Presentation is loading. Please wait.

Presentation is loading. Please wait.

Chapter 4 -- Changes in Motion

Similar presentations


Presentation on theme: "Chapter 4 -- Changes in Motion"— Presentation transcript:

1 Chapter 4 -- Changes in Motion
A force is something that can change the velocity of an object. (i.e. speed up, slow down, or change direction). In other words, a force can cause an object to accelerate. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

2 Changes in Motion We often think of a force as a push or a pull.
We push a desk by exerting a force on it, and changing its velocity. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

3 Changes in Motion If we push an object we exert a force for a period of time. If we stop pushing, the object will eventually stop. That is because other forces continue to act on it, changing its velocity. Like?.... FRICTION 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

4 Changes in Motion Friction is only one example of a force. Forces can be divided into two major categories. Contact forces are forces that exist between two objects that are in contact with each other. Field forces are forces that exist between two objects that are separated by some distance. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

5 Newtons Forces are measured in units called “Newtons” (N), Where a net force of 1.0 N will cause a mass of 1.0 kg to accelerate at a rate of 1.0 m/s2. 1 N = 1 kgm/s2 To convert a mass (in kg) to Newtons, you must multiply by acceleration due to gravity. To convert Newtons to mass(in kg), you must divide by acceleration due to gravity. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

6 Changes in Motion “Free-body diagrams” are used to focus on the forces acting on an object. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

7 Changes in Motion How would we draw a free-body diagram for the situation shown below? Fw = weight = mg = Newtons FN = force of table on book (this is called the Normal force) Holt Physics 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

8 Changes in Motion How would we draw a free-body diagram for a 5N football being kicked by a 67 N force at an angle of 56 degrees above horizontal? 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

9 Changes in Motion 67 N 5 N 56 5 N 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

10 Lesson 4-1 Changes in Motion
How would we draw a free-body diagram for the situation shown below? FN Ff FA Fw=mg 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

11 Lesson 4-1 Changes in Motion
How would we draw a free-body diagram for the situation shown below? FN FA Ff Fw=mg FN is less than mg because of the upward pull 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

12 Lesson 4-1 Changes in Motion
How would we draw a free-body diagram for the situation shown below? 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

13 Lesson 4-1 Changes in Motion
How would we draw a free-body diagram for the situation shown below? FN Ff Ff FA FN is more than mg because of the downward push Fw=mg 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

14 Section Review pg. 128 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

15 Newton’s Laws 1st Law - an object with no net force acting on it remains at rest or moves with a constant velocity in a straight line. When there are forces, up or right is positive, and down or left is negative. Inertia – the tendency of an object not to accelerate. 7th missed these two slides 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

16 Acceleration is determined by Net External Force
External force is a single force that acts on an object as a result of the interaction between the object and its environment. Net external force is the sum of all forces acting on an object (the resultant force). Ex: Tug of War… 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

17 A man if pulling a crate with a force of 89 N at an angle of 15 degrees above horizontal. What are the x and y components of this force? FAx = FAcos15 = 86N FAy = FAsin15 = 23N 89N FAy 15 FAx 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

18 A dog is pulled to the left with a force of 56 N and to the right with a force of 176 N, upward with a force of 780 N and downward with a force of 350 N. What is the net external force? ∑Fx = 176N-56N =120N ∑Fy =780N-350N= 430N 780N R2= 2011 assigned this problem and did 4a and b for homework next night R=446N R 176N 430 56N Tan-1(430/120)= 74 above horizontal 350N 120 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

19 Problems 4A Problems on page 133 Section Review page 135
9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

20 Newton’s Second Law Newton’s Second Law states – “The acceleration of an object is directly proportional to the net external force acting on the object and inversely proportional to the object’s mass.” 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

21 Newton’s Second Law Newton’s Second Law is often written with the net force isolated, as shown below; Sometimes, the “net” is left out, because the “F” is understood to be the net force. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

22 Newton’s Second Law Example If the net external force on a desk with a mass of 35.0 kg is 45.0 N to the east, what acceleration (magnitude and direction) will the desk experience? Fnet = ma 45.0 N = 35.0 kg (a) a=45.0N/35.0kg=1.29 m/s2 east 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

