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Page 1: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Norah Ali Al-moneef1

Page 2: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Conductors & Semiconductors• In conductors, the valence band is only partially-full, so

electrons can easily move from being near one atom to being near another

• In semiconductors and insulators, the valence band is completely full, so electrons must gain extra energy to move

• In semiconductors, the band gap between the full valence band and the empty conduction band is small, so electrons move easily with only thermal energy

• In insulators, the band gap is larger, so electrons will not easily move into the conduction band

Norah Ali Al-moneef2

Page 3: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Conductors & Insulators• Electric current moves easily through some materials and less

easily through other materials• Materials that have very “tightly bound” electrons have few free

electrons when an electric force is applied. These materials are insulators (e.g. rubber, glass, dry wood)

• Materials that allow the movement of a large number of free electrons are called conductors (e.g., silver, copper, aluminum)

– Electrical energy is transferred through a conductor by means of the movement of free electrons that move from atom to atom

– Displaced electrons continue to “bump” each other

– The electrons move relatively slowly but this movement creates electrical energy throughout the conductor that is transferred almost instantaneously throughout the wire (e.g., billiard ball example, wind vs. sound example)

Norah Ali Al-moneef3

Page 4: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Electrons in an Electric Field

Norah Ali Al-moneef4

Conduction electrons move randomly in all directions in the absence of a field.

If a field is applied, the electric force results in acceleration in a particular direction:

F=ma= –eE a = –eE/mAs the charges accelerate, the potential

energy stored in the electric field is converted to kinetic energy which can be converted into heat and light as the electrons collide with atoms in the wire

This acceleration produces a velocityv = at = –eEt/m

Page 5: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

ELECTRON MOTION IN A CONDUCTOR WITH AND WITHOUT AN ELECTRIC FIELD

Norah Ali Al-moneef5

Page 6: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

27.1 Electric Current

Norah Ali Al-moneef6

Whenever electric charges move, an electric current is said to exist

The current is the rate at which the charge flows through a certain cross-section

For the current definition, we look at the charges flowing perpendicularly to a surface of area A

Charge in motion through an area A. The time rate of the charge flow through A defines the current (=charges per time):

Units:1 C/s= 1 A SI unit of the current: Ampere

Definition of the current:

t

QI av

Page 7: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Electrical current

Norah Ali Al-moneef7

If an electric field points from left to right, positive charge carriers will move toward therightwhile negative charges will move toward theleft

The result of both is a net flow of positive charge to the right.

Current is the net change in positive charge per time

t

QI av

Instantaneous current i = d q / d t

• Coulomb (C) – represents the total charge of approximately 6.25 x 1018 electrons

Page 8: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Norah Ali Al-moneef8

The direction of current flow is the direction positive charge would flowThis is known as conventional (technical)

current flow, i.e., from plus (+) to minus (-)However, in a common conductor, such as copper,

the current is due to the motion of the negatively charged electrons

It is common to refer to a moving charge as a mobile charge carrierA charge carrier can be positive or negative

Page 9: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Charge Carrier Motion in a Conductor

The electric field force F imposes a drift on an electron’s random motion (106 m/s) in a conducting material. Without field the electron moves from P1 to P2. With an applied field the electron ends up at P2’; i.e., a distance vdt from P2, where vd is the drift velocity (typically 10-4 m/s).

Norah Ali Al-moneef 9

Page 10: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Does the direction of the current depend on the sign of the charge? No!

(a) Positive charges moving in the same direction of the field produce the same positive current as (b) negative charges moving in the direction opposite to the field.

Norah Ali Al-moneef 10

E

E

vd

vd

qvd

(-q)(-vd) = qvd

Page 11: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Charged particles move through a conductor of cross-sectional area A

n is the number of charge carriers per unit volume V (=“concentration”)

nAx=nV is the total number of charge carriers in V

Norah Ali Al-moneef 11

The total charge is the number of carriers times the charge per carrier, q (elementary charge)

ΔQ = (nAΔx)q [unit: (1/m3)(m2 m)As=C]

Microscopic model of current

Page 12: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Norah Ali Al-moneef12

The drift speed, vd, is the speed at which the carriers movevd = Δx/Δt

Rewritten: ΔQ = (nAvdΔt)q

current, I = ΔQ/Δt = nqvdA

Δx

If the conductor is isolated, the electrons undergo (thermal) random motionWhen an electric field is set up in the conductor, it creates an electric force on the electrons and hence a current

Page 13: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Norah Ali Al-moneef13

coulombs of charge pass a point in a wire every two seconds. Calculate current.

