SlideShare a Scribd company logo
1 of 26
Download to read offline
LIMITATIONS OF CLASSICAL MECHANICS Presentation
Centre For High Energy Physics
University Of The Punjab
_________________________________________________________________________________________________________
Presented To
Sir Ibrar
Presented By
Muhammad Awais Raza
3414ME
Msc 4th Eve
Where classical mechanics fails and
quantum mechanics arises?
Experimental results could not be explained by classical mechanics
Numerous places:
1. Black-Body radiation spectrum.
2. Photo-electric effect
3. Compton scattering.
4. Spectrum of hydrogen emissions
Result
In the development of Quantum Mechanics
treats electrons as both a particle and a wave.
All of the above can be easily explained by the
existence of 'quanta,' but are impossible to
explain through purely classical means.
Black Body Radiations
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.
Blackbody Radiation
Here are some experimental facts about blackbody radiation:
The Spectrum of Thermal Radiation depends on two types of characteristics of
Temperature and material Dependent
• With increase in temperature of material the amount of emitted radiation also
increase and wavelength decreases it means It emits more blackbody energy at
all wavelength.
• Spectrum of Thermal radiation depend upon shape and nature of material
The Explanation of Classical physics
1. Light is an electromagnetic wave that is produced
when an electric charge vibrates. Now recall that heat is just
the kinetic energy of random motion. In a hot object,
electrons vibrate in random directions and produce light as a
result. A hotter object means more energetic vibrations and
so more light is emitted by a hotter object --- it glows
brighter. So far, so good. But classical physics could not
explain the shape of the blackbody spectrum.
2. The electrons in a hot object can vibrate with a
range of frequencies, ranging from very few
vibrations per second to a huge . Classical physics
said that each frequency of vibration should have the
same energy. This means that, there should be no limit
to the energy of the light produced by the electrons
vibrating at high frequencies. WRONG!!
Experimentally, the blackbody spectrum always
becomes smaller. (short wavelength, high frequency).
At about 1900, Max Planck came up with the solution:
He proposed that
The classical idea that each frequency of vibration should have
the same energy must be wrong.
Instead, he said that energy is not shared equally by electrons
that vibrate with different frequencies. Planck said that energy
comes in clumps. He called a clump of energy a quantum. The
size of a clump of energy --- a quantum --- depends on the
frequency of vibration. Here is Planck's rule for the a quantum
of energy for a vibrating electron:
E = h f
where h, the calibration constant, is today called Planck's constant. Its value is about 6 x 10-34,
very tiny
So how does this explain the spectrum of blackbody radiation?
Planck said that an electron vibrating with a frequency f could only
have an energy of 1 hf, 2 hf, 3 hf, 4 hf, ... ; that is,
energy of vibrating electron = (any integer) x hf
But the electron has to have at least one quantum of energy if it
is going to vibrate. If it doesn't have at least an energy of 1hf,
it will not vibrate at all and can't produce any light . Planck
said: at high frequencies the amount of energy in a quantum, hf,
is so large that the high-frequency vibrations can never get
going! This is why the blackbody spectrum always becomes
small (high frequency) .
Photo Electric Effect
The Photoelectric Effect
When light shines on the surface of a metallic substance, electrons in
the metal absorb the energy of the light and they can escape from the
metal's surface. This is called the photoelectric effect, and it is used to
produce the electric current that runs many solar-powered devices.
Using the idea that light is a wave with the energy distributed evenly
throughout the wave, classical physicists expected that when using very
dim light, it would take some time for enough light energy to build up
to eject an electron from a metallic surface. WRONG!!
Experiments show that if light of a certain frequency can eject
electrons from a metal, it makes no difference how dim the light is.
There is never a time delay.
In 1905, Albert Einstein came up with the
solution. If Max Planck's idea that energy
comes in clumps (quanta) is correct, then light
must consist of a stream of clumps of energy.
Each clump of light energy is called a photon ,
said Einstein, and each photon has an energy
equal to
E = h f
Therefore the energy of light is not evenly
distributed along the wave, but is concentrated in
the photons. A dimmer light means fewer photons,
but simply turning down the light (without changing
its frequency) does not alter the energy of an
individual photon. So for a specific frequency
light, if a single photon has enough energy to
eject an electron from a metallic surface, then
