Charges. Electrons P+ n nucleus e- Source of Electrons(Force)

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Transcript of Charges. Electrons P+ n nucleus e- Source of Electrons(Force)

ChargesCharges

Electrons Electrons

P+n

nucleus

e-

Source of Electrons(Force) Source of Electrons(Force)

Matter Weight - SpaceMatter Weight - Space

Solid Liquid Gas Plasma

AtomsAtoms

Pn

nucleus

e-

valenceshell

AtomsAtoms

Atomic Number ndash Number of Protons

Atomic Weight ndash Number of Protons plus Neutrons

Number of Protons EQUALS Electrons in a neutral atom

IonizationIonization

The process where an atom gains or loses an electron

NaNa++ClCl--Na ndash Positive IonCl ndash Negative Ion

Charges (q) Charges (q)

Like Charges (++ - -)Like Charges (++ - -)

q- q-

q+ q+Repel

Charges (q) Charges (q)

Un-Like Charges (+ -)Un-Like Charges (+ -)

q+ q-Attract

Coulombrsquos LawCoulombrsquos Law

Coulomb (C)Coulomb (C)

The quantity of charge The quantity of charge on an abjecton an abject

1C = 625 x 101C = 625 x 101818 e e--

q-

Coulombrsquos LawCoulombrsquos Law

q1 q2

Coulombrsquos LawCoulombrsquos Law

What does the force What does the force depend ondepend on

q1 q2

Coulombrsquos LawCoulombrsquos Law

1The charge on q1The charge on q11 and q and q22

2The distance (d)2The distance (d)

d

q-

d d2

q1 q2

Mathematical Model for Mathematical Model for Coulombrsquos Law Force (F)Coulombrsquos Law Force (F)

d

F infinF infin q1q2 q1q2

F infinF infin 1d 1d22

q1 q2d

F =F =

qq11qq22

dd22KK

K = 90 X 10K = 90 X 1099 N Nmm22CC22

q1 q2d=3cm

d = 3cm = 3x10d = 3cm = 3x10-2-2mmK = 90 X 10K = 90 X 1099 N Nmm22CC22

qq11= +6= +6μμC = +6x10C = +6x10-6-6CCqq22= +3= +3μμC = +6x10C = +6x10-6-6C C

What is the force on qWhat is the force on q22

F =F =

(3X10(3X10-2-2m)m)22

9X109X1099NNmm22CC22(6X10(6X10-6-6C)(6X10C)(6X10-6-6C)C)

qq11qq22

dd22

KK

F =F = 18X1018X1022NN

q1 q2

Electric FieldsElectric Fields

Think of gravity or Think of gravity or gravitational field to gravitational field to

understand electric fieldsunderstand electric fields

Electric Fields Electric Fields vs vs GravityGravity

gg

Electric Electric FieldsFields

EE

neutralneutral neutralneutral

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

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

ElectricElectric Fields Fields

EE

++

++

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

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

Electric Electric FieldsFields

EE

--

--

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

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

Electric FieldsElectric Fields

A force field due to electric A force field due to electric chargescharges

EE

A force on a charge due to A force on a charge due to another chageanother chage

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

Electrons Electrons

P+n

nucleus

e-

Source of Electrons(Force) Source of Electrons(Force)

Matter Weight - SpaceMatter Weight - Space

Solid Liquid Gas Plasma

AtomsAtoms

Pn

nucleus

e-

valenceshell

AtomsAtoms

Atomic Number ndash Number of Protons

Atomic Weight ndash Number of Protons plus Neutrons

Number of Protons EQUALS Electrons in a neutral atom

IonizationIonization

The process where an atom gains or loses an electron

NaNa++ClCl--Na ndash Positive IonCl ndash Negative Ion

Charges (q) Charges (q)

Like Charges (++ - -)Like Charges (++ - -)

q- q-

q+ q+Repel

Charges (q) Charges (q)

Un-Like Charges (+ -)Un-Like Charges (+ -)

q+ q-Attract

Coulombrsquos LawCoulombrsquos Law

Coulomb (C)Coulomb (C)

The quantity of charge The quantity of charge on an abjecton an abject

1C = 625 x 101C = 625 x 101818 e e--

q-

Coulombrsquos LawCoulombrsquos Law

q1 q2

Coulombrsquos LawCoulombrsquos Law

What does the force What does the force depend ondepend on

q1 q2

Coulombrsquos LawCoulombrsquos Law

1The charge on q1The charge on q11 and q and q22

2The distance (d)2The distance (d)

d

q-

d d2

q1 q2

Mathematical Model for Mathematical Model for Coulombrsquos Law Force (F)Coulombrsquos Law Force (F)

d

F infinF infin q1q2 q1q2

F infinF infin 1d 1d22

q1 q2d

F =F =

qq11qq22

dd22KK

K = 90 X 10K = 90 X 1099 N Nmm22CC22

q1 q2d=3cm

d = 3cm = 3x10d = 3cm = 3x10-2-2mmK = 90 X 10K = 90 X 1099 N Nmm22CC22

qq11= +6= +6μμC = +6x10C = +6x10-6-6CCqq22= +3= +3μμC = +6x10C = +6x10-6-6C C

What is the force on qWhat is the force on q22

F =F =

(3X10(3X10-2-2m)m)22

9X109X1099NNmm22CC22(6X10(6X10-6-6C)(6X10C)(6X10-6-6C)C)

qq11qq22

dd22

KK

F =F = 18X1018X1022NN

q1 q2

Electric FieldsElectric Fields

Think of gravity or Think of gravity or gravitational field to gravitational field to

understand electric fieldsunderstand electric fields

Electric Fields Electric Fields vs vs GravityGravity

gg

Electric Electric FieldsFields

EE

neutralneutral neutralneutral

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

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

ElectricElectric Fields Fields

EE

++

++

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

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

Electric Electric FieldsFields

EE

--

--

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

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

Electric FieldsElectric Fields

A force field due to electric A force field due to electric chargescharges

EE

A force on a charge due to A force on a charge due to another chageanother chage

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

Source of Electrons(Force) Source of Electrons(Force)

