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ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

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Page 1: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

ELECTRICITY & MAGNETISM (Fall 2011)

LECTURE # 8

BY

MOEEN GHIYAS

Page 2: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

TODAY’S LESSON

(Resistance – Chapter 3)

Introductory Circuit Analysis by Boylested (10th Edition)

Page 3: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Today’s Lesson Contents

• Superconductors

• Types of Resistors

• Colour Coding and Standard Resistor Values

• Conductance

• Ohmmeters

• Thermistors

• Photoconductive Cells

• Varistors

Page 4: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Superconductors

• Research is on-going to develop a room-

temperature superconductor

• Implications so far-reaching that it is difficult to

forecast the vast impact

• Superconductors are conductors of

electric charge that, for all practical

purposes, have zero resistance

Page 5: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Superconductors

• In a conventional conductor, electrons travel at

average speeds in the neighbourhood of 1000 mi/s

• Einstein’s theory of relativity suggests that the

maximum speed of information transmission is the

speed of light, or 186,000 mi/s

• Relatively slow speed of conventional conduction is

due to collisions with other atoms in the material,

repulsive forces between electrons (like charges

repel), thermal agitation that results in indirect paths

Page 6: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Superconductors

• In the superconductive state, there is a pairing of

electrons, known as Cooper effect,

• There is an oscillation of energy between partners or

even “new” partners (as the need arises) to ensure

passage through the conductor at the highest possible

velocity with the least total expenditure of energy.

• Concept of superconductivity first surfaced in 1911

• For 74 years superconductivity could be established

only at temperatures colder than 23 K (-2500C).

Page 7: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Superconductors

• In 1986, Zurich Research Center found a ceramic

material, lanthanum barium copper oxide, that exhibited

superconductivity at 300 K

• In just a few short months, in USA the temperature was

raised to 950 K using a superconductor of yttrium

barium copper oxide

• Later, success has been achieved at 1250 K and 1620 K

( – 1110 C) using a thallium compound (unfortunately,

however, thallium is a very poisonous substance).

Page 8: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Superconductors

• Tremendous saving in the cooling expense since liquid

nitrogen is at least ten times cheaper than liquid helium

Page 9: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Superconductors

• The temperature at which a superconductor reverts

back to the characteristics of a conventional conductor

is called the critical temperature, denoted by Tc

Page 10: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Superconductors

• Superconductivity is currently applied in

– The design of 300-mi/h Meglev trains (trains that ride on a

cushion of air established by opposite magnetic poles)

– In powerful motors and generators

– In nuclear magnetic resonance imaging systems to obtain

cross-sectional images of the brain

– In the design of computers with operating speeds four

times that of conventional systems

– In improved power distribution systems

Page 11: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Types of Resistors

• Resistors are made in many forms, but all

belong in either of two groups:

• Fixed Resistors

– Resistance is fixed

• Variable Resistors

– Resistance is variable (but within a specified range)

Page 12: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Types of Resistors – Fixed Resistance

• The most common of the low-wattage, fixed type

resistors is the moulded carbon composition resistor.

• Resistors of this type are readily available in values

ranging from 2.7Ω to 22 MΩ.

Page 13: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Types of Resistors – Fixed Resistance

• The relative sizes of all fixed and

variable resistors change with the

wattage (power) rating, increasing

in size for increased wattage

ratings in order to withstand the

higher currents and dissipation

losses.

Page 14: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Types of Resistors – Fixed Resistance

• The temperature-versus-resistance curves for a 10kΩ-

and 0.5MΩ composition-type resistor are shown

• Note the small percent resistance change in the normal

temperature operating range.

Page 15: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Types of Resistors – Fixed Resistance

• Several other types of fixed resistors using high-

resistance wire or metal films are shown

Page 16: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Types of Resistors – Fixed Resistance

• The miniaturization of parts—used quite extensively in

computers

Page 17: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Types of Resistors – Fixed Resistance

• For use with printed circuit boards, fixed resistor

networks in a variety of configurations are available in

miniature packages

Page 18: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Types of Resistors – Variable Resistance

• Variable resistors, as the name implies, have a terminal

resistance that can be varied by turning a dial, knob,

screw, or whatever seems appropriate for the

application.

