FREE ELECTRON
THEORY
Introduction – Course Outcome and Syllabus of Module 1
 Intention of the module is to enable students to: Compare conductors,
semiconductors, dielectric and superconducting materials.
 Electrical Properties: Failures of classical free electron theory (CFT), postulates of
quantum free electron theory (QFT), merits of QFT, Fermi energy.
 Semiconductors: Fundamentals and types of semiconductors, p-n junction
formation, solar cells - working and efficiency of solar cells.
 Dielectric materials: Introduction, types of polarization in dielectrics (qualitative),
frequency and temperature dependence of polarization.
 Superconductivity: Introduction, Meissner effect, BCS theory, critical field, types of
superconductors.
 Total Duration: 12 Hours
 Blooms level selected: Comprehension
2
Importance of Electrical Properties to a budding engineer
 Copper, silicon and diamond. They are all crystalline but they have different electrical
conductivities.
 Why do they exhibit different properties? The answer will help us modify, produce, design
or engineer new materials which are special and exhibit exact properties that we require.
 This unit deals with some fundamental concepts of electrical conductivity.
3
Module 1: Electrical Properties – Classical Free Electron Theory
Classical Free Electron Theory
 Classical – the electron obey classical laws of Physics
 They are treated a gas molecules obeying the kinetic theory of gases.
4
Module 1: Electrical Properties – Classical Free Electron Theory
Postulates of Classical Free Electron Theory – 1
 Valence electrons of atoms are free to move through out the volume of
the metal, like the molecules of a perfect gas.
 The attraction between the free electrons and the lattice ions, and the
repulsion between the electrons themselves are ignored.
 The free electrons travel in a constant potential inside the metal but stay
confined within its boundaries.
 The movements of free electrons obey the laws of the classical kinetic
theory of gases, Therefore their average kinetic energy, ½ mvth
2 = 3/2 k T,
where vth is the thermal velocity, k, Boltzmann’s constant and T is
temperature.
5
Module 1: Electrical Properties – Classical Free Electron Theory
Electron movement in conductors
 Under the influence of electric field the randomly moving free
electrons drift in a direction opposite to the applied electric field and
acquire an additional velocity.
 The average velocity acquired by the free electron in the presence of
an applied electric field is known as Drift Velocity (νd)
6
Module 1: Electrical Properties – Classical Free Electron Theory
Fig 1 (a) Random motion of electron without external electric field
(b) Motion of electron with drift caused by external electric field
Some important quantities
 The average time taken by the free electron to reach steady state
velocity from zero velocity is called Relaxation Time (τr)
 The average distance travelled between two successive collisions, in
absence of an external electric field, is known as Mean Free Path (λ)
 The average time taken by a free electron between two successive
collisions is called as mean free time or Collision Time (τc)
 The average velocity of free electrons is called Root Mean Square
Velocity (νrms) or the thermal velocity of electrons.
 In this model, it is assumed that collision time (τc) is equal to
relaxation time (τr) and the thermal velocity (νrms) is equal to drift
velocity (νd).
7
Module 1: Electrical Properties – Classical Free Electron Theory
Ohm’s Law– microscopic form
 If electrons are free to move, what do they collide against?
 V= IR ohms law in macroscopic conditions
 𝑅 = ρ
𝐿
𝐴
 ρ is resistivity. Its inverse σ is conductivity
 Electric field developed across a metal is 𝑉 = 𝐸𝐿
 Current density 𝐽 =
𝐼
𝐴
 hence 𝐽 = σ𝐸 microscopic conditions
8
Module 1: Electrical Properties – Classical Free Electron Theory
Mobility and Mean free path
 Mobility is defined as the steady-state drift velocity per unit electric
field
 Mobility of an electron μ = 𝑣𝑑 / 𝐸
 μ = −𝑒 τ
𝑚
(𝑚2𝑉−1𝑠−1)
 σ =
𝑛𝑒2τ
𝑚
 Mean free Path (λ) is the average distance travelled by electrons
between collisions.