Matter Weight - SpaceMatter Weight - Space

Solid Liquid Gas Plasma

AtomsAtoms

Pn

nucleus

e-

valenceshell

AtomsAtoms

Atomic Number ndash Number of Protons

Atomic Weight ndash Number of Protons plus Neutrons

Number of Protons EQUALS Electrons in a neutral atom

IonizationIonization

The process where an atom gains or loses an electron

NaNa++ClCl--Na ndash Positive IonCl ndash Negative Ion

Charges (q) Charges (q)

Like Charges (++ - -)Like Charges (++ - -)

q- q-

q+ q+Repel

Charges (q) Charges (q)

Un-Like Charges (+ -)Un-Like Charges (+ -)

q+ q-Attract

Coulombrsquos LawCoulombrsquos Law

Coulomb (C)Coulomb (C)

The quantity of charge The quantity of charge on an abjecton an abject

1C = 625 x 101C = 625 x 101818 e e--

q-

Coulombrsquos LawCoulombrsquos Law

q1 q2

Coulombrsquos LawCoulombrsquos Law

What does the force What does the force depend ondepend on

q1 q2

Coulombrsquos LawCoulombrsquos Law

1The charge on q1The charge on q11 and q and q22

2The distance (d)2The distance (d)

d

q-

d d2

q1 q2

Mathematical Model for Mathematical Model for Coulombrsquos Law Force (F)Coulombrsquos Law Force (F)

d

F infinF infin q1q2 q1q2

F infinF infin 1d 1d22

q1 q2d

F =F =

qq11qq22

dd22KK

K = 90 X 10K = 90 X 1099 N Nmm22CC22

q1 q2d=3cm

d = 3cm = 3x10d = 3cm = 3x10-2-2mmK = 90 X 10K = 90 X 1099 N Nmm22CC22

qq11= +6= +6μμC = +6x10C = +6x10-6-6CCqq22= +3= +3μμC = +6x10C = +6x10-6-6C C

What is the force on qWhat is the force on q22

F =F =

(3X10(3X10-2-2m)m)22

9X109X1099NNmm22CC22(6X10(6X10-6-6C)(6X10C)(6X10-6-6C)C)

qq11qq22

dd22

KK

F =F = 18X1018X1022NN

q1 q2

Electric FieldsElectric Fields

Think of gravity or Think of gravity or gravitational field to gravitational field to

understand electric fieldsunderstand electric fields

Electric Fields Electric Fields vs vs GravityGravity

gg

Electric Electric FieldsFields

EE

neutralneutral neutralneutral

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

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

ElectricElectric Fields Fields

EE

++

++

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

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

Electric Electric FieldsFields

EE

--

--

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

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

Electric FieldsElectric Fields

A force field due to electric A force field due to electric chargescharges

EE

A force on a charge due to A force on a charge due to another chageanother chage

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

Matter Weight - SpaceMatter Weight - Space

Solid Liquid Gas Plasma

AtomsAtoms

Pn

nucleus

e-

valenceshell

AtomsAtoms

Atomic Number ndash Number of Protons

Atomic Weight ndash Number of Protons plus Neutrons

Number of Protons EQUALS Electrons in a neutral atom

IonizationIonization

The process where an atom gains or loses an electron

NaNa++ClCl--Na ndash Positive IonCl ndash Negative Ion

Charges (q) Charges (q)

Like Charges (++ - -)Like Charges (++ - -)

q- q-

q+ q+Repel

Charges (q) Charges (q)

Un-Like Charges (+ -)Un-Like Charges (+ -)

q+ q-Attract

Coulombrsquos LawCoulombrsquos Law

Coulomb (C)Coulomb (C)

The quantity of charge The quantity of charge on an abjecton an abject

1C = 625 x 101C = 625 x 101818 e e--

q-

Coulombrsquos LawCoulombrsquos Law

q1 q2

Coulombrsquos LawCoulombrsquos Law

What does the force What does the force depend ondepend on

q1 q2

Coulombrsquos LawCoulombrsquos Law

1The charge on q1The charge on q11 and q and q22

2The distance (d)2The distance (d)

d

q-

d d2

q1 q2

Mathematical Model for Mathematical Model for Coulombrsquos Law Force (F)Coulombrsquos Law Force (F)

d

F infinF infin q1q2 q1q2

F infinF infin 1d 1d22

q1 q2d

F =F =

qq11qq22

dd22KK

K = 90 X 10K = 90 X 1099 N Nmm22CC22

q1 q2d=3cm

d = 3cm = 3x10d = 3cm = 3x10-2-2mmK = 90 X 10K = 90 X 1099 N Nmm22CC22

qq11= +6= +6μμC = +6x10C = +6x10-6-6CCqq22= +3= +3μμC = +6x10C = +6x10-6-6C C

What is the force on qWhat is the force on q22

F =F =

(3X10(3X10-2-2m)m)22

9X109X1099NNmm22CC22(6X10(6X10-6-6C)(6X10C)(6X10-6-6C)C)

