Transcript
Page 1: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Unit 14: Electrostatics

Page 2: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Units of Chapter 16

• Static Electricity; Electric Charge and Its Conservation

• Electric Charge in the Atom

• Insulators and Conductors

• Induced Charge; the Electroscope

• Coulomb’s Law

• Solving Problems Involving Coulomb’s Law and Vectors

• The Electric Field

Page 3: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Units of Chapter 16

• Field Lines

• Electric Fields and Conductors

Page 4: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Do Now1. How do protons and electrons differ in their

electrical charge?

2. Is an electron in a hydrogen atom the same as an electron in a uranium atom?

3. Which has more mass – a proton or an electron?

4. In a normal atom, how many electrons are there compared to protons?

Page 5: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Do Now1. How do protons and electrons differ in their

electrical charge?Same magnitude, but opposite charge.

2. Is an electron in a hydrogen atom the same as an electron in a uranium atom?Yes.

3. Which has more mass – a proton or an electron?Proton

4. In a normal atom, how many electrons are there compared to protons? Same number, no net charge.

Page 6: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Atomic Structure

Page 7: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.1 Static Electricity; Electric Charge and Its Conservation

Objects can be charged by rubbing

Page 8: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Triboelectric Series• Friction can cause electrons to transfer

from one material to another• Different materials have a different degree

of attraction for electrons• The triboelectric series determines which

materials have a greater attraction.• When two materials are rubbed together,

the one with the higher attraction will end up getting some of the electrons from the other material

Page 9: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Triboelectric Series

Human Hands (if very dry) Leather Rabbit Fur Glass Human Hair Nylon Wool Fur Lead Silk Aluminum Paper Cotton Steel (neutral) Wood Amber

Hard Rubber Nickel, Copper Brass, Silver Gold, Platinum Polyester Styrene (Styrofoam) Saran Wrap Polyurethane Polyethylene (scotch tape) Polypropylene Vinyl (PVC) Silicon Teflon 

MORE POSITIVE            

MORE NEGATIVE

If two materials are rubbed together, the one that is higher in the series will give up electrons and become more positive.

Page 10: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Question

• If fur is rubbed on glass, will the glass become positively charged or negatively charged?

• Glass – positive• Fur -negative

Page 11: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.1 Static Electricity; Electric Charge and Its

Conservation

Charge comes in two types, positive and negative; like charges repel and opposite charges attract

Page 12: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Interaction Between Charged and Neutral Objects

• Any charged object - whether positively charged or negatively charged - will have an attractive interaction with a neutral object.

Page 13: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.1 Static Electricity; Electric Charge and Its Conservation

Electric charge is conserved – the arithmetic sum of the total charge cannot change in any interaction.

Page 14: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.2 Electric Charge in the Atom

Atom:

Nucleus (small, massive, positive charge)

Electron cloud (large, very low density, negative charge)

Page 15: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.2 Electric Charge in the Atom

Atom is electrically neutral.

Rubbing charges objects by moving electrons from one to the other.

Page 16: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.2 Electric Charge in the Atom

Polar molecule: neutral overall, but charge not evenly distributed

Page 17: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.3 Insulators and Conductors

Conductor:

Charge flows freely

Metals

Insulator:

Almost no charge flows

Most other materials

Some materials are semiconductors.

Page 18: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors
Page 19: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

How Charge Is Transferred

• Objects can be charged by rubbing• Metal objects can be charged by

conduction• Metal objects can be charged by• induction

Page 20: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.4 Induced Charge; the Electroscope

Metal objects can be charged by conduction:

Page 21: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Charging by Induction

• When an object gets charged by induction, a charge is created by the influence of a charged object but not by contact with a charged object.  The word induction means to influence without contact. 

• If a rubber balloon is charged negatively (perhaps by rubbing it with animal fur) and brought near (without touching) the spheres, electrons within the two-sphere system will be induced to move away from the balloon.

Page 22: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Charging By InductionWith Negatively Charged Object

In step iii, why is the charge on the right sphere almost uniformly distributed?

Page 23: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Charging By InductionWith Negatively Charged Object

What was the source of positive charge that ended up on sphere B?

Page 24: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Source of charge in induction

• In induction, the source of charge that is on the final object is not the result of movement from the charged object to the neutral object.