Coulomb (C) – represents the total charge of approximately 6.25 x 1018 electrons

Unit of Current – Ampere (A) = 1coulomb/second

A 1.5C/s 1.5s 2

C 3

t

QI

Example:

Page 14: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Example:

Norah Ali Al-moneef14

An 18-gauge copper wire (diameter 1.02 mm) carries a constant current of 1.67 A to a 200 W lamp. The density of free electrons is 8.51028 per cubic meter. Find the magnitudes of (a) the current density

(b) the drift velocity. (a) A=d 2/4=(0.00102 m)2/4=8.210-7 m2

J=I /A=1.67 A/(8.210-7 m2)=2.0106 A/m2

(b) From J=I /A=nqvd

)C1060.1)(m105.8(

m/A100.219328

26

d

nq

Jv

vd=1.510-4 m/s=0.15 mm/s

Page 15: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Example:

15 Norah Ali Al-moneef

Page 16: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

• If 240 C of charge pass a point in a conductor in 5 min, what is the current through that point in the conductor?

Convert 5 min to seconds 5.0min X 60s/1 min = 300s

A 0.80 s 300

C 240

t

Q I

Example:

16 Norah Ali Al-moneef

Page 17: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

electrons 1061.2N 101.6

s 5835.0 t Q Q )

53.860 00.2

101.6 106.4

t

t

Q )

20.04

101.6 105.6

t

t

Q

19

19-

19-21

-1914

A

e

I

eNNeb

ANe

Ic

mANe

I

To the left

Example:

17 Norah Ali Al-moneef

Page 18: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

electrons 1061.2N 101.6

s 5835.0 t Q Q )

19

19-

A

e

I

eNNeb

As

CIa 835.0

00.2

67.1

t

Q )

ANe

Ic 53.860 00.2

101.6 106.4

t

t

Q )

19-21

Example:

18 Norah Ali Al-moneef

Page 19: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

II. Electric current1. Definition

t

QI

Units: [ I ] = 1A = 1 C/s

Conventional current

Electron flow

1020 electrons passed through the electric conductor during 4 seconds. Find the electric current through this conductor.

As

C

t

qI 4

4

)10)(106.1( 2019

CsAItq 5.0)1)(5.0( CsAItq 30)60)(5.0(

Example: The electric current of 0.5 A is flowing through the electric conductor. a) What electric charge is passing through the conductor during each second b) What electric charge will pass through the conductor during 1 minute?

a)

b)

Norah Ali Al-moneef19

Example:

Page 20: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

27.2 resistance

Norah Ali Al-moneef

Norah Ali Almoneef 20

• I = n q vd A– n = number of free charge carriers/unit volume

• Current density• (The current per unit cross-section is called the

current density J) :

• Ohm's Law: E = J J = σ E– = resistivity– = 1/ = conductivity– Good conductor: low and high

• Ohm's Law: – R = resistance Measured in Volt/Ampere = Ohm ()

dd nev

A

Avne

A

IJ

)(

20

Page 21: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

In a homogeneous conductor, the current density is uniform over any cross section, and the electric field is constant along the length.

Norah Ali Al-moneef 21

a

b

V=Va-Vb=EL The ratio of the potential drop to

the current is called resistance of the segment:

Unit: 1V/A= 1ohm

Resistance in a circuit arises due to collisions between the electrons carrying the current with the fixed atoms inside the conductor

Page 22: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Ohm’s Law

Norah Ali Al-moneef22

V I V=const .I V=RIOhm’s Law is an empirical relationship that is

valid only for certain materialsMaterials that obey Ohm’s Law are said to be

ohmicI=V/R R, I0, open circuit; R0, I, short circuit

• The ratio of the potential drop to the current is called resistance of the segment:

Unit: V/A=ohm

I

VR

Page 23: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Resistivity and ResistanceJ = E/ρ where ρ is the resistivity

I = V/R

Norah Ali Al-moneef23

Consider a bar or wire of cross-section A and length L, carrying current I and with potential difference V = Vb - Va between the ends.

I = V/R

and R = ρL/A is the resistance of the bar.

also called Ohm’s Law.

