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PHYSICS UNIT 2: DYNAMICS (Explaining Motion). FORCES Force: a "push" or a "pull“ unit: Newtons, N (1 N is about ¼ lb) vector - includes direction contact.

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Presentation on theme: "PHYSICS UNIT 2: DYNAMICS (Explaining Motion). FORCES Force: a "push" or a "pull“ unit: Newtons, N (1 N is about ¼ lb) vector - includes direction contact."— Presentation transcript:

1 PHYSICS UNIT 2: DYNAMICS (Explaining Motion)

2 FORCES Force: a "push" or a "pull“ unit: Newtons, N (1 N is about ¼ lb) vector - includes direction contact forces and field forces (act over a distance) net force: total effect of all forces acting on an object

3 FORCES Typical Forces gravity, F G : object’s weight, always directed toward center of earth (F G =mg mass × acceleration due to gravity) normal force, F N : supporting force a surface exerts on an object, always directed upward perpendicular to the surface tension, F T : force transmitted by a rope or chain, directed along the rope, constant throughout the rope

4 FORCES Free body diagrams: show just one object & the forces acting on the object (NOT forces the object is exerting on other things) example: car hitting a wall

5 Examples Apple on a table Rock under water Block on a hill Water skier Child pulled forward at an angle on a sled

6 NEWTON’S LAWS OF MOTION The Law of Inertia (1 st Law): an object’s velocity stays constant unless acted upon by a net external force inertia: resistance to change in motion (mass is a measure of inertia, more mass = more inertia)

7 Example of Newton’s 1 st Law

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11 NEWTON’S 2 nd LAW OF MOTION The Law of Acceleration (2 nd Law): a net force causes an acceleration proportional to the force, in the same direction, and inversely proportional to mass. F net = ma F net : sum of all forces or net force (N), m: mass (kg), a: acceleration (m/s 2 ) 1 N = 1 kg·m/s 2

12 Second  The greater the force, the greater the acceleration  The greater the mass, the greater the force needed for the same acceleration  Calculated by: F = ma  (F = force, m = mass, a = acceleration) NEWTON’S 2 nd LAW OF MOTION

13 NEWTON’S 3 rd LAW OF MOTION The Law of Interaction (3 rd Law): for every action force from one object on another, there is an equal magnitude, opposite direction reaction force from the 2 nd object back on the 1 st action: hammer hits anvil reaction: anvil hits hammer

14 NEWTON’S 3 rd LAW OF MOTION Law of Interaction (3 rd Law) action & reaction forces do not balance each other - they are on different bodies (ex: car pulling a trailer) equal force does not mean equal acceleration - depends on mass (ex: person jumping off the ground)

15 Examples of Newton’s 3 rd law

16 FORCES Finding the Net Force (total of all forces on an object) draw a free body diagram identify & label x & y axes separate forces into x and y parts – F x =Fcos  F y =Fsin  add all x forces, add all y forces equilibrium: no net force – x forces add up to zero, y forces add up to zero

17 Example

18 LAB 2.3 – Elevator Scene 1

19 LAB 2.3 – Elevator Scene 2

20 LAB 2.3 – Elevator Scene 3

21 LAB 2.3 – Elevator Frame 1

22 LAB 2.3 – Elevator Frame 2

23 LAB 2.3 – Elevator Frame 3

24 LAB 2.3 – Elevator Frame 4

25 LAB 2.3 – Elevator Frame 5

26 LAB 2.3 – Elevator Frame 6

27 LAB 2.3 – Elevator Frame 7

28 QUIZ 2.1 Joe rolls a ball down a hill. The ball has a mass of kg. The force pulling the ball down the hill is 6.00 N. The hill is m long. (a) What is the ball’s acceleration? (b) How fast is the ball going at the bottom of the hill, if it started at rest at the top? (c) If the force on the ball doubled, what would happen to the ball’s acceleration? (d) If instead the mass of the ball doubled, what would happen to its acceleration? 12.0 m/s m/s doubles (24 m/s 2 ) halves (6 m/s 2 )

29 PHYSICS UNIT 2: DYNAMICS (Explaining Motion)

30 NEWTON’S LAWS OF MOTION Law of Inertia (1 st Law) objects slow & stop, or require continued force to keep moving, due to friction

31 FRICTION Friction Force, F f : resistance to motion between objects in contact with each other acts parallel to contact surface, opposite to motion caused by uneven surfaces, molecular attraction

