1. The document discusses the electron theory of solids, which aims to explain the structures and properties of solids through their electronic structure.
2. It describes three main stages in the development of the electron theory of solids: the classical free electron theory developed in 1900, the quantum free electron theory developed in 1928, and Bloch's zone theory also developed in 1928, known as the band theory of solids.
3. The quantum free electron theory overcomes many drawbacks of the classical theory by applying quantum mechanics and using Fermi-Dirac statistics instead of Maxwell-Boltzmann statistics.
1. The Free Electron of Metal
G. Beyene (Ph.D) (ASTU) Chapter One Cover Page - 1/22 March - 2022
Chapter One
Gashaw Beyene (Ph.D)
March 2022
ASTU
2. The Free Electron of Metal
G. Beyene (Ph.D) (ASTU) Chapter One The Free Electronโฆ - 2/22 March - 2022
๏ The electron theory of solids aims to explain the
structures and properties of solids through their
electronic structure.
๏ The electron theory of solids has been developed in
three main stages.
1. The classical free electron theory:
Drude and Lorentz developed this theory in 1900. According to this theory,
the metals containing free electrons obey the laws of classical mechanics.
2. The quantum free electron theory:
Sommerfeld developed this theory during 1928. According to this theory,
the free electrons obey quantum laws.
2. The zone theory:
Bloch states this theory in 1928. According to this theory, the free electrons move in a periodic
field provided by the lattice. This theory is also called โBand theory of Solidsโ.
3. The Free Electron of Metal
G. Beyene (Ph.D) (ASTU) Chapter One The Free Electronโฆ - 3/22 March - 2022
๏ถ The classical free electron theory of metals (Drude-Lorentz theory of metals)
๏ฑPostulates
In an atom electrons revolve around the nucleus and a metal is
composed of such atoms.
a.
The valence electrons of atoms are free to move
about the whole volume of the metals like the
molecules of a perfect gas in container. The
collection of valance electrons from the all
atoms in a given pieces of metal forms electron
gas. It is free to move throughout the volume of
the metal.
b.
4. The Free Electron of Metal
G. Beyene (Ph.D) (ASTU) Chapter One The Free Electronโฆ - 4/22 March - 2022
These free electros move in random directions and collide with
either positive ions to the lattice or other free electrons. All the
collisions are elastic i.e., there is no loss of energy.
c.
The movement of free electrons obey the laws of the classical kinetic
theory of gases.
d.
The electron velocities in the metal obey the classical Maxwell-
Boltzmann distributions of velocities.
e.
The electrons move in a completely uniform potential field
due to its ions fixed in the lattice.
f.
When an electric field is applied to the metal, the free electrons
are accelerated in the direction opposite to the direction of
applied electric field.
g.
5. The Free Electron of Metal
G. Beyene (Ph.D) (ASTU) Chapter One The Free Electronโฆ - 5/22 March - 2022
1
2
๐๐ฃ๐ท
2
=
3
2
๐๐ต๐ ๐ฃ๐ท =
3๐๐ต๐
๐ At RT ๐ฃ๐ท โ 105๐๐ โ1
๏ถ Mean free path
๏ The average distance traveled by an electron between two successive collisions inside a metal in the
presence of applied field is known as mean free path (ฮป).
๏ถ Relaxation time
๏ The time taken by the electron to reach equilibrium position from its disturbed position in the
presence of an electric field is called relaxation time (ฯ).
ฮป = ฯ๐ฃ๐ท ฮป โ 1๐๐ ฯ โ 1 ร 10โ14
๐
๏ The average velocity (๐ฃ๐ท) of the free electrons with which they move towards the positive terminal
under the influence of the electrical field.
6. The Free Electron of Metal
G. Beyene (Ph.D) (ASTU) Chapter One The Free Electronโฆ - 6/22 March - 2022
๏ฑ Success of classical free electron theory:
1. It verifies Ohmโs law
2. It explains the electrical and thermal conductivity of metals
3. It drives Wiedemann-Franz law (i.e., the relation between
electrical conductivity and thermal conductivity).
