Quantum Theory of Light

Similar documents
Chapter 27 Quantum Physics

Chapter 30 Quantum Physics 30.1 Blackbody Radiation and Planck s Hypothesis of Quantum Energy 30.2 Photons and the Photoelectric Effect 30.

Explain how Planck resolved the ultraviolet catastrophe in blackbody radiation. Calculate energy of quanta using Planck s equation.

Lecture Outline Chapter 30. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc.

Planck s Quantum Hypothesis Blackbody Radiation

General Physics (PHY 2140)

27-1 Planck Solves the Ultraviolet Catastrophe

Chapter 38. Photons Light Waves Behaving as Particles

It s a wave. It s a particle It s an electron It s a photon. It s light!

Preview. Atomic Physics Section 1. Section 1 Quantization of Energy. Section 2 Models of the Atom. Section 3 Quantum Mechanics

Chapter 7 Atomic Structure -1 Quantum Model of Atom. Dr. Sapna Gupta

The Structure of the Atom Review

Supplemental Activities. Module: Atomic Theory. Section: Electromagnetic Radiation and Matter - Key

Early Quantum Theory & Models of the Atom (Ch 27) Discovery of electron. Blackbody Radiation. Blackbody Radiation. J. J. Thomson ( )

Chapter 27 Early Quantum Theory and Models of the Atom Discovery and Properties of the electron

Chapter. 3 Wave & Particles I

Photoelectric Effect Worksheet

Title / paragraph example Topic: Quantum Computers. Course essay. Photoelectric effect summary. From Last Time. Photon interference?

CHAPTER 27 Quantum Physics

Chapter 6: The Electronic Structure of the Atom Electromagnetic Spectrum. All EM radiation travels at the speed of light, c = 3 x 10 8 m/s

Supplemental Activities. Module: Atomic Theory. Section: Electromagnetic Radiation and Matter

Physics 1C. Chapter 28 !!!!

Constants & Atomic Data. The birth of atomic physics and quantum mechanics. debroglie s Wave Equations. Energy Calculations. λ = f = h E.

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS

The birth of atomic physics and quantum mechanics. Honors Physics Don Rhine

Chapter 27. Quantum Physics

WAVES AND PARTICLES. (c)

PHYSICS 3204 PUBLIC EXAM QUESTIONS (Quantum pt.1)

Energy levels and atomic structures lectures chapter one

Particle nature of light & Quantization

Learning Objectives and Worksheet I. Chemistry 1B-AL Fall 2016

Physics 1161: Lecture 22

Particles and Waves Particles Waves

Class 21. Early Quantum Mechanics and the Wave Nature of Matter. Physics 106. Winter Press CTRL-L to view as a slide show. Class 21.

Lecture 6 - Atomic Structure. Chem 103, Section F0F Unit II - Quantum Theory and Atomic Structure Lecture 6. Lecture 6 - Introduction

Chapter. 3 Wave & Particles I

Title / paragraph example Topic: Quantum Computers. Course Essay. Photoelectric effect summary. From Last Time. Compton scattering

Physics 1C. Lecture 27A

Semiconductor Physics and Devices

c = λν 10/23/13 What gives gas-filled lights their colors? Chapter 5 Electrons In Atoms

Lecture 11 Atomic Structure

Chapter 37 Early Quantum Theory and Models of the Atom. Copyright 2009 Pearson Education, Inc.

Chapter 9: Quantization of Light

13.1 Photoelectric Effect.notebook March 11, 2015

AP Chemistry. Chapter 6 Electronic Structure of Atoms

Dual Nature of Radiation and Matter GLIMPSES 1. Electron. It is an elementary particle having a negative charge of 1.6x C and mass 9.1x kg

Downloaded from

Physics. Light Quanta

AP Physics Study Guide Modern Physics I. Atomic Physics and Quantum Effects 1. Who is generally credited with the discovery of the electron?

General Physics (PHY 2140) Lecture 15

( ) # velocity. Wavelengths of massive objects. From Last Time. Wavelength of electron. Wavelength of 1 ev electron. A little complicated ( ) " = h mv

The Photoelectric Effect

Stellar Astrophysics: The Interaction of Light and Matter

1 The Cathode Rays experiment is associated. with: Millikan A B. Thomson. Townsend. Plank Compton

Chapter One. The Old Quantum Theory. 1-1 Why Quantum Mechanics.

