1 Photoelectric effect: experiment showing light is also a particle. Energy comes in particle-like chunks- basics of quantum physics. (energy of one chunk.

Slides:



Advertisements
Similar presentations
The Photoelectric Effect
Advertisements

© John Parkinson 1 MAX PLANCK PHOTOELECTRIC EFFECT.
PH300 Modern Physics SP11 “I learned very early the difference between knowing the name of something and knowing something.” - Richard Feynman 2/17 Day.
Any questions about the satellite assignment? Problems : Q3B.1, Q3B.2 and Q3B.5 due Wednesday If there are any errors on your printout circle them and.
A potential difference V is maintained between the metal target and the collector cup Electrons ejected from C travel to A and G detects the flow Apply.
1 PH300 Modern Physics SP11 2/15 Day 9: Questions? Exam 1 Photoelectric Effect Thursday: Photoelectric Effect (continued) “Anyone who has never made a.
Physics 6C The Photoelectric Effect Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB.
The Photoelectric Effect Waves as particles? What, are you crazy??
Quantum Physics ISAT 241 Analytical Methods III Fall 2003 David J. Lawrence.
Chapter 29 - Particles and Waves. 1.Who won the Nobel prize for his explanation of the photoelectric effect? A.Planck B.Bohr C.De Broglie D.Einstein 2.The.
The Photoelectric Effect Einstein’s Triumph Graphics courtesy of Physics 2000, University of Colorado Presentation Text ©2001 Philip M. Dauber.
The Photoelectric Effect AP Physics Unit 12. History After Young’s experiment with interference (1830), light was understood to be a wave. Most physicists.
Tues. Nov. 17, 2009Phy208 Lect From Last Time… Energy and power in an EM wave Polarization of an EM wave: oscillation plane of E-field.
3.2 More about photo electricity The easiest electrons to eject are on the metals surface And will have maximum kinetic energy Other electrons need more.
Physics 6C Photons Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB.
Black body radiation BBR is the radiation emitted by a non-reflecting solid body. A perfect black body is one which absorbs all the radiations falling.
6. Atomic and Nuclear Physics Chapter 6.4 Interactions of matter with energy.
Chapter 27 Quantum Theory
Blackbody Radiation Photoelectric Effect Wave-Particle Duality sections 30-1 – 30-4 Physics 1161: Lecture 28.
2. The Particle-like Properties Of Electromagnetic Radiation
Blackbody Radiation & Planck’s Hypothesis
MAX PLANCK PHOTOELECTRIC EFFECT © John Parkinson.
Phys 102 – Lecture 25 The quantum mechanical model of light.
The photoelectric effect
Chapter 7. Light as a wave  carries energy but doesn’t actually move  Think of a cork on water and surfer. The above diagram is a typical way to visualize.
Experimental evidence that light is a wave:. Shine light of particular wavelength/frequency/color on metal plate C Electron ejected from plate C (“photo-electron”)
1 2 Recap Photoeletricity experiment presents three puzzling features that are not explainable if light were wave: 1) K max of the photoelectrons is.
L 33 Modern Physics [1] Introduction- quantum physics Particles of light  PHOTONS The photoelectric effect –Photocells & intrusion detection devices The.
QW *Use the light kits at your tables to perform and answer the following: Shine red, blue, and green lights at glow in the dark material 1. Which one.
L 35 Modern Physics [1] Introduction- quantum physics Particles of light  PHOTONS The photoelectric effect –Photocells & intrusion detection devices The.
Zinc Negatively charge Zinc Negatively charge a sheet of zinc. 2. Shine long wavelength radio waves on the zinc. 3. Zinc remains negatively.
29:006 FINAL EXAM FRIDAY MAY 11 3:00 – 5:00 PM IN LR1 VAN.
Nuclear Atom and Unanswered Questions
G. Energy of a photon You should be able to: describe the particulate nature (photon model) of electromagnetic radiation state that a photon is a quantum.
PHYS:1200 FINAL EXAM 1 FINAL EXAM: Wednesday December 17, 12:30 P - 2:30 P in LR-1 VAN FE covers Lectures 23 – 36 The study guide, formulas, and practice.
L 33 Modern Physics [1] Introduction- quantum physics Particles of light  PHOTONS The photoelectric effect –Photocells & intrusion detection devices The.
Blackbody Radiation: The light from a blackbody is light that comes solely from the object itself rather than being reflected from some other source. A.
D O N OW (2/24/14) (3 MINUTES ) What do you think Albert Einstein discovered? Is light a wave or a particle?
Quantum Theory & the History of Light
Topic 13 Quantum and nuclear physics. The Quantum nature of radiation For years it was accepted that light travels as particles (though with little direct.
Photoelectric Effect. Basically, the photoelectric effect is the ejecting of electrons from a metal by shining light of a particular frequency on it.
A. Research the photo electric effect and provide a written explanation of the effect and its importance to modern physics B. Write down the equation for.
Physics 2170 – Spring Photoelectric effect and X-rays First midterm is 7:30pm on 2/17/09 in this room.
15-2 Photoelectric Effect Wave-particle Duality of Light Chap 15 Quantum Physics Physics 1 1. Photoelectric Effect and Phenomenon V A (1) Experimental.
L 35 Modern Physics [1] Introduction- quantum physics Particles of light  PHOTONS The photoelectric effect –Photocells & intrusion detection devices The.
Physics 2170 – Spring Photoelectric effect First midterm is 7:30pm on 2/17/09 in this room. The exam will.
What is light? Is it a wave, or a particle? Light is a wave… –It reflects off surfaces, and refracts through mediums. –Light has a frequency, and wavelength.
1.2 The puzzling photoelectric effect
Lecture_04: Outline Photoelectric Effect  Experimental facts  Einstein’s explanation  Problems.
AS LEVEL PHYSICS: ELECTRONS AND PHOTONS Quantum Physics : The Photoelectric Effect By the end of this presentation you should …. Appreciate that the photoelectric.
The Wacky World of Quantum Physics
Objectives: Additional skills gained: Practical Planning
The Photoelectric Effect
L 34 Modern Physics [1] Introduction- quantum physics
Photons: Light Waves Behaving as Particles
Photoelectric Effect Topic 14.2.
MAX PLANCK PHOTOELECTRIC EFFECT © John Parkinson.
CH 221 Computer Simulation Activity
L 35 Modern Physics [1] Introduction- quantum physics
L 35 Modern Physics [1] Introduction- quantum physics
PHOTOELECTRIC EFFECT.
L 33 Atomic and Nuclear Physics-1
L 33 Modern Physics [1] Introduction- quantum physics
Atomic Physics & Quantum Effects
PHOTOELECTRIC EFFECT hhhhh 12/4/2018.
The Photoelectric Effect
L 35 Modern Physics [1] Introduction- quantum physics
L 35 Modern Physics [1] Introduction- quantum physics
Quantization of light, charge and energy Chapter 2-Class3
Visit for more Learning Resources
Presentation transcript:

1 Photoelectric effect: experiment showing light is also a particle. Energy comes in particle-like chunks- basics of quantum physics. (energy of one chunk depends on frequency, wave-like beam of light has MANY chunks, energy of beam is sum) Next 2 classes: I. Understand the P.E. experiment and what results you would expect if light were a classical wave (like physicists at the time expected the experiment should give). II. What experimental results it actually did give. III. The implications/interpretation of the results. Important to take notes today a) record predictions to compare with experiment. b) record results of experiments. The Photoelectric Effect

2 Electrons Test metal Two metal plates in vacuum, adjustable voltage between them, shine light on one plate. Measure current between plates. Photoelectric effect experiment apparatus. 10 V A B Potential difference between A and B = +10 V Measure of energy an electron gains going from A to B. + - I. Understanding the apparatus and experiment.

3 Photoelectric effect experiment apparatus. 10 V A B Potential difference between A and B = a. 0 V, b. 10 V, c. infinite volts + -

4 Photoelectric effect experiment apparatus. 10 V A B + - What is current from A to B? a. 0 amps, b. 5 amps, c. 0.2 amps 2 ohms

5 A note about units of energy J oules: good for macroscopic energy conversions But when talking about energy of single electrons Joules is inconvenient… (too big) Define new energy unit (the electron-volt (eV)) = kinetic energy gained by an electron when accelerate through 1 volt of potential difference E F 0V 1V path  KE = -  U = - q  V = - (- e)*(1V) = + (e)*(1V) = 1.6 x J = 1eV

6 pump swimming pool analogy- If no water slops over side of pool, no flow. Little pump or big pump, still no water current. If electrons stuck inside metal plate, no current for little or big V. Put bunch of energy into water, splash some out, get flow through pump. Put energy into metal by heating it very hot, gives electrons energy, some “splash” out. Gives current. ?

7 What is the current vs battery voltage? Hot plate. A few electrons get enough energy to just barely “splash” out. 0 Voltage Current C 0 Voltage Current A 0 Voltage Current B 0 Voltage Current D

8 0 Battery Voltage Current C Each electron that pops out is accelerated more so hits far plate with higher velocity, BUT # of electrons = constant sec So current is constant! What’s happening here? reverse V, no electrons flow. Vacuum tube diode. Works. - early electronic device. NOT V=IR !!