We know E = V/L so I/A = J = V/Lρ. Thus:

∆V = IR

Page 24: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Ohm’s Law, final

Plots of V versus I for (a) ohmic and (b) nonohmic materials. The resistance R=V/I is independent of I for ohmic materials, as is indicated by the constant slope of the line in (a). Norah Ali Al-moneef 24

Ohmic

Nonohmic

Page 25: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Norah Ali Al-moneef25

Ohmic Resistors• Metals obey Ohm’s Law linearly so long as their

temperature is held constant• Their resistance values do not fluctuate with

temperature• i.e. the resistance for each resistor is a constant

• Most ohmic resistors will behave non-linearly outside of a given range of temperature, pressure, etc.

Page 26: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

On What Does Resistance Depend?

• If I increase the length of a wire, the current flow decreases because of the longer path

• If I increase the area of a wire, the current flowincreases because of the wider path

R = L/A• If I change to a material with better

conductivity, the current flowincreases because charge carriers move better

• If I change the temperature, the current flowchangesNorah Ali Al-moneef26

Page 27: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

More on Resistance

I = V/R

Units of Resistivity : ρ is in Ω-m (ohm-meters), so R is in (Ω-m)(m)/(m2)

= Ω (ohms) = V/A (volts/ampere)

Resistivity ρ depends only upon the material (copper, silver…).

Resistance R depends upon the material and also upon the dimensions of the sample (L, A).

- R = ρL/A Note: Some devices (e.g.semiconductor diode) do not obey Ohm’s law!

Norah Ali Al-moneef27

Page 28: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Resistors are designed to have a specific resistance to reduce the amount of current going to a specific part of a circuit

To obey Ohm’s law means a conductor has a constant resistance regardless of the voltage.

V(Volts)

A(Amps)

R(Ohms)

28 Norah Ali Al-moneef

Page 29: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

29 Norah Ali Al-moneef

Page 30: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

V = IR = 2A x 3 = 6v

What voltage is required to produce 2a though a circuit with a 3 resistor.

V

3

I = 2a

Example:

30 Norah Ali Al-moneef

Page 31: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Resistance

I

V

I

V

Nonohmic device 2. Ohm’s Law

I

VR

IRV

Units: [ R ] = 1Ω = 1 V/A

constR Ohm’s Law:

R

VI

31 Norah Ali Al-moneef

Page 32: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Resistivity

L

AI

A

LR

L

AR

Definition:

Temperature dependence of resistivity

)(1 00 TTT

Example: What is the resistance of 1 m of nichrome wire of 2 mm diameter ?

)(

)(

00

000

TT

TTT

T

0

323

6 1018310

110

m

mm

A

LR

T

)( 00 TT 32 Norah Ali Al-moneef

Page 33: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Norah Ali Al-moneef33

The drift speed is much smaller than the average speed between collisions

When a circuit is completed, the electric field travels with a speed close to the speed of light

Although the drift speed is on the order of 10-4 m/s the effect of the electric field is felt on the order of 108 m/s

Page 34: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Drift Velocity• In a conductor the free electrons are moving very

fast in random directions (v ~ 106 m/sec)• They collide with the atoms of the lattice and are

scattered in random directions

• If an electric field is present, there is a slow net drift of electrons in the direction opposite the electric field

• vDRIFT ~ mm/secNorah Ali Al-moneef34

Page 35: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

• Amperes: the measure of the rate of current flow.– 6.24 × 1018 electrons passing a point per

second is equal to one amp.

• A current occurs whenever there is a source of electricity, conductors and a complete circuit.

Norah Ali Al-moneef35

Page 36: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Example

Norah Ali Al-moneef36

What is the current flow in a circuit with a voltage of 120 volts and a resistance of 0.23 ?

A 521.7= 0.23

V 120=

R

V=I

IR=V

ExampleWith the increase in the length of the wire, the current increases.A.TrueB.False

Page 37: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

V = IR

4v = I x 2

I = 2A

A 4v battery is placed in a series circuit with a 2 resistor.

What is the total current that will flow through the circuit?

4v

2

I = ?

Example

37 Norah Ali Al-moneef

Page 38: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

V= IR

V = 2A x 3

V = 6v

What voltage is required to produce 2A though a circuit with a 3 resistor.

V

3

I = 2A

Example

38 Norah Ali Al-moneef

Page 39: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

V = IR

12 = 4 x R

R = 3

What resistance is required to limit the current to 4 A if a 12 V battery is in the circuit?