Quantum Theory of the Atom

Accounts for certain objects being colored. Used in medicine (examples?) Allows us to learn about structure of the atom

Light Quanta. Particle-Wave History 11/2/2008. Particle-Wave Nature Continued s

SPH4U UNIVERSITY PHYSICS

We also find the development of famous Schrodinger equation to describe the quantization of energy levels of atoms.

Table of Contents Electrons in Atoms > Light and Quantized Energy > Quantum Theory and the Atom > Electron Configuration

Wave function and Quantum Physics

Chapter 6 - Electronic Structure of Atoms

12.1 The Interaction of Matter & Radiation 1 Photons & Photoelectric Effect.notebook March 25, The Interaction of Matter & Radiation

Chapter 28: Quantum Physics. Don t Copy This. Quantum Physics 3/16/13

Chapter 5 Electrons In Atoms

The ELECTRON: Wave Particle Duality. chapter 4

Properties of Light. Arrangement of Electrons in Atoms. The Development of a New Atomic Model. Electromagnetic Radiation CHAPTER 4

Announcements. Some Examples. Lecture 6 Chapter. 2 Special Relativity. Relativistic Dynamics. Problems. Problems

The Photoelectric Effect

Problems with Classical Physics. Blackbody Radiation Photoelectric Effect Compton Effect Bohr Model of Atom

PSI AP Physics How was it determined that cathode rays possessed a negative charge?

The Death of Classical Physics. The Rise of the Photon

RED. BLUE Light. Light-Matter

Visit for more fantastic resources. OCR. A Level. A Level Physics. Quantum Physics (Answers) Name: Total Marks: /30

Radiation - Electromagnetic Waves (EMR): wave consisting of oscillating electric and magnetic fields that move at the speed of light through space.

Announcements. Fast => v~c c= the velocity of light

Historical Background of Quantum Mechanics

PARTICLES AND WAVES CHAPTER 29 CONCEPTUAL QUESTIONS

Physics 6C. Photons. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Quantum Model Einstein s Hypothesis: Photoelectric Effect

SCH4U: History of the Quantum Theory

Chapter 6 Electronic structure of atoms

Chapter-11 DUAL NATURE OF MATTER AND RADIATION

Chapter 27 Lecture Notes

Physics 102: Lecture 23

Quantum Mechanics. Physics April 2002 Lecture 9. Planck Bohr Schroedinger Heisenberg

Quantum Mechanics: Blackbody Radiation, Photoelectric Effect, Wave-Particle Duality

4/14/2015. Models of the Atom. Quantum Physics versus Classical Physics The Thirty-Year War ( ) Classical Model of Atom

Quantum Mechanics: Blackbody Radiation, Photoelectric Effect, Wave-Particle Duality

Ch 7 Quantum Theory of the Atom (light and atomic structure)

Electronic structure of atoms

Chapter 7. The Quantum Mechanical Model of the Atom

5.111 Lecture Summary #3 Monday, September 8, 2014

SECTION A Quantum Physics and Atom Models

CVB102 Lecture 1 - Chemical Structure and Reactivity. Contact Information: Dr. Bill Lot Electronic Structure of Atoms

Physics 116. Nov 21, Session 31 De Broglie, duality, and uncertainty. R. J. Wilkes

Lecture 16 Quantum Physics Chapter 28

Welcome back to PHY 3305

General Physics (PHY 2140) Lecture 14

Transcription:

King Saud University College of Applied Studies and Community Service Department of Natural Sciences Quantum Theory of Light General Physics II PHYS 111 Nouf Alkathran nalkathran@ksu.edu.sa

Outline Definition The Birth of the Quantum Planck s constant Photons Definition of a black body Blackbody Radiation Implications of Planck s Law Photoelectric Effect

Outline Photoelectric Fact #1,2,3 Wave-Particle Duality De Broglie Wavelength Compton Effect Heisenberg s Uncertainty Principal The Electromagnetic Spectrum Is light a wave or a particle? Questions

Definition Quantum theory is a theory needed to describe physics on a microscopic scale, such as on the scale of atoms, molecules,electrons, protons, etc. It tells us that both light and matter consists of tiny particles which have wavelike properties associated with them. Light is composed of particles called photons matter is composed of particles called electrons, protons, neutrons. It's only when the mass of a particle gets small enough that its wavelike properties show up.