9 Electrons Test metal Photoelectric effect experiment apparatus. So if light is classical wave, predict that just puts energy into plate, heats up, get diode current voltage curve. 0 Voltage Current C Also takes time to heat up. Light on longer, heat more, e’s out faster = more current. Color light does not matter, only intensity.

10 Have now covered. I. How apparatus works. II. What would expect to see if light classical wave as previous experiments like double slit interference, heating barrels, etc. had shown. Current vs voltage step at zero then flat. Color light does not matter, only intensity. Takes time to heat up ⇒ current low and increases with time. Increase intensity, increase current. questions? III. Do actual experiment, see if agrees with prediction. Current I vs V. How depends on intensity and color of light? 0

11 I e’s First experiment- I vs. V high intensity, low intensity I vs. V two different colors write down what happens

12 I e’s HIGH intensity 0 Battery Voltage I voltage to turn around most energetic electron “stopping potential” do low I exper.

13 0 Batt. V I I I I Which graph represents low and high intensity curves? 0 Batt. V I A B C D F

14 I e’s HIGH intensity LOW intensity 0 Battery Voltage I Fewer electrons pop off metal Current decreases. Current proportional to light intensity. ans. B

15 I e’s HIGH intensity LOW intensity 0 Battery Voltage I Same KE electrons popping off metal. So same “stopping potential”.

16 Predict what happens to the initial KE of the electrons as the frequency of light changes? (Light intensity is constant) Predict shape of the graph I e’s 0 Frequency of light Initial KE look at sim for few different colors, small forward V

17 0 Frequency Initial KE 0 Frequency Initial KE 0 Frequency Initial KE 0 Frequency Initial KE AB C D E. something different

18 I e’s 0 Frequency of light Initial KE As the frequency of light increases (shorter  ), the KE of electrons being popped off increases. (it is a linear relationship) There is a minimum frequency below which the light cannot kick out electrons… even if wait a long time Correct answer is D. do sim showing graph what happens if change metal? do experiment

19 Summary of Photoelectric experiment results. (play with sim to check and thoroughly understand) 1. Current linearly proportional to intensity. 2. Current appears with no delay. 3. Electrons only emitted if frequency of light exceeds a threshold. (same as “if wavelength short enough”). 4. Maximum energy that electrons come off with increases linearly with frequency (=1/wavelength). (Max. energy = -stopping potential) 5. Threshold frequency depends on type of metal. how do these compare with classical wave predictions?

20 Classical wave predictions vs. experimental observations Increase intensity, increase current. experiment matches Current vs voltage step at zero then flat. (flat part matches, but experiment has tail of energetic electrons, energy of which depends on color) Color light does not matter, only intensity. experiment shows strong dependence on color Takes time to heat up ⇒ current low and increases with time. experiment: electrons come out immediately, no time delay to heat up

21 Summary of what we know so far: 1.If light can kick out electron, then even smallest intensities of that light will continue to kick out electrons. KE of electrons does not depend on intensity. (Light energy must be getting concentrated/focused somehow) 2. At lower frequencies, initial KE decreases & KE changes linearly with frequency. (This concentrated energy is linearly related to frequency) 3. Is minimum frequency below which light won’t kick out electrons. (Need a certain amount of energy to free electron from metal) (Einstein) Need “photon” picture of light to explain observations: - Light comes in chunks (“particle-like”) of energy (“photon”) - a photon interacts only with single electron - Photon energy depends on frequency of light, … for lower frequencies, photon energy not enough to free an electron questions?, more sim experiments?

22 An analogy with a ball and a pit Light like a Kicker… Puts in energy. All concentrated on one ball/electron. Blue kicker always kicks the same, and harder than red kicker always kicks. KE = kick energy - mgh Ball emerges with: mgh = energy needed to make it up hill and out. mgh for highest electron analogous to work function. Kick energy. Top ones get out, bottom don’t. Harder kick (shorter wavelength light), more get out. show photon view h metal electrons

23 An analogy with a ball and a pit Light like a Kicker… Puts in energy. All concentrated on one ball/electron. Blue kicker always kicks the same, and harder than red kicker always kicks. KE = kick energy - mgh Ball emerges with: show photon view sodium- easy to kick out platinum, hard to kick out large work function  deep pit h h small work function  shallow pit energy needed to get most energetic electron out of pit (“work function”)

24 Photon… Puts in kick of energy KE = photon energy – work function If photon has enough energy, electron emerges with: energy needed to kick highest electron out of metal. “WORK FUNCTION” (  ) Each photon has: Energy = Planks constant * Frequency (Energy in Joules) (Energy in eV) E=hf=(6.626* J-s)*(f s -1 ) E=hf= (4.14* eV-s)*(f s -1 ) E=hc/ = (1.99* J-m)/( m)E= hc/  1240 eV-nm)/(  nm) Initial KE of electron = E photon - energy needed to kick as it comes out of metal electron out of metal Depends on type of metal.