23 Example 2 A dachshund starts from rest at the top of a water slide that is cm long and slides down to the bottom in seconds. If the net external force on the dachshund is N then what is the mass of the dachshund? 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

24 Given: Fnet=25.8 N x = 450.0cm = 4.5 m t = 0.700 sec Formula: F = ma
A dachshund starts from rest at the top of a water slide that is 450.0cm long and slides down to the bottom in seconds. If the net external force on the dachshund is N then what is the mass of the dachshund? Given: Fnet=25.8 N x = 450.0cm = 4.5 m t = sec Formula: F = ma Need: a =? And m=? Old Formula: x = 1/2a t2 a = x/(1/2 t2) = 4.5 m/(1/2 (0.700)2) a= 18.4 m/s2 F = ma, m=F/a = 25.8N/18.4m/s2 = 1.4 kg 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

25 Problems 4B Problems on page 138
9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

26 When a car hits a deer, why does the car take so much damage?
Questions to Consider When a car hits a deer, why does the car take so much damage? If you punch someone in the face, why does it hurt your hand? When someone fires a gun, why do they feel a recoil? When you blow up a balloon and release it, why does it fly around the room? 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

27 Answer  Newton’s Third Law!
9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

28 Newton’s Third Law Newton’s Third Law
If two objects interact, the magnitude of the force exerted on object 1 by object 2 is equal To the magnitude of the force simultaneously Exerted on object 2 by object 1, and these Forces are opposite in direction. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

29 Newton’s Third Law What we call the “normal force” is a reaction force. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

30 Newton’s Third Law Newton’s Third Law can also be used to explain propulsion. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

31 Newton’s Third Law Newton’s Third Law can also be used to explain why your weight appears to change in an elevator. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

32 Equilibrium Objects at rest or moving with a constant velocity are said to be in equilibrium. Therefore the net external force acting on a body in equilibrium must be zero. The vector sum of all the forces acting on it is zero. Fx=0 and Fy=0 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

33 Newton’s Third Law If every object that you pull pulls back with an equal and opposite force, how can you ever move anything? 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

34 Newton’s Third Law Remember, when considering whether or not something will move, we want to find the net force acting on the individual object...the reaction force is on your hand!!! 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

35 Football and Newton’s Laws of Motion
9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

36 Section review pg. 140 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

37 Newton’s Laws Lab 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

38 Friction - force that opposes the motion between two surfaces.
Using Newton’s Laws Friction - force that opposes the motion between two surfaces. The direction of the force of friction is parallel to the SURFACE and in a direction that opposes the slipping of the two surfaces. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

39 Static friction(FS ) - force that opposes the start of motion.
If the magnitude of the force applied is greater than the magnitude of static friction, movement occurs. As long as the object does not move, the force of static friction (FS ) is always equal to and opposite in direction to the component of the applied force (FA ) that is parallel to the surface FS = -FA WHEN IT DOES NOT MOVE Also, FA is “just a hair” more than Fs at the start of motion (We’ll assume = for the most part.) 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

40 Kinetic friction Fk - force between surfaces in relative motion
Always LESS than static friction If moving at a constant velocity, Fk = -FA Variables Defined FA = Applied Force Ff = Force of friction FN = Normal force FW = Fg = Weight of the object Fs = Force of static friction Fk = Force of kinetic friction 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

41 Fk= kFn s = coefficient of Fs,max= sFn static friction
Equations Fk= kFn s = coefficient of Fs,max= sFn static friction Ff =Fn k = coefficient of kinetic friction  is a constant that depends on the two surfaces in contact. (See page 144) 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

42 Example A 24 kg crate initially at rest on a horizontal floor requires a 75 Newton horizontal force to set it in motion to the left (this is FA and Fs,max). Find the coefficient of static friction (s) between the crate and the floor. If it only requires 34 N to keep the crate moving at a constant velocity (this is Fk), what is the coefficient of kinetic friction (k)? 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

43 = s235N s= 75N / 235N = 0.32 Fk = kFN = k235N =0.14 k= 34N / 235N
Fs = 75N= sFN = s235N s= 75N / 235N = 0.32 Fk = kFN = k235N =0.14 k= 34N / 235N FN = 235 N Fs = 75N FA Fk = 34N Fg=24kg X9.81m/s2 = 235 N 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