32 FRICTION static friction: resistance to starting motion (at rest) beneficial (walking, building, eating, wheels rolling) kinetic friction: resistance to continued motion (sliding) undesirable (machines, moving furniture, wheels skidding) kinetic friction < static friction

33 FRICTION coefficient of friction,  : constant that depends on type of surfaces in contact  s : coefficient of static friction  k : coefficient of kinetic friction F f =  F N (friction force =  × normal force)

34 FRICTION

35 F f FRICTION on horizontal surface: mg FNFN F N = mg (normal force = body weight) so F f =  mg

36 FRICTION on tilted surface:  mg mgcos  FNFN FfFf F N = mgcos  so f =  mgcos 

37 PHYSICS UNIT 2: DYNAMICS (Explaining Motion)

38 QUIZ 2.2 A 1200 kg car sits on a horizontal road. (a) How much force does Joe need to push the car at a constant speed if the coefficient of kinetic friction is 0.600? (b) How much will the car accelerate if Joe uses a force of 10,000 N? a) 7060 N b) 2.45 m/s 2

39 PHYSICS UNIT 2: DYNAMICS (Explaining Motion)

40 PROJECTILE MOTION Projectile motion: parabolic trajectory (path) Two dimensions of motion: horizontal (x), vertical (y) vyvy vxvx  v v x = vcos  v y = vsin 

41 if a bullet was fired horizontally, and another bullet was dropped from the same height at the same time, which would hit the ground first? PROJECTILE MOTION Vertic al Motion constant vertical accelerati on due to gravity (2 nd Law)

42 PROJECTILE MOTION A monkey hangs from a tree branch. A hunter aims his tranquilizer gun barrel straight at the monkey. When the hunter fires his gun, should the monkey keep holding on to the branch, or let go?

43 PROJECTILE MOTION Vertical Motion position: y = h + v i sin  i t – ½gt 2 a. for ground launch, h=0, y = v i sin  i t – ½gt 2 b. for horizontal cliff launch,  0 =0, y = h – ½gt 2 speed: v y = v i sin  i – gt flight time, T: t when y=0 ground: cliff:

44 A tank moving at constant speed fires a shell straight up into the air. Where will the shell come back down? PROJECTILE MOTION Horizon tal Motion constan t horizont al speed due to no horizont al force (1 st Law)

45 PROJECTILE MOTION A snowmobile fires a flare, then slows down. Where does the flare land? If the snowmobile speeds up instead, where does the flare land?

46 PROJECTILE MOTION Horizontal Motion position: x = v i cos  i t for horizontal cliff launch,  i =0, x = v i t speed: v x = v i cos  i range, R: x when t = T ground: cliff:

47 PROJECTILE MOTION Example: A projectile is launched from ground level with a velocity of 50 m/s at an angle of 30 degrees. What is its position and velocity 2 seconds later? What is its flight time? What is its range?

48 PHYSICS UNIT 2: DYNAMICS (Explaining Motion)

49 A plane moving at constant speed drops a flare. Describe the path of the flare. RELATIVE MOTION Refere nce Frames : projectile motion in one reference frame can be vertical free fall in another reference frame (and vice versa)

50 PHYSICS UNIT 2: DYNAMICS (Explaining Motion)

51 QUIZ 2.3 Circle your answers! Watch sig. fig's & units! 1. Joe throws a ball from ground level at an angle of 41º and a speed of 19 m/s. (a) Find the ball's vertical position after 1.5 seconds. (b) Find the ball's horizontal speed after 1.5 seconds. 2. Jane throws a ball off a 95-m tall building horizontally at 19 m/s. (a) Find the ball's flight time. (b) Find the ball's range. y = h + v i sin  i t – ½gt 2 v y = v i sin  i – gt x = v i cos  i t v x = v i cos  i 7.67 m 14.3 m/s 4.40 s 83.6 m

52 PHYSICS UNIT 2: DYNAMICS (Explaining Motion)

53 UNIT 2 REVIEW Newton's Laws (Memorize!): 1st Law: velocity stays constant unless acted upon by a net force 2nd Law: net force = mass x acceleration 3rd Law: for every action force, there is an equal and opposite reaction force

54 UNIT 2 REVIEW  F = ma F G = mg F f =  F N v f = v i + at  x= v i t + ½at 2 v f 2 =v i 2 + 2a  x y = h + v i sin  i t – ½gt 2 x = v i cos  i t v y = v i sin  i – gt v x = v i cos  i


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