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Electrostatics Electrostatics

Electrostatics - PowerPoint Presentation

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Electrostatics - PPT Presentation

Essential Knowledge 1B2 There are only two kinds of electric charge Neutral objects or systems contain equal quantities of positive and negative charge with the exception of some fundamental particles that have no electric charge ID: 530860

field charge charged force charge field force charged electric charges lines object objects point positive electrons negative unit sphere

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Slide1

ElectrostaticsSlide2

Essential Knowledge

1.B.2

: There are only two kinds of electric charge. Neutral objects or systems contain equal quantities of positive and negative charge, with the exception of some fundamental particles that have no electric charge.

Like-charged objects and systems repel and unlike-charged objects and systems attract.

Charged objects or systems may attract neutral systems by changing the distributions of charge in neutral systems.

1.B.3

: The smallest observed unit of charge that can be isolated is the electron charge, also known as the elementary charge.

The magnitude of the elementary charge is equal to1.6 x1 10

-19

Coulombs.

Electrons have a negative elementary charge of equal magnitude, although the mass of the proton is much larger than the mass of an electron.

3.C.2:

Electric force results from the interaction of one object that has an electric charge with another object that has an electric charge.

Electric force dominates the properties of the objects in our everyday experiences. However, the large number of particles interaction that occur make it more convenient to treat everyday forces, such as normal force, friction, and tension.

Electric force may be attractive or repulsive, depending upon the charges on the objects involved.

5.A.1

: A system is an object or collection of objects. The objects are treated as having no internal structure.Slide3

Learning Objectives

1.B.2.1

: The students is able to construct and explanation of the two charge models of electric charge based on evidence produced through scientific practices.

1.B.3.1

: The student is able to challenge the claim that an electric charge smaller than elementary charge has been isolated.

3.C.2.1

: The students is able to use Coulomb’s law qualitatively and quantitatively to make predictions about the interaction between two electric point charges (

interaction between collections of electric point charges are not covered in Physics 1 and instead are restricted to Physics 2

)

3.C.2.2

: The student is able to connect concepts of gravitational forces and electric force to compare similarities and differences between the forces. Slide4

Science Practices

1.5:

The student can re-express key elements of natural phenomena across multiple representations in the domain.

2.2:

The student can

apply mathematical

routines to quantities that describe natural phenomena.

6.1:

The student can

justify claims

with evidence.

6.2:

The students can

construct explanations

of phenomena based on evidence produced through scientific practices.

6.4:

The student can

make claims and predictions about natural phenomena

based on scientific theories and models.

7.2:

The students can

connect concepts

in and across domain(s) to generalize or extrapolate in and/or across enduring understanding and/or big ideas.Slide5

Electric Charges

1. Two kinds of charges: Positive and Negative

2. Like charges repel, unlike charges attract

3. Charge is conserved

4. Charge is quantized

LINKSlide6

The

total charge in a closed system remains constant.

Charges are transferred.

The total charge in a closed system remains constant.

Neutral objects have equal amounts of positive and negative charge.

Only

electrons

are transferred in solids.

Single charges may not be created nor destroyed.Pairs of opposite charges may be created or destroyed.

Examples:

Charge separation by friction

Chemical equations

Beta Decay Pair production / pair annihilation

Law of Conservation of ChargeSlide7

SI Unit for Charge

Coulomb [C] is the SI unit for charge.

Coulomb is a derived unit based on the fundamental unit for current, Ampere.

Coulomb is a humongous amount of charge.Slide8

Natural unit for charge

On

the atomic level, the unit of charge is

the elementary charge, e.

+

e is the charge of a proton

-e is the charge of an electron+2e is the charge of an alpha particleSlide9

Balloon Charge Tester

Item

Attract

RepelSlide10

Natural unit for charge

On the sub-atomic level, fractional charges exist

.

Quarks have

+

(1/3) e or + (2/3) eSlide11

Charge is Quantized

In 1909 Robert Millikan confirmed that electric charge always

occurs in integral multiples of the fundamental unit of charge, e.

q is the standard symbol for charge (units - Coulombs)

Money is quantized, the smallest unit of US currency is the penny!