electrons will always be ejected immediately after
the light is turned on and the photons hit the metal.
Compton Effect
Compton the Effect
The Compton effect states x-rays scattered by loosely bound electrons of target
element have reduce energy and frequency. This phenomenon describe scattering
between radiation and matter and confirm the particle nature of light.
Classical Wave Theory
The X-ray are electro magnetic waves generated due to oscillation of electric-
field and magnetic-field .When such X-ray waves having frequency “f” fall on
target electrons ,the electrons start to oscillate with same frequency “f ”. The
oscillating electrons must radiate electromagnetic waves which have again same
frequency “f”.
It means scattered beam of X-ray and incident beam of X-ray should have same
frequency and same wavelength but spectrum of results of Compton Effect shows
that scattered beam has intensity peak at two wavelengths . Therefore classical
wave theory fails to explain experimental results of Compton effects.
Quantum Mechanics
Compton explained his experimental results by postulating
that incident X-rays beam is assembly of photons having
energy E = h f . These photons make collisions with free
electrons in the scattering target .The scattered radiation
consist of recoiling photons emerging from the target.
The incident photon transfer some of its energy to the free
electron during collision so scattered photon must have
reduced energy . It means scattered photon has large
wavelength than incident photon . This explains the
wavelength shift in spectrum of Compton effect.
Spectrum of hydrogen emissions
The Hydrogen Atom
When a small tube of hydrogen gas is heated, it begins to glow and
emit light. Unlike the blackbody radiation that comes from a hot
dense solid or gas, this light consists of just a few colors (wavelengths):
a red hydrogen, since it is the simplest atom. Hydrogen consists of a
positively charged proton at the center, with a negatively charged
electron orbiting around it. The electrical attraction between the
positive proton and the negative electron keeps the electron in orbit,
just like the gravitational attraction between the Sun and the Earth
holds the Earth in orbit. There was just one problem.
wavelength, a turquoise, and several violets. Classical physicists at the
beginning of the century thought they should certainly be able to
understand
Classical physics said that the orbiting electron is constantly
changing direction, it should emit electromagnetic radiation ---
light. As a result, the electron should be continually losing
energy. In fact, physicists calculated that the electron should
lose all of its energy and spiral down into the proton in only
about 0.000000000001 second! In other words, atoms should
not exist longer than a mere 10-12 seconds. WRONG!!
Niels Bohr provided an explanation in 1913. In the Bohr model of the
hydrogen atom, There are only certain allowed orbits, and each allowed
orbit has a certain radius and a certain energy. Bohr invented a rule that
allowed him to calculate the size and energy of each orbit. If you are
curious, Bohr's rule said that
2π x (electron mass) x (electron orbital speed) x (orbit radius) = (any integer) x h
which is not too obvious, to say the least! (The integer would be 1 for the
smallest orbit, 2 for the next orbit out, and so on.) Bohr also made up a new
rule to explain the stability of the hydrogen atom --- he said that when an
electron is in an allowed orbit, the electron will not produce electromagnetic
radiation. Bohr did not explain why, he just proposed a new law of nature.
And nature agreed with Niels Bohr. His new model of hydrogen gave
wavelengths for hydrogen gas that precisely agreed with what was
measured.
Question: If the electrons do not produce light when they are in their allowed
stable orbits, where is the source of the light that comes from hydrogen?
Answer:
According to Bohr, electrons have more energy when they are in larger orbits. If
an electron falls from a larger orbit down to a smaller orbit, it loses energy.
According to the law of conservation of energy, the energy lost by the electron
must go somewhere. Bohr explained that a photon carries away the lost energy
from the hydrogen atom; that is,
photon energy = (electron energy in larger orbit) - (electron energy in smaller orbit)
It works the other way, too. If a photon strikes an atom, the atom can absorb the
photon and its energy if (and only if) the photon's energy is exactly equal to the
difference between two orbital energies. In this case, an electron uses the
photon's energy to jump from the smaller orbit up to the larger orbit. This is
called a quantum jump.
The electron falls down to a lower
orbit and the atom loses energy.
A photon carries away the energy
lost by the atom.
A photon is absorbed by the atom, which
gains the photon’s energy. The electron uses
this energy to jump up to a higher orbit.
Limitations OF Classical Physics and Birth Of Quantum Mechanics