qq11qq22

dd22

KK

F =F = 18X1018X1022NN

q1 q2

Electric FieldsElectric Fields

Think of gravity or Think of gravity or gravitational field to gravitational field to

understand electric fieldsunderstand electric fields

Electric Fields Electric Fields vs vs GravityGravity

gg

Electric Electric FieldsFields

EE

neutralneutral neutralneutral

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

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

ElectricElectric Fields Fields

EE

++

++

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

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

Electric Electric FieldsFields

EE

--

--

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

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

Electric FieldsElectric Fields

A force field due to electric A force field due to electric chargescharges

EE

A force on a charge due to A force on a charge due to another chageanother chage

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

AtomsAtoms

Pn

nucleus

e-

valenceshell

AtomsAtoms

Atomic Number ndash Number of Protons

Atomic Weight ndash Number of Protons plus Neutrons

Number of Protons EQUALS Electrons in a neutral atom

IonizationIonization

The process where an atom gains or loses an electron

NaNa++ClCl--Na ndash Positive IonCl ndash Negative Ion

Charges (q) Charges (q)

Like Charges (++ - -)Like Charges (++ - -)

q- q-

q+ q+Repel

Charges (q) Charges (q)

Un-Like Charges (+ -)Un-Like Charges (+ -)

q+ q-Attract

Coulombrsquos LawCoulombrsquos Law

Coulomb (C)Coulomb (C)

The quantity of charge The quantity of charge on an abjecton an abject

1C = 625 x 101C = 625 x 101818 e e--

q-

Coulombrsquos LawCoulombrsquos Law

q1 q2

Coulombrsquos LawCoulombrsquos Law

What does the force What does the force depend ondepend on

q1 q2

Coulombrsquos LawCoulombrsquos Law

1The charge on q1The charge on q11 and q and q22

2The distance (d)2The distance (d)

d

q-

d d2

q1 q2

Mathematical Model for Mathematical Model for Coulombrsquos Law Force (F)Coulombrsquos Law Force (F)

d

F infinF infin q1q2 q1q2

F infinF infin 1d 1d22

q1 q2d

F =F =

qq11qq22

dd22KK

K = 90 X 10K = 90 X 1099 N Nmm22CC22

q1 q2d=3cm

d = 3cm = 3x10d = 3cm = 3x10-2-2mmK = 90 X 10K = 90 X 1099 N Nmm22CC22

qq11= +6= +6μμC = +6x10C = +6x10-6-6CCqq22= +3= +3μμC = +6x10C = +6x10-6-6C C

What is the force on qWhat is the force on q22

F =F =

(3X10(3X10-2-2m)m)22

9X109X1099NNmm22CC22(6X10(6X10-6-6C)(6X10C)(6X10-6-6C)C)

qq11qq22

dd22

KK

F =F = 18X1018X1022NN

q1 q2

Electric FieldsElectric Fields

Think of gravity or Think of gravity or gravitational field to gravitational field to

understand electric fieldsunderstand electric fields

Electric Fields Electric Fields vs vs GravityGravity

gg

Electric Electric FieldsFields

EE

neutralneutral neutralneutral

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

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

ElectricElectric Fields Fields

EE

++

++

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

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

Electric Electric FieldsFields

EE

--

--

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

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

Electric FieldsElectric Fields

A force field due to electric A force field due to electric chargescharges

EE

A force on a charge due to A force on a charge due to another chageanother chage

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

AtomsAtoms

Atomic Number ndash Number of Protons

Atomic Weight ndash Number of Protons plus Neutrons

Number of Protons EQUALS Electrons in a neutral atom

IonizationIonization

The process where an atom gains or loses an electron

NaNa++ClCl--Na ndash Positive IonCl ndash Negative Ion

Charges (q) Charges (q)

Like Charges (++ - -)Like Charges (++ - -)

q- q-

q+ q+Repel

Charges (q) Charges (q)

Un-Like Charges (+ -)Un-Like Charges (+ -)

q+ q-Attract

Coulombrsquos LawCoulombrsquos Law

Coulomb (C)Coulomb (C)

The quantity of charge The quantity of charge on an abjecton an abject

1C = 625 x 101C = 625 x 101818 e e--

q-

Coulombrsquos LawCoulombrsquos Law

q1 q2

Coulombrsquos LawCoulombrsquos Law

What does the force What does the force depend ondepend on

q1 q2

Coulombrsquos LawCoulombrsquos Law

1The charge on q1The charge on q11 and q and q22

2The distance (d)2The distance (d)

d

q-

d d2

q1 q2

Mathematical Model for Mathematical Model for Coulombrsquos Law Force (F)Coulombrsquos Law Force (F)

d

F infinF infin q1q2 q1q2

F infinF infin 1d 1d22

q1 q2d

F =F =

qq11qq22

dd22KK

K = 90 X 10K = 90 X 1099 N Nmm22CC22

q1 q2d=3cm

d = 3cm = 3x10d = 3cm = 3x10-2-2mmK = 90 X 10K = 90 X 1099 N Nmm22CC22

qq11= +6= +6μμC = +6x10C = +6x10-6-6CCqq22= +3= +3μμC = +6x10C = +6x10-6-6C C

What is the force on qWhat is the force on q22

F =F =

(3X10(3X10-2-2m)m)22

9X109X1099NNmm22CC22(6X10(6X10-6-6C)(6X10C)(6X10-6-6C)C)

qq11qq22

dd22

KK

F =F = 18X1018X1022NN

q1 q2

Electric FieldsElectric Fields

Think of gravity or Think of gravity or gravitational field to gravitational field to

understand electric fieldsunderstand electric fields

Electric Fields Electric Fields vs vs GravityGravity

gg

Electric Electric FieldsFields

EE

neutralneutral neutralneutral

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

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

ElectricElectric Fields Fields

EE

++

++

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

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

Electric Electric FieldsFields

EE

--

--

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

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

Electric FieldsElectric Fields

A force field due to electric A force field due to electric chargescharges

EE

A force on a charge due to A force on a charge due to another chageanother chage

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

IonizationIonization

The process where an atom gains or loses an electron

NaNa++ClCl--Na ndash Positive IonCl ndash Negative Ion

Charges (q) Charges (q)