 λ = velocity*time = 𝑣𝑟𝑚𝑠 ∗ τ
9
Module 1: Electrical Properties – Classical Free Electron Theory
Success of Classical Free Electron Theory
 Explains electrical and thermal conductivities of most metals
10
Module 1: Electrical Properties – Classical Free Electron Theory
Failures of Classical Free Electron Theory-1
 CFET could not account for specific heat of metals
(The value of electronic specific heat is equal to 3R/2. while the actual
value is about 0.01 R only)
 Temperature dependence of σ=1/T and
 The dependence of electrical conductivity on free electron
concentration 𝝈 =
𝒏𝒆𝟐𝝉
𝒎
 n(Zn)= 13.1×1028/m3 n(Cu)= 8.45×1028/m3
σ(Zn)=1.09×107 /Ωm σ(Cu)= 5.88x 107 /Ωm
11
Module 1: Electrical Properties – Classical Free Electron Theory
Central Ideas of Quantum Free Electron Theory
 Quantum – available energy values are not continuous but quantized
 The distribution of electrons in the various allowed energy levels
occurs as per Pauli Exclusion Principle.
12
Module 1: Electrical Properties – Quantum Free Electron Theory
Postulates of Quantum Free Electron Theory
 Valence electrons of atoms are free to move through out the volume
of the metal, like the molecules of a perfect gas.
 The attraction between the free electrons and the lattice ions, and the
repulsion between the electrons themselves are ignored.
 The free electrons travel in a constant potential inside the metal but
stay confined within its boundaries.
 The energy values of the conduction electrons are quantized.
13
Module 1: Electrical Properties – Quantum Free Electron Theory
Fermi Energy and its importance
Fermi energy: It is the highest energy of the free electron at 0K.
Fermi energy EF level is the maximum energy level up to which electrons
can be filled at 0K.
Fermi level acts as a reference level that separates the vacant and filled
states at 0 K.
15
Module 1: Electrical Properties – Quantum Free Electron Theory
Advantages of Quantum Free Electron Theory
 It is successfully explains the electrical and thermal conductivity of
metals.
 Temperature dependence of conductivity of metals can be explained
by this theory.
 It explains the specific heat of metals.
 Phenomenon of thermionic emission can be explained by this theory.
16
Module 1: Electrical Properties – Quantum Free Electron Theory
Multiple Choice Questions - Recollection
 In classical free electron theory
Thermal velocity is equal to
a) Drift Velocity
b) Root mean square velocity
c) Zero velocity
d) Absolute velocity
 The velocity of electrons in a
copper wire is called as
a) Drift Velocity
b) Root mean square velocity
c) Zero velocity
d) Absolute velocity
17
Module 1: Electrical Properties – Example Questions
 With respect to the classical free electron
theory choose the right statement
a) energy values of the free electrons are
discontinuous
b) free electrons obey the Pauli’s exclusion principle
c) free electrons obey the laws of kinetic theory of
gases
d) Electrons can jump to the conduction band
Multiple Choice Questions - Recollection
 Thermal velocity can be expressed in terms of
a) Moles
b) microns/milliseconds
c) eV
d) m/s-1K-1
18
Module 1: Electrical Properties – Example Questions
Multiple Choice Questions - Comprehension
 What causes the random motion of electrons in quantum free electron
theory?
a) Applied electric field
b) Electric field produced by the neighbouring ions
c) Repulsion or collision by other electrons
d) Thermal energy
19
Module 1: Electrical Properties – Example Questions
Multiple Choice Questions - Comprehension
 With increase in temperature, the root mean square velocity of
electrons in classical free electron theory
a) Increases
b) Decreases slightly
c) Remains same
d) Decreases significantly
20
Module 1: Electrical Properties – Example Questions
Multiple Choice Questions - Comprehension
 Keeping temperature constant, electrons with lower degrees of freedom will have
root mean square velocities that are
a) Higher than electrons with higher degrees of freedom
b) Lower than electrons with higher degrees of freedom
c) Similar to electrons with higher degrees of freedom
d) Independent of the degrees of freedom
21
Module 1: Electrical Properties – Example Questions

Electrical conductivity

  • 1.
  • 2.
