static electricity

113
1 Static Electricity

Upload: judith

Post on 06-Jan-2016

28 views

Category:

Documents


2 download

DESCRIPTION

Static Electricity. What does the term static mean?. Not in motion. Electricity?. Involves electrons. Atomic model positively charged nucleus (protons) negatively charged electrons. Notation. - PowerPoint PPT Presentation

TRANSCRIPT

Page 1: Static Electricity

1

Static Electricity

Page 2: Static Electricity

What does the term static mean?

2

Not in motion

Electricity?

Involves electrons

Page 3: Static Electricity

3

Atomic model positively charged nucleus (protons)

negatively charged electrons

Page 4: Static Electricity

4

Outer Part Elementary Chargeelectrons e- –1

NucleusProtons p+ +1neutrons no 0

Neutral objects have same # p+ & e-.

Charged objects have net p+ or e-

Notation

Page 5: Static Electricity

When objects have excess or deficit of charge, can exert

electrostatic force.

5

Page 6: Static Electricity

6

When objects have excess or deficit of charge, can exert electrostatic force.

Page 7: Static Electricity

7

Charged objects supply a force.Proof?

Page 8: Static Electricity

8

In solids,

Charge transferred by e- only.

How can we get positive charge object?

Loss of e-.

Page 9: Static Electricity

Uncharged objects can feel electrostatic force too:

by polarization

9

Page 10: Static Electricity

10

PolarizationAtoms can be polarized by redistributing e-. Polarization is separation of charge not imbalance.

Page 11: Static Electricity

11

Charged balloon causes wall to become polarized.

Page 12: Static Electricity

12

Conservation Law applies to charge

Although charge ( e-) can be transferred, charge cannot be created or destroyed.

Sum of charges in system remains the same. For polarization the system is the balloon and the wall.

Page 13: Static Electricity

13

2 types of materials.

• Conductors – allow charges to move around – can be polarized.

• Insulators – hold excess charge in place – hard to polarize.

Page 14: Static Electricity

14

Conductors – materials that allow e- to move freely often redistribute charge.

Metals are good conductors.

Page 15: Static Electricity

15

Metal conductors distribute charge uniformly.

Page 16: Static Electricity

16

Insulators – charges do not move freely. Tend to stay concentrated

in one spot on object.

Page 17: Static Electricity

17

What’s happening here?

Page 18: Static Electricity

18

Water Stream

• Try at home.

Page 19: Static Electricity

19

Polarization produces only a surface charge.

Page 20: Static Electricity

20

Charging Objects:

• 1. Friction – rub 2 neutral objects together.

• Conduction - Contact with charged object.

• Induction – by bringing charged object in vicinity of neutral conductor.

Page 21: Static Electricity

21

Friction

Works for insulators and conductors.

Do objects get same or opposite charge?

Opposite!

Page 22: Static Electricity

Why you get a shock.

• Charge yourself transfer e- either to or from your body to neutralize your charge. Always accompanied by E release.

22

Page 23: Static Electricity

23

Conduction: touch charged object to neutral object.

Do objects get same or opposite charge?

SAME!

Page 24: Static Electricity

Static Electricity 9:15 min.

24

http://www.youtube.com/watch?v=A893_7FGMHY&feature=relmfu

Page 25: Static Electricity

25

Induction- – no touching of objects. Need to polarize & separate them.

Page 26: Static Electricity

26

Charging by induction conductors only.

A ground can serve as an infinite source or sink of e-.

Earth, your hand, floor, wall.

Page 27: Static Electricity

27

Charge an Electroscope by Induction

Page 28: Static Electricity

Charging By Induction 9:30 Min.

• http://www.youtube.com/watch?v=pJ36EtABLAk

28

Page 29: Static Electricity

Hwk Read Tx 17-1Answer pg 633 #1-2, 4-6

pg 654 #1-10 not 3Type or write it all including

questions.

29

Page 30: Static Electricity

How do we measure amount of charge?

30

1. Elementary Charge

Page 31: Static Electricity

Conductors will share elementary charges equally if they are allowed to touch.

Example:

1. The elementary charge of each metal sphere below is shown. If they are allowed to touch, and are then separated, what will be the charge on each?

+3 -6 -9

Page 32: Static Electricity

Total charge 3 – 6 – 9 = - 12

They will share the total charge so - 12/3 spheres = -4 charges each.

Page 33: Static Electricity

33

Determining Charge on electron.