Like Charges (++ - -)Like Charges (++ - -)

q- q-

q+ q+Repel

Charges (q) Charges (q)

Un-Like Charges (+ -)Un-Like Charges (+ -)

q+ q-Attract

Coulombrsquos LawCoulombrsquos Law

Coulomb (C)Coulomb (C)

The quantity of charge The quantity of charge on an abjecton an abject

1C = 625 x 101C = 625 x 101818 e e--

q-

Coulombrsquos LawCoulombrsquos Law

q1 q2

Coulombrsquos LawCoulombrsquos Law

What does the force What does the force depend ondepend on

q1 q2

Coulombrsquos LawCoulombrsquos Law

1The charge on q1The charge on q11 and q and q22

2The distance (d)2The distance (d)

d

q-

d d2

q1 q2

Mathematical Model for Mathematical Model for Coulombrsquos Law Force (F)Coulombrsquos Law Force (F)

d

F infinF infin q1q2 q1q2

F infinF infin 1d 1d22

q1 q2d

F =F =

qq11qq22

dd22KK

K = 90 X 10K = 90 X 1099 N Nmm22CC22

q1 q2d=3cm

d = 3cm = 3x10d = 3cm = 3x10-2-2mmK = 90 X 10K = 90 X 1099 N Nmm22CC22

qq11= +6= +6μμC = +6x10C = +6x10-6-6CCqq22= +3= +3μμC = +6x10C = +6x10-6-6C C

What is the force on qWhat is the force on q22

F =F =

(3X10(3X10-2-2m)m)22

9X109X1099NNmm22CC22(6X10(6X10-6-6C)(6X10C)(6X10-6-6C)C)

qq11qq22

dd22

KK

F =F = 18X1018X1022NN

q1 q2

Electric FieldsElectric Fields

Think of gravity or Think of gravity or gravitational field to gravitational field to

understand electric fieldsunderstand electric fields

Electric Fields Electric Fields vs vs GravityGravity

gg

Electric Electric FieldsFields

EE

neutralneutral neutralneutral

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

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

ElectricElectric Fields Fields

EE

++

++

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

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

Electric Electric FieldsFields

EE

--

--

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

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

Electric FieldsElectric Fields

A force field due to electric A force field due to electric chargescharges

EE

A force on a charge due to A force on a charge due to another chageanother chage

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

Charges (q) Charges (q)

Like Charges (++ - -)Like Charges (++ - -)

q- q-

q+ q+Repel

Charges (q) Charges (q)

Un-Like Charges (+ -)Un-Like Charges (+ -)

q+ q-Attract

Coulombrsquos LawCoulombrsquos Law

Coulomb (C)Coulomb (C)

The quantity of charge The quantity of charge on an abjecton an abject

1C = 625 x 101C = 625 x 101818 e e--

q-

Coulombrsquos LawCoulombrsquos Law

q1 q2

Coulombrsquos LawCoulombrsquos Law

What does the force What does the force depend ondepend on

q1 q2

Coulombrsquos LawCoulombrsquos Law

1The charge on q1The charge on q11 and q and q22

2The distance (d)2The distance (d)

d

q-

d d2

q1 q2

Mathematical Model for Mathematical Model for Coulombrsquos Law Force (F)Coulombrsquos Law Force (F)

d

F infinF infin q1q2 q1q2

F infinF infin 1d 1d22

q1 q2d

F =F =

qq11qq22

dd22KK

K = 90 X 10K = 90 X 1099 N Nmm22CC22

q1 q2d=3cm

d = 3cm = 3x10d = 3cm = 3x10-2-2mmK = 90 X 10K = 90 X 1099 N Nmm22CC22

qq11= +6= +6μμC = +6x10C = +6x10-6-6CCqq22= +3= +3μμC = +6x10C = +6x10-6-6C C

What is the force on qWhat is the force on q22

F =F =

(3X10(3X10-2-2m)m)22

9X109X1099NNmm22CC22(6X10(6X10-6-6C)(6X10C)(6X10-6-6C)C)

qq11qq22

dd22

KK

F =F = 18X1018X1022NN

q1 q2

Electric FieldsElectric Fields

Think of gravity or Think of gravity or gravitational field to gravitational field to

understand electric fieldsunderstand electric fields

Electric Fields Electric Fields vs vs GravityGravity

gg

Electric Electric FieldsFields

EE

neutralneutral neutralneutral

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

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

ElectricElectric Fields Fields

EE

++

++

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

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

Electric Electric FieldsFields

EE

--

--

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

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

Electric FieldsElectric Fields

A force field due to electric A force field due to electric chargescharges

EE

A force on a charge due to A force on a charge due to another chageanother chage

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

Charges (q) Charges (q)

Un-Like Charges (+ -)Un-Like Charges (+ -)

q+ q-Attract

Coulombrsquos LawCoulombrsquos Law

Coulomb (C)Coulomb (C)

