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Muddiest Points
Muddiest Points:
• “What are band gaps and how do they relate to electronic
materials?”
• “Why is an insulator or semiconductor when heated, a
better conductor?”
• “How does grain size/grain boundary area affect
conductivity in metals and semiconductors?”
• “Calculations for number of charge carriers and what it
means.”
• “Relation of electron and electron-hole mobility to
conductivity.”
Electronic Properties I: Conductors,
Insulators, & Semiconductors
Conductivity Classifications
METALS (Ω-m)-1
Silver 6.8 x 107
Copper 6.0 x 107
Iron 1.0 x 107
SEMICONDUCTORS
(Ω-m)-1
Silicon 4 x 10-4
Germanium 2 x 100
GaAs 10-6
CERAMICS (Ω-m)-1
Soda-lime glass 10-10-10-11
Concrete 10-9
Aluminum oxide <10-13
POLYMERS (Ω-m)-1
Polystyrene <10-14
Polyethylene 10-15-10-17
*Values at Room Temperature
CONDUCTORS SEMICONDUCTORS INSULATORS
Band Structures
Conductors-Metals
ENERGY
Band Structures (Cont.)
Semiconductors Insulators
ENERGY
Electron and Hole Migration
ENERGY
- -+ +
Si4+
Si4+Si4+
What Affects Metal Conductivity?
Metals
Resistivity decreases with or
Conductivity increases with:
• Fewer Imperfections
o Grain Boundaries
o Impurity Atoms
o Dislocations
o Vacancies
• Decreasing temperature
Fewer imperfections
reduces scattering of
electrons
Smaller vibration
amplitude reduces
electron scattering
What Affects Semiconductor Conductivity?
Intrinsic Semiconductors
Resistivity decreases with or
Conductivity increases with:
• Larger Size of Grains or Less
Grain Boundary Area
o Only affects
polycrystalline
semiconductors
• Increasing temperature
Lower Grain
Boundary Area
reduces electron
scattering.
More Thermal Energy
creates more
electron-hole pairs
Conductivity Equation
𝛔 =
𝟏
𝛒
= 𝐧 𝐪 𝛍
General Form
σ = conductivity (ohm-m)-1
ρ = resistivity (ohm-m)
n = carrier density (# of carriers/m3)
q = electric charge 1.6x10-19 (C)
μ = mobility (m2/(V-s))
Conductivity Equation (Cont.)
𝛔 = 𝐧 𝐪 𝛍 𝒆
Metals
σ = conductivity (ohm-m)-1
n = carrier density (# of carriers/m3)
q = electric charge 1.6x10-19 (C)
μe = electron mobility (m2/(V-s))
Where does the charge carrier density
come from in a conductor?
𝒏 =
𝟏𝟎. 𝟒𝟗 𝒈
𝟏 𝒄𝒎 𝟑
∗
𝟏𝟎𝟎 𝟑
𝒄𝒎 𝟑
𝟏 𝒎 𝟑
∗
𝟏 𝒎𝒐𝒍
𝟏𝟎𝟕. 𝟗 𝒈
∗
𝟔. 𝟎𝟐 ∗ 𝟏𝟎 𝟐𝟑
𝑨𝒈 𝒂𝒕𝒐𝒎𝒔
𝟏 𝒎𝒐𝒍
∗
𝟏 𝒗𝒂𝒍𝒆𝒏𝒄𝒆 𝒆−
𝑨𝒈 𝒂𝒕𝒐𝒎
Ex: Charge Carrier Density of Silver (Ag)
𝒏 =
# 𝒂𝒕𝒐𝒎𝒔
𝟏 𝒎 𝟑
∗
# 𝒗𝒂𝒍𝒆𝒏𝒄𝒆 𝒆−
𝒂𝒕𝒐𝒎
𝐧 = 𝟓. 𝟗 ∗ 𝟏𝟎 𝟐𝟖
𝐯𝐚𝐥𝐞𝐧𝐜𝐞 𝐞−
/𝐦 𝟑
Example 1: Conductor
𝛔 = 𝐧 𝐪 𝛍 𝒆
Calculate the conductivity of the metal silver with
an electron mobility of 0.0057 (m2/(V-s)) and a
charge carrier density of 5.9 x 1028 per m3.
