Shedding light on atomic energy levels (segment of Hydrogen spectrum)
|
|
- May Caldwell
- 5 years ago
- Views:
Transcription
1 3.0 ev.85 ev.55 ev.69 ev Fri More Eergy Quatizatio RE 8.b Mo. Tues. Wed. Lab Fri. 9.-., (.8) Mometum ad Eergy i Multiparticle Systems 9.3 Rotatioal Eergy Quiz 8 Review Exam (Ch 5-8) Exam (Ch 5-8) RE 9.a HW8: Ch 8 Pr s, 3, 7(a-c) RE 9.b Practice Exam (brig to class) Sheddig light o atomic eergy levels (segmet of Hydroge spectrum)
2 Where we ve bee: Eergy o the macroscopic scale Eergy o the atomic scale Where we re goig: Eergy o the electroic scale + 0 electro m v e e electro& ucleus 4 o eq r uc hydroge 4 o e r Mathematically like solar system, but much too small ad delicate to directly see orbital radii ad speeds eed aother way to deduce
3 Hydroge Eergy Levels etc. 3.6eV ev ev -.5 ev = = 5 = 4 = 3 Excited States 3.6eV ev = 4 o e r 3.6eV -3.6 ev = Groud State
4 Hydroge Eergy Levels: Excitatio 3.6eV ev ev -.5 ev = = 5 = 4 = 3 Excited States ev = -3.6 ev = Groud State
5 Hydroge Excitatio: st i groud state 3.6eV ev ev -.5 ev = = 5 = 4 = 3 Excited States ev = -3.6 ev Marks the occupied state = Groud State
6 Hydroge Excitatio: d Adsorbs eergy from Collisio 3.6eV ev ev -.5 ev excites to d state = = 5 = 4 = 3 Excited States ev = -3.6 ev = Groud State
7 Hydroge Excitatio: 3 rd Looses Eergy by photo emissio, 3.6eV ev ev -.5 ev de-excites to groud state = = 5 = 4 = 3 Excited States ev = Photo Emissio E E E ph ph ph E H 3.6eV 0.eV 3.6eV -3.6 ev = Groud State
8 Example Atoms i Gas-Discharge Tube 06_Adsorb_emit.py.
9 Frak-Hertz Experimet Moitorig electro beam s loss of eergy to the atoms Hydroge Gas Discharge Tube e Eergy of Hydroge s = to trasitio 0.eV Electro s kietic eergy High acceleratig voltage Medium acceleratig voltage Low acceleratig voltage Distace alog tube Differet exitig kietic eergies are reflected i differet curret readigs
10 Here are the quatized eergy levels (+) for a atomic or molecular object, ad the object is i the "groud state" (marked by a dot). A electro with kietic eergy 6 ev is fired at the object ad excites the object to the 5 ev eergy state. What is the remaiig kietic eergy of this electro? a) 9 ev b) 6 ev c) 4 ev d) 3 ev e) ev - ev - ev -5 ev -9 ev
11 Absorptio Spectrum 06_spectrum.py.
12 A collectio of some atoms objects is kept very cold, so that all the objects are i the groud state. Light cosistig of photos with a rage of eergies from to 7.5 ev passes through this collectio of objects. What photo eergies will be depleted from the light beam ( dark lies )? a) ev, 5 ev, 9 ev b) 3 ev, 4 ev c) 0.5 ev, 3 ev, 4 ev d) 4 ev, 7 ev e) 3 ev, 4 ev, 7 ev - ev - ev -5 ev -9 ev
13 Quatitatively Relatig Light s Eergy ad Frequecy The Photo-electric Effect Ioizig metal plate Shie moo-chromatic (sigle color) light o metal ith low frequecy light, o matter how bright, o electros are freed, o curret measured ur up frequecy; at ad above some threshold frequecy, f, electros are freed, curret Threshold frequecy relates to metal plate s ioizatio eergy (work fuctio) by E = hf Deduce: light falls like rai with packets of eergy related to its frequecy E = hf h = Js = evs
14 Example: He-Ne laser. Gas discharge tube filled with He ad Ne. They have a rich emissio spectrum but the tube s legth, like the strig of a piao is right to help light resoate at just oe frequecy, Hz, a rich red. How much eergy does oe red photo of from the He-Ne have? This is a 0.95mW = J/s laser; that s the rate at which the beam of photos carry away eergy. How may photos are emitted per secod?