    Introduction – CourseOutcome and Syllabus of Module 1  Intention of the module is to enable students to: Compare conductors, semiconductors, dielectric and superconducting materials.  Electrical Properties: Failures of classical free electron theory (CFT), postulates of quantum free electron theory (QFT), merits of QFT, Fermi energy.  Semiconductors: Fundamentals and types of semiconductors, p-n junction formation, solar cells - working and efficiency of solar cells.  Dielectric materials: Introduction, types of polarization in dielectrics (qualitative), frequency and temperature dependence of polarization.  Superconductivity: Introduction, Meissner effect, BCS theory, critical field, types of superconductors.  Total Duration: 12 Hours  Blooms level selected: Comprehension 2
  • 3.
    Importance of ElectricalProperties to a budding engineer  Copper, silicon and diamond. They are all crystalline but they have different electrical conductivities.  Why do they exhibit different properties? The answer will help us modify, produce, design or engineer new materials which are special and exhibit exact properties that we require.  This unit deals with some fundamental concepts of electrical conductivity. 3 Module 1: Electrical Properties – Classical Free Electron Theory
  • 4.
    Classical Free ElectronTheory  Classical – the electron obey classical laws of Physics  They are treated a gas molecules obeying the kinetic theory of gases. 4 Module 1: Electrical Properties – Classical Free Electron Theory
  • 5.
    Postulates of ClassicalFree Electron Theory – 1  Valence electrons of atoms are free to move through out the volume of the metal, like the molecules of a perfect gas.  The attraction between the free electrons and the lattice ions, and the repulsion between the electrons themselves are ignored.  The free electrons travel in a constant potential inside the metal but stay confined within its boundaries.  The movements of free electrons obey the laws of the classical kinetic theory of gases, Therefore their average kinetic energy, ½ mvth 2 = 3/2 k T, where vth is the thermal velocity, k, Boltzmann’s constant and T is temperature. 5 Module 1: Electrical Properties – Classical Free Electron Theory
  • 6.
    Electron movement inconductors  Under the influence of electric field the randomly moving free electrons drift in a direction opposite to the applied electric field and acquire an additional velocity.  The average velocity acquired by the free electron in the presence of an applied electric field is known as Drift Velocity (νd) 6 Module 1: Electrical Properties – Classical Free Electron Theory Fig 1 (a) Random motion of electron without external electric field (b) Motion of electron with drift caused by external electric field
  • 7.
    Some important quantities The average time taken by the free electron to reach steady state velocity from zero velocity is called Relaxation Time (τr)  The average distance travelled between two successive collisions, in absence of an external electric field, is known as Mean Free Path (λ)  The average time taken by a free electron between two successive collisions is called as mean free time or Collision Time (τc)  The average velocity of free electrons is called Root Mean Square Velocity (νrms) or the thermal velocity of electrons.  In this model, it is assumed that collision time (τc) is equal to relaxation time (τr) and the thermal velocity (νrms) is equal to drift velocity (νd). 7 Module 1: Electrical Properties – Classical Free Electron Theory
  • 8.
    Ohm’s Law– microscopicform  If electrons are free to move, what do they collide against?  V= IR ohms law in macroscopic conditions  𝑅 = ρ 𝐿 𝐴  ρ is resistivity. Its inverse σ is conductivity  Electric field developed across a metal is 𝑉 = 𝐸𝐿  Current density 𝐽 = 𝐼 𝐴  hence 𝐽 = σ𝐸 microscopic conditions 8 Module 1: Electrical Properties – Classical Free Electron Theory
  • 9.
    Mobility and Meanfree path  Mobility is defined as the steady-state drift velocity per unit electric field  Mobility of an electron μ = 𝑣𝑑 / 𝐸  μ = −𝑒 τ 𝑚 (𝑚2𝑉−1𝑠−1)  σ = 𝑛𝑒2τ 𝑚  Mean free Path (λ) is the average distance travelled by electrons between collisions.  λ = velocity*time = 𝑣𝑟𝑚𝑠 ∗ τ 9 Module 1: Electrical Properties – Classical Free Electron Theory
  • 10.
