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Conductors and Resistors Chapter 14

Conductors and Resistors

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Conductors and Resistors. Chapter 14. Imperfections solutes , vacancies , etc. dislocations grain boundaries act as scattering centres and thereby decrease the mean free path and thus decrease  . - PowerPoint PPT Presentation

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Page 1: Conductors and Resistors

Conductors and Resistors

Chapter 14

Page 2: Conductors and Resistors

Material Resistivity, Ohm m

Material Resistivity, Ohm m

Ag 1.6×10-8 Ni (com) 6.8×10-8

Cu (com) 1.7×10-8 S. Steel 7.1×10-7

Au 2.4×10-8 Nichrome 1.08×10-6

Al (com) 2.9×10-8 Graphite 1 ×10-5

Brass (70-30)

6.2×10-8 SiC 1 ×10-1

Page 3: Conductors and Resistors

Material Resistivity, Ohm m

Material Resistivity, Ohm m

SiC 1 ×10-1 Bakelite 107 - 1011

Ge, pure 4.5 ×10-1 Window glass

>1010

Si, pure 2.3 ×103 Ai2O3 1010-1012

Mica 1011-1015

Diamond >1014

SiO2 >1016

Page 4: Conductors and Resistors

Imperfections solutes, vacancies, etc.dislocationsgrain boundaries

act as scattering centres and thereby decrease the mean free path and thus decrease .Of all the imperfections, dissolved impurities (solutes) are more effective than the others as scattering centres.

Page 5: Conductors and Resistors

Phonons: elastic waves produced by the random vibrations of

atoms

Random nature destroys the ideal periodicity and interferes with the electron motion.

Conductivity thus decreases with increasing temperature.

Page 6: Conductors and Resistors

Cu-3%

Ni

Cu-2%

Ni

Pur

e Cu

Fig. 14.6

T

Experiment 9

Dependence of resistivity on temperature and composition

= T + r

= resitivity

T = thermal part of the resitivity

r =residual resitivity due to impurity and imperfections

Mattheissen’s Rule : T and r

are independent of each other; i.e., T depends only on tempearture and r depends only on compositon

Page 7: Conductors and Resistors

Applications

Conductors: Requirements

1. Low I2R loss

(High Conductivity)

2. Fabricability

3. Cost

4. Strength

Page 8: Conductors and Resistors

Candidate MaterialsLong distance transmission lines - Al- ACSR: Al conductor steel reinforced

Page 9: Conductors and Resistors

(Cu is more expensive)

Distribution lines, Bus bars, Energy Conversion Applications

- OFHC copper

Use of Cd as solute in improving the strength

Page 10: Conductors and Resistors

Electrical Requirements

Contacts: 1. High switches 2. High Thermal brushes

Conductivity

relays 3. High m.p.

4. Good Oxidation

Resistance

Page 11: Conductors and Resistors

Candidate Materials - Cu and Ag

Cu is cheaper

Ag, which is expensive, is preferred for critical contacts.

Strength of Ag is increased by dispersed CdO

(Dispersion Strengthening)

Absorbs heat by decomposing

Page 12: Conductors and Resistors

Resistors:Requirements

1. Uniform resistivity

2. Stable resistance

3. Small temp. Coefficient of resistivity

4. Low thermoelectric pot. w.r.t. copper

5. Good resistance to atmospheric corrosion

Page 13: Conductors and Resistors

Candidates:

Manganin (87% Cu, 13% Mn)

= 20 × 10-6 K-1 low as compare to that for Cu, which is 4000 × 10-6 K-1 .

Constantan (60% Cu, 40% Ni)

Ballast Resistors are used in circuits to maintain constant current – these must have high .

71% Fe, 29% Ni alloy is used

= 4500 × 10-6 K-1

Page 14: Conductors and Resistors

Heating RequirementsElements:1. High m.p.