The Birth of the Quantum Max Planck made two assumptions Firstly the energy contained in radiation is related to the frequency of the radiation by the relationship E = nhf n is a positive integer called the quantum number f is the frequency of the oscillation Second, the molecules in the walls can only absorb energy in discreet packets, later to become known as photons

Planck s constant Planck proposed that light could only have certain energies E=hf Then the energy of oscillators in the black body could only have certain fixed values

Photons Max Planck in 1900 stated that the light emitted by a hot object (black body radiation) is given off in discrete units or quanta. The higher the frequency of the light, the greater the energy per quantum

Definition of a black body A black body is an ideal body which allows the whole of the incident radiation to pass into itself (without reflecting the energy) and absorbs within itself this whole incident radiation (without passing on the energy). This property is valid for radiation corresponding to all wavelengths and to all angels of incidence. Therefore, the black body is an ideal absorber of incident radiation.

Blackbody Radiation An object at any temperature emits radiation The wavelength of the radiation decreases as the body gets hotter A black-body is a perfect absorber It does not reflect ambient light The only light coming from the body is the radiation of the body itself The light from a black-body is in thermal equilibrium with the body This radiation has two important properties, The peak wavelength decreases with increasing temperature The total power emitted increases with increasing temperature

Black-Body Radiation The Planck Law gives a distribution that peaks at a certain wavelength, the peak shifts to shorter wavelengths for higher temperatures, and the ar ea under the curve grows rapidly with increasing temperature

Implications of Planck s Law The energy levels of the molecules must be discreet. Only transitions by an amount E=hf are allowed. The implication is that light exists in discrete quanta of energy. 4hf 3hf 2hf 1hf 0 These quantum levels are now known as number states n

Photoelectric Effect One of the most popular concepts concerning Quantum Mechanics is called, The Photoelectric Effect. In 1905, Albert Einstein published this theory for which he won the Nobel Prize in 1921. When light strikes a material, electrons are emitted. The radiant energy supplies the work necessary to free the electrons from the surface."

Photoelectric Fact #1 The LIGHT ENERGY (E) is in the form of quanta called PHOTONS. Since light is an electromagnetic wave it has an oscillating electric field. The more intense the light the more the field oscillates. In other words, its frequency is greater.

Photoelectric Fact #1 the energy of the light particle (photon) must overcome the binding energy of the electron to the nucleus. If the energy of the photon exceeds the binding energy, the electron is emitted with a KE = E photon E binding. The energy of the photon is given by E=hf, where the constant h = 6.6x10-34 [J s] is Planck s constant. Light parbcle Before Collision

Photoelectric Fact #1 Planck s Constant is the SLOPE of an Energy vs. Frequency graph! Make sure you USE the correct constant!

Photoelectric Fact #2 The frequency of radiation must be above a certain value before the energy is enough. This minimum frequency required by the source of electromagnetic radiation to just liberate electrons from the metal is known as threshold frequency, f 0 The threshold frequency is the X- intercept of the Energy vs. Frequency graph!

Photoelectric Fact #3 The MAXIMUM KINETIC ENERGY is the energy difference between the MINIMUM AMOUNT of energy needed (ie. the work function) and the LIGHT ENERGY of the incident photon. Light Energy, E KE=hf-hf o The energy NOT used to do work goes into KINETIC ENERGY as the electron LEAVES the surface. WORK done to remove the electron

Photoelectric Fact #3 KINETIC ENERGY can be plotted on the y axis and FREQUENCY on the x-axis. The WORK FUNCTION is the y intercept as the THRESHOLD FREQUNECY is the x intercept. PLANCK S CONSTANT is the slope of the graph. E hf K W hf K hf W K hf y mx b

Wave-Particle Duality The results of the photoelectric effect allowed us to look at light completely different. First we have Thomas Young s Diffraction experiment proving that light behaved as a WAVE due to constructive and destructive interference. Then we have Max Planck who allowed Einstein to build his photoelectric effect idea around the concept that light is composed of PARTICLES called quanta.

