Presentation is loading. Please wait.

Presentation is loading. Please wait.

Electrostatics Chapter 23 Week-1-2 What’s Happening Clicker use will start on Friday (maybe). Today we begin the study of charge with make-believe clickers.

Similar presentations


Presentation on theme: "Electrostatics Chapter 23 Week-1-2 What’s Happening Clicker use will start on Friday (maybe). Today we begin the study of charge with make-believe clickers."— Presentation transcript:

1

2 Electrostatics Chapter 23 Week-1-2

3 What’s Happening Clicker use will start on Friday (maybe). Today we begin the study of charge with make-believe clickers. NOTThere will NOT be a quiz this week. WILLThere WILL be a quiz next Friday. WebAssigns are now active.

4 Electricity Probable First Observation Electricity

5 Idiot! If lightening had actually traveled down the kite string, old Ben Franklin would have been toast! Probably never happened, but good story!

6 A Quick Experiment

7 History 600 BC  Thales of Miletos rubs amber (electron in Greek) with cat fur and uses it to pick up feathers. Important questions:  Why was he doing this?  Didn’t he have a job??  What happened to the skinned cat?

8 Amber Million years ago large stands of forests in some parts of the world began to seep globs of sticky resin! This aromatic resin oozed down the sides of trees, as well as filling internal fissures, trapping debris, such as seeds, leaves, feathers and insects. As geologic time progressed the forests were buried and the resin hardened into a soft, warm, golden gem, known as amber. Amber is the fossilized resin of ancient trees which forms through a natural polymerization of the original organic compounds. Most of the world's amber is in the range of 30-90 million years old.Amber

9 Demo – Lets make some observations Rubber Dead Cat or Rabbit Glass Wool NOT Shown: Aluminum Rods

10 Experimental Procedure Pivot The sequence of Experiments 1.Identify the two rods 2.Treat each rod 3.Bring one rod near to the other 4.PREDICT WHAT WILL HAPPEN 5.VOTE ON POSSIBILITIES 6.Observe what happens 7.Did we learn anything?

11 Predictions 1. Rods will attract each other 2. Rods will repel each other 3. Nothing will happen 4. Something not listed above will happen

12 Experiment #1 Pivot Rubber rod 1. Rods will attract each other 2. Rods will repel each other 3. Nothing will happen 4. Something not listed above will happen

13 Experiment #2 Pivot Rubber rubbed with skin of dead rabbit Rubber rubbed with skin of dead rabbit 1. Rods will attract each other 2. Rods will repel each other 3. Nothing will happen 4. Something not listed above will happen

14 Experiment #3 Pivot Glass rubbed with wool 1. Rods will attract each other 2. Rods will repel each other 3. Nothing will happen 4. Something not listed above will happen Glass rubbed with wool

15 What is the effect of DISTANCE??

16 Experiment #4 Pivot 1. Rods will attract each other 2. Rods will repel each other 3. Nothing will happen 4. Something not listed above will happen Glass rubbed with wool Rubber rubbed with skin of dead rabbit

17 What’s Going On? All of these effects involve rubbing two surfaces together. Or pulling two surfaces apart. Something has “happened “to each of these objects. These objects have a new PROPERTY Other properties are mass, color We call this NEW PROPERTY CHARGE.

18 From whence this charge ??? -+-+

19 Pivot Experiment #5 Rubber rubbed with skin of dead rabbit Metal Rod 1. Rods will attract each other 2. Rods will repel each other 3. Nothing will happen 4. Something not listed above will happen

20 Neutral Object Positive charge attracts negative charges. Rod becomes “polarized. Negative end is closer to positive charge Distance effect causes attraction.

21 Induction

22 Polarize

23 Ground

24 Remove Ground

25 Positive !

26 Balloon Physics

27 Same as before: Polarization

28 From WebAssign Three are brought close to each other, two at a time. When objects A and B are brought together, they attract. When objects B and C are brought together, they repel. From this, we conclude which of the following? (Select all that apply.) [_] Objects A and C possess charges of the same sign. [_] All three of the objects possess charges of the same sign. [_] One of the objects is neutral. [_] Objects A and C possess charges of opposite sign. [_] We need to perform additional tests to determine information about the charges on the object

29 Example PITH BALLS

30 Another Example

31 Example - Tape

32

33 Effect of Charge

34 We have also observed that there must be TWO kinds of charge. Call these two types positive (+) negative(-) We “define” the charge that winds up on the rubber rod when rubbed by the dead cat to be NEGATIVE. The charge on the glass rod or the dead cat is defined as POSITIVE.

35 What happens when two surfaces touch or rub? Bonding!

36 The Triboelectric Series No! When two of the following materials are rubbed together under ordinary circumstances, the top listed material becomes positively charged and the lower listed material becomes negatively charged. MORE POSITIVE rabbit's fur glass mica nylon wool cat's fur silk paper cotton wood acrylic cellophane tape polystyrene polyethylene rubber balloon saran wrap MORE NEGATIVE No!

37 Summary - Rubbings

38 What have we found? There are TWO types of charge. Positive Negative Like Charges Attract Un-Like charges repel The force between charges increases as they are brought closer together. This charge separation results from chemical bonds which are severe in the pocess.

39 Forces Between Charges Q1Q1 Q2Q2 AttractRepel ++X +-X -+X --X

40 Types of Materials Insulators “Holds” a charge Conductors Allows charge to easily move (current)

41

42 This is WAR You are fighting the enemy on the planet Mongo. The evil emperor Ming’s forces are behind a strange green haze. You aim your blaster and fire … but …… Ming the merciless this guy is MEAN !

