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1 Unit Four: Force and Motion John Elberfeld 518 872 2082 GE253 Physics.

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1 1 Unit Four: Force and Motion John Elberfeld GE253 Physics

2 2 Schedule Unit 1 – Measurements and Problem Solving Unit 2 – Kinematics Unit 3 – Motion in Two Dimensions Unit 4 – Force and Motion Unit 5 – Work and Energy Unit 6 – Linear Momentum and Collisions Unit 7 – Solids and Fluids Unit 8 – Temperature and Kinetic Theory Unit 9 – Sound Unit 10 – Reflection and Refraction of Light Unit 11 – Final

3 3 Chapter 4 Objectives Relate force and motion and explain what is meant by a net or unbalanced force. State and explain Newton's first law of motion and describe inertia and its relationship to mass State and explain Newton's second law of motion, apply it to physical situations, and distinguish between weight and mass.

4 4 Chapter 4 Objectives State and explain Newton's third law of motion and identify action-reaction force pairs. Apply Newton's second law in analyzing various situations, use free-body diagrams, and understand the concept of translational equilibrium Explain the causes of friction and how friction is described by using coefficients of friction.

5 5 Reading Assignment Read and study Chapters 4 in College Physics: Wilson and Buffa Expect a quiz on any of the material covered in the course so far

6 6 Written Assignments Do all the exercises on the handout. You must show all your work, and carry through the units in all calculations Use the proper number of significant figures and, when reasonable, scientific notation

7 7 Introduction In the previous week, you explored the motion of objects when the velocity and acceleration of the object are known. In real life, you have to know what actions we need to perform to cause and control this motion

8 8 Introduction For example, when pushing an object, you have to know what to push, where to push it, and how hard to push it. You also want to understand what happens to an object when you push it. In other words, you want to understand the relation between forces and the motion of objects that forces act upon.

9 9 Force A force is a push or a pull. For example, when you try to lift a heavy object, you feel the force of gravity pulling the object down. Springs and magnets also exert forces, as do your muscles. Force is also associated with motion because when you exert force on an object, it may move. Force is a vector quantity because it has direction. When you exert force, it is in a particular direction.

10 10 Net Force This brings us to the concept of net force or total force. If the forces acting on an object are equal and in opposite directions, they will cancel each other out. In such a case, the total force or net force is zero.

11 11 Net Forces

12 12 Net Forces If two forces of equal magnitude but opposite direction are applied to the same object, the vector resultant, or net force acting on the crate, in the x direction, is zero. –The forces are balanced If the forces are not equal in magnitude, the resultant is not zero –A net force accelerates an object in the direction of the force

13 13 Classes of Forces There are two classes of forces: The action-at-a-distance forces are gravity, magnetism, and electrostatic forces. Contact forces include friction and the so-called normal forces. –For example, the force exerted by a table on an object resting on it is a contact force.

14 14 Thought Experiment Force is associated with motion, but the relationship between the two may not be clear at first. The diagram shows an experiment performed by Galileo in which a ball rolls down and then up an inclined plane, always reaching the same level. Therefore, if the surface is horizontal and perfectly frictionless, the ball will continue to move without stopping. However, the ball will stop if another force (like friction) acts upon it.

15 15 Thought Experiment How far would the ball roll on a frictionless horizontal surface?

16 16 Newton’s First Law Based upon Galileo’s experiment and other observations, Newton derived the first law of motion. An object at rest stays at rest unless acted upon by a net external force. An object moving at a constant velocity will continue to move at that velocity unless acted on by a net external force.

17 17 Common Sense Newton’s law is in sharp contrast to the science of ancient Greece. According to Aristotle, an ancient Greek scientist, the natural state of an object is to be at rest. An object moves only when a force acts on it.

18 18 Inertia All objects have mass. This means Newton’s first law can be considered a property of mass called inertia. Inertia is the property of mass which determines its resistance to changes in velocity.

19 19 Mass is in Kilograms Mass is always measured in kilograms in physics The mass in kilograms determines how much gravity affects an object (weight) as well as how hard it is to start or stop its motion (inertia)

20 20 Practice Every object on earth experiences the force of the earth’s gravity, and every object in the solar systems experiences the force of the sun’s gravity All mass always has some type of force on it An object at rest, or at constant velocity (no change in speed OR direction), has no net force on it – all forces add up to zero If an object has a net force on it, the velocity will change (acceleration!)

21 21 Practice On a jet airliner that is taking off, you feel that you are being pushed back into the seat. Why? –You are at rest and will stay at rest unless a force acts upon you. When the plane takes off, you feel the force of the plane acting on you. Is the opposite true when a car stops?