2. High resistivity3. Good Oxidation Resistance4. Good Creep Strength5. Resistance to thermal fatigue

- low elastic modulus- low therm.

expansion

Page 15: Conductors and Resistors

CandidatesNichrome (80% Ni, 20% Cr)Kanthal (69% Fe, 23% Cr, 6% Al, 2% Co)

SiC

MoSi2Graphite in inert atmosphereMo, Ta Poor oxidation resistance

W (filaments) – ThO2 dispersion to improve creep resistance

Page 16: Conductors and Resistors

Resistance Thermometers:

Requirement - High Candidate - Platinum (pure metal)

Page 17: Conductors and Resistors

Superconductors

Section 14.5

Page 18: Conductors and Resistors

1. Phenomenon

Resistivity of silver

(1

0-11 o

hm m

)

T, K

Fig. 14.7 a

Page 19: Conductors and Resistors

Resistivity of tin

Can be used for producing large permanent magnetic field

(1

0-11 o

hm m

)

T, K

Fig. 14.7 b

Page 20: Conductors and Resistors

Loss of superconductivity

0 H

c, W

b m

-2

T, K Tc

Superconductor

Normal

Fig. 14.8

Page 21: Conductors and Resistors

The maximum current that a superconductor carries at a given temperature below Tc is limited by the magnetic field it produces at the surface of the superconductor

J c,

A m

-2

T, KTc

Superconductor

Normal

Fig not in book

Page 22: Conductors and Resistors

Meissner Effect

NormalSuperconductor

Fig. 14.9

T>Tc T<Tc

Page 23: Conductors and Resistors

BCS Theory (Bardeen, Cooper, Schreiffer)

Three way interaction between two electrons and a phonon

Electron pair (cooper pair):

The attractive interaction energy

The repulsive energy

Attraction is disrupted at T Tc

Page 24: Conductors and Resistors

2. Two types I and II of superconductors

-M -M

Type I Type II

Hc

HH

Hc1 Hc2

Page 25: Conductors and Resistors

Type II

Great practical interest because of high Jc.

This state is determined by the microstructural conditions of the material

Page 26: Conductors and Resistors

Heavily cold worked & recovery annealed

Cell walls of high dislocation density

Magnetic flux lines are pinned effectively

Fine grain size Grain boundaries

Pinning action

Dispersed fine precipitate

Interparticle spacing of about 300 Å

Pinning action

Page 27: Conductors and Resistors

Nb-40% Ti at 4.2 K, 0.9 Hc2

Microstructure Jc, A m-2

Recrystallised 105

Cold worked and recovery annealed

107

Cold worked and precipitation hardened

108

Page 28: Conductors and Resistors

3. Potential Applications

• Strong Magnets (50 Tesla)

MHD power generation

• Logic and Storage functions in computers

switching times 10 ps

• Levitation

transportation

Page 29: Conductors and Resistors

• Transmission

No I2R loss

Page 30: Conductors and Resistors

Yamanashi Maglev Test Line

Magnetic Levitation (Maglev) is a system in which the vehicle runs levitated from the tracks by using electromagnetic forces between superconducting magnets on board the vehicle and coils on the ground.

December 2, 2003, maximum speed 581 km/h (manned run).

Max speed of Rajdhani Express 140 km/h

Page 31: Conductors and Resistors

Magnetic Resonance Imaging

Page 32: Conductors and Resistors

4. New Developments

Nb3Ge 23 K 1976

La-Ba-Cu-O 34 K 1986,

Bednorz and

Muller

YBa2Cu3O7-x 90 K 1988

Page 33: Conductors and Resistors

Recipe: Y2O3, BaCO3, CuO

compacted powder in right proportion

is heated (900 - 1100°C)

BaCO3 BaO + CO2

Annealing at 800 °C in O2 atmosphere

The super conducting properties appear to be sensitive function of the oxygen content and, therefore, of the partial pressure of oxygen during heat treatment

Page 34: Conductors and Resistors

YBa2Cu3O7-x

Ba

Y

Cu

O

Page 35: Conductors and Resistors

Engineering aspects remain ElusiveReactive and Brittle

• Unable to support any significant stress• Cannot be easily formed or joined

Superconducting properties deteriorate during heating for forming purposes

Or even in humid room

Attempts

Explosive forming 50 000 atm (100°C)

Isostatic Pressing