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AMIRAJ COLLEGE OF AMIRAJ COLLEGE OF ENG & TECH ENG & TECH NAME: Alpesh Patel NAME: Alpesh Patel Er.No:151080106008 Er.No:151080106008 Subject : EEE(2110005) Subject : EEE(2110005) Topic: Faraday’s, Coulomb’s, Gauss Laws Topic: Faraday’s, Coulomb’s, Gauss Laws Guiden by: Anukar sir Guiden by: Anukar sir

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Page 1: faraday law

AMIRAJ COLLEGE OF AMIRAJ COLLEGE OF ENG & TECH ENG & TECH

NAME: Alpesh PatelNAME: Alpesh Patel Er.No:151080106008Er.No:151080106008 Subject : EEE(2110005) Subject : EEE(2110005) Topic: Faraday’s, Coulomb’s, Gauss LawsTopic: Faraday’s, Coulomb’s, Gauss Laws

Guiden by: Anukar sirGuiden by: Anukar sir

Page 2: faraday law

Faraday’s LawFaraday’s Law

Page 3: faraday law

Area ChangeArea Change The sliding bar creates an emf The sliding bar creates an emf

by changing the area in the by changing the area in the magnetic field.magnetic field.• Constant magnetic fieldConstant magnetic field

The potential was due to the The potential was due to the time rate of change of area.time rate of change of area.

tABvBLV

Page 4: faraday law

Field ChangeField Change An emf can also be generated An emf can also be generated

by changing the magnetic field.by changing the magnetic field.

The time rate of change of the The time rate of change of the field through a fixed loop field through a fixed loop provides the potential.provides the potential.

tBAV

Page 5: faraday law

Field OrientationField Orientation The emf depends on the The emf depends on the

change in field or the change change in field or the change in area.in area.• Area perpendicular to the fieldArea perpendicular to the field

This suggests that the product This suggests that the product of the field and area of the field and area perpendicular matters.perpendicular matters.

t

ABtBAV

cos

Page 6: faraday law

Magnetic FluxMagnetic Flux The product of the field and area perpendicular to the The product of the field and area perpendicular to the

field is the field is the magnetic fluxmagnetic flux..

The magnetic flux is measured in webers.The magnetic flux is measured in webers.• 1 Wb = 1 T m1 Wb = 1 T m22

The magnetic field can be thought of as a flux density.The magnetic field can be thought of as a flux density.

cosABM

AB M

Page 7: faraday law

Faraday’s LawFaraday’s Law The flux can be used to get The flux can be used to get

the induced emf.the induced emf.• Sign indicates polaritySign indicates polarity

This is Faraday’s Law of This is Faraday’s Law of induction.induction.

For multiple turns the emf is For multiple turns the emf is multiplied.multiplied.• NN turns of wire turns of wire• NN is the flux linkage is the flux linkage

tM

tN M

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Coil FluxCoil Flux A circular flat coil has 200 A circular flat coil has 200

turns of wire with a total turns of wire with a total resistance of 25 resistance of 25 and an and an enclosed area of 100 cmenclosed area of 100 cm22. .

There is a perpendicular There is a perpendicular magnetic field of 0.50 T that is magnetic field of 0.50 T that is turned off in 200 ms.turned off in 200 ms.

Find the current induced in the Find the current induced in the coil.coil.

This problem has three parts.This problem has three parts.

To get the current from the To get the current from the resistance the voltage is resistance the voltage is needed.needed.

To get the voltage the flux is To get the voltage the flux is needed.needed.• Flux linkage works, tooFlux linkage works, too

Find the flux first.Find the flux first.

Page 9: faraday law

Flux to CurrentFlux to Current The magnetic flux is The magnetic flux is = BA= BA..

• = (0.50 T)(100 cm= (0.50 T)(100 cm22))• = (0.50 T)(0.010 m= (0.50 T)(0.010 m22))• = 0.0050 T m= 0.0050 T m22

The change in flux is The change in flux is negative since it is turned negative since it is turned off.off.

The induced emf isThe induced emf is• EE = = NN //tt• EE = -(200)(-0.0050 Tm = -(200)(-0.0050 Tm22) / ) /

(0.20 s)(0.20 s)• EE = = VV = 5.0 V = 5.0 V

The induced current comes The induced current comes from Ohm’s Law.from Ohm’s Law.• I = V/RI = V/R• II = (5.0 V) / (25 = (5.0 V) / (25 ))• II = 0.20 A = 0.20 A

next

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September 26, 2007September 26, 2007

Gauss’ LawGauss’ Law We are going to be most interested in We are going to be most interested in closedclosed

surfaces, in which case the outward direction surfaces, in which case the outward direction becomes self-evident.becomes self-evident.