Total Charge

Number of fundamental charges

Elementary

Charge

1.6 x 10

-19

CSlide12

Particle

Mass

Charge

electron

9.11 x 10

-31

kg

-1.6 x 10

-19

C

-1e

proton

1.672 x 10

-27

kg

+1.6 x 10

-19

C

+1e

neutron

1.674 x 10

-27

kg

0

Fundamental particle propertiesSlide13

An object has a net charge of +3 Coulombs

How many more protons than electrons are on the object?

Can you determine the total number of protons on the object?Slide14

Object

# of Excess Protons/Electrons

Quantity of Charge (Q)

in Coulombs (C)

A

1 x 10

6

excess electrons

- 1.6 x 10

-13

C

B

2 x 10

8

excess protons

+ 3.2 x 10

-11

C

C

2 x 10

10

excess electrons

- 3.2 x 10

-9

C

Ex: Find the total charge on the object in each caseSlide15

Conductors and Insulators

Good conductors have many “free” electrons

EX: Metals

Insulators have few “free” electrons

Ex: Rubber, woodSlide16

Insulators and Conductors

Electrical Conductibility

Insulators

Conductors

No movement of charges within the object

Free

movement

of charges

Semi-conductors

Limited number of free carriers

Wood, plastics, glass

Silicon, Germanium

Metals (Cu, Ag, Al)

Grounding: The “Earth” is considered an infinite sink of chargesSlide17

Ground (

Earthing

)

Grounding

: The “Earth” is considered an infinite source or sink for excess charge.

Grounding

prevents charge from building up on the chassis of appliances.Mutual grounding provides a common reference point.Slide18

Coulomb’s Law

In 1785 Charles Coulomb established a law of electric force

between two

stationary

charged particles.

Force inversely proportional to square of distance

Force along the line joining the particles

Force proportional to the product of the charges

Force attractive between opposite sign charges.

Force repulsive between charges of the same sign

k = Coulomb constant

= 8.99 x 10

9 Nm

2/C2Slide19

Direction of the Coulomb Force

Force can be attractive or repulsive

Equal in magnitude

Opposite in directionSlide20

Ex:

If q

1

=-3uC, q

2

= +4uC, and d = 2 m,

find the electric force between the charges.

+

-

q

1

q

2

d

F

12

F

21Slide21

Coulomb Force is proportional to 1/r

2

Hyperbolic relationship between force and distance

linkSlide22

Analogy to

Gravitational

Force

Coulomb Force

Gravitational Force

The gravitational force can only be attractive.

Example: Compare the gravitational force in the hydrogen atom to the Coulomb (electric) force. Which is stronger?Slide23

Atomic

Radius:

10

-10

meters

Nuclear

Diameter:

10-15 meters

Mass of electron: me = 9.11 x 10

-31 kgMass of proton:

m

p = 1.67 x 10-27 kg

Compare the gravitational force in the hydrogen atom to the Coulomb (electric) force. Which is stronger? How much stronger?Slide24

Difference and Similarities between Electricity and Gravity

Coulomb Law and Law of Gravitation similarities

Gravitation is always attractive

Electrical force can be attractive or repulsive

Electric force dominates the atomic world

Gravitational forces dominates the macroscopic scale: people, planets, galaxies

Electric forces are stronger !!!

Slide25

A metal sphere is charged by losing 5.18 x 10

13

electrons while a second sphere is charged by losing 15.54 x 10

13

electrons. The two spheres are 25 cm apart. Determine the force between the two spheres. Slide26

Two charged objects have a repulsive force of .080 N. If the charge of one is doubled, and the distance separating them is doubled what is the new force?

Two charged objects have a repulsive force of .080 N. If the charge of both of the objects is doubled and the distance separating the objects is doubled what is the new force?

Two charged objects have an attractive force of .080 N. If the charge of one of the objects is quadrupled, and the distance separating the objects is doubled what is the new force?

4.

Two charged objects have an attractive force of .080 N. If the charge of one is tripled and the distance separating the objects is tripled what is the new force?Slide27

Two uniformly charged spheres are firmly fastened to and electrically insulated from a table. The charge on sphere 2 is three times the charge on sphere 1. Which diagram correctly shows the magnitude and direction of the electrostatic forces:Slide28

Alternate Form of Coulomb’s law

Coulomb’s constant k is often written in terms of the permittivity of free space e

0

Coulomb’s Law can then be written as:Slide29

Superposition Principle

When more than two charges are present, the resultant force on any one of them is equal to the

vector

sum of the forces exerted by each of the individual charges.Slide30

Solution:

Note the direction of forces

Resolve F

32

and F

31

into their x and y components

Add the x and y components of F32 and F

31 to find x and y components of F

3Find the magnitude and direction of F

3

45

0

F

32

F

31

45

0

Three point charges located at corners of triangle as shown.