22 22 Newton’s Second Law When a net force acts on an object, the object accelerates. a = Δv/Δt The mass of an object affects its acceleration. According to Newton’s second law F = ma where F and a are vectors. The unit of force is Newton (N), defined as 1N = kg m / s 2

23 23 Second Law Assuming no additional forces, like friction:

24 24 F = ma

25 25 Weight The weight of an object (mass) is the force of gravity acting on the object. Near the earth’s surface, the acceleration due to gravity is about (-) 9.8 m/s 2 downward So, you can calculate the weight of a 1-kg object as follows: F gravity = ma = W = mg = m (-9.8m/s 2 ) The weight of a 1 kg mass is: F = ma = (1kg)(-9.8m/s 2 ) = - 9.8kg m/s 2 = -9.8N

26 26 Gravity Gravity is an example of an action-at-a-distance force. The universal law of gravity, discovered by Newton, is that every mass in the universe is attracted to every other mass with a gravitational force proportional to the two masses and inversely proportional to the square of the distance between the two masses. F = Gm 1 m 2 /d 2

27 27 Forces are the Same F = Gm 1 m 2 /d 2 The force of m 1 on m 2 is the same as the force of m 2 on m 1 The sun is so much more massive than the earth, the earth has little noticeable affect on the sun, but astronomers use the motion of stars to discover invisible planet

28 28 On the Earth Weight = mass x gravity W = m g W = m (- 9.8 m/s 2 ) A person pulls on the earth as much as the earth pulls on the person The force caused by gravity (weight) causes falling objects to accelerate at at rate of 9.8 m/s 2 downward F = m a = W = m g a = g = m/s 2 on the earth’s surface

29 29 Practice A tractor pulls a loaded wagon with a mass of 275 kg on a level road with a constant force of 440 N, as shown below. (a) What is the acceleration of the wagon? (b) What would the acceleration of the wagon be if there was an opposing frictional force of 140 N? (c) Suppose the wagon starts from rest (with friction). How far will the wagon travel in 4.0 s?

30 30 Calculations a) F = ma a = F/m = 440N/275 kg =1.60 N/kg 1.60 N/kg (kg m/s 2 / N) = 1.60 m/s 2 b) F = F tractor – F Friction F = 440N – 140 N = 300 N a = F/m = 300N/275kg = 1.09 m/s 2 c) x = x 0 +v 0 t +at 2 /2 x = (1.09 m/s 2 ) *(4s) 2 /2 x = 8.72 m X0X0 X

31 31 Practice A student weighs 588 N on the surface of the earth. What is her mass? What would be her mass on the moon? What would be her mass at the bottom of the ocean?

32 32 Calculations W = mg m = W/g = 588 N / 9.8m/s 2 m = 60 kg (about 132 pounds) –1 kg has a weight of 2.2 pounds on the surface of the earth –Her mass is 60 kg on the Moon, at the bottom of the ocean, on Mars… –Mass does NOT change with location

33 33 Practice In a college homecoming competition, 15 students lift a sports car. While holding the car off the ground, each student exerts an upward force of 420 N. (a) What is the mass of the car in kilograms? (b) What is the weight in pounds?

34 34 Calculations Total upward force = 15 x 420 N F = 6,300 N W = mg m = W/g = 6300N / 9.8m/s 2 m = 643 kg W = 643 kg (2.2 pounds/kg) on earth’s surface W = 1,415 pounds

35 35 Practice In an emergency stop to avoid an accident, a shoulder-strap seat belt holds a 50-kg passenger firmly in place. If the car were initially traveling at 80 km/h and came to a stop in 6 s along a straight, level road, what was the average force applied to the passenger by the seatbelt? Suppose the time is reduced to.5 s?

36 36 Calculations Find velocity in m/s 80 km/hr (1000m/km)(1hr/3600s)= 22.2m/s v = v 0 + at 0 = 22.2m/s + a 6s a = -22.2m/s / 6s = -3.7 m/s 2 F = ma = 50 kg (-3.7m/s 2 ) = -185 N –Minus indicates the force acts in a direction opposite of the initial velocity a = -22.2m/s /.5 s = m/s 2 F = ma = 50 kg (-44.4m/s 2 ) = N F = -493 pounds for a fast stop!

37 37 Introduction In the previous lessons, you learned what a force is because you learned the connection between force and acceleration. In this lesson, you will study why forces exist and where they come from. The law of action and reaction will also be examined here.