De Broglie Wavelength If light is a WAVE and is ALSO a particle, does that mean ALL MATTER behave as waves? That was the question that Louis de Broglie pondered. He used Einstein's famous equation to answer this question.

De Broglie Wavelength YOU are a mater WAVE! Basically all mater could be said to have a momentum as it moves. The momentum however is inversely proportional to the wavelength. So since your momentum would be large normally, your wavelength would be too small to measure for any practical purposes. An electron, however, due to it s mass, would have a very small momentum relative to a person and thus a large enough wavelength to measure thus producing measurable results. This led us to start using the Electron Microscopes rather than traditional Light microscopes.

Compton Effect The Compton effect is based on treating light as consisting of particles of a given energy related to the frequency of the light wave. In 1924, A. H. Compton performed an experiment where X- rays impinged on mater, and he measured the scattered radiation. High energy photons knock electrons out of atoms. The wavelength of a photon scattered from an electron is increased due to loss of photon energy. 2 > 1 where me is the mass of the electron and me c2 = 511 kev =.511 MeV.

Compton Effect Compton found that if you treat the photons as if they were particles of zero mass, with energy E=hc/λ and momentum p=h/λ The collision behaves just as if it were 2 billiard balls colliding! Photon behaves like a particle with energy & momentum as given above!

Heisenberg s Uncertainty Principal Quantum theory tells us that If you know where something is, you cannot also know its momentum If you know the energy of the object, you cannot also know the time at which the object had that energy many scientists had a hard time buying this idea NON DETERMINISTIC

Uncertainty Change (uncertainty) in posibon Change (uncertainty) in MOMENTUM x p h / 4

Uncertainty For LARGE objects, uncertainty is SMALL For small objects (like atoms and electrons) the uncertainty is LARGE Plank s constant is VERY VERY SMALL 6.626068 10-34 m 2 kg/s

The Electromagnetic Spectrum Shortest wavelengths (Most energetic photons) E = h = hc/ h = 6.6x10-34 [J*sec] (Planck s constant) Longest wavelengths (Least energebc photons)

Is light a wave or a particle? So is light a wave or a particle? On macroscopic scales, we can treat a large number of photons as a wave. When dealing with subatomic phenomenon, we are often dealing with a single photon, or a few. In this case, you cannot use the wave description of light. It doesn t work.

Questions In the Compton experiment, the wavelength of the scattered light is the wavelength of the incident light. (A) longer than (B) the same as (C) shorter than

Questions Suppose visible light of wavelength = 5 x 10-7 m is used to determine the position of an electron to within the wavelength of the light. What is the minimum uncertainty in the electron's speed? (Ans. 6.63x10-23 kg m/s)

Questions (a)calculate the wavelength in meters of an electron traveling at 1.24 x10 7 m/s. The mass of an electron is 9.11x 10-28 g.

Questions A green line of wavelength 4.86x10 7 m is observed in the emission spectrum of hydrogen. Calculate the energy of one photon of this green light.

Questions Planck's constant. A) remains unknown to this day. B) is the inverse of Einstein's constant. C) is used to find the quantum energy associated with a certain frequency of light. D) is not really constant since it varies from one part of the universe to another.

Questions A light source of wavelength λ illuminates a metal and ejects photoelectrons with a maximum kinetic energy of 1.00 ev. A second light source with half the wavelength of the first ejects photoelectrons with a maximum kinetic energy of 4.00 ev. Determine the work function of the metal.

Questions Which statement is TRUE? A) Light always behaves like a wave and electrons always behave like particles. B) Light always behaves like a particle and electrons always behave like waves. C) Both light and electrons behave sometimes like waves and sometimes like particles. D) Light and electrons never behave like waves or particles.

Questions How many Joules of energy are contained in a photon with λ = 550 nm? Use f = c / λ to get the frequency: f= (3.00 x 10 8 m s 1) / (550 x 10 9 m)= 5.4508 x 10 14 s 1. Now use E = hν to get the energy: E= (6.6260755 x 10 34 J s) (5.4508 x 10 14 s 1)= 3.612x10 19 J.

Questions What is the energy of a quantum of light with a frequency of 3.87 x 10 19 Hz? E hf hf 6.626 10 J 2.45 10 1.62 10-19 J