class_2_navamathavan_c1_c2_phy101
TRANSCRIPT
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Division of Physics
School of Advanced Sciences
Dr. R. Navamathavan
Physics Division
School of Advanced Sciences ( SAS)
Course: Modern Physics
PHY 101
1414--0707--20142014
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Division of Physics
School of Advanced Sciences
Course: Modern Physics
PHY 101
Electromagnetic Waves
Black Body Radiation
Planck Radiation Formula
OutlineOutline
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Introduction Black body radiation Limitations of classical theory
Rayleigh Jeans formula Statistical concepts (FD distributions)
Basic idea of quantization Plancks radiation - Compton effect
Experimental verification Dual nature of Electromagnetic radiation
de-Broglie waves - Davision Germer experiment Heissenberguncertainty principle - Schordinger equation (Time independent and
dependent) Particles in a 1D box Eigen values and Eigen functions
- Quantum Mechanical tunneling Scanning electron microscope -
Quantum confinement quantum well Wire Dots Introduction to
nanomaterials Moores law Properties of nanomaterials Carbons
nanotubes- Applications of nanotechnology in sensors
18 hours
Unit - IUnit - I
CAT - 1
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School of Advanced Sciences
Unit - IIUnit - II
12 hoursCAT - 2
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School of Advanced Sciences
Unit - IIIUnit - III
15 hoursTEE
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School of Advanced Sciences
Text BooksText Books
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School of Advanced Sciences
ReferencesReferences
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IntroductionIntroduction
Three Failures of Classical Physics:Three Failures of Classical Physics:1. Blackbody Radiation
2. The Photoelectric Effect
3. The Hydrogen Atom
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Some experimental facts:
1. The blackbody spectrum depends only on the temperature of the
object, and not on what it is made of. An iron horseshoe, a ceramic
vase, and a piece of charcoal --- all emit the same blackbody
spectrum if their temperatures are the same.
2. As the temperature of an object increases, it emits more blackbodyenergy at all wavelengths.
3. As the temperature of an object increases, the peak wavelength of
the blackbody spectrum becomes shorter (bluer). For example,
blue stars are hotter than red stars.
4. The blackbody spectrum always becomes small at the left-hand
side (the short wavelength, high frequency side).
Black Body RadiationBlack Body Radiation
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Any object with a temperature above absolute zero emits light at
all wavelengths. If the object is perfectly black (so it doesn't
reflect any light), then the light that comes from it is
called blackbody radiation.
The energy of blackbody radiation is not shared evenly by all
wavelengths of light.
The spectrum of blackbody radiation (below) shows that somewavelengths get more energy than others.
Black Body RadiationBlack Body Radiation
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Three spectra are shown, for three different temperatures.
(One of the curves is for the surface temperature of the Sun)
Black Body RadiationBlack Body Radiation
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When you listen to the radio,
watch TV, or cook dinner in a
microwave oven
Electromagnetic WavesElectromagnetic Waves
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Electromagnetic WavesElectromagnetic Waves
Waves in the electromagnetic
spectrum vary in size from very
long radio waves the size of
buildings, to very short gamma-rayssmaller than the size of the nucleus
of an atom.
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Electric and Magnetic Fields in EM WavesElectric and Magnetic Fields in EM Waves
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Interference of Water WavesInterference of Water Waves
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Origin of Interference PatternOrigin of Interference Pattern
Constructive interference occurs
when the difference in path lengths
from the slits to the screen is , 2,
3and so on
Destructive interference occurs
where the path difference is
/2, 3 /2, 5 /2and so on