Page 25: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Ground

• An infinite source or sink for charge

Page 26: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.4 Induced Charge; the Electroscope

They can also be charged by induction:

Page 27: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.4 Induced Charge; the Electroscope

The electroscope can be used for detecting charge:

Page 28: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.4 Induced Charge; the ElectroscopeThe electroscope can be charged either by conduction or by induction.

Page 29: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.4 Induced Charge; the Electroscope

The charged electroscope can then be used to determine the sign of an unknown charge.

Page 30: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.4 Induced Charge; the Electroscope

Nonconductors won’t become charged by conduction or induction, but will experience charge rearrangement. The atoms or molecules become polarized.

:

Page 31: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.4 Induced Charge; the Electroscope

Nonconductors won’t become charged by conduction or induction, but will experience charge separation:

Page 32: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Do Now

True or False? Explain your reasoning.

1. An object that is positively charged contains all protons and no electrons.

False Positively charged objects have electrons; they simply possess more protons than electrons.

2. An object that is electrically neutral contains only neutrons.

False

Electrically neutral atoms simply possess the same number of electrons as protons.

Page 33: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Do Now

True or False? Explain your reasoning.

1. An object that is positively charged contains all protons and no electrons.

2. An object that is electrically neutral contains only neutrons.

Page 34: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Coulomb’s Law

• The French physicist Charles Coulomb (1736 – 1806) investigated electric forces in the 1780s using a torsion balance.

Page 35: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.5 Coulomb’s Law

Experiment shows that the electric force between two charges is proportional to the product of the charges and inversely proportional to the distance between them.

Page 36: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Coulomb’s Law

1. If two point charges and are a distance r apart, the charges exert forces on each object of magnitude:

These forces are an action/reaction pair, equal in magnitude but opposite in direction.

1Q 2Q

2

211221 r

QQkFF onon

Page 37: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.5 Coulomb’s Law2. The forces are along the line connecting the

charges, and is attractive if the charges are opposite, and repulsive if they are the same.

Page 38: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.5 Coulomb’s Law

Unit of charge: coulomb, C

The proportionality constant in Coulomb’s law is then:

Charges produced by rubbing are typically around a microcoulomb:

229 /100.9 CmNk When we only need two significant figures:

Page 39: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.5 Coulomb’s Law

Charge on the electron:

Electric charge is quantized in units of the electron charge.

This is the smallest charge in nature – fundamental or elementary charge.

The net charge of any object must be a multiple of that charge.

Page 40: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.5 Coulomb’s Law

The proportionality constant k can also be written in terms of , the permittivity of free space:

(16-2)

Page 41: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.5 Coulomb’s LawCoulomb’s law strictly applies only to point charges.

Superposition: for multiple point charges, the forces on each charge from every other charge can be calculated and then added as vectors.

Page 42: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.6 Solving Problems Involving Coulomb’s Law and Vectors

The net force on a charge is the vector sum of all the forces acting on it.

Page 43: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.6 Solving Problems Involving Coulomb’s Law and Vectors

Vector addition review:

Page 44: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Example 1

Suppose that two point charges, each with a charge of +1.00 Coulomb are separated by a distance of 1.00 meter. Determine the magnitude of the electrical force of repulsion between them.

Given: Find: F - ?

IQI I= 1.00 C

Q2 I= 1.00 C

r = 1.00 m

Page 45: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Solve:

221

r

QQkF

NF 92

9

100.91

)1)(1)(100.9(

The force of repulsion of two +1.00 Coulomb charges held 1.00 meter apart is 9 billion Newton. This is an incredibly large force that compares in magnitude to the weight of more than 2000 jetliners.

Page 46: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Example 2

Determine the magnitude and direction of the electric force on the electron of a hydrogen atom exerted by the single proton that is the atom’s nucleus. Assume the average distance between the revolving electron an the proton

Given: Find: F-?

mr 101053.0

CQQ 1921 106.1

mr 101053.0

Page 47: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Solution:

Nm

CCCmN

r

QQkF 8

210

1919229

2

21 102.8)1053.0(

)106.1)(106.1)(/100.9(

Page 48: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Problem 1

A balloon with a charge of is held a distance of 0.10m from a second balloon having the same charge. Calculate the magnitude of the electrical force between the charges. Draw a diagram.