We can ask, what is the electric flux out of such a We can ask, what is the electric flux out of such a closed surface? Just integrate over the closed closed surface? Just integrate over the closed surface:surface:

The symbol has a little circle to indicate that The symbol has a little circle to indicate that the integral is over a closed surface.the integral is over a closed surface.

The closed surface is called a The closed surface is called a gaussian surfacegaussian surface, , because such surfaces are used by Gauss’ Law, because such surfaces are used by Gauss’ Law, which states that:which states that:

AdEd

Gauss’ LawThe flux of electric field through a closed surface is proportional to the charge enclosed.

Flux positive => out Flux negative => in

Page 11: faraday law

FluxFlux Flux in Physics is used to two distinct ways. Flux in Physics is used to two distinct ways. The first meaning is the rate of flow, such as the amount of water flowing in The first meaning is the rate of flow, such as the amount of water flowing in

a river, i.e. volume per unit area per unit time. Or, for light, it is the amount a river, i.e. volume per unit area per unit time. Or, for light, it is the amount of energy per unit area per unit time.of energy per unit area per unit time.

Let’s look at the case for light:Let’s look at the case for light:

Page 12: faraday law

September 26, 2007September 26, 2007

Flux of Electric FieldFlux of Electric Field1. Which of the following figures correctly shows a positive 1. Which of the following figures correctly shows a positive

electric flux out of a surface element?electric flux out of a surface element?A.A. I.I.B.B. II.II.C.C. III.III.D.D. IV.IV.E.E. I and III.I and III.

E

A

EA

E

A

E

A

I. II.

III. IV.

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September 26, 2007September 26, 2007

Mathematical Statement of Mathematical Statement of Gauss’ LawGauss’ Law

The constant of proportionality in Gauss’ Law is our The constant of proportionality in Gauss’ Law is our old friend old friend ..

Recall that I said that we would see later why Recall that I said that we would see later why Coulomb’s constant is written ?Coulomb’s constant is written ?

We can see it now by integrating the electric flux of We can see it now by integrating the electric flux of a point charge over a spherical gaussian surface. a point charge over a spherical gaussian surface.

enc

enc

qAdE

q

0

0

041

Ek

r

qenc

encqrEdAEAdE 2000 4

204

1r

qE enc

dAEAdE

Solving for E gives Coulomb’s Law.

Page 14: faraday law

September 26, 2007September 26, 2007

Example of Gauss’ LawExample of Gauss’ Law Consider a dipole with equal positive and negative Consider a dipole with equal positive and negative

charges.charges. Imagine four surfaces Imagine four surfaces SS11, , SS22, , SS33, , SS44, as shown., as shown. SS11 encloses the positive charge. Note that the field encloses the positive charge. Note that the field

is everywhere outward, so the flux is positive.is everywhere outward, so the flux is positive. SS22 encloses the negative charge. Note that the field encloses the negative charge. Note that the field

is everywhere inward, so the flux through the is everywhere inward, so the flux through the surface is negative.surface is negative.

SS33 encloses no charge. The flux through the encloses no charge. The flux through the surface is negative at the upper part, and positive at surface is negative at the upper part, and positive at the lower part, but these cancel, and there is no net the lower part, but these cancel, and there is no net flux through the surface.flux through the surface.

SS44 encloses both charges. Again there is no net encloses both charges. Again there is no net charge enclosed, so there is equal flux going out charge enclosed, so there is equal flux going out and coming in—no net flux through the surface.and coming in—no net flux through the surface.

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1515

Coulomb’s LawCoulomb’s Law Electric chargeElectric charge

• The positive charge The positive charge and negative charge:and negative charge:

Matter is made of atoms. Matter is made of atoms.

Inside an atom, there is the nucleus that is surrounded by electrons.Inside an atom, there is the nucleus that is surrounded by electrons.Inside the nucleus, there are two particles called proton and neutron. The Inside the nucleus, there are two particles called proton and neutron. The smallest nucleus contains only one proton. This is the nucleus inside a hydrogen smallest nucleus contains only one proton. This is the nucleus inside a hydrogen atom. atom. Proton and electron attract each other. Proton and proton, electron and electron Proton and electron attract each other. Proton and proton, electron and electron repel each other. This is a property of these matters (proton and electron) and we repel each other. This is a property of these matters (proton and electron) and we call it call it chargecharge..