More Related Content

What's hot

Quantum Mechanics Presentation
Quantum Mechanics PresentationQuantum Mechanics Presentation
Quantum Mechanics Presentation
Jasmine Wang
 
Quantum mechanics
Quantum mechanics Quantum mechanics
Quantum mechanics
Kumar
 
6563.nuclear models
6563.nuclear models6563.nuclear models
6563.nuclear models
akshay garg
 
Statistical mechanics
Statistical mechanics Statistical mechanics
Statistical mechanics
Kumar
 
Particle in a box- Application of Schrodinger wave equation
Particle in a box- Application of Schrodinger wave equationParticle in a box- Application of Schrodinger wave equation
Particle in a box- Application of Schrodinger wave equation
Rawat DA Greatt
 

What's hot (20)

Schrodinger's time independent wave equation
Schrodinger's time independent wave equationSchrodinger's time independent wave equation
Schrodinger's time independent wave equation
 
Quantum Mechanics Presentation
Quantum Mechanics PresentationQuantum Mechanics Presentation
Quantum Mechanics Presentation
 
Quantum Chemistry
Quantum ChemistryQuantum Chemistry
Quantum Chemistry
 
statistic mechanics
statistic mechanicsstatistic mechanics
statistic mechanics
 
Band theory of solids
Band theory of solidsBand theory of solids
Band theory of solids
 
Quantum mechanics
Quantum mechanics Quantum mechanics
Quantum mechanics
 
6563.nuclear models
6563.nuclear models6563.nuclear models
6563.nuclear models
 
Statistical mechanics
Statistical mechanics Statistical mechanics
Statistical mechanics
 
Introduction to molecular spectroscopy
Introduction to molecular spectroscopyIntroduction to molecular spectroscopy
Introduction to molecular spectroscopy
 
Lecture7
Lecture7Lecture7
Lecture7
 
Nuclear Shell models
Nuclear Shell modelsNuclear Shell models
Nuclear Shell models
 
Schrodinger equation and its applications: Chapter 2
Schrodinger equation and its applications: Chapter 2Schrodinger equation and its applications: Chapter 2
Schrodinger equation and its applications: Chapter 2
 
Photochemistry
PhotochemistryPhotochemistry
Photochemistry
 
Introduction to quantum mechanics and schrodinger equation
Introduction to quantum mechanics and schrodinger equationIntroduction to quantum mechanics and schrodinger equation
Introduction to quantum mechanics and schrodinger equation
 
Particle in a box- Application of Schrodinger wave equation
Particle in a box- Application of Schrodinger wave equationParticle in a box- Application of Schrodinger wave equation
Particle in a box- Application of Schrodinger wave equation
 
Lect. 23 rotational vibrational raman spectroscopy
Lect. 23 rotational   vibrational raman spectroscopyLect. 23 rotational   vibrational raman spectroscopy
Lect. 23 rotational vibrational raman spectroscopy
 
Nonstoichiometric defects
Nonstoichiometric defectsNonstoichiometric defects
Nonstoichiometric defects
 
Quantum chemistry ppt
Quantum chemistry pptQuantum chemistry ppt
Quantum chemistry ppt
 
Introduction statistical thermodynamics.pptx
Introduction statistical thermodynamics.pptxIntroduction statistical thermodynamics.pptx
Introduction statistical thermodynamics.pptx
 
Photochemistry by Shakti
Photochemistry by ShaktiPhotochemistry by Shakti
Photochemistry by Shakti
 

Viewers also liked

Delay-Differential Equations. Tools for Epidemics Modelling
Delay-Differential Equations. Tools for Epidemics ModellingDelay-Differential Equations. Tools for Epidemics Modelling
Delay-Differential Equations. Tools for Epidemics Modelling
Ignasi Gros
 
Compton effect and pair production
Compton effect and pair productionCompton effect and pair production
Compton effect and pair production
Pramod Tike
 

Viewers also liked (20)