Page 19: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Types of Resistors – Variable Resistance

• Variable resistor can have two or three terminals, but

most have three terminals

• If the two- or three-terminal device is used as a variable

resistor, it is usually referred to as a rheostat

• If the three terminal device is used for controlling

potential levels, it is then commonly called a

potentiometer

• Even though a three-terminal device can be used as

a rheostat or potentiometer (depending on how it is

connected), it is typically called a potentiometer

Page 20: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Types of Resistors – Variable Resistance

• The symbol for a three-terminal potentiometer appears

in Fig (a)

• When used as a variable resistor (or rheostat), it can be

hooked up in one of two ways (b) and (c)

• The universally accepted symbol for a rheostat appears

in Fig (d)

Page 21: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Types of Resistors – Variable Resistance

• The resistance between the outside terminals a and c of

Fig (a) is always fixed at the full rated value of the

potentiometer, regardless of the position of the wiper

arm b (i.e. 1-MΩ potentiometer will always be 1 MΩ, no

matter how we turn the control element and move the

contact)

Page 22: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Types of Resistors – Variable Resistance

• The resistance can be varied from a minimum of 0Ω to

a maximum value of the potentiometer.

• The sum of the resistances between the wiper arm and

each outside terminal will equal the full rated resistance

of the potentiometer.

Page 23: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Types of Resistors – Variable Resistance

• Some commercially available potentiometers appear as

shown in fig

Page 24: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Types of Resistors – Variable Resistance

• When the device is used as a potentiometer,

the connections are as shown in Fig.

• It can be used to control the level of Vab, Vbc, or

both, depending on the application

Page 25: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Colour Coding and Standard Resistor Values

• On large size resistances it is

possible to print their values in

ohms on the casing.

• However, some resistance sizes

are too small to have numbers

printed on them, so a system of

colour coding is used.

• The colour bands are always read

from the end that has the band

closest to it.

Page 26: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Colour Coding and Standard Resistor Values

• The 1st and 2nd bands represent the first and second

digits, respectively

• The 3rd band determines the power-of-ten multiplier

for the first two digits (number of zeros that follow the

second digit) or a multiplying factor if gold or silver.

• The 4th band is the manufacturer’s tolerance (of the

precision) by which the resistor was made. If the 4th

band is omitted, tolerance is assumed to be ± 20%.

• The 5th band is a reliability factor, which gives the

percentage of failure per 1000 hours of use.

Page 27: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Colour Coding and Standard Resistor Values

Page 28: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Colour Coding and Standard Resistor Values

• Example – Find the range in which a resistor having the

following colour bands must exist to satisfy the

manufacturer’s tolerance:

a) 1st band 2nd band 3rd band 4th band 5th band

Gray Red Black Gold Brown

8 2 0 5% 1%

• Solution: 82Ω ± 5% (1% reliability)

• Since 5% of 82 = 4.10, the resistor should be within the

range 82Ω ± 4.10Ω , or between 77.90Ω and 86.10Ω .

Page 29: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Colour Coding and Standard Resistor Values

• Example – Find the range in which a resistor having the

following colour bands must exist to satisfy the

manufacturer’s tolerance:

a) 1st band 2nd band 3rd band 4th band 5th band

Orange White Gold Silver No

colour

3 9 0.1 10%

• Solution: 3.9Ω ± 10% = 3.9 ± 0.39Ω

• The resistor’s actual value should lie somewhere

between 3.51Ω and 4.29Ω .

Page 30: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Colour Coding and Standard Resistor Values

• One might expect that resistors

would be available for a full range

of values such as 10 Ω, 20 Ω, 30 Ω,

40 Ω, and so on. However, this is

not the case in actual

• There is a reason for the chosen

values, which is best demonstrated

by examining the list of standard

values of commercially available

resistors

Page 31: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Colour Coding and Standard Resistor Values

Page 32: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Conductance

• The reciprocal of the resistance of a material gives a

measure of how well the material will conduct

electricity

• The quantity is called conductance, has the symbol G,

and is measured in mhos or siemens (S)

• In equation form, conductance is

or

• i.e. increasing the area or decreasing either the length

or the resistivity will increase the conductance

Page 33: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Conductance

• Example – What is the relative increase or decrease

in conductivity of a conductor if the area is reduced by

30% and the length is increased by 40%? The

resistivity is fixed.