15 q Simple Harmoic Oscillator Eergy spectrum & Structure Eergy 3 s m ax. eq eq eq s m ax. k Imagie a charged particle ridig a mass o a sprig E system = E light = hf s (stretch) ssmax. kssmax. kssmax.3 eq f kss ks m Radiates light with the same frequecy as its ow oscillatio hf E light Mass-o-sprig must loose this much eergy Still oscillatig at same f agai radiates light of frequecy f. Etc. eq
16 q Simple Harmoic Oscillator Eergy spectrum & Structure Imagie a charged particle ridig a mass o a sprig f ks m We ve deduced Eergy s m ax. s (stretch) eq eq kss k s s max. E mi Takes real Quatum Mechaics to ail dow E mi : hf Emi eq hf where =,,3, eq k s s max. eq
17 Example: Macro-scopic mass o sprig We certaily do t otice that a mass o a sprig has oly specific allowed eergies, it seems to be able to oscillate with ay eergy / amplitude (util it breaks). Give a 0.0 kg mass o our 3 N/m sprig, iitially displaced 0.m, how much eergy has it got, ad how big is the step to the ext eergy level lower? How about a H molecule, what s the eergy step size for its vibratios? Roughly 0-7 kg mass protos ad 00 N/m sprig costat.
18 Two atoms joied by a chemical bod ca be modeled as two masses coected by a sprig. I oe such molecule, it takes 0.05 ev to raise the molecule from its vibratioal groud state to the first excited vibratioal eergy state. How much eergy is required to raise the molecule from its first excited state to the secod excited vibratioal state? ) 0.05 ev ) 0.05 ev 3) 0.05 ev 4) 0.0 ev 5) 0.0 ev
19 Molecule A: atoms of mass M A Molecule B: atoms of mass 4*M A Stiffess of iteratomic bod is approximately the same for both. Which molecule has vibratioal eergy levels spaced closer together? ) A ) B 3) the spacig is the same Suppose the atoms i diatomic molecules C ad D had approximately the same masses, but Stiffess of bod i C is 3 times as large as stiffess of bod i D. Which molecule has vibratioal eergy levels spaced closer together? ) C ) D 3) the spacig is the same
20 Pb: k s ~ 5 N/m Al: k s ~ 6 N/m Which vibratioal eergy level diagram represets Pb, ad which is Al? ) A is Pb ad B is Al ) A is Al ad B is Pb 3) A is both Pb ad Al 4) B is both Pb ad Al
21 Stiffer / stroger bods, bigger steps betwee eergy levels Type of State Eergy Scale Hadroic (quark composites) 0 8 ev Nuclear (ucleo composites) 0 6 ev Electroic (atoms & molecules) ev Vibratioal (molecules) 0 - ev Rotatioal (molecules) 0-4 ev
Phys 102 Lecture 25 The quantum mechanical model of light
Phys 102 Lecture 25 The quatum mechaical model of light 1 Recall last time Problems with classical physics Stability of atoms Atomic spectra Photoelectric effect Quatum model of the atom Bohr model oly
More informationThe power of analytical spectroscopy
The power of aalytical spectroscopy Daiila et al. J. Rama Spectr. 33, 807 (00) Reflected light Red lake varish UV light Rama spectrum Lead white ciabar Caput mortuum Byzatie Ico (AD Our 534), Lady, Our
More informationBohr s Atomic Model Quantum Mechanical Model
September 7, 0 - Summary - Itroductio to Atomic Theory Bohr s Atomic Model Quatum Mechaical Model 3- Some Defiitio 3- Projects Temperature Pressure Website Subject Areas Plasma is a Mixture of electros,
More informationPHYS-3301 Lecture 7. CHAPTER 4 Structure of the Atom. Rutherford Scattering. Sep. 18, 2018
CHAPTER 4 Structure of the Atom PHYS-3301 Lecture 7 4.1 The Atomic Models of Thomso ad Rutherford 4.2 Rutherford Scatterig 4.3 The Classic Atomic Model 4.4 The Bohr Model of the Hydroge Atom 4.5 Successes
More informationExercises and Problems
HW Chapter 4: Oe-Dimesioal Quatum Mechaics Coceptual Questios 4.. Five. 4.4.. is idepedet of. a b c mu ( E). a b m( ev 5 ev) c m(6 ev ev) Exercises ad Problems 4.. Model: Model the electro as a particle