Simple harmonic oscillator - Classical Mechanics
Simple harmonic oscillator - Classical MechanicsSimple harmonic oscillator - Classical Mechanics
Simple harmonic oscillator - Classical Mechanics
 
quantum view of Harmonic oscillator
quantum view of Harmonic oscillator quantum view of Harmonic oscillator
quantum view of Harmonic oscillator
 
Harmonic oscillator
Harmonic oscillatorHarmonic oscillator
Harmonic oscillator
 
How the Bohr Model of the Atom Accounts for Limitations with Classical Mechan...
How the Bohr Model of the Atom Accounts for Limitations with Classical Mechan...How the Bohr Model of the Atom Accounts for Limitations with Classical Mechan...
How the Bohr Model of the Atom Accounts for Limitations with Classical Mechan...
 
Organic Nanoparticles (ONPs)
Organic Nanoparticles (ONPs)Organic Nanoparticles (ONPs)
Organic Nanoparticles (ONPs)
 
Lecture 10: Schrodinger and Particle in Box
Lecture 10: Schrodinger and Particle in BoxLecture 10: Schrodinger and Particle in Box
Lecture 10: Schrodinger and Particle in Box
 
Particle Physics & Beyond Physics
Particle Physics & Beyond PhysicsParticle Physics & Beyond Physics
Particle Physics & Beyond Physics
 
History of Physics (Classical Mechanics)
History of Physics (Classical Mechanics)History of Physics (Classical Mechanics)
History of Physics (Classical Mechanics)
 
Bohr model
Bohr modelBohr model
Bohr model
 
The SIR Model and the 2014 Ebola Virus Disease Outbreak in Guinea, Liberia an...
The SIR Model and the 2014 Ebola Virus Disease Outbreak in Guinea, Liberia an...The SIR Model and the 2014 Ebola Virus Disease Outbreak in Guinea, Liberia an...
The SIR Model and the 2014 Ebola Virus Disease Outbreak in Guinea, Liberia an...
 
Classical inference in/for physics
Classical inference in/for physicsClassical inference in/for physics
Classical inference in/for physics
 
Bohr's model
Bohr's modelBohr's model
Bohr's model
 
Pathria statistical mechanics
Pathria statistical mechanicsPathria statistical mechanics
Pathria statistical mechanics
 
Classical Physics
Classical PhysicsClassical Physics
Classical Physics
 
Quick run through on classical mechancis and quantum mechanics
Quick run through on classical mechancis and quantum mechanics Quick run through on classical mechancis and quantum mechanics
Quick run through on classical mechancis and quantum mechanics
 
Delay-Differential Equations. Tools for Epidemics Modelling
Delay-Differential Equations. Tools for Epidemics ModellingDelay-Differential Equations. Tools for Epidemics Modelling
Delay-Differential Equations. Tools for Epidemics Modelling
 
Markov chain and SIR epidemic model (Greenwood model)
Markov chain and SIR epidemic model (Greenwood model)Markov chain and SIR epidemic model (Greenwood model)
Markov chain and SIR epidemic model (Greenwood model)
 
Ludwig Boltzmann-moartea termică a universului
Ludwig Boltzmann-moartea termică a universuluiLudwig Boltzmann-moartea termică a universului
Ludwig Boltzmann-moartea termică a universului
 
Fisika Modern (10) statistical physics
Fisika Modern (10) statistical physicsFisika Modern (10) statistical physics
Fisika Modern (10) statistical physics
 
Compton effect and pair production
Compton effect and pair productionCompton effect and pair production
Compton effect and pair production
 

Similar to Limitations OF Classical Physics and Birth Of Quantum Mechanics

Chapter 4 electrons in atoms
Chapter 4 electrons in atomsChapter 4 electrons in atoms
Chapter 4 electrons in atoms
tanzmanj
 
19_quantum [Autosaved].ppt
19_quantum [Autosaved].ppt19_quantum [Autosaved].ppt
19_quantum [Autosaved].ppt
VEERSHARMA35
 
Unit 6 Presentation.ppt
Unit 6 Presentation.pptUnit 6 Presentation.ppt
Unit 6 Presentation.ppt
ssuser2ac9e9
 