4. It explains the optical properties of metals
๏ฑ Drawbacks of classical free electron theory:
๏ The phenomena such a photoelectric effect, Compton effect and the black body radiation couldnโt
be explained by classical free electron theory.
๏ According to classical free electron theory the value of specific heat of metals is given by 4.5๐ ๐ข is the
universal gas constant whereas the experimental value nearly equal to 3๐ ๐ข. Also according to this
theory the value of electric specific heat is equal to 1.5๐ ๐ข while the actual value is about 0.01๐ ๐ข.
7. The Free Electron of Metal
G. Beyene (Ph.D) (ASTU) Chapter One The Free Electronโฆ - 7/22 March - 2022
๏ Electrical conductivity of semiconductor or insulators couldnโt explained using this model.
๏ Through ๐ ๐๐ is a constant (Wiedemann-Franz law) according to classical free electron theory, it is
not a constant at low temperature.
๏ Ferromagnetism couldnโt be explained by this theory. The theoretical value of paramagnetic
susceptibility is greater than the experimental value.
๏ถ Electrical Conductivity
๏ In the presence of an electric field E, the electrons acquire a
drift velocity ๐ฃ๐ท which is superimposed on the thermal motion.
๏ Drude assumed that the probability that an electron collides with
an ion during a time interval ๐๐ก is simply proportional to ๐๐ก ฯ ,
where ฯ is called the collision time or relaxation time.
8. The Free Electron of Metal
G. Beyene (Ph.D) (ASTU) Chapter One The Free Electronโฆ - 8/22 March - 2022
๏ผ Then Newtonโs law gives ๐
๐๐ฃ๐ท
๐๐ก
+
๐ฃ๐ท
ฯ
= โ๐๐ธ
๏ The behavior of ๐ฃ๐ท(๐ก) as a function of time is given by
๐ฃ๐ท ๐ก = ๐ฃ๐ท(0)๐โ๐ก/ฯ ๏ง In the steady-state (where ๐๐ฃ๐ท ๐๐ก = 0), ๐ฃ๐ท is given by
๐ฃ๐ท = โ
๐๐ธฯ
๐
๏ The quantity ๐ฯ ๐ , the drift velocity per unit electric field, is called ๐, the drift mobility. The velocity
of an electron including both thermal and drift components is
๐ฃ = ๐ฃ๐ โ
๐๐ธฯ
๐
๏ง The current density caused by the electric
field ๐ธ is simply
๐ฝ = ๐โ1
๐๐๐
๐๐๐๐๐ก๐๐๐๐
(๐๐ฃ)
9. The Free Electron of Metal
G. Beyene (Ph.D) (ASTU) Chapter One The Free Electronโฆ - 9/22 March - 2022
But
๐๐๐
๐๐๐๐๐ก๐๐๐๐
๐ฃ๐ = 0
so that
๐ฝ = ๐โ1๐ โ๐ โ
๐๐ธฯ
๐
= ๐๐ธ
๏ Here ๐, the electrical conductivity, is equal to ๐0๐2
ฯ ๐ where ๐0 = ๐ ๐ is the electron concentration.
๏ถ WiedemannโFranz Law
๏ง The ratio of ๐ to ๐ is given by
๐
๐
=
1
3
๐ฃ๐
2ฯ๐ถ๐ฃ
๐0๐2ฯ ๐
๏ Now Drude applied the classical gas laws to evaluation of ๐ฃ๐
2 and ๐ถ๐ฃ, viz.,
1
2
๐๐ฃ๐
2
=
3
2
๐๐ต๐ and ๐ถ๐ฃ = ๐0(
3
2
๐๐ต).
This gave
๐
๐
=
3
2
๐๐ต
๐
2
๐ = ๐ฟ๐ where ๐ฟ =
3
2
๐๐ต
๐
2
is a constant and it is known as Lorentz number.
10. ๏ถ Quantum Free Electron Theory:
The Free Electron of Metal
G. Beyene (Ph.D) (ASTU) Chapter One The Free Electronโฆ - 10/22 March - 2022
๏ถ He developed this theory by applying the principles of quantum mechanics.