43 Nothing Happens ! The Green thing is a Force Field ! The Force may not be with you ….

44 Side View The FORCE FIELD Force Position o |Force| Big!

45 Properties of a FORCE FIELD It is a property of the position in space. There is a cause but that cause may not be known. The force on an object is usually proportional to some property of an object which is placed into the field.

46 Fields Imagine an object is placed at a particular point in space. When placed there, the object experiences a force F. We may not know WHY there is a force on the object, although we usually will. Suppose further that if we double some property of the object (mass, charge, …) then the force is found to double as well. Then the object is said to be in a force field. The strength of the field (field strength) is defined as the ratio of the force to the property that we are dealing with.

47 Example – Gravitational Field. Property is MASS (m). Force is m g. Field strength is defined as Force/Property

48 The Gravitational Field That We Live In. m M mgmg MgMg

49 Coulomb’s Law – Force between charges The force between two charges is proportional to the product of the two charges and inversely proportional to the square of the distance between them.

50 Remember

51 Coulomb’s Law The Unit of Charge is called THE COULOMB Smallest Charge: e ( a positive number) 1.6 x 10 -19 Coul. electron charge = -e Proton charge = +e

52 Three point charges are located at the corners of an equilateral triangle as shown in Figure P23.7. Calculate the resultant electric force on the 7.00-μC charge.

53 Two small beads having positive charges 3q and q are fixed at the opposite ends of a horizontal, insulating rod, extending from the origin to the point x = d. As shown in Figure P23.10, a third small charged bead is free to slide on the rod. At what position is the third bead in equilibrium? Can it be in stable equilibrium?

54 The Electric Field

55

56 This is WAR You are fighting the enemy on the planet Mongo. The evil emperor Ming’s forces are behind a strange green haze. You aim your blaster and fire … but …… Ming the merciless this guy is MEAN !

57 Nothing Happens ! The Green thing is a Force Field ! The Force may not be with you ….

58 Side View The FORCE FIELD Force Position o |Force| Big!

59 Properties of a FORCE FIELD It is a property of the position in space. There is a cause but that cause may not be known. The force on an object is usually proportional to some property of an object which is placed into the field.

60 Mysterious Force F

61 Electric Field If a charge Q is in an electric field E then it will experience a force F. The Electric Field is defined as the force per unit charge at the point. Electric fields are caused by charges and consequently we can use Coulombs law to calculate it. For multiple charges, add the fields as VECTORS.

62 Two Charges

63 Doing it Q r q A Charge The spot where we want to know the Electric Field F

64 General-

65 Force  Field

66

67 Two Charges What is the Electric Field at Point P?

68 The two S’s S uperposition S ymmetry

69 What is the electric field at the center of the square array?

70 Kinds of continuously distributed charges Line of charge  or sometimes = the charge per unit length. dq=  ds (ds= differential of length along the line) Area  = charge per unit area dq=  dA dA = dxdy (rectangular coordinates) dA= 2  rdr for elemental ring of charge Volume  =charge per unit volume dq=  dV dV=dxdydz or 4  r 2 dr or some other expressions we will look at later.

71 Continuous Charge Distribution

72 ymmetry

73 Let’s Do it Real Time Concept – Charge per unit length  dq=  ds

74 The math Why?

75 A Harder Problem A line of charge  =charge/length setup dx L r   x dEdE dE y

76 (standard integral)

77 Completing the Math 1/r dependence

78 Dare we project this?? Point Charge goes as 1/r 2 Infinite line of charge goes as 1/r 1 Could it be possible that the field of an infinite plane of charge could go as 1/r 0 ? A constant??

79 The Geometry Define surface charge density  =charge/unit-area dq=  dA dA=2  rdr (z 2 +r 2 ) 1/2 dq=  x dA = 2  rdr

80 (z 2 +r 2 ) 1/2 

81 Final Result

82 Look at the “Field Lines”

83 What did we learn in this chapter?? FIELD We introduced the concept of the Electric FIELD. We may not know what causes the field. (The evil Emperor Ming) If we know where all the charges are we can CALCULATE E. E is a VECTOR. The equation for E is the same as for the force on a charge from Coulomb’s Law but divided by the “q of the test charge”.

84 What else did we learn in this chapter? We introduced continuous distributions of charge rather than individual discrete charges. Instead of adding the individual charges we must INTEGRATE the (dq)s. There are three kinds of continuously distributed charges.

85 Kinds of continuously distributed charges Line of charge  or sometimes = the charge per unit length. dq=  ds (ds= differential of length along the line) Area  = charge per unit area dq=  dA dA = dxdy (rectangular coordinates) dA= 2  rdr for elemental ring of charge Volume  =charge per unit volume dq=  dV dV=dxdydz or 4  r 2 dr or some other expressions we will look at later.

86 The Sphere thk=dr dq=  dV=  x surface area x thickness =  x 4  r 2 x dr dq

87 Summary (Note: I left off the unit vectors in the last equation set, but be aware that they should be there.)

88 To be remembered … If the ELECTRIC FIELD at a point is E, then E = F /q (This is the definition!) Using some advanced mathematics we can derive from this equation, the fact that:


Download ppt "Electrostatics Chapter 23 Week-1-2 What’s Happening Clicker use will start on Friday (maybe). Today we begin the study of charge with make-believe clickers."

Similar presentations


Ads by Google