38 38 Newton’s Third Law Newton’s second law says F = ma Newton’s third law says the forces come from other objects Your muscles (first object) push the crate (second object), but that crate pushes back just as hard

39 39 Newton’s Third Law Newton’s third law of motion: For every action there is an equal and opposite reaction. In other words, for every force, there is an equal and opposite force. In notation form, the law is written as follows: F 12 = – F 21

40 40 Pairs of Forces When an object exerts force on another object, the second object exerts an equal force at the same time on the first object. Objects interact in pairs; and the interacting forces come in equal and opposite pairs.

41 41 Free Fall When the briefcase is released, there is an unbalanced, or nonzero net force acting on the briefcase (its weight force,) and it accelerates downward at g or -9.8m/s 2 for free fall

42 42 Action-Reaction Both skateboarders move toward the center point

43 43 Paired Forces The third law is illustrated with any kind of propulsion. When you walk, for example, your muscles exert a horizontal force against the ground and the ground exerts an equal and opposite horizontal force against you, which propels you in the direction you are walking.

44 44 Jet Propulsion In this case, the action-reaction pair is the force of the hot gases on the plane propelling the plane forward and the force of the plane on the hot gases ejecting the gases backward.

45 45 Finding Forces The diagram shows two blocks m 1 and m 2 of masses 2.5 kg and 3.5 kg, respectively, resting on a frictionless surface. A force of 12 N acts on m 1, which tautens the massless string connecting the two masses. As a result, the string exerts a force on m 2. Therefore, both masses accelerate. What is the acceleration of the system, and what is the force that the string exerts on m 2 ?

46 46 Calculations For the system of masses F = ma 12 N = (2.5kg + 3.5kg) a a = 12 N / (6 kg) = 2.0 m/s 2 For the second mass F = ma F = 3.5 kg 2.0 m/s 2 = 7 N

47 47 Action and Reaction m 2 pulls back on m 1 with the same force a m 1 pulls forward on m 2 The net force on m 2 = 7N and the net force on m 1 = 12N – 7N = 5 N –If m 1 were alone, only 5N would be needed to accelerate it at 2.0m/s 2 F = ma = 5N = 2.5 kg 2 m/s 12N -7N7N

48 48 Force A car traveling at 72.0 km/h along a straight, level road comes uniformly to a stop at a distance of 40.0 m. If the car weighs 8800 N, what is the breaking force?

49 49 Calculations F = ma – need both m and a v 2 -v 0 2 =2a(Δx) now this is very useful 72km/hr (1000m/km)(1hr/3600s)=20m/s 0 - (20m/s) 2 = 2 a 40m a = 5 m/s 2 W = 8800 N = m 9.8m/s 2 m = 898kg F = ma = 898kg 5m/s = 4490 N

50 50 Normal Force The diagram shows a block resting on a table. The table is exerting an upward force on the block that is perpendicular to the surface of the table. This is called the normal force because normal means perpendicular. The weight of the block is equal to the normal force because the block is in equilibrium.

51 51 Normal Force The normal force is a contact force and is the force of the table pressing up on the block It is paired with the force of the block pressing down on the table due to gravity

52 52 Inclined Plane Problems Set up a new axis pair that is perpendicular and parallel to the plane W=mg Θ Θ mgsin Θ mgcos Θ

53 53 Inclined Plane Geometry – the angle of inclination is the same as the angle between gravity and the perpendicular to the plane (normal) W=mg Θ Θ mgsin Θ mgcos Θ

54 54 Angle Details Θ Θ mgcos Θ Φ Φ 90

55 55 Slide Down the Plane With no friction, a block will slide with constant acceleration W=mg Θ Θ mgsin Θ mgcosΘ N = mgcosΘ

56 56 Normal Force N = mgcos Θ The plane balances the component of the weight perpendicular to the plane with N

57 57 Typical Problem If m = 35 kg, find acceleration down the 25º plane W=mg Θ Θ mgsin Θ mgcos Θ

58 58 Typical Problem If m = 35 kg, find acceleration down a 25º plane 35 kg 9.8m/s 2 Θ Θ 35 kg 9.8m/s 2 sin25º 35 kg 9.8m/s 2 cos25º

59 59 Find Acceleration F = ma 35 kg 9.8m/s 2 sin25º = 35 kg a a = 35 kg 9.8m/s 2 sin25º / 35 kg a = 4.14 m/s 2 Acceleration is constant Velocity is increasing at a constant rate while the object slides down the plane Acceleration is independent of the mass of the object AND is less than g!