𝛍 𝒆= 0.0057 (m2/(V-s)) 𝒏 = 5.9 x 1028 m-3
𝛔 = (5.9 x 1028 m-3)(1.6x10-19 C)(0.0057 m2/(V-s))
𝛔 = 𝟓. 𝟑𝟖 𝐱 𝟏𝟎 𝟕
(Ω-m)-1
Conductivity Equation (Cont.)
𝛔 = 𝐧𝐪𝛍 𝒆 + 𝐩𝐪𝛍 𝒉
Intrinsic Semiconductors (n=p)
σ = conductivity (ohm-m)-1
ni = intrinsic carrier density (# of carriers/m3)
q = electric charge 1.6x10-19 (C)
μe = electron mobility (m2/(V-s))
μh = electron hole mobility (m2/(V-s))
𝛔 = 𝒏𝒊 𝒒(𝛍 𝒆 + 𝛍 𝒉)
Example 2: Semiconductor
Calculate the conductivity of intrinsic silicon with an
electron mobility of 0.14 (m2/(V-s)), hole mobility of
0.05 (m2/(V-s)), and an intrinsic charge carrier density of
1.3 x 1016 per m3.
𝛍 𝒆= 0.14 (m2/(V-s)) 𝛍 𝒉= 0.05 (m2/(V-s)) 𝒏𝒊= 1.3 x 1016 m-3
𝛔 = (1.3 x 1016 m-3)(1.6x10-19 C)(0.14 + 0.05) m2/(V-s)
𝛔 = 𝟑. 𝟗𝟓𝐱 𝟏𝟎−𝟒
(Ω-m)-1
𝛔 = 𝒏𝒊 𝒒(𝛍 𝒆 + 𝛍 𝒉)𝛔 = 𝐧𝐪𝛍 𝒆 + 𝐩𝐪𝛍 𝒉
Conductivity Equation (Cont.)
𝛔 = 𝐧𝐪𝛍 𝒆 + 𝐩𝐪𝛍 𝒉
Insulators (n=p)
σ = conductivity (ohm-m)-1
ni = intrinsic carrier density (# of carriers/m3)
q = electric charge 1.6x10-19 (C)
μe = electron mobility (m2/(V-s))
μh = electron hole mobility (m2/(V-s))
𝛔 = 𝒏𝒊 𝒒(𝛍 𝒆 + 𝛍 𝒉)
*There will not be an insulator example calculation due to extremely low conductivity.
Conductivity Comparison
• Conductor-Silver
– 𝟓. 𝟑𝟖 𝐱 𝟏𝟎 𝟕
(Ω-m)-1
– (5.9 x 1028 m-3)(1.6x10-19 C)(0.0057 m2/(V-s))
• Semiconductor-Silicon
– 𝟑. 𝟗𝟓 𝐱 𝟏𝟎−𝟒 (Ω-m)-1
– (1.3 x 1016 m-3)(1.6x10-19 C)(0.14 + 0.05) m2/(V-s)
• Insulator-Concrete & Polyethylene
– Concrete= 𝟏𝟎−𝟗 (Ω-m)-1
– Polyethylene= 𝟏𝟎−𝟏𝟓 − 𝟏𝟎−𝟏𝟕 (Ω-m)-1
Conductivity Classifications
METALS (Ω-m)-1
Silver 6.8 x 107
Copper 6.0 x 107
Iron 1.0 x 107
SEMICONDUCTORS
(Ω-m)-1
Silicon 4 x 10-4
Germanium 2 x 100
GaAs 10-6
CERAMICS (Ω-m)-1
Soda-lime glass 10-10-10-11
Concrete 10-9
Aluminum oxide <10-13
POLYMERS (Ω-m)-1
Polystyrene <10-14
Polyethylene 10-15-10-17
*Values at Room Temperature
CONDUCTORS SEMICONDUCTORS INSULATORS
Wrap-Up
• “What are band gaps and how do they relate to
electronic materials?”
• “Why is an insulator or semiconductor when
heated, a better conductor?”
• “How does grain size/grain boundary area affect
conductivity in metals and semiconductors?”
• “Calculations for number of charge carriers and
what it means.”
• “Relation of electron and electron-hole mobility
to conductivity.”