The quantity of charge The quantity of charge on an abjecton an abject

1C = 625 x 101C = 625 x 101818 e e--

q-

Coulombrsquos LawCoulombrsquos Law

q1 q2

Coulombrsquos LawCoulombrsquos Law

What does the force What does the force depend ondepend on

q1 q2

Coulombrsquos LawCoulombrsquos Law

1The charge on q1The charge on q11 and q and q22

2The distance (d)2The distance (d)

d

q-

d d2

q1 q2

Mathematical Model for Mathematical Model for Coulombrsquos Law Force (F)Coulombrsquos Law Force (F)

d

F infinF infin q1q2 q1q2

F infinF infin 1d 1d22

q1 q2d

F =F =

qq11qq22

dd22KK

K = 90 X 10K = 90 X 1099 N Nmm22CC22

q1 q2d=3cm

d = 3cm = 3x10d = 3cm = 3x10-2-2mmK = 90 X 10K = 90 X 1099 N Nmm22CC22

qq11= +6= +6μμC = +6x10C = +6x10-6-6CCqq22= +3= +3μμC = +6x10C = +6x10-6-6C C

What is the force on qWhat is the force on q22

F =F =

(3X10(3X10-2-2m)m)22

9X109X1099NNmm22CC22(6X10(6X10-6-6C)(6X10C)(6X10-6-6C)C)

qq11qq22

dd22

KK

F =F = 18X1018X1022NN

q1 q2

Electric FieldsElectric Fields

Think of gravity or Think of gravity or gravitational field to gravitational field to

understand electric fieldsunderstand electric fields

Electric Fields Electric Fields vs vs GravityGravity

gg

Electric Electric FieldsFields

EE

neutralneutral neutralneutral

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

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

ElectricElectric Fields Fields

EE

++

++

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

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

Electric Electric FieldsFields

EE

--

--

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

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

Electric FieldsElectric Fields

A force field due to electric A force field due to electric chargescharges

EE

A force on a charge due to A force on a charge due to another chageanother chage

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

Coulombrsquos LawCoulombrsquos Law

Coulomb (C)Coulomb (C)

The quantity of charge The quantity of charge on an abjecton an abject

1C = 625 x 101C = 625 x 101818 e e--

q-

Coulombrsquos LawCoulombrsquos Law

q1 q2

Coulombrsquos LawCoulombrsquos Law

What does the force What does the force depend ondepend on

q1 q2

Coulombrsquos LawCoulombrsquos Law

1The charge on q1The charge on q11 and q and q22

2The distance (d)2The distance (d)

d

q-

d d2

q1 q2

Mathematical Model for Mathematical Model for Coulombrsquos Law Force (F)Coulombrsquos Law Force (F)

d

F infinF infin q1q2 q1q2

F infinF infin 1d 1d22

q1 q2d

F =F =

qq11qq22

dd22KK

K = 90 X 10K = 90 X 1099 N Nmm22CC22

q1 q2d=3cm

d = 3cm = 3x10d = 3cm = 3x10-2-2mmK = 90 X 10K = 90 X 1099 N Nmm22CC22

qq11= +6= +6μμC = +6x10C = +6x10-6-6CCqq22= +3= +3μμC = +6x10C = +6x10-6-6C C

What is the force on qWhat is the force on q22

F =F =

(3X10(3X10-2-2m)m)22

9X109X1099NNmm22CC22(6X10(6X10-6-6C)(6X10C)(6X10-6-6C)C)

qq11qq22

dd22

KK

F =F = 18X1018X1022NN

q1 q2

Electric FieldsElectric Fields

Think of gravity or Think of gravity or gravitational field to gravitational field to

understand electric fieldsunderstand electric fields

Electric Fields Electric Fields vs vs GravityGravity

gg

Electric Electric FieldsFields

EE

neutralneutral neutralneutral

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

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

ElectricElectric Fields Fields

EE

++

++

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

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

Electric Electric FieldsFields

EE

--

--

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

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

Electric FieldsElectric Fields

A force field due to electric A force field due to electric chargescharges

EE

A force on a charge due to A force on a charge due to another chageanother chage

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

q-

Coulombrsquos LawCoulombrsquos Law

q1 q2

Coulombrsquos LawCoulombrsquos Law

What does the force What does the force depend ondepend on

q1 q2

Coulombrsquos LawCoulombrsquos Law

1The charge on q1The charge on q11 and q and q22

2The distance (d)2The distance (d)

d

q-

d d2

q1 q2

Mathematical Model for Mathematical Model for Coulombrsquos Law Force (F)Coulombrsquos Law Force (F)

d

F infinF infin q1q2 q1q2

F infinF infin 1d 1d22

q1 q2d

F =F =

qq11qq22

dd22KK

K = 90 X 10K = 90 X 1099 N Nmm22CC22

q1 q2d=3cm

d = 3cm = 3x10d = 3cm = 3x10-2-2mmK = 90 X 10K = 90 X 1099 N Nmm22CC22

qq11= +6= +6μμC = +6x10C = +6x10-6-6CCqq22= +3= +3μμC = +6x10C = +6x10-6-6C C

What is the force on qWhat is the force on q22

F =F =

(3X10(3X10-2-2m)m)22

9X109X1099NNmm22CC22(6X10(6X10-6-6C)(6X10C)(6X10-6-6C)C)

qq11qq22

dd22

KK

F =F = 18X1018X1022NN

q1 q2

Electric FieldsElectric Fields

Think of gravity or Think of gravity or gravitational field to gravitational field to