F

ind

The resultant force on

q

3

q

1

= q

3

= 5

C

q

2

= -2 C

a = .1 mSlide31

Two 2 gram balloons are suspended by strings that are 60 cm long. The two balloons establish equilibrium with an angle between the two strings of 25

0

. Determine the charge on each balloon. Assume the same amount of charge is on each. Slide32

Methods of Charging

Ouch!

Friction -

Transfer of electrons between

neutral

objects.

Induction

-

A neutral object becomes charges without ever contacting the charged object.

Conduction -

A

charged

body comes in contact with another body and charge is transferred between them. Slide33

1. Friction

-

When two neutral objects are rubbed together. One gives up its negative charges to the other. One becomes positively charged while the other becomes equally negative.

Hair gives up electrons to the balloon.Slide34

Frictional

charging is a result of

transfer

of electrons

Some materials are greedy and steal electrons, they have a high

electroconductivity

, while others are willing to give them up.Slide35

2. Induction

- When an object is charged by the influence of a charged object near, but not in contact with it. The word induction means to influence

without contact

Positively charged object brought near, does not touch the electroscope.

Ground’s attached and electrons are drawn up.

Ground is removed trapping electrons on the electroscope.

Electroscope ends up oppositely charged to the object brought near. Slide36

Electrons attracted by the positive object toward the top of the electroscope. The foil leaves at the bottom have a positive charge so they repel each other.

Electrons pushed by negative object toward the bottom of the electroscope. The foil leaves at the bottom have a negative charge so they repel each other.

Temporary polarization by inductionSlide37

Electrostatic Induction

occurs only in conductors.

Ground -

Is an infinite source or sink for electrons. Slide38

InductionSlide39

InductionSlide40

Polarization and InductionSlide41

A negatively charged rubber rod is brought near an uncharged sphere

The charges in the sphere are redistributed.

After the sphere is grounded they leave the sphere

The positive charge on the sphere is evenly distributed

Charging by induction requires no contact with the object inducing the charge

InductionSlide42

3. Conduction

– Charging by contact

When charging something by contact

:

A charged objects must touch and transfer some electrons.

The objects become charged

alike

.

The original charged object becomes less charged.Slide43

Conduction

A charged object (the rod) is placed in contact with another object (the sphere)

Some electrons on the rod can move to the sphere

When the rod is removed, the sphere is left with a charge

The object being charged is always left with a charge having the same sign as the object doing the chargingSlide44

Grounding neutralizes a charged objectSlide45

Polarization and charging by contactSlide46

Polarization-Induced Attractions

Attraction is more common than repulsion

Charged objects can attract uncharged ones

A charged rod attracts a neutral metal ball

It redistributes the charge

 separation of charge in the uncharged object. The attractive force is then greater.

Water faucet comb demoSlide47

Conduction or Induction?Slide48

After rubbing the balloon, why does balloon stick to wall?

How do you know that this force is stronger than gravity?Slide49

Negatively charged paint adheres

to positively charged metal. Slide50

Van

def

Graff generator and charging by contactSlide51
Slide52
Slide53

Charge Distributions

The excess charge on a conductor resides on the outer surface concentrating on rough edges and corners.

Automobiles are a safe haven from lightening.

Lightening rods and point dischargeSlide54

Gravitational Fields

Surround anything with mass

Vector fields (have magnitude and direction)

Weaken as you move away from a single mass

Magnitude of field can be calculated by:Slide55

q

0

is the test charge

Q is the charged object in the area

E is the electric field experienced by q

0

due to Q

Electric Fields

Surround charged objects

Vector fields (magnitude and direction)

Direction depends on the charge

Weaken as you move away from isolated one charge

Magnitude of field calculated by:Slide56

Electric Field Strength

The Electric Field Strength at a point in an Electric Field is the Force per unit positive test charge exerted on a charge at that point.