Electric charge is a property of matter that can cause attraction and repulsion.Electric charge is a property of matter that can cause attraction and repulsion. We call We call the charge carried by electrons “negative (-the charge carried by electrons “negative (-e)e) ” ” and and the charge carried by the charge carried by protons “positive (+protons “positive (+ee)”.)”. Charge is a value, or a scalar, not a vector. It is fully Charge is a value, or a scalar, not a vector. It is fully described by a number. described by a number.

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1616

The unit of electric chargeThe unit of electric charge

The SIThe SI11 unit for charge is the unit for charge is the coulomb.coulomb. An electron or a proton has a charge of An electron or a proton has a charge of magnitude magnitude ee = 1.602 18×10 = 1.602 18×10−19−19 C (coulombs). Some scientists, chemists in  C (coulombs). Some scientists, chemists in particular, use another unit, the particular, use another unit, the esuesu or or electrostatic unitelectrostatic unit. One esu equals . One esu equals 3.335 64×103.335 64×10−10−10 C.  C.

To provide you with an idea of the magnitude of a coulomb, approximately To provide you with an idea of the magnitude of a coulomb, approximately 0.8 C of charge flows through a 100 watt light bulb every second. Or about 5 0.8 C of charge flows through a 100 watt light bulb every second. Or about 5 million trillion electrons every second. The rate of charges flowing through a million trillion electrons every second. The rate of charges flowing through a conductor is called a current. We will get to this a few chapters later. conductor is called a current. We will get to this a few chapters later.

No one has ever seen the charge, but we sure all see its effect in everyday No one has ever seen the charge, but we sure all see its effect in everyday life: electrostatic discharge in dry winter days to all the appliances (lights to life: electrostatic discharge in dry winter days to all the appliances (lights to motors to cell phones) that are powered by electricity.motors to cell phones) that are powered by electricity.

How much more do we know about the charge?How much more do we know about the charge?

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1717

Charge and charge upCharge and charge up

• When the numbers of electrons and When the numbers of electrons and protons in an object are the same, we protons in an object are the same, we say that this object is (electrically) say that this object is (electrically) neutral. When they are not, we call it neutral. When they are not, we call it charged. charged.

• There are many ways to charge up an There are many ways to charge up an object. A demo here:object. A demo here:

In this demo, we rub away or rub in In this demo, we rub away or rub in electrons to make anelectrons to make anobject positively or negatively charged.object positively or negatively charged.

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1818

Conservation of electric chargesConservation of electric charges• Electric charge is conserved. Electric charge is conserved. Charge can move between objects in the system, Charge can move between objects in the system,

but the net charge of the system remains unchanged. Charges cannot be but the net charge of the system remains unchanged. Charges cannot be created or destroyed in the system, because charge is just a property of created or destroyed in the system, because charge is just a property of electrons and protons. They both are matter and matter conserves. A remark electrons and protons. They both are matter and matter conserves. A remark on anti-matter: matter and anti-matter annihilate into energy. So what’s more on anti-matter: matter and anti-matter annihilate into energy. So what’s more fundamental is the conservation of energy, but that’s beyond this class.fundamental is the conservation of energy, but that’s beyond this class.

8 = 10 + (-2), so O-21 decays to Ne-21 plus two electrons.

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1919

Movement of electric charges in matterMovement of electric charges in matter• A conductor: A conductor: An object or material in which charge can flow relatively freely. An object or material in which charge can flow relatively freely.

Example: metal, carbon, …Example: metal, carbon, …• An insulator: An insulator: An object or material in which charge does not flow freely. Example: An object or material in which charge does not flow freely. Example:

plastic, glass, …plastic, glass, …• To ground: To ground: Charge flows from a charged object to the ground, leaving the object Charge flows from a charged object to the ground, leaving the object

neutral. neutral. • The ground: The ground: A neutral object that can accept or supply an essentially unlimited A neutral object that can accept or supply an essentially unlimited

number of charges. The Earth functions as an electric ground. Application based number of charges. The Earth functions as an electric ground. Application based on these physics concepts: the lightning rod on tall buildings.on these physics concepts: the lightning rod on tall buildings.

Page 20: faraday law

2020

Electrostatics – forces between chargesElectrostatics – forces between charges• Unlike charges attract; Like charges repel.Unlike charges attract; Like charges repel.

