Reading quiz – get out a sheet of paper and a writing utensil. In the Davisson Germer experiment, Davisson and Germer shot a beam of electrons at a lattice.

Slides:



Advertisements
Similar presentations
The 4 important interactions of photons
Advertisements

Chapter 4.
Dilemma Existence of quanta could no longer be questioned e/m radiation exhibits diffraction => wave-like photoelectric & Compton effect => localized packets.
AP Physics Chapter 28 Quantum Mechanics and Atomic Physics
PHYS140Matter Waves1 The Wave Nature of Matter Subatomic particles De Broglie Electron beam Davisson-Germer Experiment Electron Interference Matter Waves.
Atoms: Not to Be Cut. Dalton’s Theory He deduced that all elements are composed of atoms. He deduced that all elements are composed of atoms. Atoms are.
The de Broglie Wavelength Lesson 11. Review Remember that it has been proven that waves can occasionally act as particles. (ie: photons are particles.
Topic 13: Quantum and Nuclear physics “The wave nature of matter” Matter behaving as a wave? Ridiculous!
Vacuum tube - V, only for shorter than certain wavelength Current V VoVo Fixed wavelength Varying intensity I2I 3I Maximum electron energy 0.
Quantum Theory Micro-world Macro-world Lecture 14.
Lecture 15: Bohr Model of the Atom
Light: oscillating electric and magnetic fields - electromagnetic (EM) radiation - travelling wave Characterize a wave by its wavelength,, or frequency,
De Broglie Waves, Uncertainty, and Atoms
Successes of the Bohr model Explains the Balmer formula and predicts the empirical constant R using fundamental constants: Explains the spectrum for other.
3: Interference, Diffraction and Polarization
Physics 361 Principles of Modern Physics Lecture 5.
Modern Physics.
When heated to high temps, gases give off light. If this light is passed through a slit, then through a prism or diffraction grating, the following patterns.
Lecture 11b Atomic Physics & Nuclear Reactions Copyright © 2009 Pearson Education, Inc.
Wave Nature of Matter Light/photons have both wave & particle behaviors. Waves – diffraction & interference, Polarization. Acts like Particles – photoelectric.
Physics Education Department - UNS 1 From Last Time… Light waves are particles and matter particles are waves! Electromagnetic radiation (e.g. light) made.
Physics 1C Lecture 28B Compton effect: photons behave like particles when colliding with electrons. Electrons and particles in general can behave like.
Quantum Theory Chapter 5. Lecture Objectives Indicate what is meant by the duality of matter. Indicate what is meant by the duality of matter. Discuss.
Quantum Mechanics and Atomic Theory Wave models for electron orbitals.
Nature of Light YoungEinstein Particle (photon)Wave Wave-Particle Duality (What does this mean?)
1 Chapter 7 Atomic Structure. 2 Light n Made up of electromagnetic radiation n Waves of electric and magnetic fields at right angles to each other.
Particle Physics A Quick Tour. Models of the Atom Thomson – Plum Pudding Why? Known that negative charges can be removed from atom. Problem: just a random.
-The Bohr Model -The Quantum Mechanical Model Mrs. Coyle Chemistry.
Physics 2170 – Spring Davisson – Germer experiment Homework set 7 is due Wednesday. Problem solving sessions.
What’s coming up??? Oct 25The atmosphere, part 1Ch. 8 Oct 27Midterm … No lecture Oct 29The atmosphere, part 2Ch. 8 Nov 1Light, blackbodies, BohrCh. 9 Nov.
Chapter 7 Atomic Structure. Light Made up of electromagnetic radiation Waves of electric and magnetic fields at right angles to each other.
Methods of Math. Physics Thus. 2 Dec Brief review of forces, energy, oscillations Bohr atom – quantization of angular momentum E.J. Zita.
AP Notes Chapter 6 Atomic Structure Describe properties of electromagnetic radiation Describe properties of electromagnetic radiation Light & relationship.
Contents: Copenhagen Interpretation of Young’s Double slit The Quantum atom Heisenberg uncertainty principle The Einstein Bohr debate Quantum Mechanics.
Physics 2170 – Spring Franck-Hertz experiment, Bohr atom, de Broglie waves Homework solutions for Homework.
Chapter 7 Atomic Structure. Light  Made up of electromagnetic radiation  Waves of electric and magnetic fields at right angles to each other.
Chapter 7. Electromagnetic Radiation  aka. Radiant energy or light  A form of energy having both wave and particle characteristics  Moves through a.
Physics 2170 – Spring X-rays and Compton effect Next weeks homework will be available late this afternoon.
Physics 102: Lecture 23, Slide 1 De Broglie Waves, Uncertainty, and Atoms Physics 102: Lecture 23.
Chapter 10. Matter and energy were thought to be distinct in the early 19 th century. Matter consisted of particles; whereas electromagnetic radiation.
Wave Particle Duality Quantum Physics Lesson 3 Today’s Objectives Explain what is meant by wave-particle duality. Explain what is meant by wave-particle.
Plan for Today (AP Physics 2) Ch 24, 27, and 28 Review Day More Review Materials.
THE ENERGY OF LIGHT. HOW LIGHT IS ‘MADE’ Today we are going to take a look at how light is made and how we can determine the energy of light In order.
Atomic Structure. Model A: The plum pudding model J.J. Thompson Negative charges like raisins in plumb pudding Positive charge is spread out like the.
Quantization part 2 –particles as waves ch 37. The world – a) matter - atoms nucleus of tightly packed protons and neutrons. Protons-positive charge electrons.
Problem Solving hints Use white AP constant sheet hc = 1.99  J  m = 1.24  10 3 eV  nm h = 6.63  J  s = 4.14  eV  s 1 eV =
Today’s Lecture Interference Diffraction Gratings Electron Diffraction
Plan for Today (AP Physics 2) Go over AP Problems Lecture/Notes on X-Rays, Compton Effect, and deBroglie Ch 27 HW due Monday.
Physics 102: Lecture 23, Slide 1 De Broglie Waves, Uncertainty, and Atoms Today’s Lecture will include material from textbook sections 27.5, 28.2, 4 Physics.
Models of the Atom Rutherford, Bohr, De Broglie and Quantum Physics.
Chapter 11 Modern Atomic Theory. Rutherford’s Atom What are the electrons doing? How are the electrons arranged How do they move?
Quantum Mechanics and Atomic Physics
Bohr vs. Correct Model of Atom
Physics 4 – April 27, 2017 P3 Challenge –
Reading quiz – get out a sheet of paper and a writing utensil.
The Wave Nature of Matter
Quantum Physics Lesson 6
Ch25 Modern Optics and Matter Waves
Quantum Mechanics Reference: Concepts of Modern Physics “A. Beiser”
de Broglie Waves de Broglie argued
CHAPTER 4 Electron Configurations (current model of the atom)
Matter Waves Louis de Broglie
Matter Waves Louis de Broglie
Wave-Particle Duality
Bohr vs. Correct Model of Atom
Bohr vs. Correct Model of Atom
Chemistry 141 Wednesday, November 1, 2017 Lecture 24
Quantum Mechanics.
CHAPTER 4 Electron Configurations (current model of the atom)
Presentation transcript:

Reading quiz – get out a sheet of paper and a writing utensil. In the Davisson Germer experiment, Davisson and Germer shot a beam of electrons at a lattice of Nickel atoms and found that the electrons were only detected at certain angles. Explain the reason for this result and why it was important.

Review of Bohr and deBroglie Background: –Balmer found equation for Hydrogen spectrum but didn’t know what it meant. –Rutherford found that atoms had a nucleus, but didn’t know why electrons didn’t spiral in. Bohr postulates quantized energy levels for no good reason, and predicts Balmer’s equation. deBroglie postulates that electrons are waves, and predicts Bohr’s quantized energy levels. Note: no experimental difference between Bohr model and deBroglie model, but deBroglie is a lot more satisfying.

Thomson – Plum Pudding –Why? Known that negative charges can be removed from atom. –Problem: just a random guess Rutherford – Solar System –Why? Scattering showed hard core. –Problem: electrons should spiral into nucleus in ~ sec. Bohr – fixed energy levels –Why? Explains spectral lines. –Problem: No reason for fixed energy levels deBroglie – electron standing waves –Why? Explains fixed energy levels –Problem: still only works for Hydrogen. Schrodinger – will save the day!! Models of the Atom – – – – – –

deBroglie Waves This is a great story. But is it true? If so, why no observations of electron waves? What would you need to see to believe that this is actually true? Today: Electron interference! Why electron waves are hard to see Designing experiment possible to see with early 1900s tech. How done by Clinton Davisson and Lester Germer Why their technique still used today (LEED) How to interpret.

Reminder- what do we mean by interference? Waves (water, sound, …) interfering. zilch Peaks where add, zilch where cancel (destructive interference) Phet Wave Interference Sim 1 2

Two slit interference with light

Question in 1920s So can we just do same experiment but replace beam of light with beam of electrons to check deBroglie? Let’s work through the design to see what expect to see, what required to do proper experiment. step 1. Go off and play with making beams of electrons. Find can make beams of energies between ~ eV. V step 2. Calculate signal would expect to see from double slit. Typical for light: slits ~0.5 mm apart

Can we just repeat light double slit experiment with electrons? a. yes. (if so, precisely what would experimental results would you expect?) b. no. (if so, precisely why not?) step 1. Go off and play with making beams of electrons. Find can make beams of energies between ~ eV. step 2. Calculate signal would expect to see from double slit. Typical for light: slits ~0.5 mm apart

Double-slit experiment (see textbook) Determining the space between bright regions (H) 0.5 mm =D r1r1 r2r2  H L Screen far away so  1 ~  2 ~  & small angle approx. sin  =    D   r = Dsin(  )=D  H= Lsin(  )=L  H=L  bright  r = r 2 -r 1  r = m (where m=1,2,3…) D  =m

Double-slit experiment Determining the space between bright regions (H) 5 x10 -4 m = D r1r1 r2r2  r = r 2 -r 1  r = m (where m=1,2,3…)  r=m = Dsin(  )=D  =m  H L H= L  m = 1, = 500 nm, so angle to first bright  = λ/D = 500 x /(5 x ) = rad if L = 3m, then H= 3 m x = 3mm. Calculating pattern for light So what will pattern look like with electrons? How figure out?