Similar to Limitations OF Classical Physics and Birth Of Quantum Mechanics (20)

3(1) (1).pptx
3(1) (1).pptx3(1) (1).pptx
3(1) (1).pptx
 
Quantum mechanics S5
Quantum mechanics S5 Quantum mechanics S5
Quantum mechanics S5
 
Particle Properties of Wave
Particle Properties of WaveParticle Properties of Wave
Particle Properties of Wave
 
Quantum Mechanics: Electrons, Transistors, & LASERS.
Quantum Mechanics: Electrons, Transistors, & LASERS. Quantum Mechanics: Electrons, Transistors, & LASERS.
Quantum Mechanics: Electrons, Transistors, & LASERS.
 
Chapter 4 electrons in atoms
Chapter 4 electrons in atomsChapter 4 electrons in atoms
Chapter 4 electrons in atoms
 
13.1
13.113.1
13.1
 
L3electronicstructureofatom 130906000837-
L3electronicstructureofatom 130906000837-L3electronicstructureofatom 130906000837-
L3electronicstructureofatom 130906000837-
 
19_quantum [Autosaved].ppt
19_quantum [Autosaved].ppt19_quantum [Autosaved].ppt
19_quantum [Autosaved].ppt
 
Quantum theory ppt
Quantum theory ppt Quantum theory ppt
Quantum theory ppt
 
Presentation laser
Presentation  laserPresentation  laser
Presentation laser
 
Dual nature of radiation
Dual nature of radiationDual nature of radiation
Dual nature of radiation
 
Chapter4electronsinatoms 111110092817-phpapp02
Chapter4electronsinatoms 111110092817-phpapp02Chapter4electronsinatoms 111110092817-phpapp02
Chapter4electronsinatoms 111110092817-phpapp02
 
Hp 21 win
Hp 21 winHp 21 win
Hp 21 win
 
Unit 6 Presentation.ppt
Unit 6 Presentation.pptUnit 6 Presentation.ppt
Unit 6 Presentation.ppt
 
Strawberry model2new
Strawberry model2newStrawberry model2new
Strawberry model2new
 
Photon and energy levels
Photon and energy levelsPhoton and energy levels
Photon and energy levels
 
Module 3 Engg Phys.pptx
Module 3 Engg Phys.pptxModule 3 Engg Phys.pptx
Module 3 Engg Phys.pptx
 
7.1 Atomic, nuclear and particle physics
7.1 Atomic, nuclear and particle physics7.1 Atomic, nuclear and particle physics
7.1 Atomic, nuclear and particle physics
 
Chemistry Chapter 5.pptx
Chemistry Chapter 5.pptxChemistry Chapter 5.pptx
Chemistry Chapter 5.pptx
 
lezione_3.ppt
lezione_3.pptlezione_3.ppt
lezione_3.ppt
 

Recently uploaded

The basics of sentences session 3pptx.pptx
The basics of sentences session 3pptx.pptxThe basics of sentences session 3pptx.pptx
The basics of sentences session 3pptx.pptx
heathfieldcps1
 
Spellings Wk 3 English CAPS CARES Please Practise
Spellings Wk 3 English CAPS CARES Please PractiseSpellings Wk 3 English CAPS CARES Please Practise
Spellings Wk 3 English CAPS CARES Please Practise
AnaAcapella
 
Salient Features of India constitution especially power and functions
Salient Features of India constitution especially power and functionsSalient Features of India constitution especially power and functions
Salient Features of India constitution especially power and functions
KarakKing
 

Recently uploaded (20)

Kodo Millet PPT made by Ghanshyam bairwa college of Agriculture kumher bhara...
Kodo Millet  PPT made by Ghanshyam bairwa college of Agriculture kumher bhara...Kodo Millet  PPT made by Ghanshyam bairwa college of Agriculture kumher bhara...
Kodo Millet PPT made by Ghanshyam bairwa college of Agriculture kumher bhara...
 