E = F/q

*

Vector Quantity

*[N/C]Slide57

Field of an isolated point chargeSlide58

Coulomb Force is proportional to 1/r

2

Hyperbolic relationship between force and distanceSlide59

Calculate the force exerted by E = 4 N/C

to

the right(

→) on each of the following:

q

1

= +1 C q2 = +4 Cq3 = - 4 Cq4 = + 1.5 Cq

5 = - 1.5 Cq6 = 6 μCq

7 = p+

q8 = e-

q9 = 2e-Slide60

What is the strength of the electric field 2 cm fron a +3uC charge?

If you double the distance from the charge what will be the new electric field strength at that point?

Ans

: ¼ the original strengthSlide61

The number of lines per unit area through the surface is proportional to the magnitude of the electric field

The closer the lines the stronger the field, ‘E’.Slide62

Drawing Electric Field Lines

Lines begin on positive and end on negative charges.

No two field lines can cross.

Number of field lines leaving is proportional to the charge.

Strength of the field is proportional to the density of lines.Slide63

Electric field lines are

proportional to magnitude of the charge

Electric field is tangent at any pointSlide64

If charges are not equal in magnitude the greater charge will

have more field lines

Twice the charge, twice the field linesSlide65

Double the charge means double the field linesSlide66

Field the same strength at every point along the circleSlide67

The diagram below is a representation of the electric field

arising

from?

a single negative charge

two unlike charges

a single positive charge

a pair of positive charges

a pair of negative chargesSlide68

Must Know what the electric fields looks like around

A positive point charge

A negative point charge

A positive and negative point charge

Two positive point charges

Two negative point charges

Around and inside a conducting sphere

Between 2 parallel plates

NOTE:

Point

Charges have no dimensionsSlide69

Positive Point Charge

+

+

Field emanates from positive charge

Perpendicular to the surface

Field lines never cross

Field weakens as 1/r

2

Slide70

Field terminates on it

Field perpendicular to the surface

Field lines never cross

Field weakens as the distance increases

Negative Point ChargeSlide71

Inverse square law: 1/r

2

Double the distance the field is a ¼ the original strength.

Less field lines per unit area.

Positive Point ChargeSlide72

Out of the positive and into the negative

Strongest between the charges

Field lines are perpendicular to the surface

Field lines never cross

One Positive and one Negative Point ChargeSlide73

Field zero between the charges

Field lines diverge

Field lines never cross

Field lines perpendicular to surface

Two Positive Point ChargesSlide74

Field 0 between the charges

Field lines diverge

Field lines never cross

Field lines perpendicular to surface

Two Negative Point Charges

Same as positive charge diagram except field lines go into the chargesSlide75

Negatively Charged Conducting Sphere

E=0

_

_

_

_

_

_

_

_

Field ends on the charge

Field

ZERO

inside the sphere

All excess charge is on the surface

More charge equals more field lines

It’s NOT dimensionlessSlide76

E=0

Everywhere

inside

Field lines perpendicular to surface

Double the distance, field is ¼ original strength.

Inverse square lawSlide77

Field begins on the charge

Field

ZERO

inside the sphere

All excess charge is on the surface

More charge equals more field lines

Positively Charged Conducting SphereSlide78

Edge effects-

Electric field lines bulge out slightly around the edges of Parallel Plates – Field weakerSlide79

Magnitude - The force on a charge placed in the field divided by the charge itself.

Direction

- The direction that the force would be on a positive test charge placed at that point.

All fields are vectors:Slide80

The field lines for a large positively charged plate.  The field lines flow away from the plate on both sides.  (Note: this is a small section near the center of a large plate.  This is why the field lines are not coming from the outside rim of the plate.)Slide81

A uniform electric field is created between two parallel

metal plates if the plates are connected to a battery.

The way the terminals are connected

determines the direction of the fieldSlide82

Field around and between charged parallel plates

Field comes out of the positive plate goes into the negative plate

Field is

UNIFORM,

same strength everywhere

Field above and below the plates is zero.Slide83

+ + + + + + + + + + + + + + + + + +

- - - - - - - - - - - - - - - - - - - - - - - - -

Positive plate

Negative

Plate

E

=const

. Uniform field

Parallel Plate Capacitor

Everywhere outside the plates the field is zeroSlide84

A charged particle introduced perpendicular to the electric field will follow a parabolic path

Like a projectile in a gravitational field