C5100.4

Nm

CCCmN

r

QQkF 14401014400

)10.0(

)100.4)(100.4)(/100.9( 12

55229

2

21

Page 49: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Problem 2

• Calculate the electrical force exerted between a 22-gram balloon with a charge of -2.6μC and a wool sweater with a charge of +3.8μC; the separation distance is 75cm. (Note: ) CC 61011

NNm

CCCmN

r

QQkF 158.01008.158

)75.0(

)106.2)(106.2)(/100.9( 32

66229

221

Page 50: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors
Page 51: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Neutral vs. Charged Objects

• if an atom contains equal numbers of protons and electrons, the atom is described as being electrically neutral.

• if an atom has an unequal number of protons and electrons, then the atom is electrically charged and referred to as an ion.

• Any particle, whether an atom, molecule or ion, that contains less electrons than protons is said to be positively charged.

• Conversely, any particle that contains more electrons than protons is said to be negatively charged.

Page 52: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Charged Objects as an Imbalance of Protons and Electrons

• Electrons can move to the electrons’ shells of other atoms of different materials.

• For electrons to make a move from the atoms of one material to the atoms of another material, there must be an energy source and a low-resistance pathway.

• rubbing your feet on carpet• clothes tumble in the dryer

Page 53: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Charged Objects as an Imbalance of Protons and Electrons

• The principle stated earlier for atoms can be applied to objects.

• Objects with more electrons than protons are charged negatively; objects with fewer electrons than protons are charged positively.

Page 54: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

True or False?

1. An object that is positively charged contains all protons and no electrons.

False Positively charged objects have electrons; they simply possess more protons than electrons.2. An object that is electrically neutral contains only neutrons.FalseElectrically neutral atoms simply possess the same number of electrons as protons.

Page 55: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Do Now

Suppose you rub a glass rod with a silk cloth and a second glass rod with rabbit fur. The silk clothwill acquire a __________ (+ , -) charge; the rabbit fur will acquire a __________ (+ , -) charge. The rabbit fur and the silk cloth will then be observed to ______________________ (attract, repel, notinteract with) each other.

Page 56: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Three Ways to Charge an Object

1. Friction (by rubbing)

2. Conduction(with contact) 3. Induction(without contact)

Page 57: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Ground An infinite source or sink for charge

• Charge always distributes itself evenly around a conducting sphere

• We can think of ground as a conductor that is so large that it can always accept more charge (or provide more charge).

Symbol

Page 58: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Charging by Conduction• When charging something by

contact it is important to note the following properties

• The objects must actually touch and transfer some electrons.

• The objects become charged alike.

• The original charged object becomes less charged because it actually lost some charge.

Page 59: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

The Electroscope

The electroscope can be used for detecting charge:

Page 60: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Electroscope Can be Charged by Induction

Page 61: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Electroscope Can be Charged by Conduction

• Once the contact of the rod to the electroscope is made, the electrons move from the electroscope to the rod. The electroscope is positively charged.

Page 62: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Nonconductors

Nonconductors won’t become charged by conduction or induction, but will experience charge rearrangement. The atoms or molecules become polarized.

Page 63: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Do Now

• Object A is rubbed with object B. Object C is rubbed with• object D. Objects A and D are observed to repel each

other.• Object B is observed to repel a negatively charged

balloon.• This is conclusive evidence that …• … object A acquired a __________ (+ , -) charge.• … object B acquired a __________ (+ , -) charge.• … object C acquired a __________ (+ , -) charge.• … object D acquired a __________ (+ , -) charge.

Page 64: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Law of Universal Gravitation Analogy

• Coulomb’s Law • Law of Universal Gravitation

221

d

qqkF

221

d

mmGF

Page 65: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Questions:

1. Two charged objects have a repulsive force of .080 N. If the charge of one of the objects is doubled, then what is the new force?

2. Two charged objects have a repulsive force of .080 N. If the distance separating the objects is doubled, then what is the new force?

Page 66: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Do Now

• Object A is rubbed with object B. • Object C is rubbed with object D. • Objects A and D are observed to repel each other.• Object B is observed to repel a negatively charged

balloon.This is conclusive evidence that …… object A acquired a __________ (+ , -) charge.… object B acquired a __________ (+ , -) charge.… object C acquired a __________ (+ , -) charge.… object D acquired a __________ (+ , -) charge.

