1 dimensional collision: bodies of equal mass (one body initially stationary) © D Hoult 2010

7 © D Hoult 2010

8 A B uA Before collision, the total momentum is equal to the momentum of body A © D Hoult 2010

9 After collision, the total momentum is equal to the momentum of body B
vB After collision, the total momentum is equal to the momentum of body B © D Hoult 2010

10 The principle of conservation of momentum states that the total momentum after collision equal to the total momentum before collision (assuming no external forces acting on the bodies) © D Hoult 2010

11 The principle of conservation of momentum states that the total momentum after collision equal to the total momentum before collision (assuming no external forces acting on the bodies) mAuA = mBvB © D Hoult 2010

12 so, if the masses are equal the velocity of B after
The principle of conservation of momentum states that the total momentum after collision equal to the total momentum before collision (assuming no external forces acting on the bodies) mAuA = mBvB so, if the masses are equal the velocity of B after © D Hoult 2010

13 The principle of conservation of momentum states that the total momentum after collision equal to the total momentum before collision (assuming no external forces acting on the bodies) mAuA = mBvB so, if the masses are equal the velocity of B after is equal to the velocity of A before © D Hoult 2010

14 Bodies of different mass
© D Hoult 2010

15 A B © D Hoult 2010

16 A B uA © D Hoult 2010

17 Before the collision, the total momentum is equal to the momentum of body A
© D Hoult 2010

18 A B vA vB © D Hoult 2010

19 After the collision, the total momentum is the sum of the momenta of body A and body B
vA vB © D Hoult 2010

20 If we want to calculate the velocities, vA and vB we will use the
© D Hoult 2010

21 If we want to calculate the velocities, vA and vB we will use the principle of conservation of momentum A B vA vB © D Hoult 2010

22 The principle of conservation of momentum can be stated here as
© D Hoult 2010

23 The principle of conservation of momentum can be stated here as
mAuA = mAvA + mBvB © D Hoult 2010

24 The principle of conservation of momentum can be stated here as
mAuA = mAvA + mBvB If the collision is elastic then © D Hoult 2010

25 The principle of conservation of momentum can be stated here as
mAuA = mAvA + mBvB If the collision is elastic then kinetic energy is also conserved © D Hoult 2010

26 The principle of conservation of momentum can be stated here as
mAuA = mAvA + mBvB If the collision is elastic then kinetic energy is also conserved ½ mAuA2 = ½ mAvA2 + ½ mBvB2 © D Hoult 2010

27 The principle of conservation of momentum can be stated here as
mAuA = mAvA + mBvB If the collision is elastic then kinetic energy is also conserved ½ mAuA2 = ½ mAvA2 + ½ mBvB2 mAuA2 = mAvA2 + mBvB2 © D Hoult 2010

28 From these two equations, vA and vB can be found
mAuA = mAvA + mBvB mAuA2 = mAvA2 + mBvB2 From these two equations, vA and vB can be found © D Hoult 2010

29 From these two equations, vA and vB can be found
mAuA = mAvA + mBvB mAuA2 = mAvA2 + mBvB2 From these two equations, vA and vB can be found BUT © D Hoult 2010

30 It can be shown* that for an elastic collision, the velocity of body A relative to body B before the collision is equal to the velocity of body B relative to body A after the collision © D Hoult 2010

31 It can be shown* that for an elastic collision, the velocity of body A relative to body B before the collision is equal to the velocity of body B relative to body A after the collision * a very useful phrase ! © D Hoult 2010

32 It can be shown* that for an elastic collision, the velocity of body A relative to body B before the collision is equal to the velocity of body B relative to body A after the collision uA In this case, the velocity of A relative to B, before the collision is equal to © D Hoult 2010

33 It can be shown* that for an elastic collision, the velocity of body A relative to body B before the collision is equal to the velocity of body B relative to body A after the collision uA In this case, the velocity of A relative to B, before the collision is equal to uA © D Hoult 2010