The basics of sentences session 3pptx.pptx
The basics of sentences session 3pptx.pptxThe basics of sentences session 3pptx.pptx
The basics of sentences session 3pptx.pptx
 
Spellings Wk 3 English CAPS CARES Please Practise
Spellings Wk 3 English CAPS CARES Please PractiseSpellings Wk 3 English CAPS CARES Please Practise
Spellings Wk 3 English CAPS CARES Please Practise
 
Explore beautiful and ugly buildings. Mathematics helps us create beautiful d...
Explore beautiful and ugly buildings. Mathematics helps us create beautiful d...Explore beautiful and ugly buildings. Mathematics helps us create beautiful d...
Explore beautiful and ugly buildings. Mathematics helps us create beautiful d...
 
Accessible Digital Futures project (20/03/2024)
Accessible Digital Futures project (20/03/2024)Accessible Digital Futures project (20/03/2024)
Accessible Digital Futures project (20/03/2024)
 
Unit-IV; Professional Sales Representative (PSR).pptx
Unit-IV; Professional Sales Representative (PSR).pptxUnit-IV; Professional Sales Representative (PSR).pptx
Unit-IV; Professional Sales Representative (PSR).pptx
 
Fostering Friendships - Enhancing Social Bonds in the Classroom
Fostering Friendships - Enhancing Social Bonds  in the ClassroomFostering Friendships - Enhancing Social Bonds  in the Classroom
Fostering Friendships - Enhancing Social Bonds in the Classroom
 
Dyslexia AI Workshop for Slideshare.pptx
Dyslexia AI Workshop for Slideshare.pptxDyslexia AI Workshop for Slideshare.pptx
Dyslexia AI Workshop for Slideshare.pptx
 
Basic Civil Engineering first year Notes- Chapter 4 Building.pptx
Basic Civil Engineering first year Notes- Chapter 4 Building.pptxBasic Civil Engineering first year Notes- Chapter 4 Building.pptx
Basic Civil Engineering first year Notes- Chapter 4 Building.pptx
 
Spatium Project Simulation student brief
Spatium Project Simulation student briefSpatium Project Simulation student brief
Spatium Project Simulation student brief
 
Making communications land - Are they received and understood as intended? we...
Making communications land - Are they received and understood as intended? we...Making communications land - Are they received and understood as intended? we...
Making communications land - Are they received and understood as intended? we...
 
Google Gemini An AI Revolution in Education.pptx
Google Gemini An AI Revolution in Education.pptxGoogle Gemini An AI Revolution in Education.pptx
Google Gemini An AI Revolution in Education.pptx
 
Micro-Scholarship, What it is, How can it help me.pdf
Micro-Scholarship, What it is, How can it help me.pdfMicro-Scholarship, What it is, How can it help me.pdf
Micro-Scholarship, What it is, How can it help me.pdf
 
Application orientated numerical on hev.ppt
Application orientated numerical on hev.pptApplication orientated numerical on hev.ppt
Application orientated numerical on hev.ppt
 
Mixin Classes in Odoo 17 How to Extend Models Using Mixin Classes
Mixin Classes in Odoo 17  How to Extend Models Using Mixin ClassesMixin Classes in Odoo 17  How to Extend Models Using Mixin Classes
Mixin Classes in Odoo 17 How to Extend Models Using Mixin Classes
 
Sociology 101 Demonstration of Learning Exhibit
Sociology 101 Demonstration of Learning ExhibitSociology 101 Demonstration of Learning Exhibit
Sociology 101 Demonstration of Learning Exhibit
 
Salient Features of India constitution especially power and functions
Salient Features of India constitution especially power and functionsSalient Features of India constitution especially power and functions
Salient Features of India constitution especially power and functions
 
How to Give a Domain for a Field in Odoo 17
How to Give a Domain for a Field in Odoo 17How to Give a Domain for a Field in Odoo 17
How to Give a Domain for a Field in Odoo 17
 
ComPTIA Overview | Comptia Security+ Book SY0-701
ComPTIA Overview | Comptia Security+ Book SY0-701ComPTIA Overview | Comptia Security+ Book SY0-701
ComPTIA Overview | Comptia Security+ Book SY0-701
 
Unit-IV- Pharma. Marketing Channels.pptx
Unit-IV- Pharma. Marketing Channels.pptxUnit-IV- Pharma. Marketing Channels.pptx
Unit-IV- Pharma. Marketing Channels.pptx
 