Electronic Properties I: Conductors,
Insulators, & Semiconductors

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MSEASUSlides: Muddiest points: Electronic Properties I

  • 1. Muddiest Points Muddiest Points: • “What are band gaps and how do they relate to electronic materials?” • “Why is an insulator or semiconductor when heated, a better conductor?” • “How does grain size/grain boundary area affect conductivity in metals and semiconductors?” • “Calculations for number of charge carriers and what it means.” • “Relation of electron and electron-hole mobility to conductivity.” Electronic Properties I: Conductors, Insulators, & Semiconductors
  • 2. Conductivity Classifications METALS (Ω-m)-1 Silver 6.8 x 107 Copper 6.0 x 107 Iron 1.0 x 107 SEMICONDUCTORS (Ω-m)-1 Silicon 4 x 10-4 Germanium 2 x 100 GaAs 10-6 CERAMICS (Ω-m)-1 Soda-lime glass 10-10-10-11 Concrete 10-9 Aluminum oxide <10-13 POLYMERS (Ω-m)-1 Polystyrene <10-14 Polyethylene 10-15-10-17 *Values at Room Temperature CONDUCTORS SEMICONDUCTORS INSULATORS
  • 5. Electron and Hole Migration ENERGY - -+ + Si4+ Si4+Si4+
  • 6. What Affects Metal Conductivity? Metals Resistivity decreases with or Conductivity increases with: • Fewer Imperfections o Grain Boundaries o Impurity Atoms o Dislocations o Vacancies • Decreasing temperature Fewer imperfections reduces scattering of electrons Smaller vibration amplitude reduces electron scattering
  • 7. What Affects Semiconductor Conductivity? Intrinsic Semiconductors Resistivity decreases with or Conductivity increases with: • Larger Size of Grains or Less Grain Boundary Area o Only affects polycrystalline semiconductors • Increasing temperature Lower Grain Boundary Area reduces electron scattering. More Thermal Energy creates more electron-hole pairs
  • 8. Conductivity Equation 𝛔 = 𝟏 𝛒 = 𝐧 𝐪 𝛍 General Form σ = conductivity (ohm-m)-1 ρ = resistivity (ohm-m) n = carrier density (# of carriers/m3) q = electric charge 1.6x10-19 (C) μ = mobility (m2/(V-s))
  • 9. Conductivity Equation (Cont.) 𝛔 = 𝐧 𝐪 𝛍 𝒆 Metals σ = conductivity (ohm-m)-1 n = carrier density (# of carriers/m3) q = electric charge 1.6x10-19 (C) μe = electron mobility (m2/(V-s))
  • 10. Where does the charge carrier density come from in a conductor? 𝒏 = 𝟏𝟎. 𝟒𝟗 𝒈 𝟏 𝒄𝒎 𝟑 ∗ 𝟏𝟎𝟎 𝟑 𝒄𝒎 𝟑 𝟏 𝒎 𝟑 ∗ 𝟏 𝒎𝒐𝒍 𝟏𝟎𝟕. 𝟗 𝒈 ∗ 𝟔. 𝟎𝟐 ∗ 𝟏𝟎 𝟐𝟑 𝑨𝒈 𝒂𝒕𝒐𝒎𝒔 𝟏 𝒎𝒐𝒍 ∗ 𝟏 𝒗𝒂𝒍𝒆𝒏𝒄𝒆 𝒆− 𝑨𝒈 𝒂𝒕𝒐𝒎 Ex: Charge Carrier Density of Silver (Ag) 𝒏 = # 𝒂𝒕𝒐𝒎𝒔 𝟏 𝒎 𝟑 ∗ # 𝒗𝒂𝒍𝒆𝒏𝒄𝒆 𝒆− 𝒂𝒕𝒐𝒎 𝐧 = 𝟓. 𝟗 ∗ 𝟏𝟎 𝟐𝟖 𝐯𝐚𝐥𝐞𝐧𝐜𝐞 𝐞− /𝐦 𝟑