More informationLecture 36 (Atomic Spectra) Physics Spring 2018 Douglas Fields
Lecture 36 (Atomic Spectra) Physics 6-1 Sprig 18 Douglas Fields Frauhofer Lies I the late 17s ad early 18s, oe of the premier skills was that of glassmaker. Joseph Frauhofer became oe of the most skilled
More informationPhysics Methods in Art and Archaeology
Physics Methods i Art ad Archaeology Michael Wiescher PHYS 78 Archaeologist i the 90ties Somewhere i South America 80 years later --- i the Valley of the Kigs, gypt Physics Tools & Techology Dager & Adveture
More informationName Solutions to Test 2 October 14, 2015
Name Solutios to Test October 4, 05 This test cosists of three parts. Please ote that i parts II ad III, you ca skip oe questio of those offered. The equatios below may be helpful with some problems. Costats
More informationSPEC/4/PHYSI/SPM/ENG/TZ0/XX PHYSICS PAPER 1 SPECIMEN PAPER. 45 minutes INSTRUCTIONS TO CANDIDATES
SPEC/4/PHYSI/SPM/ENG/TZ0/XX PHYSICS STANDARD LEVEL PAPER 1 SPECIMEN PAPER 45 miutes INSTRUCTIONS TO CANDIDATES Do ot ope this examiatio paper util istructed to do so. Aswer all the questios. For each questio,
More informationExperimental Fact: E = nhf
CHAPTR 3 The xperimetal Basis of Quatum PHYS-3301 Lecture 4 Sep. 6, 2018 3.1 Discovery of the X Ray ad the lectro 3.2 Determiatio of lectro Charge 3.3 Lie Spectra 3.4 Quatizatio 3.5 Blackbody Radiatio
More informationDevelopment of QM. What do we know from classical physics? 1. Energy can take any continuous value.
Developmet of QM 1-1 What do we kow from classical physics? 1. Eergy ca take ay cotiuous value.. Electromagetic radiatio is a electric field oscillatig perpedicular to the directio of propagatio. 3. Ay
More informationPHYS-3301 Lecture 9. CHAPTER 5 Wave Properties of Matter and Quantum Mechanics I. 5.3: Electron Scattering. Bohr s Quantization Condition
CHAPTER 5 Wave Properties of Matter ad Quatum Mecaics I PHYS-3301 Lecture 9 Sep. 5, 018 5.1 X-Ray Scatterig 5. De Broglie Waves 5.3 Electro Scatterig 5.4 Wave Motio 5.5 Waves or Particles? 5.6 Ucertaity
More informationThe Pendulum. Purpose
The Pedulum Purpose To carry out a example illustratig how physics approaches ad solves problems. The example used here is to explore the differet factors that determie the period of motio of a pedulum.
More informationChapter 5 Vibrational Motion
Fall 4 Chapter 5 Vibratioal Motio... 65 Potetial Eergy Surfaces, Rotatios ad Vibratios... 65 Harmoic Oscillator... 67 Geeral Solutio for H.O.: Operator Techique... 68 Vibratioal Selectio Rules... 7 Polyatomic
More informationsessions lectures 3-4
Chemistry 1B Fall 016 quatizatio of eergy Chemistry 1B Fall 016 sessios lectures 3-4 E photo = h absorptio ad emissio spectra of hydroge atom 18 Z E. 17810 J Z=1 for H atom, =1,, 3,... 18 1. 17810 J 1
More informationPhysics 201 Final Exam December
Physics 01 Fial Exam December 14 017 Name (please prit): This test is admiistered uder the rules ad regulatios of the hoor system of the College of William & Mary. Sigature: Fial score: Problem 1 (5 poits)
More informationThings you should know when you leave Discussion today for one-electron atoms:
E = -R Thigs ou should kow whe ou leave Discussio toda for oe-electro atoms: = -.79 0-8 J = -.6eV ΔEmatter=E-Em ; Ioizatio Eerg=E E(iitial) ΔΕlight=hνlight= IE +KE. Cosider the followig eerg levels of
More informationReview Sheet for Final Exam
Sheet for ial To study for the exam, we suggest you look through the past review sheets, exams ad homework assigmets, ad idetify the topics that you most eed to work o. To help with this, the table give
More informationPHYS-3301 Lecture 10. Wave Packet Envelope Wave Properties of Matter and Quantum Mechanics I CHAPTER 5. Announcement. Sep.