34 and the velocity of B relative to A after the collision is equal to
It can be shown* that for an elastic collision, the velocity of body A relative to body B before the collision is equal to the velocity of body B relative to body A after the collision vA vB and the velocity of B relative to A after the collision is equal to © D Hoult 2010

35 It can be shown* that for an elastic collision, the velocity of body A relative to body B before the collision is equal to the velocity of body B relative to body A after the collision vA vB and the velocity of B relative to A after the collision is equal to vB – vA © D Hoult 2010

36 It can be shown* that for an elastic collision, the velocity of body A relative to body B before the collision is equal to the velocity of body B relative to body A after the collision vA vB and the velocity of B relative to A after the collision is equal to vB – vA for proof click here © D Hoult 2010

37 We therefore have two easier equations to “play with” to find the velocities of the bodies after the collision equation 1 © D Hoult 2010

38 We therefore have two easier equations to “play with” to find the velocities of the bodies after the collision equation 1 mAuA = mAvA + mBvB equation 2 © D Hoult 2010

39 We therefore have two easier equations to “play with” to find the velocities of the bodies after the collision equation 1 mAuA = mAvA + mBvB equation 2 uA = vB – vA © D Hoult 2010

40 © D Hoult 2010

41 © D Hoult 2010

42 A B uA © D Hoult 2010

43 A B uA Before the collision, the total momentum is equal to the momentum of body A © D Hoult 2010

44 A B vA vB After the collision, the total momentum is the sum of the momenta of body A and body B © D Hoult 2010

45 Using the principle of conservation of momentum
© D Hoult 2010

46 Using the principle of conservation of momentum
mAuA = mAvA + mBvB © D Hoult 2010

47 Using the principle of conservation of momentum
mAuA = mAvA + mBvB A B vA vB © D Hoult 2010

48 Using the principle of conservation of momentum
mAuA = mAvA + mBvB A B vA vB © D Hoult 2010

49 Using the principle of conservation of momentum
mAuA = mAvA + mBvB A B vA vB One of the momenta after collision will be a negative quantity © D Hoult 2010

50 2 dimensional collision
© D Hoult 2010

51 2 dimensional collision
© D Hoult 2010

52 © D Hoult 2010

53 A B © D Hoult 2010

54 A B Before the collision, the total momentum is equal to the momentum of body A © D Hoult 2010

55 © D Hoult 2010

56 After the collision, the total momentum is equal to the sum of the momenta of both bodies
© D Hoult 2010

57 Now the sum must be a vector sum
© D Hoult 2010

58 mAvA © D Hoult 2010

59 mAvA mBvB © D Hoult 2010

60 mAvA mBvB © D Hoult 2010

61 mAvA mBvB © D Hoult 2010

62 mAvA mBvB © D Hoult 2010

63 mAvA p mBvB © D Hoult 2010

64 mAvA p mAuA mBvB © D Hoult 2010

65 mAvA p mAuA mBvB © D Hoult 2010

66 mAvA p mAuA mBvB © D Hoult 2010

67 mAvA p mAuA mBvB p = mAuA © D Hoult 2010

68 2 dimensional collision: Example
Body A has initial speed uA = 50 ms-1 © D Hoult 2010

69 2 dimensional collision: Example
Body A has initial speed uA = 50 ms-1 Body B is initially stationary © D Hoult 2010

70 2 dimensional collision: Example
Body A has initial speed uA = 50 ms-1 Body B is initially stationary Mass of A = mass of B = 2 kg © D Hoult 2010

71 2 dimensional collision: Example
Body A has initial speed uA = 50 ms-1 Body B is initially stationary Mass of A = mass of B = 2 kg After the collision, body A is found to be moving at speed vA = 25 ms-1 in a direction at 60° to its original direction of motion © D Hoult 2010

72 2 dimensional collision: Example
Body A has initial speed uA = 50 ms-1 Body B is initially stationary Mass of A = mass of B = 2 kg After the collision, body A is found to be moving at speed vA = 25 ms-1 in a direction at 60° to its original direction of motion Find the kinetic energy possessed by body B after the collision © D Hoult 2010


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