Page 67: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Six Flags Trip

1. Meet in the auditorium after Pd.2.2. 1PM Check in at buffet in Old Country Picnic

Grove.3. 5 PM Meet at fountain.

4. Cell phone.5. Sunscreen.

Page 68: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors
Page 69: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors
Page 70: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors
Page 71: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors
Page 72: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors
Page 73: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors
Page 74: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Do Now

• Find the force exerted on the test charge. Indicate the direction of that force(Hint: Calculate individual forces on the test charge and add them as vectors.)

qA= +2nC qtest=-1C qB=+3nC

1m 1m

Page 75: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Solution

Nr

QQkF TA

AonT 18)1(

)1)(102)(109(2

99

2

to the left

Nr

QQkF TB

BonT 27)1(

)1)(103)(109(2

99

2

to the right

NNNFnet 91827 to the right

Page 76: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Gravitational Force

• Objects near surface of Earth

• Gravitational force always directed towards the center of Earth.

r

Force2r

GMmmgF

2r

GMg

Page 77: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Gravitational Force

Force depends on mass of object.

Gravitational force always directed towards center of earth.

Even when there is no mass nearby the earth, we can still talk about a gravitational field near the earth- pointing towards earth.

gmF

Page 78: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Electric Field

• Space around Earth and every mass is filled with gravitational field.

• Space around every electric charge is filled with electric field.

Page 79: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Strength of Electric Field

• An electric field is a vector. It has both magnitude and direction.

• Its magnitude can be measured by its effect on a small positive test charge q placed in it.

• The greater the force acting on the charge, the stronger the electric field.

• E – strength of electric field

Units – N/Cq

FE electric

Page 80: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.7 The Electric Field

The electric field is the force on a small (point) charge, divided by the charge:

• If you know the direction and magnitude of the electric field, you can determine the direction of the force.• Negatively charged particles will have opposite direction of force.

Page 81: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

The Electric Field

2

2

/

r

kQ

q

Fr

kqQF

qFE

General Expression for point charge: 2r

QkE

q- test charge

Q – source charge

Page 82: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Gravitational Field Analogy

• Strength of electric field:

• Strength of gravitational field:

F=mg

q

FE electric

m

Fg nalgravitatio

Page 83: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Example 1

Jack pulls his wool sweater over his head, which charges his cotton t-shirt as the sweater rubs against it. a) What is the magnitude and direction of the electric field at a location where a -piece of lint experiences a force of as it floats near Jack?Given:

C191060.1

N9102.3

Cq 191060.1

NF 9102.3

Page 84: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

• Solution:

CNC

N

q

FE /100.2

1060.1

102.3 1019

9

Page 85: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Example 2

Charge Q acts as a point charge to create an electric field. Its strength, measured a distance of 30 cm away, is 40 N/C. What would be the electric field strength ...a)30 cm away from a source with charge 2Q? b)60 cm away from a source with charge Q?a) 80N/cb) 10N/C 2r

QkE

Page 86: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Example 3

What is the magnitude and direction of the electric field 0.25 meters away from a source charge with -5.0 μC. Draw a diagram.

CNr

kQE /102.7

)25.0(

100.5)(109( 52

)69

2

Page 87: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.7 The Electric Field

Force on a point charge in an electric field:

(16-5)

Superposition principle for electric fields:

Page 88: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.7 The Electric Field

Problem solving in electrostatics: electric forces and electric fields

1. Draw a diagram; show all charges, with signs, and electric fields and forces with directions

2. Calculate forces using Coulomb’s law

3. Add forces vectorially to get result

Page 89: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.8 Field Lines

The electric field can be represented by field lines. These lines start on a positive charge and end on a negative charge.

Page 90: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.8 Field LinesThe number of field lines starting (ending) on a positive (negative) charge is proportional to the magnitude of the charge.

The electric field is stronger where the field lines are closer together.

Page 91: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.8 Field Lines

Electric dipole: two equal charges, opposite in sign:

Page 92: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.8 Field Lines

The electric field between two closely spaced, oppositely charged parallel plates is constant.

Page 93: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.8 Field Lines

Summary of field lines:

1. Field lines indicate the direction of the field; the field is tangent to the line.

2. The magnitude of the field is proportional to the density of the lines.

3. Field lines start on positive charges and end on negative charges; the number is proportional to the magnitude of the charge.

