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CHAPTER 2 – MOTION.

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Presentation on theme: "CHAPTER 2 – MOTION."— Presentation transcript:

1 CHAPTER 2 – MOTION

2 GOALS 1. Distinguish between instantaneous and average speeds. 2. Use the formula v = d/t to solve problems that involve distance, time, and speed. 3. Distinguish between scalar and vector quantities and give several examples of each. 4. Use the Pythagorean theorem to add two vector quantities of the same kind that act as right angles to each other. 5. Define acceleration and find the acceleration of an object whose speed is changing. Use the formula v = v + at to solve problems that involve speed, acceleration, and time. 1 7. Use the formula d = v t + ½ at to solve problems that involve distance, time, speed, and 2 acceleration. 8. Explain what is meant by the acceleration of gravity. 9. Describe the effect of air resistance on falling objects. 10. Separate the velocity of an object into vertical and horizontal components in order to determine its motion. 11. Define force and indicate its relationship to the first law of motion. 12. Discuss the significance of the second law of motion, F = ma. 13. Distinguish between mass and weight and find the weight of an object of given mass. 14. Use the third law of motion to relate action and reaction forces. 15. Explain the significance of centripetal force in motion along a curved path. 16. Relate the centripetal force on an object moving in a circle to its mass, speed, and the radius of the circle. 17. State Newton's law of gravity and describe how gravitational forces vary with distance. 18. Account for the ability of a satellite to orbit the earth without either falling to the ground or flying off into space. 19. Define escape speed.

3 Motion Everything in the universe is in nonstop motion
The laws of motion that govern the behavior of atoms and stars apply just as well to the objects of everyday life Motion is the ability of an object to move from one place to another The first step in analyzing motion is to describe how fast or slow the motion is

4 Motion SPEED Rate at which something covers distance
Speed is distance divided by time v = speed d = distance t = time

5 Speed Example 2.1 A car going 40 miles/hour in a 6 hour period travels how far? v = 40 mi/hr t = 6 hours d = v x t 240 miles This is an average speed. The speedometer of a car shows an instantaneous speed.

6 Vector Quantities Vectors have direction as well as magnitude
They tell us “which way” as well as “how much” velocity (v) and force (F) are examples An arrowed line that represents the magnitude and direction of a quantity is called a vector

7 Vector Quantities have Direction And Magnitude
Vector v is 40 km/s to the right Tam2s6_3 Figure 2-4

8 Vectors can be Added Figure 2-5 Tam2s6_4

9 Adding Vectors Besides manually measuring the length of “C” as in the previous slide, vectors can be added using the Pythagorean theorem when you have a right angle triangle More accurate than using a scale drawing a2 + b2 = c2

10 Using the Pythagorean theorem
Example 2.3 – use the Pythagorean theorem to find the displacement of a car that goes north for 5 km and then east for 3 km, as in Fig. 2-5

11 Scalar Quantities Need only a number and a unit; Not direction
mass (m) speed (v)

12 Vector and Scalar Quantities
Vector quantities are printed in boldface type Scalar quantities are printed in italic type.

13 Acceleration A change in velocity or direction (Curved Path)
Acceleration, in general, is a vector quantity For our purposes, we will be calculating straight line motion, where acceleration is the rate of change of speed (a scalar quantity) SI units are m/s2 It is customary to write (m/s)/s as just m/s2 since

14 Acceleration a=acceleration v2=final speed v1=initial speed t=time

15 Acceleration Example 2.4 Figure 2-8
The speed of a car changes from 15 m/s to 25 m/s in 20 s when its gas pedal is pressed hard. Find its acceleration. Figure 2-8 Tam2s6_6

16 Acceleration Example 2.4 = 0.5m/s2

17 Free Fall Galileo Galilei ( ) – Italian physicist who discovered that the higher a stone is when dropped, the greater its speed when it reached the ground

18 Free Fall This means the stone is accelerated
Acceleration is the same for all stones, big or small Galileo’s experiments showed that if there were NO AIR for them to push their way through, all falling objects near the Earth’s surface would have the same acceleration of 9.8 m/s2

19 Free Fall In general, the speed of an object falling from rest can be calculated as Vdownward = g t v=downward speed g=acceleration due to gravity t=time

20 How Far does a Falling Object Fall?
To find out how far, h, the object has fallen in the time, t, use h=½ g t 2 t2 factor means the “h” increases much faster than the object’s speed “v”

21 Example 2.7 A stone dropped from a bridge strikes the water 2.2 s later. How high is the bridge above the water? Using this formula, you can figure the height of a bridge over water using just a stop watch

22 Distance Traveled when Accelerating
When starting from rest it is D= ½ at2 If tossed vertically h = ½ gt2 When starting with an Initial Velocity v1 D = V1 t + ½ at2 If falling due to gravity, a becomes g ( 9.8m/s2 )

23 Air Resistance Keeps falling things from developing the full g
In air, a stone falls faster than a feather because air resistance affects the stone less In a vacuum, the stone and feather fall with the same acceleration (9.8m/s2) Air resistance increases with speed until the object cannot go any faster It then continues to fall at a constant terminal speed that depends upon the size, shape, and weight

24 Free Fall at terminal Velocity
If a sky diver is falling at a constant velocity i.e, her terminal velocity, and weighs 400N, What is the force exerted by the AIR on the skydiver? If the sky diver rolls into a ball, would the force be different?