Aoucemet Course webpage http://www.phys.ttu.edu/~slee/3301/ PHYS-3301 Lecture 10 HW3 (due 10/4) Chapter 5 4, 8, 11, 15, 22, 27, 36, 40, 42 Sep. 27, 2018 Exam 1 (10/4) Chapters 3, 4, & 5 CHAPTER 5 Wave
More informationTrue Nature of Potential Energy of a Hydrogen Atom
True Nature of Potetial Eergy of a Hydroge Atom Koshu Suto Key words: Bohr Radius, Potetial Eergy, Rest Mass Eergy, Classical Electro Radius PACS codes: 365Sq, 365-w, 33+p Abstract I cosiderig the potetial
More informationEXPERIMENT OF SIMPLE VIBRATION
EXPERIMENT OF SIMPLE VIBRATION. PURPOSE The purpose of the experimet is to show free vibratio ad damped vibratio o a system havig oe degree of freedom ad to ivestigate the relatioship betwee the basic
More informationHE ATOM & APPROXIMATION METHODS MORE GENERAL VARIATIONAL TREATMENT. Examples:
5.6 4 Lecture #3-4 page HE ATOM & APPROXIMATION METHODS MORE GENERAL VARIATIONAL TREATMENT Do t restrict the wavefuctio to a sigle term! Could be a liear combiatio of several wavefuctios e.g. two terms:
More informationAtomic Physics 4. Name: Date: 1. The de Broglie wavelength associated with a car moving with a speed of 20 m s 1 is of the order of. A m.
Name: Date: Atomic Pysics 4 1. Te de Broglie wavelegt associated wit a car movig wit a speed of 0 m s 1 is of te order of A. 10 38 m. B. 10 4 m. C. 10 4 m. D. 10 38 m.. Te diagram below sows tree eergy
More information1. Szabo & Ostlund: 2.1, 2.2, 2.4, 2.5, 2.7. These problems are fairly straightforward and I will not discuss them here.
Solutio set III.. Szabo & Ostlud:.,.,.,.5,.7. These problems are fairly straightforward ad I will ot discuss them here.. N! N! i= k= N! N! N! N! p p i j pi+ pj i j i j i= j= i= j= AA ˆˆ= ( ) Pˆ ( ) Pˆ
More informationVibrational Spectroscopy 1
Applied Spectroscopy Vibratioal Spectroscopy Recommeded Readig: Bawell ad McCash Chapter 3 Atkis Physical Chemistry Chapter 6 Itroductio What is it? Vibratioal spectroscopy detects trasitios betwee the
More informationPHYS-3301 Lecture 3. EM- Waves behaving like Particles. CHAPTER 3 The Experimental Basis of Quantum. CHAPTER 3 The Experimental Basis of Quantum
CHAPTER 3 The Experimetal Basis of Quatum PHYS-3301 Lecture 3 Sep. 4, 2018 3.1 Discovery of the X Ray ad the Electro 3.2 Determiatio of Electro Charge 3.3 Lie Spectra 3.4 Quatizatio 3.5 Blackbody Radiatio
More informationLecture 11. Applying Boltzmann Statistics. Heat capacities. Elasticity of a Polymer. C V of molecules for real!! When equipartition fails
Lecture 11 Applyig Boltzma Statistics Elasticity of a Polymer Heat capacities C V of molecules for real!! Whe equipartitio fails Readig for this Lecture: Elemets Ch 8 Readig for Lecture 12: Elemets Ch
More informationProblem 1. Problem Engineering Dynamics Problem Set 9--Solution. Find the equation of motion for the system shown with respect to:
2.003 Egieerig Dyamics Problem Set 9--Solutio Problem 1 Fid the equatio of motio for the system show with respect to: a) Zero sprig force positio. Draw the appropriate free body diagram. b) Static equilibrium
More informationTypes of Waves Transverse Shear. Waves. The Wave Equation
Waves Waves trasfer eergy from oe poit to aother. For mechaical waves the disturbace propagates without ay of the particles of the medium beig displaced permaetly. There is o associated mass trasport.