1. find expected wavelength =h/p, h = 6.6 x J s 2. plug into  = λ/D = (h/p)(1/D), calculate angle (radians) Best to do experiment with a. higher energy electron beam b. lower energy electron beam c. does not make any difference b. lower. Smaller energy  smaller momentum  larger λ means bigger angle, easier to see. Steps to predict pattern for debroglie electron wave. D  =m H= L 

OR λ = hc/(2Emc 2 ) 1/2 λ = λ = = λ = 1/5 nm ~ 1nm Energy E = ½mv 2 = p 2 /2m …so p = (2Em) 1/2 …so λ = h/p = h/(2Em) 1/2 λ = λ = 2.4 x m = 0.24 nm ~ 1nm 1. find expected wavelength =h/p, h = 6.6 x J s 2. plug into  = λ/D = (h/p)(1/D), calculate angle (radians) Steps to predict pattern for debroglie electron wave. For lowest energy electron beam (E = 25eV), how big is electron wavelength? A. λ ~ 1pm ( m)D. λ ~ 1mm (10 -3 m) B. λ ~ 1nm (10 -9 m)E. λ ~ 1m C. λ ~ 1  m (10 -6 m) Compare with visible light: λ ~ nm 6.6x Js (2 * 25eV * 1.6x J/eV * 9.1x kg) 1/ eV nm (2 * 25eV *.511 x 10 6 eV) 1/2 1 x 10 3 nm (25 x 10 6 ) 1/2 1 x 10 3 nm 5 x 10 3

Energy and Momentum for Massive vs. Massless Particles Massive Particles (e.g. electrons) E = ½mv 2 = p 2 /2m = h 2 /2mλ 2 p = (2Em) 1/2 λ = h/p = h/(2Em) 1/2 Massless Particles (e.g. photons) E = pc = hc/λ p = E/c λ = h/p = hc/E Lowest energy e - s E = 25eV p = 2.7x kg m/s v = 3x10 6 m/s = c/ 100 λ = 0.24 nm Typical photons E = 2.5eV p = 1.3x kg m/s v = c = 3x10 8 m/s λ = 500 nm deBroglie relationship is universal

1. find expected wavelength =h/p, h = 6.6 x J s 2. plug into  = λ/D = (h/p)(1/D), calculate angle (radians) lowest energy 25 eV gives λ = 2.4 x m So for slit separation D ~ 0.5mm, expect  to be a. 1, d. >>1.  = λ/D = (2.4 x m)/(5 x m) = 4.9 x radians!!! D Much too small an angle to see! (If L = 3m, then H=L  = 1.5 x m = 150 nm) Big problem, if electron has wavelength deBroglie predicted it is REALLY SMALL ~ 2.4 x m. Why not seen. Steps to predict pattern for debroglie electron wave.

predict pattern for debroglie electron wave =h/p, h = 6.6 x J s,  = λ/D = (h/p)(1/D), = 2.4 x m  = λ/D if D = 5 x m,  = 4.9 x radians Much too small an angle to see! What now? Any way to make angle bigger? a. make D much smaller, b. make electron energy lower, c. make D much bigger, d. a. and b. e. b. and c. ans. a) make D smaller (already said cannot make E smaller, electron beam no good)

designing experiment to see debroglie electron wave =h/p, h = 6.6 x J s,  = λ/D = (h/p)(1/D) = 2.4 x m  = λ/D to make  easy to see, like ~1rad, need D = 0.25 nm Is that a problem? yes, it is about the same size as one atom! Would like to have slits separated by about an atom diameter. Impossible. Making lemonade out of lemons

Brilliant idea: But two slits are just two sources. Hard to get two sources size of atom. Easy to get two objects that scatter electrons that are size of atom!

But two slits are just two sources. hard to get only two atoms next to each other. But multiple that are same separation just work better. Just like reflection diffraction grating. What stuff in nature is made out of things the size of atoms with equal spacing between them?

Davisson and Germer -- VERY clean nickel crystal. Interference is electron scattering off Ni atoms. e e e e e e e e e e e scatter off atoms e det. move detector around, see what angle electrons coming off Ni

e e e e e e e e e det. Ni Observe pattern of scattering electrons off atoms Looks like …. Wave! # e’s scatt. angle  See peak!! so probability of angle where detect electron determined by interference of deBroglie waves!

PhET Sim: Davisson Germer Careful… near field view: D  = m doesn’t work here. For qualitative use only!