Page 94: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.9 Electric Fields and Conductors

The static electric field inside a conductor is zero – if it were not, the charges would move.

The net charge on a conductor is on its surface.

Page 95: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Faraday’s Cage, Shielding

A conducting box used for shielding delicate instruments from unwanted external electric fields.

Page 96: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.9 Electric Fields and Conductors

The electric field is perpendicular to the surface of a conductor – again, if it were not, charges would move.

Page 97: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

16.12 Photocopy Machines and Computer Printers Use Electrostatics

Laser printer is similar, except a computer controls the laser intensity to form the image on the drum

Page 98: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

• Two kinds of electric charge – positive and negative

• Charge is conserved

• Charge on electron:

• Conductors: electrons free to move

• Insulators: nonconductors

Summary of Chapter 16

Page 99: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Summary of Chapter 16

• Charge is quantized in units of e

• Objects can be charged by conduction or induction

• Coulomb’s law:

• Electric field is force per unit charge:

Page 100: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Summary of Chapter 16

• Electric field of a point charge:

• Electric field can be represented by electric field lines

• Static electric field inside conductor is zero; surface field is perpendicular to surface

2r

kQE

Page 101: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Chapter 17

Electric Potential

Page 102: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Units of Chapter 17

• Electric Potential Energy and Potential Difference

•Relation between Electric Potential and Electric Field

•Equipotential Lines

•Capacitance

Page 103: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

17.1 Electrostatic Potential Energy and Potential Difference

The electrostatic force is conservative – potential energy can be defined

Change in electric potential energy is negative of work done by electric force:

(17-1)

Page 104: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Electric Potential

eCh

nergyPotentialEElectricaltentialElectricPo

arg

coulomb

joulevolt 11

Page 105: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

17.1 Electrostatic Potential Energy and Potential Difference

Electric potential is defined as potential energy per unit charge:

(17-2a)

Unit of electric potential: the volt (V).

1 V = I J/C.

Page 106: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

17.1 Electrostatic Potential Energy and Potential Difference

Only changes in potential can be measured, allowing free assignment of V = 0.

(17-2b)

Page 107: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Example 4

What is the potential difference between the terminals of a battery if 60.J of work are done when 3.0 C are pushed trough a wire from one terminal to the other?

Given: Find: V-?

W=60J

q= 3.0C

Page 108: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Solution:

VC

J

q

WV .20

0.3

.60

Page 109: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

17.1 Electrostatic Potential Energy and Potential Difference

Analogy between gravitational and electrical potential energy:

Page 110: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Electrical Potential Energy

• Work is done when you move an object in the direction of the force.

• When you raise an object, you move it against gravitational field, you increase its potential energy.

• When you move electric charge against electric field, you increase its potential energy.

Page 111: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Diagram A.• Moving a positive test charge

against the direction of an electric field is like moving a mass upward within Earth's gravitational field.

• Both movements would be like going against nature and would require work by an external force.

Diagram B.• Work would not be

required to move an object from a high potential energy location to a low potential energy location.

Page 112: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

17.2 Relation between Electric Potential and Electric Field

Work is charge multiplied by potential:

Work is also force multiplied by distance:

Page 113: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

17.2 Relation between Electric Potential and Electric Field

Solving for the field,

(17-4b)

If the field is not uniform, it can be calculated at multiple points:

Page 114: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

17.3 Equipotential Lines

An equipotential is a line or surface over which the potential is constant.

Electric field lines are perpendicular to equipotentials.

The surface of a conductor is an equipotential.

Page 115: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Equipotential Lines

• Equipotential lines are like contour lines on a map which trace lines of equal altitude. In this case the "altitude" is electric potential or voltage.

• Equipotential lines are always perpendicular to the electric field.

• Movement along an equipotential line requires no work because such movement is always perpendicular to the electric field.

Page 116: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

17.3 Equipotential Lines

Page 117: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Equipotential Lines

• Dashed lines are equipotential lines• Solid lines are electric field lines

Page 118: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Summary of Chapter 17

• Electric potential energy:

• Electric potential difference: work done to move charge from one point to another

• Relationship between potential difference and field:

Page 119: Unit 14: Electrostatics. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom Insulators and Conductors

Summary of Chapter 17

• Equipotential: line or surface along which potential is the same


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