12v

3

I = 4a

Example

39 Norah Ali Al-moneef

Page 40: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Example

Norah Ali Al-moneef40

A cylindrical copper rod has resistance R. It is reformed to twice its original length with no change of volume. Its new resistance is:

1. R

2. 2R

3. 4R

4. 8R

5. R/2

Page 41: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Norah Ali Al-moneef41

Two conductors are made of the same material and have the same length. Conductor A is a solid wire of diameter 1 mm. Conductor B is a hollow tube of inside diameter 1 mm and outside diameter 2 mm. The ratio of their resistances RA/RB is

1. 1/2

2. 1

3. 2

4. 3

5. 4B

A

Page 42: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Norah Ali Al-moneef42

Two cylinders are made of the same material and have the same length but different diameters. They are joined end-to-end and a potential difference is maintained across the combination. Which of the following quantities is the same for the two cylinders?

1. the potential difference

2. the current

3. the current density

4. the electric field

5. none of the above

Page 43: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Two cylindrical resistors, R1 and R2, are made of identical material. R2 has twice the length of R1 but half the radius of R1. They are connected to a battery V as shown. Compare the currents flowing through R1 and through R2.

A. I1 < I2 B. I1 = I2 C. I1 > I2

?/

2/

2

12

2

12

12

12

II

rA

rr

LL

4/12 AAA

LR

11

1

2

22 8

4/

2R

A

L

A

LR

VI1 I2

112

2 8

1

8I

R

V

R

VI

Norah Ali Al-moneef43

Example

Page 44: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Voltage and Current Relationship for Linear Resistors

Norah Ali Al-moneef44

Voltage versus Current for a 10 ohm Resistor

00.10.20.30.40.50.6

0 1 2 3 4 5 6

Voltage (V)

Cu

rre

nt

(A)

Voltage and current are linear when resistance is held constant.

Page 45: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Which one of the following graphs correctly represents Ohm's law, where V is the voltage and I is the current?

(a)A(b)B(c)C(d)D(e)A and C

45 Norah Ali Al-moneef

Page 46: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

If a piece of wire has a certain resistance, which wire made of the same material will have a lower resistance?

A )a hotter wire B ) a thicker wire C ) a longer wire D) a thinner wire

ANS: B

46 Norah Ali Al-moneef

Page 47: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Norah Ali Al-moneef47

27.4 Resistance and Temperature

The resistivity (and hence resistance) varies with temperature.

For metals, this dependence on temperature is linear over a broad range of temperatures.

An empirical relationship for the temperature dependence of the resistivity of metals is given by

Copper

)](1[ 00 TT

•Resistance (R) is proportional to resistivity (): R = L / A The resistivity () depends on temperature and the physical properties of the material, so it has a different value for each material

Page 48: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Norah Ali Al-moneef48

• Some materials, when very cold, have a resistivity which abruptly drops to zero. Such materials are called superconductors.

)(1 00 TTT )( 000 TTT

T

0

)( 00 TT

0

T

• is the resistivity at temperature T• 0 is the resistivity at some standard temperature T0

• is the “temperature coefficient” of electric resistivity for the material under consideration

• The temperature coefficient of resistivity can be expressed as.

Page 49: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Norah Ali Al-moneef49

• In everyday applications we are interested in the temperature dependence of the resistance of various devices.

• The resistance of a device depends on the length and the cross sectional area.

• These quantities depend on temperature• However, the temperature dependence of linear

expansion is much smaller than the temperature dependence of resistivity of a particular conductor.

• So the temperature dependence of the resistance of a conductor is, to a good approximation,

)(1 00 TTRR

where R0 and T0 are the resistance and temperature at a standard temperature, usually room temperature or 20o C.

Page 50: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Reminder: Battery as a “ski lift for charges”:

Ski lift raises objects to higher potential energy - flow may vary, but potential energy difference fixedBattery also fixed potential diff. , but current may vary

50 Norah Ali Al-moneef

Page 51: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

27.6 Electrical Power

• The chemical energy of the battery is converted to U, electrical potential energy: Echem U

• The resulting electric field causes the electrons to accelerate: UK

• Collisions in the lattice structure transfer the energy to the lattice as thermal energy: KEth

• Thermal energy is a dissipative energy (i.e. can’t be recovered like mechanical energy.