44 Motion on a Horizontal A desk with a mass of 75.0 kg sits on a floor, where the coefficient of static friction in between the two surfaces is How much force must someone apply in a direction parallel to the surface of the floor to get the desk moving? 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

45 Motion on a Horizontal Sketch the diagram:
The net force in the y-dimension is zero. The box will move when the applied force (FA) just overcomes the maximum force of static friction. FN s s 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

46 Motion on a Horizontal Given: m = 75.0 kg g = 9.81 m/s2 Find:
FN m = 75.0 kg g = 9.81 m/s2 s Find: FN and then, Fs Solution: s FN = -Fw = mg = -(75.0 kg)(-9.81 m/s2) = 736 N Fs = msFN = (0.40)(736 N) = 290 N so our applied force must be just greater than 290 N 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

47 Problems 4C, page 145 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

48 Motion on a Horizontal A boy exerts a horizontal force of 12.0 N on a 20.0 N box to slide it across a table where the coefficient of kinetic friction between the surfaces is Sketch the free-body diagram and find the acceleration on the box. Do this problem on october 7 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

49 Motion on a Horizontal Sketch the diagram.
Use Fnet = ma. We will need to find the net force on the box and then divide it by the mass, in order to find the acceleration. FN k k 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

50 Motion on a Horizontal Sketch the diagram.
The net force in the y-dimension will be zero. We will need to calculate the force of friction (Fk), and subtract it from the applied force (Fa) to get the net force (FNet). FN k k 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

51 Motion on a Horizontal Given: mk = 0.34 Find: Solution: FN
Fw = 20.0 N g = 9.81 m/s2 Fa = 12.0 N mk = 0.34 k Find: Fk, Fnet, m and then a k Solution: Fk = mkFN = mkFw = (0.34)(20.0 N) = 6.8 N Fnet = Fa - Fk = 12.0 N N = 5.2 N 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

52 Everyday Forces Motion on a Horizontal
When the applied force (FA) is exerted at an angle above the horizontal, it is necessary to resolve the applied force into x (FAx) and y (FAy) components and subtract FAy from the Weight. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

53 Everyday Forces Motion on a Horizontal
A girl is pulling a sled with a mass of 16.0 kg across a level patch of grass by exerting a force of 42.0 N along a rope that forms an angle of 33.0o above the ground. The coefficient of kinetic friction between the sled and the grass is Sketch the free-body diagram and find the acceleration of the sled. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

54 Everyday Forces Motion on a Horizontal
Sketch the diagram. Fn = (mg - Fay) Because a component of the applied force is in the y-dimension, the normal force is going to be less than the weight of the sled. The net force in the y-dimension is still zero, and FN = (Fw - Fay). 42N Fk k 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

55 Everyday Forces Motion on a Horizontal
Sketch the diagram. Fn = (mg - Fay) The key to this problem is to decrease the normal force (FN) by the force applied in the y (Fay), before you calculate the force of friction (Fk). 42N Fk k 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

56 Everyday Forces Motion on a Horizontal
Given: m = 16.0 kg Fa = 42.0 N q = 33.0o mk = 0.25 42N Find: Fax, Fay, FN, Fk, Fnet, a Solution: Fax = FaCosq = (42.0 N)(Cos 33.0o) = 35.2 N Fay = FaSinq = (42.0 N)(Sin 33.0o) = 22.9 N FN = (Fw - Fay) = (mg - Fay) = (16.0 kg)(9.81 m/s2) - (22.9 N)) = 134 N 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

57 Everyday Forces Motion on a Horizontal
Given: m = 16.0 kg Fa = 42.0 N q = 33.0o mk = 0.25 42N Find: Fax, Fay, FN, Ff, Fnet, a Solution: Fk = mkFN = (0.25)(134 N) = 33.5 N Fnet = Fax -Fk = 35.2 N N = 1.7 N 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

58 Everyday Forces Motion on a Horizontal
When the applied force (Fa) is exerted below the horizontal, the y component of the applied force (Fay) will increase the normal force (FN). 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

59 Everyday Forces Motion on a Horizontal
Example. A woman applies a force of N on the handle of a 180 N lawnmower, at an angle of below the horizontal. The coefficient of kinetic friction between the grass and lawnmower is Draw a free-body diagram, and find the force of kinetic friction. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