Page 34: Static Electricity

34

1909 Robert Millikan measured charge on e-

Page 35: Static Electricity

Millikan 1:15

http://www.youtube.com/watch?v=XMfYHag7Liw

35

Page 36: Static Electricity

36

Robert Millikan found charge is quantized. There is a smallest unit of charge.

Charge can only exist in whole number integers of the charge on 1e-. Cannot have in between numbers.

Page 37: Static Electricity

Can an object have a charge of 3.53 x 10-19C?

• No.

• 3.53 x 10-19C ÷ 1.6 x 10-19 C = 2.2.

• Charges must be whole number integrals of 1.6 x 10-19 C .

37

Page 38: Static Electricity

38

Units of charge = coulombs (C) Charge on e- is -1.6 x 10-19 C

Charge on p+ is +1.6 x 10-19 C

or can consider fundamental units e- has charge –1p+ has charge +1

Charge Units

Page 39: Static Electricity

39

It takes 6.25 x 1018 elementary charges (e- or p+) to carry 1 C of charge.

Take the inverse of 1.6 x 10-19C.

Page 40: Static Electricity

2. What would be the charge on an object with 2.2 x 1015 excess electrons?

3.52 x 10-4 C

Page 41: Static Electricity

3. How many protons does it take to carry 0.001 C of charge?

6.25 x 1015 p+

Page 42: Static Electricity

42

4. What is the total charge (in C) on 6.2 x 108 electrons?

• 9.9 x 10 -11 C

Page 43: Static Electricity

5. A metal sphere with an excess of 2 x 109 electrons is connected to a sphere with a deficit of 1 x 109 electrons.

• What is the charge in Coulombs on each sphere before they’re connected?

• What is the charge in Coulombs on each after they’ve been connected?

Page 44: Static Electricity

44

Electrostatic Force

Charles Coulomb measured force exerted on one charged object by another.

He used torsion balance.

Page 45: Static Electricity

45

Coulomb’s Torsion Balance

Page 46: Static Electricity

46

Coulomb’s Law Relates Force btw. 2 charged objects.

Fe = kq1q2 r2

k = constant 8.99 x 109 N m2/C2. q charge on obj in Coulombs (C)r is dist in meters.F is force (N)

Page 47: Static Electricity

Ex 1: An alpha particle is a nucleus with 2 protons and 2 neutrons. It is near a proton.

1. What is the charge in Coulombs of each?

2. They are separated by a distance of 3 nm. What is the force between them?

3. Is the force repulsive or attractive?47

Page 48: Static Electricity

• nucl = 3.2 x 10-19 C.

• p+ = 1.6 x 10-19 C.

• F = 5.11 x 10-11 N

48

Page 49: Static Electricity

2: Two protons are 0.025 m apart. Calculate:

a) the gravitational attraction between them.

B) the electrostatic force between them.

C) what is the ratio between the forces.

D) What do you think the sign + or – indicates for electrostatic force?

Page 50: Static Electricity

Hwk read text 17 -2 and pg 634 – 636

• Do pg 636 #1-4 and pg 654 #1, 2, 6, 10.

50

Page 51: Static Electricity

Textbook ProbsHwk read 17 -2 and pg 634 – 636

Read 634 – 636. Peruse example prb.

Do:

•Pg 636 # 1 – 4 Show equations and work.

•& pg 655 #16-19.

51

Page 52: Static Electricity

52

Mech Universe “Static Electricity”

Page 53: Static Electricity

53

Electric Fields

Page 54: Static Electricity

Electric Fieldsregion of space around charged

object where a “test charge” feels an electrostatic force.

Page 55: Static Electricity

55

Electric Fields-Charge alters space around it. Charged objects feel a force.

Either repulsion or attraction.

Page 56: Static Electricity

Electric Field (E) defined as:The force and direction a small positive “test” charge feels in presence of field created by a larger charge Q.

E = F/q.

E = Electric Field (N/C)F is force on test charge (N).q is amt of charge on test charge (C).

Page 57: Static Electricity

Ex 1: A charge of 2 C feels a force of 10 N in an electric field. What is the field strength at that point.

E = F/q. = 10 N

2 C

E = 5 N/C

Page 58: Static Electricity

 Ex 2: How much force does a test charge with + 0.4 C feel in a field of 8 N/C?

• E = Fe/q

• Fe = qE

• 0.4 C x 8 N/C = 3.2 N.

58

Page 59: Static Electricity

59

Ex 3. An electron is placed in a field of 100 N/C.

a. What is the force on the electron?

b. What is the acceleration of the electron?

