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ppt on quantum mechanics for engineering students
Typology: Lecture notes
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There are a few phenomenon which the classical mechanics
failed to explain.
Max Planck in 1900 at a meeting of German Physical
Society read his paper “On the theory of the Energy
distribution law of the Normal Spectrum”. This was the start
of the revolution of Physics i.e. the start of Quantum
Mechanics.
It is able to explain
The most outstanding development in modern science was
the conception of Quantum Mechanics in 1925. This new
approach was highly successful in explaining about the
behavior of atoms, molecules and nuclei.
The emission of electrons from a metal plate when illuminated
by light or any other radiation of any wavelength or frequency
(suitable) is called photoelectric effect. The emitted electrons
are called ‘photo electrons’.
V
Evacuated
Quartz
tube Metal
plate
Collecting
plate
Light
^^^^^^^^
A
+
_
electrons. At frequencies below a certain critical frequency
(characteristics of each particular metal), no electron is
emitted.
Voltage
Photo Current
v 1
v
2
v
3
The energy of a incident photon is utilized in two ways
known as photoelectric workfunction (W
o
).
electron.
2
2
1
mv
2
o
This is called Einstein’s photoelectric equation.
It is in form of. The graph with on y-axis
and on x-axis will be a straight line with slope
o o
eV h h
o
If is the stopping potential, then
max o
o
o
o
Einstein postulated the existence of a particle called a photon,
to explain detailed results of photoelectric experiment.
hc
E h
p
Photon has zero rest mass, travels at speed of light
Explains “instantaneous” emission of electrons in photoelectric
effect, frequency dependence.
From Theory of Relativity, total energy of the recoiled electron
with v ~ c is
2 2
E mc K m c
o
Similarly, momentum of recoiled electron is
2 2
K mc m c
o
2
2 2
2
m c
v c
m c
o
o
2 2
2
v c
K m c
o
2 2
1 v c
m v
mv
o
Now from Energy Conversation
cos
cos
2 2
v c
m v
c
h
c
h
o
2 2
2
v c
h h m c
o
From Momentum Conversation
(ii) along x-axis
sin
sin
2 2
v c
m v
c
h
o
(iii)
along y-axis
and
On squaring, we get
Subtracting (vi) from (vii)
(vii)
2 2
2 2
2
2
2 2
2 2
v c
m c
hm
c
h
m c
c
h
c
h
o
o o
( 1 cos ) 2 ( ') 0
2
2
o
hm
c
h
( 1 cos )
2
2
c
h
hm
o
( 1 cos )
2
c
h
m
o
But
is the Compton Shift.
c
( 1 cos )
h
m c
o
and
c
So,
( 1 cos )
h
m c
o
m c
h
o
It neither depends on the incident wavelength nor on the
scattering material. It only on the scattering angle i.e.
is called the Compton wavelength of the electron
and its value is 0.0243 Å.
o
( 1 cos ) 0.0243 (1- cosθ) Å
m c
h
o
max
So Compton effect can be observed only for radiation having
wavelength of few Å.
Compton effect can’t observed in Visible Light
is maximum when (1- cosθ) is maximum i.e. 2.
0.05 Å
For 1Å ~ 1%
For 5000Å ~ 0.001% (undetectable)
When a photon (electromagnetic energy) of sufficient
energy passes near the field of nucleus, it materializes into
an electron and positron. This phenomenon is known as pair
production.
In this process charge, energy and momentum remains
conserved prior and after the production of pair.
Photon
Nucleus (+ve)