25 Photoelectric effect experiment: Apply Conservation of Energy Inside metal Electron Potential Energy work function (  ) = energy needed to kick highest electron out of metal Energy in = Energy out Energy of photon = energy needed to kick + Initial KE of electron electron out of metal as exits metal Loosely stuck electron, takes least energy to kick out Tightly stuck, needs more energy to escape Outside metal

26 Apply Conservation of Energy. Inside metal Electron Potential Energy work function (  ) Energy in = Energy out Energy of photon = energy needed to kick + Initial KE of electron electron out of metal as exits metal Outside metal What happens if send in bunch of blue photons? Electrons have equal chance of absorbing photon:  Max KE of electrons = photon energy -   Min KE = 0  Some electrons, not enough energy to pop-out, energy into heat. E photon Photon gives electron “kick of energy”.

27 Electrons over large range of energy have equal chance of absorbing photons. Inside metal Electron potential energy You initially have blue light shining on metal. If you change the frequency to violet light (at same # of photons per second), what happens to the number of electrons coming out? a. fewer electrons kicked out b. same # of electrons c. more electrons kicked out d. not enough information work function  E phot

28 Electrons over large range of energy have equal chance of absorbing photons. metal elect. potential energy work function  E phot c. more electrons come out with violet absorb blue light and have enough energy to leave absorb blue light, but don’t come out so the more energy the light has, the more electrons that come out, until so much energy that every electron comes out. (violet and ultraviolet would not be very different in this case)

29 Typical energies Each photon has: Energy = Planks constant * Frequency (Energy in Joules) (Energy in eV) E=hf=(6.626* J-s)*(f s -1 ) E=hf= (4.14* eV-s)*(f s -1 ) E=hc/ = (1.99* J-m)/( m)E= hc/  1240 eV-nm)/(  nm) Photon Energies: Work functions of metals (in eV): Aluminum4.08 eVCesium2.1Lead4.14Potassium2.3 Beryllium5.0 eVCobalt5.0Magnesium3.68Platinum6.35 Cadmium4.07 eVCopper4.7Mercury4.5Selenium5.11 Calcium2.9Gold5.1Nickel5.01Silver4.73 Carbon4.81Iron4.5Niobium4.3Sodium2.28 Uranium3.6 Zinc4.3 Red Photon: 650 nm E photon = 1240 eV-nm = 1.91 eV 650 nm

30 Photomultiplier tubes- application of photoelectric effect most sensitive way to detect visible light, see single photons (eye is incredibly good, can see a few photons) glass vacuum enclosure cq2. what would be the best choice of these materials to make this out of? a. Platinum  = 6.35 eV b. Magnesium = 3.68 eV c. Nickel = 5.01 eV d. lead = 4.14 eV e. Sodium = 2.28 eV current Time (millisec) Time (millisec) big voltage electron amplifier, gives pulse of current for each photoelectron

31 Clicker question discussion After decide on answer, don’t stop thinking/discussing! Think of as many reasons as possible to support your answer and/or rule out other answers. Other perspectives, other situations and information that may have relevance. “Line on electron energy vs frequency graph must go to zero before zero frequency, because sunlight hits stuff but doesn’t make electrons come out of everything.” Ability to think of multiple ways to test ideas and conclusions, ability to relate to many different contexts, is a learned skill of expert scientists and engineers. Useful in many aspects of life and work, tested for in interviews.

32 CQ: A photon at 300 nm will kick out an electron with an amount of kinetic energy, KE 300. If the wavelength is halved to 150 nm and the photon hits an electron in the metal with same energy as the previous electron, the energy of the electron coming out is a. less than ½ KE 300. b. ½ KE 300 c. = KE 300 d. 2 x KE 300 e. more than 2 x KE 300 (remember hill/kicker analogy, draw pictures to reason out answer, don’t just pick answer without careful reasoning) KE 300 V

33 CQ: Shine in light of 300 nm. The most energetic electrons come out with kinetic energy, KE 300. A voltage diff of 1.8 V is required to stop these electrons. What is the work function  for this plate? (e.g. the minimum amount of energy needed to kick electron out of metal?) a. 1.2 eV b. 2.9 eV c. 6.4 eV d eV e. none of the above KE 300 V