Limitations OF Classical Physics and Birth Of Quantum Mechanics

  • 1.
  • 2. LIMITATIONS OF CLASSICAL MECHANICS Presentation
  • 3. Centre For High Energy Physics University Of The Punjab _________________________________________________________________________________________________________ Presented To Sir Ibrar Presented By Muhammad Awais Raza 3414ME Msc 4th Eve
  • 4. Where classical mechanics fails and quantum mechanics arises? Experimental results could not be explained by classical mechanics Numerous places: 1. Black-Body radiation spectrum. 2. Photo-electric effect 3. Compton scattering. 4. Spectrum of hydrogen emissions
  • 5. Result In the development of Quantum Mechanics treats electrons as both a particle and a wave. All of the above can be easily explained by the existence of 'quanta,' but are impossible to explain through purely classical means.
  • 7. 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. Blackbody Radiation Here are some experimental facts about blackbody radiation: The Spectrum of Thermal Radiation depends on two types of characteristics of Temperature and material Dependent • With increase in temperature of material the amount of emitted radiation also increase and wavelength decreases it means It emits more blackbody energy at all wavelength. • Spectrum of Thermal radiation depend upon shape and nature of material
  • 8. The Explanation of Classical physics 1. Light is an electromagnetic wave that is produced when an electric charge vibrates. Now recall that heat is just the kinetic energy of random motion. In a hot object, electrons vibrate in random directions and produce light as a result. A hotter object means more energetic vibrations and so more light is emitted by a hotter object --- it glows brighter. So far, so good. But classical physics could not explain the shape of the blackbody spectrum.
  • 9. 2. The electrons in a hot object can vibrate with a range of frequencies, ranging from very few vibrations per second to a huge . Classical physics said that each frequency of vibration should have the same energy. This means that, there should be no limit to the energy of the light produced by the electrons vibrating at high frequencies. WRONG!! Experimentally, the blackbody spectrum always becomes smaller. (short wavelength, high frequency).
  • 10.
  • 11. At about 1900, Max Planck came up with the solution: He proposed that The classical idea that each frequency of vibration should have the same energy must be wrong. Instead, he said that energy is not shared equally by electrons that vibrate with different frequencies. Planck said that energy comes in clumps. He called a clump of energy a quantum. The size of a clump of energy --- a quantum --- depends on the frequency of vibration. Here is Planck's rule for the a quantum of energy for a vibrating electron: E = h f where h, the calibration constant, is today called Planck's constant. Its value is about 6 x 10-34, very tiny
  • 12. So how does this explain the spectrum of blackbody radiation? Planck said that an electron vibrating with a frequency f could only have an energy of 1 hf, 2 hf, 3 hf, 4 hf, ... ; that is, energy of vibrating electron = (any integer) x hf But the electron has to have at least one quantum of energy if it is going to vibrate. If it doesn't have at least an energy of 1hf, it will not vibrate at all and can't produce any light . Planck said: at high frequencies the amount of energy in a quantum, hf, is so large that the high-frequency vibrations can never get going! This is why the blackbody spectrum always becomes small (high frequency) .
  • 14. The Photoelectric Effect When light shines on the surface of a metallic substance, electrons in the metal absorb the energy of the light and they can escape from the metal's surface. This is called the photoelectric effect, and it is used to produce the electric current that runs many solar-powered devices. Using the idea that light is a wave with the energy distributed evenly throughout the wave, classical physicists expected that when using very dim light, it would take some time for enough light energy to build up to eject an electron from a metallic surface. WRONG!! Experiments show that if light of a certain frequency can eject electrons from a metal, it makes no difference how dim the light is. There is never a time delay.
  • 15. In 1905, Albert Einstein came up with the solution. If Max Planck's idea that energy comes in clumps (quanta) is correct, then light must consist of a stream of clumps of energy. Each clump of light energy is called a photon , said Einstein, and each photon has an energy equal to E = h f
  • 16. Therefore the energy of light is not evenly distributed along the wave, but is concentrated in the photons. A dimmer light means fewer photons, but simply turning down the light (without changing its frequency) does not alter the energy of an individual photon. So for a specific frequency light, if a single photon has enough energy to eject an electron from a metallic surface, then electrons will always be ejected immediately after the light is turned on and the photons hit the metal.