๏ It overcomes many of the drawbacks of classical theory.
๏ Sommerfeld explained them by choosing Fermi- Dirac statistics instead of Maxwell-Boltzmann
statistics.
๏ถ Assumptions of Quantum Free Electron Theory
๏ Valence electrons move freely in a constant potential within the boundaries of metal and is prevented from
escaping the metal at the boundaries (high potential). Hence the electron is trapped in a potential well.
๏ The distribution of electrons in various allowed energy levels occurs as per Pauli Exclusion Principle.
๏ The attraction between the free electrons and lattice ions and the repulsion between electrons themselves
are ignored.
11. ๏ To find the possible energy values of electron Schrodinger time independent wave equation is applied. The
problem is similar to that of particle present in a potential box.
The Free Electron of Metal
G. Beyene (Ph.D) (ASTU) Chapter One The Free Electronโฆ - 11/22 March - 2022
๏ The distribution of energy among the free electrons is according to Fermi-Dirac statistics.
๏ The energy values of free electrons are quantized.
energy of electron is ๐ธ๐ =
๐2โ2
8๐๐ฟ2 , where ๐ = 1, 2, 3, โฆ
๏ถ Merits of quantum free electron theory
๏ It successfully explains the electrical and thermal conductivity of metals.
๏ It can explain the Thermionic phenomenon.
๏ It explains temperature dependence of conductivity of metals.
12. ๏ It gives the correct mathematical expression for the thermal conductivity of metals.
The Free Electron of Metal
G. Beyene (Ph.D) (ASTU) Chapter One The Free Electronโฆ - 12/22 March - 2022
๏ It can explain the specific heat of metals.
๏ It explains magnetic susceptibility of metals.
๏ It can explain photo electric effect, Compton Effect and block body radiation etc.
๏ It is unable to explain the metallic properties exhibited by only certain crystals.
Demerits of quantum free electron theory
๏ It is unable to explain why the atomic arrays in metallic crystals should prefer certain structures only.
๏ This theory fails to distinguish between metal, semiconductor and Insulator.
๏ It also fails to explain the positive value of Hall Co efficient.
13. ๏ According to this theory, only two electrons are present in the Fermi level and they are responsible for
conduction which is not true.
The Free Electron of Metal
G. Beyene (Ph.D) (ASTU) Chapter One The Free Electronโฆ - 13/22 March - 2022
๏ถ Fermi Dirac Distribution:
๏ง As we know that for a metal containing N atoms, there will be N number of energy levels in each band.
๏ According to Pauliโs exclusion principle, each energy level can accommodate a maximum of two
electrons, one with spin up (+
1
2
) and the other with spin down (โ
1
2
).
๏ง At absolute zero temperature, two electrons with opposite spins will occupy the lowest available energy
level.
๏ง The next two electrons with opposite spins will occupy the next energy level and so on. Thus, the top most energy
level occupied by electrons at absolute zero temperature is called Fermi-energy level.
14. ๏ง The energy corresponding to that energy level is called Fermi energy.
The Free Electron of Metal
G. Beyene (Ph.D) (ASTU) Chapter One The Free Electronโฆ - 14/22 March - 2022
๏ง The energy of the highest occupied level at zero degree absolute is called Fermi energy, and the energy
level is referred to as the Fermi level. The Fermi energy is denoted as ๐ธ๐น.
๏ง At temperatures above absolute zero, the electrons get thermally
excited and move up to higher energy levels.
๏ง As a result there will be many vacant energy levels below as
well as above Fermi energy level.
15. ๏ง The function ๐(๐ธ) is called Fermi-factor and this gives the probability of occupation of a given energy level
under thermal equilibrium. The expression for ๐(๐ธ) is given by
๏ง Under thermal equilibrium, the distribution of electrons among various energy levels is given by statistical
function ๐(๐ธ).