Page 60: Static Electricity

60

Electric Field Strength is Inversely Proportional to Distance Around a

Point Charge.

Page 61: Static Electricity

Sketching Electric Fields

• Do Now

61

Page 62: Static Electricity

Field Lines represent electric fields.

Electric field lines show the force that a small positive test charge feels in a field created by a much larger charge. They represent the strength and direction of the field.

Page 63: Static Electricity

63

Sketch vectors to show force magnitude& direction on a + test charge at each point.

+

Page 64: Static Electricity

64

Field around positive object.

Page 65: Static Electricity

65

Page 66: Static Electricity

66

The denser the field lines are, the stronger the field.

Stronger field near charge.

Page 67: Static Electricity

67

What are the field lines now?

Page 68: Static Electricity

68

Page 69: Static Electricity

69

What if field was formed between parallel plates? Sketch it.

+++++

-----

Page 70: Static Electricity

70

Field Between Parallel Plates

How would the strength of the field vary if a charge moves from the + to the – plate?

Page 71: Static Electricity

71

Fields have strength and direction.

Density of lines shows strength.Direction shown as arrows.

Direction is determined by a + test charge.

Electric Field lines don’t touch or cross.

Lines start on + end on neg.

Page 72: Static Electricity

Electric field due to more than one charge.

Field is stronger near the larger charge. Density of lines show the increased

strength.

Page 73: Static Electricity

E field due to more than one charge.

Force due to more than one charge is the vector sum of all the forces on a charged particle.

Page 74: Static Electricity

Electrostatic Equilibrium

Fields produced by more that a single charge will have spots where the forces on a charge in the field will be balanced.

F net = 0.

Page 75: Static Electricity

Film Mech Universe E fields.15 minutes.

75

Page 76: Static Electricity

76

• Review Elec Field youtube lesson kahn.

• http://www.youtube.com/watch?v=vaDT4GwAZ2I&feature=relmfu

Hwk elect field wksht andAnd Rev book 206 #2, 4, 7,9,

10-15, 24-25, 30-34

Page 77: Static Electricity

Work & EnergyElectric Potential

Page 78: Static Electricity

Do Now.

• 1. Define gravitational PE.

• 2. How is Energy related to work. Explain.

78

Page 79: Static Electricity

• Coulomb’s Law between 2 charged objects:

Fe = kq1q2.

r 2

• As region of space.

• Electric Field

Fe = qE

79

We discussed Force due to charges in 2 ways?

Page 80: Static Electricity

• What is the definition of Energy?

• Things that have E can do work.

• When work is done on an object it gains energy.

80

Do Charged particles in an electric field can have Energy?

Page 81: Static Electricity

Voltage Potential

81

Page 82: Static Electricity

It takes work to move charges in a field.

82

Where does a positive test charge have more PE – close to or far from a large positive sphere?

++

Page 83: Static Electricity

83

The amt of work done on every coulomb of charge moving it is called electric potential, V.

V = W/q. W work in Jq is charge in C.V is Volts = J/C.

V defines the potential at P at a point.

P is like a particular height in a gravity field.

Page 84: Static Electricity

Ex 1. It takes 150 x 10-6 J to move a 2.0 C charge to point P. What is the electric potential (voltage) at P?

V = W/q = 150 x 10-6J = 75 V

2 x 10-6C

How much PE did every C of charge gain?

75 J

Page 85: Static Electricity

85

To find PE or work done by E field:

Since W = PE and V = W/q:

PE elc = qV also W = qV.

PE – JoulesQ – CoulombsV = Volts

Page 86: Static Electricity

Ex 2. The electric potential at point P is 12.0 V.

A 3C charge is placed at P. What is the PE of q at P?

PE = W = qV

(3 C)(12 V) = 36 J

Page 87: Static Electricity

87

Ex 2b. If q = -2 C is moved to a point P = 12 V, What is the PE of q?

PE = qV

• (-2 C)(12 V) = -24 J

• q lost PE, the field did work on it. Think of the charge as falling.

Page 88: Static Electricity

Potential DifferenceVolage Dif betw 2 points in field ~ heightEnergy Dif involves moving charge in field = qV

A = 13 VB = 28 V

pd = 28V – 13V = 15 V.

Page 89: Static Electricity

89

Potential Difference in a Uniform Field.

The field intensity F/q between plates is constant, the work done (Fd) to move a charge

between plates is constant, the potential difference (voltage) is constant.

Page 90: Static Electricity

Ex 3: What work must be done to move a +5 C charge from the – to the + plate in the 250 V pd across plates?