understand electric fieldsunderstand electric fields

Electric Fields Electric Fields vs vs GravityGravity

gg

Electric Electric FieldsFields

EE

neutralneutral neutralneutral

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

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

ElectricElectric Fields Fields

EE

++

++

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

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

Electric Electric FieldsFields

EE

--

--

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

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

Electric FieldsElectric Fields

A force field due to electric A force field due to electric chargescharges

EE

A force on a charge due to A force on a charge due to another chageanother chage

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

q1 q2

Coulombrsquos LawCoulombrsquos Law

What does the force What does the force depend ondepend on

q1 q2

Coulombrsquos LawCoulombrsquos Law

1The charge on q1The charge on q11 and q and q22

2The distance (d)2The distance (d)

d

q-

d d2

q1 q2

Mathematical Model for Mathematical Model for Coulombrsquos Law Force (F)Coulombrsquos Law Force (F)

d

F infinF infin q1q2 q1q2

F infinF infin 1d 1d22

q1 q2d

F =F =

qq11qq22

dd22KK

K = 90 X 10K = 90 X 1099 N Nmm22CC22

q1 q2d=3cm

d = 3cm = 3x10d = 3cm = 3x10-2-2mmK = 90 X 10K = 90 X 1099 N Nmm22CC22

qq11= +6= +6μμC = +6x10C = +6x10-6-6CCqq22= +3= +3μμC = +6x10C = +6x10-6-6C C

What is the force on qWhat is the force on q22

F =F =

(3X10(3X10-2-2m)m)22

9X109X1099NNmm22CC22(6X10(6X10-6-6C)(6X10C)(6X10-6-6C)C)

qq11qq22

dd22

KK

F =F = 18X1018X1022NN

q1 q2

Electric FieldsElectric Fields

Think of gravity or Think of gravity or gravitational field to gravitational field to

understand electric fieldsunderstand electric fields

Electric Fields Electric Fields vs vs GravityGravity

gg

Electric Electric FieldsFields

EE

neutralneutral neutralneutral

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

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

ElectricElectric Fields Fields

EE

++

++

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

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

Electric Electric FieldsFields

EE

--

--

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

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

Electric FieldsElectric Fields

A force field due to electric A force field due to electric chargescharges

EE

A force on a charge due to A force on a charge due to another chageanother chage

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

q1 q2

Coulombrsquos LawCoulombrsquos Law

1The charge on q1The charge on q11 and q and q22

2The distance (d)2The distance (d)

d

q-

d d2

q1 q2

Mathematical Model for Mathematical Model for Coulombrsquos Law Force (F)Coulombrsquos Law Force (F)

d

F infinF infin q1q2 q1q2

F infinF infin 1d 1d22

q1 q2d

F =F =

qq11qq22

dd22KK

K = 90 X 10K = 90 X 1099 N Nmm22CC22

q1 q2d=3cm

d = 3cm = 3x10d = 3cm = 3x10-2-2mmK = 90 X 10K = 90 X 1099 N Nmm22CC22

qq11= +6= +6μμC = +6x10C = +6x10-6-6CCqq22= +3= +3μμC = +6x10C = +6x10-6-6C C

What is the force on qWhat is the force on q22

F =F =

(3X10(3X10-2-2m)m)22

9X109X1099NNmm22CC22(6X10(6X10-6-6C)(6X10C)(6X10-6-6C)C)

qq11qq22

dd22

KK

F =F = 18X1018X1022NN

q1 q2

Electric FieldsElectric Fields

Think of gravity or Think of gravity or gravitational field to gravitational field to

understand electric fieldsunderstand electric fields

Electric Fields Electric Fields vs vs GravityGravity

gg

Electric Electric FieldsFields

EE

neutralneutral neutralneutral

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

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

ElectricElectric Fields Fields

EE

++

++

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

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

Electric Electric FieldsFields

EE

--

--

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

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

Electric FieldsElectric Fields

A force field due to electric A force field due to electric chargescharges

EE

A force on a charge due to A force on a charge due to another chageanother chage

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

q-

d d2

q1 q2

Mathematical Model for Mathematical Model for Coulombrsquos Law Force (F)Coulombrsquos Law Force (F)

d

F infinF infin q1q2 q1q2

F infinF infin 1d 1d22

q1 q2d

F =F =

qq11qq22

dd22KK

K = 90 X 10K = 90 X 1099 N Nmm22CC22

q1 q2d=3cm

d = 3cm = 3x10d = 3cm = 3x10-2-2mmK = 90 X 10K = 90 X 1099 N Nmm22CC22

qq11= +6= +6μμC = +6x10C = +6x10-6-6CCqq22= +3= +3μμC = +6x10C = +6x10-6-6C C

What is the force on qWhat is the force on q22

F =F =

(3X10(3X10-2-2m)m)22

9X109X1099NNmm22CC22(6X10(6X10-6-6C)(6X10C)(6X10-6-6C)C)

qq11qq22

dd22

KK

F =F = 18X1018X1022NN

q1 q2

Electric FieldsElectric Fields

Think of gravity or Think of gravity or gravitational field to gravitational field to

understand electric fieldsunderstand electric fields

Electric Fields Electric Fields vs vs GravityGravity

gg

Electric Electric FieldsFields

EE

neutralneutral neutralneutral

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

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

ElectricElectric Fields Fields

EE

++

++

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

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

Electric Electric FieldsFields

EE

--

--

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

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

Electric FieldsElectric Fields

A force field due to electric A force field due to electric chargescharges

EE

A force on a charge due to A force on a charge due to another chageanother chage

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

q1 q2

Mathematical Model for Mathematical Model for Coulombrsquos Law Force (F)Coulombrsquos Law Force (F)