60 60 Frictionless Inclined Plane Two masses m 1 and m 2 are connected by a light string running over a light pulley. The pulley offers negligible friction. Mass m 1 (Mass = 5.0 kg) is on a frictionless 20° inclined plane. Mass m 2 (Mass = 1.5 kg) is freely suspended. What is the acceleration of the masses?

61 61 Force Diagrams

62 62 Forces F = ma – What is the total force used to accelerate BOTH objects? F = W – m 1 gsin Θ = m 2 g – m 1 gsin Θ F = 1.5kg9.8m/s 2 – 5kg 9.8m/s 2 sin20º F = -2.06N a = F/m = -2.06N/(1.5kg+5kg) = -.32m/s 2 The mass on the plane will slide down the plane and drag the mass on the pulley up

63 63 Components of Force A force of 10.0 N is applied at an angle of 30° to the horizontal on a 1.25-kg block at rest on a frictionless surface. (a) What is the magnitude of the resulting acceleration of the block? (b) What is the magnitude of the normal force? The space diagram displays all the forces acting on the block and the free-body diagram displays the block as a point mass. The x-axis is along the table surface because motion is along that direction.

64 64 Calculations W = mg = 1.25kg (–9.8m/s 2 ) = N F x = 10N cos30º = 8.66 N F y = 10N sin30º = -5N (down) N = 12.25N + 5N = 17.25N (vertical) F = ma (horizontal) a = F / m a = 8.66N / 1.25 kg a = 6.93 m/s 2

65 65 Equilibrium

66 66 Equilibrium Equilibrium is the state where the object is at rest or at constant velocity because the net force acting on it is zero. Therefore, in equilibrium, in the diagram, the woman is in a state of static translational equilibrium because she is at rest. An object moving at constant speed is in translational equilibrium.

67 67 Practice Jane and John, with masses of 50 kg and 60 kg, respectively, stand on a frictionless surface 10 m apart. John pulls on a rope that connects him to Jane, giving Jane an acceleration of 0.92 m/s 2. At what rate will John accelerate? What is the direction of his acceleration?

68 68 Calculations F = ma = 50kg.92m/s 2 = 46 N on the Jane This is the same force that is exerted back on John F = ma = 46N = 60kg a a = 46N / 60 kg =.767 m/s 2 = boy’s acceleration The more massive object has less acceleration, but the forces are the same

69 69 Practice A boy pulls a box of mass 30 kg with a force of 25 N at angle of 30º from the horizontal (a) Ignoring friction of the box, what is the acceleration of the box? (b) What is the normal force exerted on the box by the ground?

70 70 Calculations F x = 25N cos(30º) = 21.7 N F y = 25N sin(30º) = 12.5 N N = 12.5N – 30kg9.8m/s 2 = -282N –Not enough to overcome weight, so moves in horizontal direction F = ma a = 21.7N/30kg a =.723 m/s 2 294N 282N 21.7N 12.5N

71 71 Practice The Atwood machine consists of two masses suspended from a fixed pulley. If m1 = 0.5 kg and m2 = 1.0 kg, (a) What is the acceleration of the system (b) What is the magnitude of the tension in the string?

72 72 Atwood Machine

73 73 Atwood Machine The tension is the same at both ends Acceleration is the same on both blocks but opposite in direction T W=m 1 g m1m1 m2m2 T W=m 2 g

74 74 Calculations F = ma – Total force accelerating both objects F = m 2 g-m 1 g = (m 1 +m 2 ) a 1kg 9.8m/s 2 -.5kg 9.8m/s 2 = (1.5kg) a a = (4.9 kg m/s 2 ) / 1.5 kg a = m/s 2 T = mg + ma T =.5kg 9.8m/s 2 +.5kg m/s 2 T = N on string to m 1

75 75 Check If T = 6.54 N, F m1 = T - W = 6.54 N N F m1 = 1.634N UP a = N/.5kg a = 3.27 m/s 2 UP F m2 = T - W F m2 = N – 9.8 N a = 3.27 N/ 1kg DOWN a = 3.27 m/s 2 DOWN T W=m 1 g m1m1 m2m2 T W=m 2 g

76 76 Equal Masses If the masses are the same: m 1 g = m 2 g There is no net force There is no acceleration There is NO MOTION The blocks do not change position Starting heights do not matter T W=m 1 g m1m1 m2m2 T W=m 2 g

77 77 Friction Friction is the force that dictates many of our daily activities. It is because of the force of friction that you take small steps on a slippery surface and press down on a piece of paper when writing with a pencil. It is friction that prevents you from moving heavy objects and hurts your joints in old age. This lesson covers the various types of friction and what determines the force of friction.