• Solution: We know that

• with the subscript ‘i’ for the initial value.

• Using the subscript ‘n’ for new value:

Page 34: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Ohmmeters

• The ohmmeter is an instrument used to :

1) Measure the resistance of individual or combined

elements

2) Detect open-circuit (high-resistance) and short-circuit

(low-resistance) situations

3) Check continuity of network connections and identify

wires of a multi-lead cable

4) Test some semiconductor (electronic) devices

Page 35: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Ohmmeters

• In general, the resistance of a resistor can be

measured by simply connecting the two leads of the

meter across the resistor, as shown

• There is no need to be concerned about which lead

goes on which end; the result will be the same in

either case since resistors offer the same resistance

to the flow of charge (current) in either direction.

Page 36: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Ohmmeters

• When measuring the resistance of a single resistor, it

is usually best to remove the resistor from the network

before making the measurement.

• If this is difficult or impossible, at least one end of the

resistor must not be connected to the network, or the

reading may include the effects of the other elements

of the system.

Page 37: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Ohmmeters

• A connectivity between two points can be checked with

the help of DMM / Ohmmeter as shown in fig

• If the resistance is zero, the connection is secure i.e.

shorted.

• If it is other than zero, the connection could be weak

• if reading is infinite, there is no connection at all.

Page 38: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Ohmmeters

• If one wire of a harness is known, a second can be

found as shown in Fig.

• Simply connect the end of the known lead to the end of

any other lead.

• When the ohmmeter indicates zero ohms (or very low

resistance), the second lead has been identified.

Page 39: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Ohmmeters

• Preliminary measurements of the condition of diode

and transistor can also be made using the ohmmeter.

Page 40: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Ohmmeters

• Important notes about the use of any

ohmmeter:

– Never hook up an ohmmeter to a live circuit!

• The reading will be meaningless and you may

damage the instrument.

• The ohmmeter section of any meter is designed to

pass a small sensing current through the resistance

to be measured. A large external current could

damage the movement and would certainly throw off

the calibration of the instrument.

Page 41: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Ohmmeters

• Important notes about the use of any

ohmmeter:

– Never store a VOM or a DMM in the resistance

mode.

• The two leads of the meter could touch and the small

sensing current could drain the internal battery.

• VOMs should be stored with the selector switch on

the highest voltage range, and the selector switch of

DMMs should be in the off position.

Page 42: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Thermistors

• A thermistor is a two-terminal

semiconductor device whose resistance is

temperature sensitive.

• A representative characteristic appears in

Fig with the graphic symbol for the device.

• Note the (negative temperature coefficient

behaviour) nonlinearity of the curve and

the drop in resistance from about 5000 Ω

to 100 Ω for an increase in temperature

from 20°C to 100°C

Page 43: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Thermistors

• Note that temperature of the device can be changed internally

or externally to control mechanisms.

• Materials used in the manufacture of thermistors include

oxides of cobalt, nickel, strontium, manganese

Page 44: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Photoconductive Cell

• The photoconductive cell is a two-terminal

semiconductor device whose terminal resistance is

determined by the intensity of the incident light on its

exposed surface.

• As the applied illumination increases in intensity, the

energy state of the surface electrons and atoms

increases, with a resultant increase in the number of

“free carriers” and a corresponding drop in resistance.

Page 45: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Photoconductive Cell

• Note the negative illumination coefficient in a typical set

of characteristics.

• Several cadmium sulfide photoconductive cells appear

in Fig on right.

Page 46: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Varistor

• Varistors are voltage-dependent, nonlinear resistors

used to suppress high-voltage transients;

• That is, their characteristics are such as to limit the

voltage that can appear across the terminals of a

sensitive device or system.

Page 47: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Varistor

• A typical set of characteristics

appears in Fig (a), along with a

linear resistance characteristic for

comparison purposes

• Note that at a particular “firing

voltage,” the current rises rapidly

but the voltage is limited to a level

just above this firing potential.

Page 48: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS

Summary / Conclusion

• Types of Resistors

– Fixed Resistors

– Variable Resistors

• Colour Coding and Standard Resistor Values

• Conductance

• Ohmmeters

• Thermistors, Photoconductive Cells, Varistors

Page 49: ELECTRICITY & MAGNETISM (Fall 2011) LECTURE # 8 BY MOEEN GHIYAS