d

F infinF infin q1q2 q1q2

F infinF infin 1d 1d22

q1 q2d

F =F =

qq11qq22

dd22KK

K = 90 X 10K = 90 X 1099 N Nmm22CC22

q1 q2d=3cm

d = 3cm = 3x10d = 3cm = 3x10-2-2mmK = 90 X 10K = 90 X 1099 N Nmm22CC22

qq11= +6= +6μμC = +6x10C = +6x10-6-6CCqq22= +3= +3μμC = +6x10C = +6x10-6-6C C

What is the force on qWhat is the force on q22

F =F =

(3X10(3X10-2-2m)m)22

9X109X1099NNmm22CC22(6X10(6X10-6-6C)(6X10C)(6X10-6-6C)C)

qq11qq22

dd22

KK

F =F = 18X1018X1022NN

q1 q2

Electric FieldsElectric Fields

Think of gravity or Think of gravity or gravitational field to gravitational field to

understand electric fieldsunderstand electric fields

Electric Fields Electric Fields vs vs GravityGravity

gg

Electric Electric FieldsFields

EE

neutralneutral neutralneutral

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

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

ElectricElectric Fields Fields

EE

++

++

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

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

Electric Electric FieldsFields

EE

--

--

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

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

Electric FieldsElectric Fields

A force field due to electric A force field due to electric chargescharges

EE

A force on a charge due to A force on a charge due to another chageanother chage

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

q1 q2d

F =F =

qq11qq22

dd22KK

K = 90 X 10K = 90 X 1099 N Nmm22CC22

q1 q2d=3cm

d = 3cm = 3x10d = 3cm = 3x10-2-2mmK = 90 X 10K = 90 X 1099 N Nmm22CC22

qq11= +6= +6μμC = +6x10C = +6x10-6-6CCqq22= +3= +3μμC = +6x10C = +6x10-6-6C C

What is the force on qWhat is the force on q22

F =F =

(3X10(3X10-2-2m)m)22

9X109X1099NNmm22CC22(6X10(6X10-6-6C)(6X10C)(6X10-6-6C)C)

qq11qq22

dd22

KK

F =F = 18X1018X1022NN

q1 q2

Electric FieldsElectric Fields

Think of gravity or Think of gravity or gravitational field to gravitational field to

understand electric fieldsunderstand electric fields

Electric Fields Electric Fields vs vs GravityGravity

gg

Electric Electric FieldsFields

EE

neutralneutral neutralneutral

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

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

ElectricElectric Fields Fields

EE

++

++

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

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

Electric Electric FieldsFields

EE

--

--

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

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

Electric FieldsElectric Fields

A force field due to electric A force field due to electric chargescharges

EE

A force on a charge due to A force on a charge due to another chageanother chage

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

q1 q2d=3cm

d = 3cm = 3x10d = 3cm = 3x10-2-2mmK = 90 X 10K = 90 X 1099 N Nmm22CC22

qq11= +6= +6μμC = +6x10C = +6x10-6-6CCqq22= +3= +3μμC = +6x10C = +6x10-6-6C C

What is the force on qWhat is the force on q22

F =F =

(3X10(3X10-2-2m)m)22

9X109X1099NNmm22CC22(6X10(6X10-6-6C)(6X10C)(6X10-6-6C)C)

qq11qq22

dd22

KK

F =F = 18X1018X1022NN

q1 q2

Electric FieldsElectric Fields

Think of gravity or Think of gravity or gravitational field to gravitational field to

understand electric fieldsunderstand electric fields

Electric Fields Electric Fields vs vs GravityGravity

gg

Electric Electric FieldsFields

EE

neutralneutral neutralneutral

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

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

ElectricElectric Fields Fields

EE

++

++

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

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

Electric Electric FieldsFields

EE

--

--

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

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

Electric FieldsElectric Fields

A force field due to electric A force field due to electric chargescharges

EE

A force on a charge due to A force on a charge due to another chageanother chage

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

F =F =

(3X10(3X10-2-2m)m)22

9X109X1099NNmm22CC22(6X10(6X10-6-6C)(6X10C)(6X10-6-6C)C)

qq11qq22

dd22

KK

F =F = 18X1018X1022NN

q1 q2

Electric FieldsElectric Fields

Think of gravity or Think of gravity or gravitational field to gravitational field to

understand electric fieldsunderstand electric fields

Electric Fields Electric Fields vs vs GravityGravity

gg

Electric Electric FieldsFields

EE

neutralneutral neutralneutral

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

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

ElectricElectric Fields Fields

EE

++

++

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

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

Electric Electric FieldsFields

EE

--

--

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

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

Electric FieldsElectric Fields

A force field due to electric A force field due to electric chargescharges

EE

A force on a charge due to A force on a charge due to another chageanother chage

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

Electric FieldsElectric Fields

Think of gravity or Think of gravity or gravitational field to gravitational field to