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2121

Forces between charges – charge inductionForces between charges – charge induction• The force between charges provides a second way to charge up an object:The force between charges provides a second way to charge up an object: This This

process is call induction.process is call induction.• Charging an inductor:Charging an inductor:

• Charge rearrangement in insulators:Charge rearrangement in insulators:

Page 22: faraday law

2222

To quantitatively study the forces between charges, we introduce the law To quantitatively study the forces between charges, we introduce the law of this chapter:of this chapter:The Coulomb’s Law of forces between two point charges in vector form:The Coulomb’s Law of forces between two point charges in vector form:

PLAYACTIVE FIGURE

22120

0

0

2290

21

12

mNC 1085428

space. free ofty permittivi theis 4

1CmN 1098768

constant. Coulomb thecalled is to from directedr unit vecto theis

. of because experience force theis Here

/.

/.k

k.qq

qq

e

12

12

rF

Page 23: faraday law

2323

Discussions about Coulomb’s LawDiscussions about Coulomb’s Law• The term point charge refers to a particle of zero size that carries an electric The term point charge refers to a particle of zero size that carries an electric

chargecharge• The force is inversely proportional to the square of the separation r between the The force is inversely proportional to the square of the separation r between the

charges and directed along the line joining themcharges and directed along the line joining them• The force is proportional to the product of the charges, The force is proportional to the product of the charges, qq11 and and qq22, on the two , on the two

particlesparticles• The force is attractive if the charges are of opposite signThe force is attractive if the charges are of opposite sign• The force is repulsive if the charges are of like signThe force is repulsive if the charges are of like sign• Electrical forces obey Newton’s Third LawElectrical forces obey Newton’s Third Law

The force on The force on qq11 is equal in magnitude and opposite in direction to the force on is equal in magnitude and opposite in direction to the force on qq22

• With like signs for the charges, With like signs for the charges, the product the product qq11qq22 is positive and is positive and the force is repulsivethe force is repulsive

• With unlike signs for the charges, With unlike signs for the charges, the product the product qq11qq22 is negative and is negative and the force is attractivethe force is attractive

2112 FF

Page 24: faraday law

2424

The Superposition PrincipleThe Superposition Principle• The resultant force on any one charge equals the vector sum of the The resultant force on any one charge equals the vector sum of the

forces exerted by the other individual charges that are presentforces exerted by the other individual charges that are present• If there are four charges from If there are four charges from qq11 to to qq44, the resultant force on , the resultant force on qq11 is the is the

vector sum of all the forces exerted on it by other charges: vector sum of all the forces exerted on it by other charges: Remember to add forces as vectors: Remember to add forces as vectors:

Problem solving templateProblem solving template1 21 31 41 F F F F

TemplateStep 1, formulas or related concepts.Step 2, known quantities.Step 3, direct application of the formulas/concept or the condition to form an equation.Step 4, vector involved?Step 5, unit in the final answer correct? Answered all were asked?

Page 25: faraday law

2525

Example 1Example 1

X axis

Step 1, formula

Step 2, known quantities:x F

r F

221

x

221

:axis-X theAlong

, Law sCoulomb'

rqq

k

rqq

k

e

e

C. 10601electron an of charge theand constant The

m 3m 14 m, 6m )5(1 distances536

19

2312

321

.ek

rr,eq,eq,eq

e

Page 26: faraday law

2626

Step 3, direct application of the formula twice:

Step 4, vector involved? Yes, and the answer is given in vector form.

Step 5, unit? Answered all asked? Yes. SI is used. Unit Newton for force.

x

xFF F

xx F

xx F

(N)10005

(N) )10601)(3

356

36(10618

is 2 chargeon forcenet The

(N) 3

3510618

(N) 6

3610618

28

21922

1132122

211

223

2332

211

212

2112

.

..

ee.rqq

k

ee.rqq

k

e

e

Page 27: faraday law

2727

Example 2Example 2

Particle 1 and 2 carry the same amount of charge. What is the value of q for the particles to balance under the electrical and gravitational forces?The gravitational constant G = 6.67×10−11 N·m2/kg2

Step 1, formulas:

Step 2, known quantities:

221

221

221

221

F and F :only magnitude

Law sNewton' , Law sCoulomb'

rmm

Grqq

k

rmm

Grqq

k

e

e

r Fr F

ge

ge

Gk.r.mm e and Constants m, 001 kg, 00121

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