60 free-body diagram and find the force of friction.
Draw the free-body diagram and find the force of friction. FN = (Fw + Fay) = (180 N N) = N Fax = FaCosq = (125.0N)(Cos 35.0o) = N Fk 35.0o mk = 0.35 Fa = 25.0 N Fay = FaSinq = (125.0N)(Sin 35.0o) = 71.7 N Fw = 180 N You can find a the same way as the previous problem Fk = mkFN = (0.35) (251.7 N) = 88 N 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

61 Practice 4D, 1 and 4 on page 147 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

62 Everyday Forces Motion on an Inclined Plane
Fw =Fg= mg The weight (Fw) is directed straight down. It ignores the incline. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

63 Everyday Forces Motion on an Inclined Plane
Fwy = mgcosq Fw =Fg= mg The y component of the weight is (Fwy) is perpendicular to the surface of the ramp. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

64 Everyday Forces Motion on an Inclined Plane
Fwy = mgcosq Fwx = mgsinq Fw = mg The x component of the weight is (Fwx) is parallel to the surface of the ramp. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

65 Everyday Forces Motion on an Inclined Plane
Fwx = mgsinq Fwy = mgcosq Fw = mg We can redraw the x component of the weight (Fwx), to make it clear that it helps to move the object down the ramp. We might also rename it Fa If it is the only applied force working. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

66 Everyday Forces Motion on an Inclined Plane
Ff Fwx = mgsinq Fwy = mgcosq Fw = mg If there is friction between the ramp and the object, it will oppose the motion of the object down the ramp. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

67 Everyday Forces Motion on an Inclined Plane
Fk = mkFN Fwx = mgsinq Fwy = mgcosq Fw = mg If the object is in motion, the force of friction (Ff) can be calculated with Fk = mkFN. IF the object is being pulled up the ramp, then the force of friction will be the other direction and Fg will also work against you. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

68 Everyday Forces Motion on an Inclined Plane
FN = -Fwy Ff = mkFN Fwx = mgsinq Fwy = mgcosq Fw = mg The normal force (FN) will be equal and opposite to the y component of the weight (unless you are pulling up or pushing down at an angle). 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

69 Everyday Forces Motion on an Inclined Plane
FN = -Fwy Ff = mkFN Fwx = mgsinq q Fwy = mgcosq q Fw = mg The two triangles in the picture are similar, so they share like angles. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

70 Please Copy Problem and Draw a Large Diagram!!
A crate with a mass of 35.0 kg is sliding down an inclined plane with an angle of 43.0o above the horizontal. If the crate is accelerating at a rate of 3.45 m/s2, find the coefficient of kinetic friction between the ramp and crate. Start with a diagram. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

71 Everyday Forces Motion on an Inclined Plane
Fk Fw=35.0kgX9.81m/s2 = 343N 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

72 Everyday Forces Motion on an Inclined Plane
Given: m = 35.0 kg g = 9.81 m/s2 a = 3.45 m/s2 Find: FN, Fwx, Fnet, Fk, mk Solution: Fwx = mgsinq = (35.0 kg)(9.81 m/s2)(sin 43.0o) = 234 N Fnet = ma = (35.0 kg)(3.45 m/s2) = 121 N Fnet=Fwx-Fk Fk=Fwx-Fnet Fk = Fwx - Fnet = 234 N – 121 N = 113 N 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

73 A 45kg BOX is moved up a ramp inclined at 56 degrees above horizontal
A 45kg BOX is moved up a ramp inclined at 56 degrees above horizontal. If the box starts from rest at the bottom of the ramp and is pulled at an angle of 35 degrees with respect to the incline and with a force of 572 N, what is the acceleration up the ramp? Assume that K is 0.25. FN FA=572 N Fay 35 FK Fax 56 Fwy=mgcos 56 45kg Fwx=mgsin X9.81=441N 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

74 Find FN, FN=(Fw,y-Fa,y )=(441N)cos56-272N(sin35) = 91 N
Find FK, FK = K FN = (0.25)(91N) = 23N Find ax, ax = Fnet,x /m = = (FA,x- Fk - Fw sin56)/m = (572cos35 – 23N – 441sin56)/45kg= 1.78 m/s2 FN FA=234 N Fay 32 FK Fax 23 Fwy=mgcos mgcos 23 245N mgsin Fwx=mgsin 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