understand electric fieldsunderstand electric fields

Electric Fields Electric Fields vs vs GravityGravity

gg

Electric Electric FieldsFields

EE

neutralneutral neutralneutral

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

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

ElectricElectric Fields Fields

EE

++

++

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

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

Electric Electric FieldsFields

EE

--

--

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

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

Electric FieldsElectric Fields

A force field due to electric A force field due to electric chargescharges

EE

A force on a charge due to A force on a charge due to another chageanother chage

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

Electric Fields Electric Fields vs vs GravityGravity

gg

Electric Electric FieldsFields

EE

neutralneutral neutralneutral

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

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

ElectricElectric Fields Fields

EE

++

++

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

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

Electric Electric FieldsFields

EE

--

--

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

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

Electric FieldsElectric Fields

A force field due to electric A force field due to electric chargescharges

EE

A force on a charge due to A force on a charge due to another chageanother chage

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

Electric Electric FieldsFields

EE

neutralneutral neutralneutral

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

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

ElectricElectric Fields Fields

EE

++

++

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

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

Electric Electric FieldsFields

EE

--

--

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

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

Electric FieldsElectric Fields

A force field due to electric A force field due to electric chargescharges

EE

A force on a charge due to A force on a charge due to another chageanother chage

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

ElectricElectric Fields Fields

EE

++

++

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

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

Electric Electric FieldsFields

EE

--

--

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

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

Electric FieldsElectric Fields

A force field due to electric A force field due to electric chargescharges

EE

A force on a charge due to A force on a charge due to another chageanother chage

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

Electric Electric FieldsFields

EE

--

--

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

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

Electric FieldsElectric Fields

A force field due to electric A force field due to electric chargescharges

EE

A force on a charge due to A force on a charge due to another chageanother chage

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

Electric FieldsElectric Fields

A force field due to electric A force field due to electric chargescharges

EE

A force on a charge due to A force on a charge due to another chageanother chage

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

Electric Field Point ChargeElectric Field Point Charge

qq

E =E = kqkqrr22

rr

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

Force on a charge lsquoqrsquo in an Force on a charge lsquoqrsquo in an Electric FieldElectric Field

QQqq

E =E = FFqq

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

E =E = FFqq

E =E = NewtonNewtonCoulombCoulomb

E =E = NNCC

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

Energy and WorkEnergy and Work

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

Energy and WorkEnergy and Work

++ --

It takes work to move It takes work to move the ldquo-rdquo chargethe ldquo-rdquo charge

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV =V =

Work on Work on qrsquoqrsquo

qrsquoqrsquo

JoulJouleeCoulomCoulom

bb=== volt= volt

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

++

qrsquoqrsquo

ΔΔV = VV = VBB - V - VAA

VVAA VVBB

ldquoldquoPotential DifferencerdquoPotential DifferencerdquoVoltageVoltage

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Fd Fd

q q ΔΔV V = = Eqd Eqd

q q

E = E = F F q q

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

Electric Potential (Energy)Electric Potential (Energy)VoltageVoltage

ΔΔV V = = Ed Ed

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

Example Example Two parallel plates are given Two parallel plates are given opposite charges A opposite charges A

voltmeter measures the voltmeter measures the electric potental differnece electric potental differnece to be 60V The plates are to be 60V The plates are 3ocm apart What is the 3ocm apart What is the magnitude of the electric magnitude of the electric

field between them field between them

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

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

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

EΔV

d

ΔV=600V D=0030m

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

ΔΔV V = = Ed Ed

= E = E ΔΔVVd d

= E = E

60V60V003003m m

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

20002000J(mJ(mmiddotC)= E middotC)= E

2000 2000 NNC = E C = E

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

CurrentCurrent

Flow of chargeFlow of charge

Charge - Coulomb(C) Charge - Coulomb(C) 624 X 10624 X 101818 electrons electrons

e ee e ee e e e e e eeee e

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

Leyden JarLeyden Jar

ConductorsConductors

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

Leyden JarLeyden Jar

++++

++++

++++------------ ----

--------

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

------

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

CapacitorCapacitor

A capacitor is a passive electronic component that stores energy in the form of an electrostatic field

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

CapacitorCapacitor

Metal Plates

Insulating MaterialDielectric

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

CapacitorCapacitor

-+e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

e-

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

CapacitorCapacitor

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

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

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

CopperCopperZincZinc

--

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

CurrentCurrent

e ee e ee e e e e e eeee e

Number of electrons Number of electrons passing a point in a passing a point in a secondsecond

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

CurrentCurrent

Symbol - Symbol - II

Unit ndash Unit ndash Ampere (Amps)Ampere (Amps)

Amperes - Amperes - AA

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

ForceForce

e ee e ee e e e e e eeee e

VoltageVoltage

Potential DifferencePotential Difference

Electromotive Force (EMF)Electromotive Force (EMF)

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

VoltageVoltage

Symbol - Symbol - VV

Unit ndash Unit ndash VoltVolt

Volt - Volt - VV

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High ResistanceHigh ResistanceInsulatorInsulator

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

Low ResistanceLow ResistanceConductorConductor

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

ResistanceResistance

Opposition to Current FlowOpposition to Current Flow

High and Low ResistanceHigh and Low ResistanceSemiConductorSemiConductor

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

ResistanceResistance

Symbol - Symbol - RR

Unit ndash Unit ndash OhmOhm

Ohm - Ohm - ΩΩ

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

Putting it all TogetherPutting it all Together

LoadSource

Path

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper

Homework 1-1Homework 1-1

WorksheetWorksheetDue 9902Due 9902Test 9902Test 9902

  • Electric Fields vs Gravity
  • Electric Fields
  • Slide 22
  • Slide 23
  • Electric Field Point Charge
  • Force on a charge lsquoqrsquo in an Electric Field
  • Slide 27
  • Slide 28
  • Example
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 43
  • Capacitor
  • Slide 45
  • Slide 46
  • Slide 47
  • Copper