  • 11. Example 1: Conductor 𝛔 = 𝐧 𝐪 𝛍 𝒆 Calculate the conductivity of the metal silver with an electron mobility of 0.0057 (m2/(V-s)) and a charge carrier density of 5.9 x 1028 per m3. 𝛍 𝒆= 0.0057 (m2/(V-s)) 𝒏 = 5.9 x 1028 m-3 𝛔 = (5.9 x 1028 m-3)(1.6x10-19 C)(0.0057 m2/(V-s)) 𝛔 = 𝟓. 𝟑𝟖 𝐱 𝟏𝟎 𝟕 (Ω-m)-1
  • 12. Conductivity Equation (Cont.) 𝛔 = 𝐧𝐪𝛍 𝒆 + 𝐩𝐪𝛍 𝒉 Intrinsic Semiconductors (n=p) σ = conductivity (ohm-m)-1 ni = intrinsic carrier density (# of carriers/m3) q = electric charge 1.6x10-19 (C) μe = electron mobility (m2/(V-s)) μh = electron hole mobility (m2/(V-s)) 𝛔 = 𝒏𝒊 𝒒(𝛍 𝒆 + 𝛍 𝒉)
  • 13. Example 2: Semiconductor Calculate the conductivity of intrinsic silicon with an electron mobility of 0.14 (m2/(V-s)), hole mobility of 0.05 (m2/(V-s)), and an intrinsic charge carrier density of 1.3 x 1016 per m3. 𝛍 𝒆= 0.14 (m2/(V-s)) 𝛍 𝒉= 0.05 (m2/(V-s)) 𝒏𝒊= 1.3 x 1016 m-3 𝛔 = (1.3 x 1016 m-3)(1.6x10-19 C)(0.14 + 0.05) m2/(V-s) 𝛔 = 𝟑. 𝟗𝟓𝐱 𝟏𝟎−𝟒 (Ω-m)-1 𝛔 = 𝒏𝒊 𝒒(𝛍 𝒆 + 𝛍 𝒉)𝛔 = 𝐧𝐪𝛍 𝒆 + 𝐩𝐪𝛍 𝒉
  • 14. Conductivity Equation (Cont.) 𝛔 = 𝐧𝐪𝛍 𝒆 + 𝐩𝐪𝛍 𝒉 Insulators (n=p) σ = conductivity (ohm-m)-1 ni = intrinsic carrier density (# of carriers/m3) q = electric charge 1.6x10-19 (C) μe = electron mobility (m2/(V-s)) μh = electron hole mobility (m2/(V-s)) 𝛔 = 𝒏𝒊 𝒒(𝛍 𝒆 + 𝛍 𝒉) *There will not be an insulator example calculation due to extremely low conductivity.
  • 15. Conductivity Comparison • Conductor-Silver – 𝟓. 𝟑𝟖 𝐱 𝟏𝟎 𝟕 (Ω-m)-1 – (5.9 x 1028 m-3)(1.6x10-19 C)(0.0057 m2/(V-s)) • Semiconductor-Silicon – 𝟑. 𝟗𝟓 𝐱 𝟏𝟎−𝟒 (Ω-m)-1 – (1.3 x 1016 m-3)(1.6x10-19 C)(0.14 + 0.05) m2/(V-s) • Insulator-Concrete & Polyethylene – Concrete= 𝟏𝟎−𝟗 (Ω-m)-1 – Polyethylene= 𝟏𝟎−𝟏𝟓 − 𝟏𝟎−𝟏𝟕 (Ω-m)-1
  • 16. Conductivity Classifications METALS (Ω-m)-1 Silver 6.8 x 107 Copper 6.0 x 107 Iron 1.0 x 107 SEMICONDUCTORS (Ω-m)-1 Silicon 4 x 10-4 Germanium 2 x 100 GaAs 10-6 CERAMICS (Ω-m)-1 Soda-lime glass 10-10-10-11 Concrete 10-9 Aluminum oxide <10-13 POLYMERS (Ω-m)-1 Polystyrene <10-14 Polyethylene 10-15-10-17 *Values at Room Temperature CONDUCTORS SEMICONDUCTORS INSULATORS
  • 17. Wrap-Up • “What are band gaps and how do they relate to electronic materials?” • “Why is an insulator or semiconductor when heated, a better conductor?” • “How does grain size/grain boundary area affect conductivity in metals and semiconductors?” • “Calculations for number of charge carriers and what it means.” • “Relation of electron and electron-hole mobility to conductivity.” Electronic Properties I: Conductors, Insulators, & Semiconductors