51 Norah Ali Al-moneef

Page 52: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

52 Norah Ali Al-moneef

Page 53: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

the rate at which the system loses electric potential energy as the charge Q passes through the resistor:

V I V Q

) V Q ( dt

d

dt

d

dt

du

53 Norah Ali Al-moneef

Page 54: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Electrical Energy = Voltage x Electrical Current x Time Interval

energy = V x I (amps) x t (sec)E = V x I x t

•The system regains this potential energy when the charge passes through the battery,• Since a resistor obeys Ohm’s Law:

PR = I2R = (∆VR)2/R

54 Norah Ali Al-moneef

Page 55: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

How is Electrical Power calculated?

Electrical Power is the product of the current (I) and the voltage (v)

The unit for electrical power is watt (W)

How much power is used in a circuit which is 110 volts and has a current of 1.36 amps?

P = I V Power = (1.36 amps) (110 V) = 150 W

Example

55 Norah Ali Al-moneef

Page 56: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

electrical energy: Electrical energy is a measure of the amount of power used and the time of use.Electrical energy is the product of the power and the time.

Example

energy = Power X time

P = I V

P = (2A) (120 V) = 240 W

E = (240 W) (4 h) = 960Wh = 0.96 kWh

Electrical Energy = Voltage x Electrical Current x Time Interval

energy = V x I (amps) x t (sec)E = V x I x t

56 Norah Ali Al-moneef

Page 57: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

a. 0.44 Ab. 2.25 Ac. 5 Ad. 36 A

ANS:

B

example

A 9-volt battery drives an electric current through a circuit with 4-ohm resistance. What is the electric current running through the circuit?

57 Norah Ali Al-moneef

Page 58: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

• Joule’s Law– States that the rate at which heat

produced in a conductor is directly proportional to the square of the current provided its resistance is constant

– i.e. P = I 2R In order to prevent power lines from

overheating, electricity is transmitted at a very high voltage

From Joule’s law the larger the current the more heat produced hence a transformer is used to increase voltage and lower current

i.e. P = V I 58 Norah Ali Al-moneef

Page 59: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Power dissipated by a bulb relates to the brightness of the bulb.

The higher the power, the brighter the bulb. For example, think of the bulbs you use at home. The

100W bulbs are brighter than the 50W bulbs.

59 Norah Ali Al-moneef

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Page 61: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

If an electric fire uses 1.8 MJ of energy in a time of 10 minutes, calculate the power output of the fire.

Energy = 1.8 MJ = 1.8x106 Jt=10 minutes = 600 sPower = Energy / time p = 1.8x106 J / 600 =3 10 3 watt

example

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Page 62: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Calculate the power of a vacuum cleaner if the operating voltage is 120v, and the current flowing

through it when it is used is 7.90A.

P = V x IP = 120V x 7.9AP = 948 W

example

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Page 63: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Calculate the voltage of a computer that has 600W of power and 1.9A flowing into the

monitor?

V = P I

V = 600W 1.9A

V = 316V

example

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Page 64: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

If a 500 watt speaker need 10 amps to operate, what is the voltage requirement?

example

VV

V

5010

500

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Page 65: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Example

• How much would you be charged for using a 60 Watt light bulb for 10 hours if electricity costs 0.07 $per kWh?

• E = PT= 0.06kW x 10h = 0.6kWh

• Cost = 0.6kWh x 0.07 $/kWh= 0.04$

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Page 66: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

If an electric fire uses 1.8 MJ of energy in a time of 10 minutes, calculate the power output of the fire.

E = 1.8 MJ = 1.8x106 Jt=10 minutes = 600 s

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Page 67: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Power• Power is the rate of doing work.• Electrical power is usually expressed in watts or

kilowatts• In DC and AC circuits, with resistance loads, power can be determined by:

• Examples of resistance loads are heaters and incandescent lamps.

Volts=V

Amps=I

Watts=P

IV=P

example

• Determine the power consumed by a resistor in a 12 volt system when the current is 2.1 amps.

W 25.2=V 12A x 2.1=IV=P

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Page 68: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

IVP

ELECTRIC POWER

When there is current in a circuit as a result of a voltage, the electricpower delivered to the circuit is:

SI Unit of Power: watt (W)

Many electrical devices are essentially resistors:

RIIRIP 2

R

VV

R

VP

2

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Page 69: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Rank in order, from largest to smallest, the powers Pa to Pd dissipated in resistors a to d.