W = q V = (5 x 10-6C)(250 J/C - 0)

= 1.25 x 10-3J.

250 V

It helps to assume 1 plate is 0, the other is 250 Volts.

250 0 V

Page 91: Static Electricity

Moving Charges in Fields.

As a charge moves thru a field, its total E (the E) is constant. By consv of Energy.

If a charges “falls” toward the oppositely charged plate its PEelc decreases, What increases?

KE

Page 92: Static Electricity

Is acceleration between parallel plates uniform? Explain.

• Work done by field will accelerate charge: W = KE = qV.

• So: before after

• ET = ET .

92

Page 93: Static Electricity

93

Uniform Electric FieldsParallel Plates

Page 94: Static Electricity

94

There is a potential difference – voltage between the two plates based on their charge & distance between them.

A +q near the positive plate is at a high potential (E).

What is the potential of a proton stuck to the negative plate? (0)

Page 95: Static Electricity

9595

How can I calculate PE of a mass in a gravity field?

• PEg = mgh

95

How can I calculate PE of a charge q in an Electric field?

• PEelc = qV.

Page 96: Static Electricity

Prove that V = Ed in uniform field

V = W/q = Fd/q but F/q = E

So

V = Ed

For parallel plates.96

Page 97: Static Electricity

Hwk

• Reg Prob set “Intro to Voltage”.

97

http://www.youtube.com/watch?v=F1p3fgbDnkY&list=UUN7TW2MSHt-VLT04z_-t2rg&index=13

Old but good Voltage Clip 9:36 min.

Page 98: Static Electricity

Define

• Gravitational Field

• Electric Field

• Electric Potential

• Electric Potential Difference

98

Page 99: Static Electricity

99

The electron-volt: unit of work & E.

For very small changes in PEelc (on the order of 10-

19J) unit eV is used.

The electron-volt, eV, is the work & E required to push 1 e- (or p+) through a voltage of 1V.

W = qV = (1.6 x 10-19 C)(1V) = 1.6 x 10-19 J = eV.

1.6 x 10-19 J = eV

Page 100: Static Electricity

100

If 1 e- is pushed across 1V then (1e)(1V)= 1 eV of work is done.

If a charge of 2e- is pushed across a 1V pd then (2e )(1V) = 2eV.

If 2e- pushed across 6V then work is 12 eV.

To find eV given elementary charges:

(# e )(# V ) = eV.

Page 101: Static Electricity

101

36 eV

What if 3e- move across 12 V?

To find eV (# elm charges) (voltage)

Page 102: Static Electricity

7. How many joules of energy are represented by 6.9 x 1029 eV.

6.9 x 1029 eV x 1. 6 x 10-19 J. = 1.1 x 1011 J

eV

Page 103: Static Electricity

103

Ex 8. A field does 3.3 x 10-7 J of work on an e-. How many eV is that?

• 3.3 x 10-7 J x 1eV = 2.1 x 1012 eV

• 1.6 x 10-19 J

Page 104: Static Electricity

104

Ex 9: A proton is accelerated in a 100 V pd. How much work is done in eV?

• W = qV but if we use elem charge, we can just multiply by the voltage.

• (1 p+)(100 V) = 100 eV

Page 105: Static Electricity

105

Summery Voltage or Electric Potential

V = Wk per Coulomb to bring a charged particle to point in field from infinity.

Potential / Voltage difference Wk per Coulomb to move charge between two

points at different potentials.

Charges in field have PEelc.High PE charge near point with same charge.

Low PE charge near point with opposite charge.

Page 106: Static Electricity

106

Charges set lose in E fields will accelerate!

The average lightning bolt contains 5 coulombs

Page 107: Static Electricity

107

Some typical voltages

Page 108: Static Electricity

Can calculate acceleration of charges in E fields & through

Voltages.

108

Set PE elc = KE

Page 109: Static Electricity

109

Kahn Elec Potential

Elec Potential & Potential E

Page 110: Static Electricity

110

Prove that for parallel plates

E = Vd

•V = W = Fd but F = E V = Ed

q q q

• Rearranging E = V

d

Page 111: Static Electricity

111

Plates with battery

AC Delco 12 volts

d

- +d = 1 cm

A B

Batteries are meant to maintain the potential difference.

ABV Ed

AB /E V d12 / 0.01E 12000 N/CE

Page 112: Static Electricity

Electric PE review youtube. Kahn

http://www.youtube.com/watch?v=wT9AsY79f1k

112

Page 113: Static Electricity

113