More informationHydrogen (atoms, molecules) in external fields. Static electric and magnetic fields Oscyllating electromagnetic fields
Hydroge (atoms, molecules) i exteral fields Static electric ad magetic fields Oscyllatig electromagetic fields Everythig said up to ow has to be modified more or less strogly if we cosider atoms (ad ios)
More informationRecombiatio Lies Itroductio to Radio Spectral Lies Á Ü Spectral lies are arrow ( ) emissio or absorptio features i the spectra of gaseous sources. Examples of radio spectral lies iclude the Õ = cm hyperfie
More informationTotal number of nucleons: mass number 238 Number of protons: atomic number 92U
9 The Nucleus Protos Neutros Nucleos Total umber of ucleos: mass umber 8 Number of protos: atomic umber 9U Isotopes: idetical atomic umbers differet mass umbers same chemical properties differet uclear
More informationAndrei Tokmakoff, MIT Department of Chemistry, 5/19/
drei Tokmakoff, MT Departmet of Chemistry, 5/9/5 4-9 Rate of bsorptio ad Stimulated Emissio The rate of absorptio iduced by the field is E k " (" (" $% ˆ µ # (" &" k k (4. The rate is clearly depedet o
More informationCoherent control of Rydberg atoms
Coheret cotrol of Rydberg atoms Haruka Maeda Departmet of Phys. & Math., Aoyama Gakui Uiversity Why Rydberg atom? Multilevel ladder system What ca we study with Rydberg atom? Microwave multiphoto ioizatio
More informationAll Excuses must be taken to 233 Loomis before 4:15, Monday, April 30.
Miscellaeous Notes The ed is ear do t get behid. All Excuses must be take to 233 Loomis before 4:15, Moday, April 30. The PHYS 213 fial exam times are * 8-10 AM, Moday, May 7 * 8-10 AM, Tuesday, May 8
More informationPaper-II Chapter- Damped vibration
Paper-II Chapter- Damped vibratio Free vibratios: Whe a body cotiues to oscillate with its ow characteristics frequecy. Such oscillatios are kow as free or atural vibratios of the body. Ideally, the body
More informationPHYS-3301 Lecture 5. CHAPTER 3 The Experimental Basis of Quantum. 3.8: Compton Effect. 3.8: Compton Effect. Sep. 11, 2018
CHAPTER 3 The Experimetal Basis of Quatum PHYS-3301 Lecture 5 Sep. 11, 2018 3.1 Discovery of the X Ray ad the Electro 3.2 Determiatio of Electro Charge 3.3 Lie Spectra 3.4 Quatizatio 3.5 Blackbody Radiatio
More informationUniversity of Washington Department of Chemistry Chemistry 453 Winter Quarter 2015
Uiversity of Wasigto Departmet of Cemistry Cemistry 453 Witer Quarter 15 Lecture 14. /11/15 Recommeded Text Readig: Atkis DePaula: 9.1, 9., 9.3 A. Te Equipartitio Priciple & Eergy Quatizatio Te Equipartio
More informationCHAPTER 8 SYSTEMS OF PARTICLES
CHAPTER 8 SYSTES OF PARTICLES CHAPTER 8 COLLISIONS 45 8. CENTER OF ASS The ceter of mass of a system of particles or a rigid body is the poit at which all of the mass are cosidered to be cocetrated there
More informationSound II. Sound intensity level. Question. Energy and Intensity of sound waves
Soud. Eergy ad tesity terferece of soud waes Stadig waes Complex soud waes Eergy ad tesity of soud waes power tesity eergy P time power P area A area A (uits W/m ) Soud itesity leel β 0log o o 0 - W/m
More information1. Collision Theory 2. Activation Energy 3. Potential Energy Diagrams
Chemistry 12 Reactio Kietics II Name: Date: Block: 1. Collisio Theory 2. Activatio Eergy 3. Potetial Eergy Diagrams Collisio Theory (Kietic Molecular Theory) I order for two molecules to react, they must
More information2C09 Design for seismic and climate changes
2C09 Desig for seismic ad climate chages Lecture 02: Dyamic respose of sigle-degree-of-freedom systems I Daiel Grecea, Politehica Uiversity of Timisoara 10/03/2014 Europea Erasmus Mudus Master Course Sustaiable