1. Pb > Pa = Pc = Pd 2. Pb = Pc > Pa > Pc 3. Pb = Pd > Pa > Pc 4. Pb > Pc > Pa > Pd 5. Pb > Pd > Pa > Pc

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Page 70: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Example• Determine the amount of energy a 100

Watt light bulb will use when operated for 8 hours.

Energy=Power x Time

=100 watts x 8 hour

=800 wh

• What will it cost to operate the light bulb if the electrical energy costs 0.12 $/kWh?

$ =0.12 $

kWh x 800 W x

1 kW

1,000 W x 8 h =0.77 $

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Page 71: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Energy Use Calculations

How much electrical energy will an electric blanket use per month if it is used 8 hours a day? The blanket is on a 120 V circuit and draws 1.5 amp.

kWh 43.2= W1,000

kW 1 x

month

day 30 x

day

h 8 W xA) 1.5 x V (120=(kWh)Energy

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Page 72: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

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Energy = Power x Time

E = (100 W) (300 s)

E = 30,000 J

E = 30 kJ

Page 73: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

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Rated for 4.2 kWUsed 20 h/month

Cost of 12 $ per kWh

Energy = Power x Time

= (4.2 kW) x (20 h)

= 84 kWh

Cost = Energy x rate per kWh

= (84 kWh) x ($0.12)

= $10.08

Page 74: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

ExampleGiven copper wire 1mm diameter . 100m long has a

potential diffidence of 12 V Find

a) resistance, b) current in wire, c) current density,

d) electric field in wire, e) concentration of electrons (assuming 1electron / atm), f) drift velocity,

g) amount of electric charge flowing in 1 minute

Resistivity ρ = 1.72x10-8 Ohm-mDensity D = 8.9 E 3 kg/m3

molecular weight M = 63.546 g/moleAvogadro's # 6.022x10 23

electric charge e = 1.6x10-19 Cr = 5x10-4m radius, L=100m, t=60sec

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Page 75: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Equations: Answers:a) R= ρL/A, A=πr2 A=7.85x10-7, R=2.19

Ωb) V=IR I=V/R I=5.48 Ac) J=I/A J=6.977x106 A/m2

d) E = ρJ 0.12 V/me) n =D Na /M 8.434E28 e/m3

f) I = n q vd A vd = I/nqA = 5.17x10-4 m/s

g) I= dQ/dt Q = It = 329 C

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Page 76: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Example100 W light bulb connected to 110V what is a) current b) resistance c) at

10cents/kwhour how much to illuminate for a year, d) how many can be connected to a 15 ampere circuit breaker, e) how much electric power consumed by all these bulbs, f) if the temperature is 4500K and made from tungsten (α = 0.0038/K) what is the room temperature resistance at 300K

Given P=100 W, V= 100V Imax = 15A price = 0.1 $/kW h T=4500 K To = 300 Kα = 0.0038/K

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Page 77: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Equations Answersa) P = IV I=P/V = 0.909 Ab) V = IR R=V/I = 121 Ωc) cost = ($0.1)(.1KW)(24 x 365) = $87.60d) Imax> Nmax I Nmax = 16e) Pmax = Nmax P Pmax = 1600Wf) R=Ro(1 + α (T-To)) = Ro =

7.13 Ω

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OHM’S LAW FORMULAS

Current equalsvoltage dividedby resistance

Voltage equalscurrent multiplied

by resistance

Resistance equalsvoltage divided

by current

Find Current Find Voltage Find Resistance

summaryFind current: I=ΔQ/Δt I=nqAvd

Page 79: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

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Quantity Unit of Measure

FunctionName NameSymbol Symbol

Voltage V, emfor E

Voltage VPressure whichmakes currentflow

Current I Ampere A Rate of flowof electrons

Resistance R Ohm Opposition tocurrent flow

Page 80: Norah Ali Al-moneef 1 Conductors & Semiconductors In conductors, the valence band is only partially-full, so electrons can easily move from being near

Resistance related to physical parameters

The dimensions and geometry of the resistor as well as the particularmaterial used to construct a resistor influence its resistance. Theresistance is approximately given by

A

LR

Norah Ali Al moneef80

)(1 00 TTRR

)(1 00 TTT

IVP

RIP 2

R

VP

2