The Free Electron of Metal
G. Beyene (Ph.D) (ASTU) Chapter One The Free Electronโฆ - 15/22 March - 2022
๐ ๐ธ =
1
1 + ๐
๐ธโ๐ธ๐น
๐พ๐
๏ผ where ๐(๐ธ) is called Fermi-Dirac distribution function or
Fermi factor, ๐ธ๐น is the Fermi energy, ๐พ is the Boltzmann
constant and ๐ is the temperature of metal under thermal
equilibrium.
Note:
1. The Fermi-Dirac distribution function ๐(๐ธ) is used to calculate the probability of an electron occupying
a certain energy level.
2. The distribution of electrons among the different energy levels as a function of temperature is known as
Fermi-Dirac distribution function.
16. The Free Electron of Metal
G. Beyene (Ph.D) (ASTU) Chapter One The Free Electronโฆ - 16/22 March - 2022
๏ถ Variation of Fermi factor with Energy and Temperature
Case 1:
๐(๐ฌ) for ๐ฌ < ๐ฌ๐ญ at ๐ป = ๐๐ฒ; from the probability function ๐(๐ธ) we have
๐ ๐ธ =
1
๐โโ + 1
=
1
0 + 1
= 1
๏ผ This implies that at absolute zero temperature, all the
energy levels below ๐ธ๐น are 100% occupied which is
true from the definition of Fermi energy.
Case 2:
๐(๐ฌ) for ๐ฌ > ๐ฌ๐ญ at ๐ป = ๐๐ฒ; from the probability function ๐(๐ธ) we have
๐ ๐ธ =
1
๐โ + 1
=
1
โ + 1
=
1
โ
= 0
๏ผ This implies that at absolute zero temperature, all the
energy levels above ๐ธ๐น are unoccupied (completely
empty) which is true from the definition of Fermi
energy.
17. The Free Electron of Metal
G. Beyene (Ph.D) (ASTU) Chapter One The Free Electronโฆ - 17/22 March - 2022
Case 3:
๐(๐ฌ) for ๐ฌ = ๐ฌ๐ญ at ๐ป = ๐๐ฒ; from the probability function ๐(๐ธ) we have
๐ ๐ธ =
1
๐0/0 + 1
= ๐๐๐๐๐ก๐๐๐๐๐๐๐ก๐
๐ ๐ฌ = โ for ๐ฌ = ๐ฌ๐ญ at ๐ป = ๐๐ฒ
๏ผ Hence, the occupation of Fermi level at ๐ = 0๐พ has an
undetermined value ranging between zero and unity (0 &
1). The Fermi-Dirac distribution function is
discontinuous at ๐ธ = ๐ธ๐น for ๐ = 0๐พ.
Case 4:
๐(๐ฌ) for ๐ฌ = ๐ฌ๐ญ at ๐ป > ๐๐ฒ; from the probability function ๐(๐ธ) we have
๐ ๐ธ =
1
๐0 + 1
=
1
1 + 1
=
1
2
๏ผ If ๐ธ < ๐ธ๐น, the probability starts decreasing from 1 and reaches 0.5
(1 2) at ๐ธ = ๐ธ๐น and for ๐ธ > ๐ธ๐น, it further falls off as shown in
figure. In conclusion, the Fermi energy is the most probable or
average energy of the electrons in a solid.
18. The Free Electron of Metal
G. Beyene (Ph.D) (ASTU) Chapter One The Free Electronโฆ - 18/22 March - 2022
๏ถ Homework
1. Find the probability of an electron occupying an energy level 0.02 eV above the Fermi level at 200 K
and 400 K in a material.
2. Find the temperature at which there is 1 % probability that a state with 0.5 eV energy above the Fermi
energy is occupied.
19. The Free Electron of Metal
G. Beyene (Ph.D) (ASTU) Chapter One The Free Electronโฆ - 18/22 March - 2022
๏ถ Density of states:
๏ถ Assignment 1, #1
1. Show that the sum of the probability of occupancy of an energy state at โE above the Fermi level and
that at โE below the Fermi level is unity.
20. End
G. Beyene (Ph.D) (ASTU) Chapter One End of chapter one - 22/22 March - 2022
Assignment I
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