78 78 Friction Opposes Motion When you slide a file cabinet across the floor, the force of friction acts opposite to the motion of the heavy object. The force of friction ALWAYS points in the direction opposite to the direction of the external force. The attraction between the molecules of the two surfaces gives rise to the force of friction.

79 79 Friction The attraction between the molecules of the two surfaces gives rise to the force of friction. In addition, any surface roughness can contribute to friction as the sliding object must go up (and down). The force of friction opposes motion. The force of friction points opposite the direction of motion

80 80 Static and Kinetic Friction STATIC BIG – KINETIC SMALL It takes a big force to get a still object to start moving – you have to overcome static friction Once it is moving, the same force is more than needed to over come kinetic friction You can apply less force and get constant velocity, or keep the same force and get constant acceleration

81 81 Static and Kinetic Friction

82 82 Coefficients of Friction The force of friction is proportional to the force pressing the surfaces together (the Normal force) F Friction = μ F Normal μ is the coefficient of friction μ Static is used if the object is stationary μ Kinetic is used if the object is moving μ Static is big, μ Kinetic is small

83 83 Big Small

84 84 Friction Force The force of friction is directly proportional ONLY to the Normal force AND the coefficient of friction F Friction does NOT depend on the surface area F f = μ N where μ is the coefficient of friction You must know μ and N (F Normal, F N,…) to calculate friction Use Static Friction if the object is stationary Use Kinetic Friction if the object is moving

85 85 Practice What is the force needed to keep a mass of 158 kg moving horizontally across a level floor if the coefficient of kinetic friction is.27? (No acceleration, force is horizontal) F mg μNμN N

86 86 Calculation F friction = μN N = mg = 158 kg 9.8m/s 2 N = 1,548 N F friction = μN F friction =.27 x 1,548 N F friction = 418 N

87 87 Practice The coefficient of static friction between the 40.0-kg crate and the floor is What minimum horizontal force must the worker apply to move the crate? If the worker maintains the force once the crate starts to move and the coefficient of kinetic friction between the surfaces is 0.500, what is the magnitude of the acceleration of the crate?

88 88 Calculations W = mg W = 40kg(- 9.8m/s 2 ) W = -392 N N = +392N f s = μ s N f s =.650 x 392N f s = 255N This is the force needed to start motion

89 89 Maintain Motion 255N is applied even after the crate starts to slide f k = μ s N f s =.500 x 392N = 196N F = ma = 255N – 196N = 59 N a = F / m = 59 N / 40 Kg = 1.48 m/s 2 in the direction of the applied force Acceleration is constant Velocity increases at a steady rate

90 90 Terminal Velocity An object moving through the air meets air resistance that opposes motion Air resistance is very complicated, but it increases with velocity Eventually, an object in free fall has enough air resistance to balance the pull of gravity An object reaches terminal velocity when air friction balances gravity: acceleration is zero and velocity remains constant

91 91 No Friction vs Friction

92 92 Friction increases with velocity

93 93 Practice A packing crate is placed on a plane inclined at an angle of 35 o from horizontal. If the coefficient of static friction between the crate and the plane is 0.65, will the crate slide down the plane? Justify your answer.

94 94 Slide Down the Plane W=mg Θ Θ mgsin Θ mgcos Θ N ff=μNff=μN

95 95 Calculations Is the force down the plane greater than the force of friction? Is mgsin Θ > μmgcosΘ ? Is sin Θ > μ cosΘ ? Is sin35º >.65 cos35º Is.573 >.532 => Yes, so crate slides down the plane, no matter what the mass is or acceleration due to gravity

96 96 Slide Down the Plane Find μ if a = 0 W=mg Θ Θ mgsin Θ mgcos Θ N ff=μNff=μN

97 97 Calculations to find μ If the object slides down the plane with no acceleration, find μ N = mgcos Θ μ N = mgsinΘ μ mgcos Θ = mgsinΘ μ = mgsinΘ / mgcos Θ μ = sinΘ / cos Θ μ = tanΘ Note: This is independent of the mass, g, shape of the object, etc.

98 98 No Math The slope of an inclined plane is increased until a crate slides down the plane Describe the motion of the crate after it starts moving

99 99 Reasoning The slope is increased until the component of gravity down the plane is just barely greater than the force of static friction This same force than is much bigger the force of kinetic friction which opposes motion as soon as the crate moves The object will accelerate down the plane with a constant acceleration less than g Velocity will increase at a steady rate

100 100 Summary What is the net force acting on an object? What is inertia and Newton’s first law of motion? What is Newton’s second law of motion? What is Newton’s third law of motion?


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