engr-1600 materials science for engineers lecture 24: electrical conductivity 1
TRANSCRIPT
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ENGR-1600Materials Science for Engineers
Lecture 24: Electrical Conductivity
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• Copper vs. Aluminum wiring
Electrical Conductivity
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• Electrical conductivity between different materials varies by over 20 orders of magnitude
• The greatest variation of any physical property
Metals: > 105 (m)-1
Semiconductors: 10-6 < < 105 (m)-1
Insulators: < 10-6 (m)-1
Electrical Conductivity
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Macroscopic Ohm’s Law
Resistivity, ρ (m) and Conductivity, σ (m)-1
material properties are independent of sample size and geometry
VI
AoV: voltage (volts = joule/coulomb) VI: current (ampere = coulomb/sec) AR: resistance (ohm = volt/amp) Ω
Ohm’s Law
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Macroscopic Ohm’s Law
VI
AoV: voltage (volts = joule/coulomb) VI: current (ampere = coulomb/sec) AR: resistance (ohm = volt/amp) Ω
electric field
current density
(amp/m2)
*** Don’t confuse A for “ampere” with Ao for “cross-sectional area” ***
Ohm’s Law
Ohm’s Law
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Team Problem
What’s the difference between resistance and resistivity?
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Team Problem
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Electron Energy Band Structures• Pauli Exclusion Principle: no
two e- in an interacting system can have exactly same energy
• When N atoms are far apart, they do not interact, so electrons in a given shell in different atoms have same energy
• As atoms come closer together, they do interact, perturbing electron energy levels
• Electrons from each atom then have slightly different energies, producing a “band” of allowed energies
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Relating Energy Band Structures to Bonding
MetalsSemiconductors
Eg < 2 eVInsulators Eg > 2 eV
• In metals, highest occupied band is partially filled or bands overlap• Highest filled state at 0 K is the Fermi Energy, EF
• at 0 K, all e- states below EF are filled, all above are vacant• Electrons in a filled band cannot conduct• Only e- with energies above EF can conduct
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Conduction & Electron TransportMetals: • Empty energy states are adjacent to filled states• Thermal energy excites electrons into empty higher energy states• Hence, these electrons conduct electricity
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Energy Band StructuresSemiconductors / insulators: • highest occupied band is filled at 0 K • electronic conduction requires thermal excitation across a bandgap, T• EF is in the bandgap
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vd = eE = n e e
Microscopic Electric Conductivity
• When an electric field E is applied, e- experience a force. Hence, they accelerate.
• This force is counteracted by scattering events (analogy to friction).
• When the forces balance out, there is a constant mean value of e- velocity vd.
vd drift velocity [m/s] μ e- mobility [m2/Vs] n # of free electrons|e| charge of an e- [C]
• The vd is proportional to E by the factor μ, the “electron mobility”
due to imperfections in
the crystal
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metal >> semi
Conductivity of Metals and Semiconductors
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Resistivity of Metals
- grain boundaries- dislocations- impurities- vacancies
these all scatter electrons so that they take a less direct path lower σ
• Resistivity increases with
=
deformed Cu + 1.12 at%Ni
T (°C)-200 -100 0
1
2
3
4
5
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Resi
stivi
ty, ρ
(10
-8 O
hm-m
)
0
Cu + 1.12 at% Ni
“Pure” Cu
d -- % cold work
+ deformation
i
-- % impurity
+ impurityt
-- temperature T = o + aT
thermal
Cu + 3.32 at%Ni
Imperfections:
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Team Problem
Cold working Copper alloy causes an increase in resistivity.
Explain why.
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• Solid solution: i = A ci(1-ci)
• Two phases (+): i = V + V
Influence of Impurities
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Materials Choices for Metal Conductors
• Most widely used conductor is copper: inexpensive, abundant, very high
• Silver has highest of metals at RT, but use restricted due to cost
• Aluminum used to be main material for electronic circuits, transition to electrodeposited Cu
• Remember deformation reduces conductivity, so high strength generally means lower : trade-off.
• Heating elements require low (high R), and resistance to high temperature oxidation.
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Team Problem