75 4D 2 and 3 on page 147 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

76 A 25kg crate is moved up a ramp inclined at 23 degrees above horizontal. If the box starts from rest at the bottom of the ramp and is pulled at an angle of 32 degrees with respect to the incline and with a force of 234 N, what is the acceleration up the ramp? Assume that K is 0.19. FN FA=234 N Fay 32 FK Fax 23 Fwy=mgcos 23 25kg Fwx=mgsin X9.81=245N 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

77 Find FN, FN = (Fw,y - Fa,y )= (25kg)(9
Find FN, FN = (Fw,y - Fa,y )= (25kg)(9.81m/s2)cos N(sin32) = 102N FN FA=234 N Fay 32 FK Fax 23 Fwy=mgcos mgcos 23 245N mgsin Fwx=mgsin 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

78 Find FK, FK = K FN = (0.19)(102N) = 19.38N
Fay 32 FK Fax 23 Fwy=mgcos mgcos 23 245N Fwx=mgsin mgsin 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

79 Find ax, ax = Fnet,x /m = = (FA,x- Fk - Fw sin23)/m = (234cos32 – 19
Find ax, ax = Fnet,x /m = = (FA,x- Fk - Fw sin23)/m = (234cos32 – 19.38N – 245sin23)/m = 83 kgm/s2/25kg = 3.3 m/s2 WEIGHT and Fk are SUBTRACTED because they are working against the box going up the ramp. FN 102 N 234 N 32 FK 23 Fwy=mgcos mgcos 23 245N Fwx=mgsin mgsin 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

80 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

81 Using Newton’s Laws When an object is resting with no additional external forces on a horizontal surface, then FW = Fn When pushing down at an angle, force is added to FN (Fay+Weight), so FN increases to Weight+FAy. When pulling up at an angle, force is subtracted from the FN (weight-FAy), so FN decreases to Weight-FAy When moving at constant velocity Fk = FAx ,so Fk =Fn or FAx =Fn. This is also true of static friction until the maximum is reached. FAx means parallel to the surface When on an incline, Fgx makes the object go down and Fgy equals the normal force (unless pulled up at an angle, then Fgy is subtracted from the normal force.) Ff always opposes the motion. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

82 Everyday Forces Motion on an Inclined Plane
A block with a mass of 5.00 kg is placed on a frictionless inclined plane at an angle of 48.0o above the horizontal. Draw a diagram for the problem and find the acceleration of the block. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

83 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

84 Everyday Forces Motion on an Inclined Plane
Given: m = 5.00 kg q = 48.0o g = 9.81 m/s2 Find: Fw, Fwx, m and a Solution: Remember...there is no friction in this example. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

85 Lesson 4-1 Changes in Motion
How would we draw a free-body diagram for the situation shown below? FN Ff Ff Fw=mg mgsin is the applied force! 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

86 Lesson 4-1 Changes in Motion
How would we draw a free-body diagram for the situation shown below? Fw=mg 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

87 Example 2 What forces are at work on a 22N physics book on a 15 degree incline where the force of friction is 3N?What is the net external force? Normal Force (NOT 22 N) 3 N 15 22N 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

88 Now…can we figure out whether it will move? What else do we need?
Components!!! FN 3 N 15 15 22N 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

89 Now…sum all the x and y components!!!!!!!!!!!!!!!!!
FN 3 N 15 Fwcos 15 22N Fwsin 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

90 Assume x is in the direction of the inclined plane…
X components (Fwsin15 – Ffriction) 22sin15-3N = 5.7N-3N = +2.7N Y components cancel Fwcos15 - Normal Force (= Fwcos15) = 0 So….the book does move! Newton’s Second Law can tell us how fast, but we’ll get to that later. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

91 Newton’s Third Law Newton’s Third Law tells us that forces always come in pairs. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

92 Newton’s Third Law Newton’s Third Law tells us that forces always come in pairs. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM

93 Newton’s Third Law These force pairs are called “action-reaction forces”, or “action-reaction pairs”. 9/18/2018 2:14:19 AM9/18/2018 2:14:19 AM


Download ppt "Chapter 4 -- Changes in Motion"

Similar presentations


Ads by Google