  • 18. Compton the Effect The Compton effect states x-rays scattered by loosely bound electrons of target element have reduce energy and frequency. This phenomenon describe scattering between radiation and matter and confirm the particle nature of light. Classical Wave Theory The X-ray are electro magnetic waves generated due to oscillation of electric- field and magnetic-field .When such X-ray waves having frequency “f” fall on target electrons ,the electrons start to oscillate with same frequency “f ”. The oscillating electrons must radiate electromagnetic waves which have again same frequency “f”. It means scattered beam of X-ray and incident beam of X-ray should have same frequency and same wavelength but spectrum of results of Compton Effect shows that scattered beam has intensity peak at two wavelengths . Therefore classical wave theory fails to explain experimental results of Compton effects.
  • 19. Quantum Mechanics Compton explained his experimental results by postulating that incident X-rays beam is assembly of photons having energy E = h f . These photons make collisions with free electrons in the scattering target .The scattered radiation consist of recoiling photons emerging from the target. The incident photon transfer some of its energy to the free electron during collision so scattered photon must have reduced energy . It means scattered photon has large wavelength than incident photon . This explains the wavelength shift in spectrum of Compton effect.
  • 20. Spectrum of hydrogen emissions
  • 21. The Hydrogen Atom When a small tube of hydrogen gas is heated, it begins to glow and emit light. Unlike the blackbody radiation that comes from a hot dense solid or gas, this light consists of just a few colors (wavelengths): a red hydrogen, since it is the simplest atom. Hydrogen consists of a positively charged proton at the center, with a negatively charged electron orbiting around it. The electrical attraction between the positive proton and the negative electron keeps the electron in orbit, just like the gravitational attraction between the Sun and the Earth holds the Earth in orbit. There was just one problem. wavelength, a turquoise, and several violets. Classical physicists at the beginning of the century thought they should certainly be able to understand
  • 22. Classical physics said that the orbiting electron is constantly changing direction, it should emit electromagnetic radiation --- light. As a result, the electron should be continually losing energy. In fact, physicists calculated that the electron should lose all of its energy and spiral down into the proton in only about 0.000000000001 second! In other words, atoms should not exist longer than a mere 10-12 seconds. WRONG!!
  • 23. Niels Bohr provided an explanation in 1913. In the Bohr model of the hydrogen atom, There are only certain allowed orbits, and each allowed orbit has a certain radius and a certain energy. Bohr invented a rule that allowed him to calculate the size and energy of each orbit. If you are curious, Bohr's rule said that 2π x (electron mass) x (electron orbital speed) x (orbit radius) = (any integer) x h which is not too obvious, to say the least! (The integer would be 1 for the smallest orbit, 2 for the next orbit out, and so on.) Bohr also made up a new rule to explain the stability of the hydrogen atom --- he said that when an electron is in an allowed orbit, the electron will not produce electromagnetic radiation. Bohr did not explain why, he just proposed a new law of nature. And nature agreed with Niels Bohr. His new model of hydrogen gave wavelengths for hydrogen gas that precisely agreed with what was measured.
  • 24. Question: If the electrons do not produce light when they are in their allowed stable orbits, where is the source of the light that comes from hydrogen? Answer: According to Bohr, electrons have more energy when they are in larger orbits. If an electron falls from a larger orbit down to a smaller orbit, it loses energy. According to the law of conservation of energy, the energy lost by the electron must go somewhere. Bohr explained that a photon carries away the lost energy from the hydrogen atom; that is, photon energy = (electron energy in larger orbit) - (electron energy in smaller orbit) It works the other way, too. If a photon strikes an atom, the atom can absorb the photon and its energy if (and only if) the photon's energy is exactly equal to the difference between two orbital energies. In this case, an electron uses the photon's energy to jump from the smaller orbit up to the larger orbit. This is called a quantum jump.
  • 25. The electron falls down to a lower orbit and the atom loses energy. A photon carries away the energy lost by the atom. A photon is absorbed by the atom, which gains the photon’s energy. The electron uses this energy to jump up to a higher orbit.