    Success of ClassicalFree Electron Theory  Explains electrical and thermal conductivities of most metals 10 Module 1: Electrical Properties – Classical Free Electron Theory
  • 11.
    Failures of ClassicalFree Electron Theory-1  CFET could not account for specific heat of metals (The value of electronic specific heat is equal to 3R/2. while the actual value is about 0.01 R only)  Temperature dependence of σ=1/T and  The dependence of electrical conductivity on free electron concentration 𝝈 = 𝒏𝒆𝟐𝝉 𝒎  n(Zn)= 13.1×1028/m3 n(Cu)= 8.45×1028/m3 σ(Zn)=1.09×107 /Ωm σ(Cu)= 5.88x 107 /Ωm 11 Module 1: Electrical Properties – Classical Free Electron Theory
  • 12.
    Central Ideas ofQuantum Free Electron Theory  Quantum – available energy values are not continuous but quantized  The distribution of electrons in the various allowed energy levels occurs as per Pauli Exclusion Principle. 12 Module 1: Electrical Properties – Quantum Free Electron Theory
  • 13.
    Postulates of QuantumFree Electron Theory  Valence electrons of atoms are free to move through out the volume of the metal, like the molecules of a perfect gas.  The attraction between the free electrons and the lattice ions, and the repulsion between the electrons themselves are ignored.  The free electrons travel in a constant potential inside the metal but stay confined within its boundaries.  The energy values of the conduction electrons are quantized. 13 Module 1: Electrical Properties – Quantum Free Electron Theory
  • 14.
    Fermi Energy andits importance Fermi energy: It is the highest energy of the free electron at 0K. Fermi energy EF level is the maximum energy level up to which electrons can be filled at 0K. Fermi level acts as a reference level that separates the vacant and filled states at 0 K. 15 Module 1: Electrical Properties – Quantum Free Electron Theory
  • 15.
    Advantages of QuantumFree Electron Theory  It is successfully explains the electrical and thermal conductivity of metals.  Temperature dependence of conductivity of metals can be explained by this theory.  It explains the specific heat of metals.  Phenomenon of thermionic emission can be explained by this theory. 16 Module 1: Electrical Properties – Quantum Free Electron Theory
  • 16.
    Multiple Choice Questions- Recollection  In classical free electron theory Thermal velocity is equal to a) Drift Velocity b) Root mean square velocity c) Zero velocity d) Absolute velocity  The velocity of electrons in a copper wire is called as a) Drift Velocity b) Root mean square velocity c) Zero velocity d) Absolute velocity 17 Module 1: Electrical Properties – Example Questions  With respect to the classical free electron theory choose the right statement a) energy values of the free electrons are discontinuous b) free electrons obey the Pauli’s exclusion principle c) free electrons obey the laws of kinetic theory of gases d) Electrons can jump to the conduction band
  • 17.
    Multiple Choice Questions- Recollection  Thermal velocity can be expressed in terms of a) Moles b) microns/milliseconds c) eV d) m/s-1K-1 18 Module 1: Electrical Properties – Example Questions
  • 18.
    Multiple Choice Questions- Comprehension  What causes the random motion of electrons in quantum free electron theory? a) Applied electric field b) Electric field produced by the neighbouring ions c) Repulsion or collision by other electrons d) Thermal energy 19 Module 1: Electrical Properties – Example Questions
  • 19.
    Multiple Choice Questions- Comprehension  With increase in temperature, the root mean square velocity of electrons in classical free electron theory a) Increases b) Decreases slightly c) Remains same d) Decreases significantly 20 Module 1: Electrical Properties – Example Questions
  • 20.
    Multiple Choice Questions- Comprehension  Keeping temperature constant, electrons with lower degrees of freedom will have root mean square velocities that are a) Higher than electrons with higher degrees of freedom b) Lower than electrons with higher degrees of freedom c) Similar to electrons with higher degrees of freedom d) Independent of the degrees of freedom 21 Module 1: Electrical Properties – Example Questions

Editor's Notes

  • #2 NOTE: Want a different image on this slide? Select the picture and delete it. Now click the Pictures icon in the placeholder to insert your own image.