25 Vacuum vs. Air Resistance
tam2s6_12 Figure 2-15

26 Force and Motion What makes something at rest begin to move?
Why do some objects move faster than others? Why are some accelerated and others not? Questions like these led Isaac Newton to formulate three principles that summarize behavior of moving bodies

27 Force and Motion These are known as Newton’s Three Laws of Motion

28 Force and Motion Newton’s First Law of Motion
If no net force acts on it, an object at rest remains at rest and an object in motion remains in motion at constant velocity (that is, at constant speed in a straight line) An object at rest never begins to move all by itself-a force is needed to start it off If an object is moving, the object will continue going at constant velocity unless a force acts to slow it down, speed it up, or change its direction Only a Net Force Can Accelerate an Object

29 Force, Inertia, Mass Force is defined as any influence that can change the speed or direction of motion of an object SI unit of force is the Newton (N) Inertia is the reluctance of an object to change its state of rest or of uniform motion in a straight line Mass is the property of matter that shows itself as inertia The more mass something has, the greater its inertia and the more matter it contains SI unit of mass is the kilogram (kg)

30 Inertia Figure 2-19 Tam2s6_15

31 Force and Motion Newton’s Second Law of Motion
Force is equal to the product of mass and acceleration of an object The direction of the force is the same as that of the acceleration F = Force (SI unit is the Newton which is a (kg)(m / s2) m=mass (SI unit is the kilogram (kg)) a=acceleration (SI unit m/s2)

32 Newton’s Second Law of Motion
Twice the force means twice the acceleration When the same force acts On different masses, the Greater mass receives the Smaller acceleration Figure 2-22 Tam2s6_17

33 Mass and Weight Weight Force with which something is attracted by the earth’s gravitational pull. Weight is a force; if you weigh 150 lbs, the Earth is pulling you down with a FORCE of 150 lbs Although weight and mass are very closely related, weight is different from mass Mass refers to how much matter something contains

34 Calculating Weight w = mg Newton’s second law of motion says F=ma
In the case of an object at the Earth’s surface, the force gravity exerts on it is its own weight So, substituting w for F and g for a in the F=ma equation leads to: w = mg weight = (mass) (acceleration of gravity) w = weight m = mass g = acceleration of gravity

35 Weight Weight and mass are always proportional to one another
Twice the weight means twice the mass Mass rather than weight is normally specified in the SI system SI system unit for weight is the Newton, since weight is a force

36 Weight The weight of 5 kg of potatoes is:
w=mg = (5kg)(9.8m/s2)=49 (kg)(m/s2)=49 N Mass is a more basic property than weight since the pull of gravity vary from place to place Pull of gravity is less on a mountaintop than at sea level, less at the equator than near the poles (earth bulges at equator) Mass remains the same no matter where you are in the universe Weight changes depending where you are in the universe, since g changes

37 Force and Motion Newton’s Third Law of Motion
When one object exerts a force on a second object, the second object exerts an equal force in the opposite direction on the first object Another way to state this is for every action force there is an equal and opposite reaction force This law is responsible for walking-as you move forward the Earth is moving backward Recoil of a canon Action of a rocket

38 Newton’s Third Law of Motion
Figure 2-27 Tam2s6_21

39 Circular Motion Before we consider how gravity works, we must look into exactly how curved paths come about Planets orbit the sun in curved paths, not straight lines A curved path requires an inward pull known as centripetal force

40 Centripetal Force The velocity vector v is always tangent to the circle and the centripetal force vector Fc is always directed toward the center of the circle Figure 2-31 Tam2s6_23

41 Centripetal Force Centripetal force (Fc) is calculated using the following equation where: m = mass v = velocity r = radius of circle

42 What Happens to Centripetal Force when
Mass, Velocity, and Radius are changed? Figure 2-32 Tam2s6_24

43 Centripetal Force Example 2.10
Find the centripetal force needed by a 1000-kg car moving at 5 m/s to go around a curve 30 m in radius m= 1000 kg v= 5 m/s r= 30 m 833 N

44 Centripetal Force Example
Figure 2-33 Tam2s6_25

45 The slaying of the giant
David was told there was a giant needing slain He selected his 1.0 m sling and his best smooth flat river rock weighing .35 kg He knew his accuracy suffered if the centripetal force on the sling was more than 80 pounds ( made his arm tired ) How fast can he launch the stone at the giant? What was the kinetic energy of the stone

46 Newton’s Law of Gravity
Newton arrived at the Law of Gravity that bears his name using Kepler’s 1st and 2nd laws and Galileo’s work on falling bodies Every object in the universe attracts every other object with a force proportional to both of their masses and inversely proportional to the square of the distance between them

47 Newton’s Law of Gravity
R – distance between the objects G – Gravitational Constant of nature, the same number everywhere in the universe = 6.670 X N m2/kg2 m - mass of objects

48 Newton’s Law of Gravity
The inverse square – 1/R2 – means the gravitational force drops off rapidly with increasing R Figure 2-35 Tam2s6_26

49 Orbital Velocity All objects in orbit have a perfect balance of centripetal force and Gravitational Force Fc = mv2/ r Centripetal Force F = GMm/ r2 Gravitational Force Solving for v v= (GM/r)0.5

50 Weight and Distance Relationship
Figure 2-37 Tam2s6_28

51 The End

52 EXAMPLES

53 Ex. 2.1

54 Ex. 2.2

55 Ex. 2.3

56 Ex. 2.4

57 Ex. 2.5

58 Ex. 2.6

59 Ex. 2.7

60 Ex. 2.8

61 Ex. 2.9

62 Ex. 2.10

63 Ex. 2.11

64 Ex. 2.12

65 Ex. 2.13

66 Ex. 2.14

67 Ex. 2.15


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