More informationChem Discussion #13 Chapter 10. Correlation diagrams for diatomic molecules. Key
Chem 101 017 Discussio #13 Chapter 10. Correlatio diagrams for diatomic molecules. Key 1. Below is a plot of the first 10 ioizatio eergies for a sigle atom i 3 rd row of the periodic table. The x- axis
More informationWhy? The atomic nucleus. Radioactivity. Nuclear radiations. The electrons and the nucleus. Length scale of the nature
The atomic ucleus. Radioactivity. Nuclear radiatios László Smeller Why? Medical alicatios of the uclear radiatio: - Nuclear imagig - Radiotheray Legth scale of the ature m meter me -3 millimeter size of
More informationMechanics Physics 151
Mechaics Physics 151 Lecture 4 Cotiuous Systems ad Fields (Chapter 13) What We Did Last Time Built Lagragia formalism for cotiuous system Lagragia L = L dxdydz d L L Lagrage s equatio = dx η, η Derived
More informationKinetics of Complex Reactions
Kietics of Complex Reactios by Flick Colema Departmet of Chemistry Wellesley College Wellesley MA 28 wcolema@wellesley.edu Copyright Flick Colema 996. All rights reserved. You are welcome to use this documet
More informationAnnouncements, Nov. 19 th
Aoucemets, Nov. 9 th Lecture PRS Quiz topic: results Chemical through Kietics July 9 are posted o the course website. Chec agaist Kietics LabChec agaist Kietics Lab O Fial Exam, NOT 3 Review Exam 3 ad
More informationWhy? The atomic nucleus. Radioactivity. Nuclear radiations. Length scale of the nature. The electrons and the nucleus
The atomic ucleus. Radioactivity. Nuclear radiatios László Smeller Why? Medical alicatio of uclear radiatio: Nuclear imagig Radiotheray Legth scale of the ature m meter me -3 millimeter size of letters
More informationHarmonic Quantum Integer
Harmoic Quatum Iteger The hypothesis of this paper is that there is a quatum iteger umber system that is aalogous to the umbers associated with the elemets, the isotopes, or the differet eergy states of
More informationPhysics 2D Lecture Slides Lecture 25: Mar 2 nd
Cofirmed: D Fial Eam: Thursday 8 th March :3-:3 PM WH 5 Course Review 4 th March am WH 5 (TBC) Physics D ecture Slides ecture 5: Mar d Vivek Sharma UCSD Physics Simple Harmoic Oscillator: Quatum ad Classical
More informationAccuracy of TEXTOR He-beam diagnostics
Accuracy of TEXTOR He-beam diagostics O. Schmitz, I.L.Beigma *, L.A. Vaishtei *, A. Pospieszczyk, B. Schweer, M. Krychoviak, U. Samm ad the TEXTOR team Forschugszetrum Jülich,, Jülich, Germay *Lebedev
More informationIntrinsic Carrier Concentration
Itrisic Carrier Cocetratio I. Defiitio Itrisic semicoductor: A semicoductor material with o dopats. It electrical characteristics such as cocetratio of charge carriers, deped oly o pure crystal. II. To
More informationPhysics 2D Lecture Slides Lecture 22: Feb 22nd 2005
Physics D Lecture Slides Lecture : Feb d 005 Vivek Sharma UCSD Physics Itroducig the Schrodiger Equatio! (, t) (, t) #! " + U ( ) "(, t) = i!!" m!! t U() = characteristic Potetial of the system Differet
More informationPhysics Oct Reading
Physics 301 21-Oct-2002 17-1 Readig Fiish K&K chapter 7 ad start o chapter 8. Also, I m passig out several Physics Today articles. The first is by Graham P. Collis, August, 1995, vol. 48, o. 8, p. 17,
More informationLecture 25 (Dec. 6, 2017)
Lecture 5 8.31 Quatum Theory I, Fall 017 106 Lecture 5 (Dec. 6, 017) 5.1 Degeerate Perturbatio Theory Previously, whe discussig perturbatio theory, we restricted ourselves to the case where the uperturbed
More informationPhys 172 Modern Mechanics Summer 2010
Phys 172 Modern Mechanics Summer 2010 r r Δ p = F Δt sys net Δ E = W + Q sys sys net surr r r Δ L = τ Δt Lecture 14 Energy Quantization Read:Ch 8 Reading Quiz 1 An electron volt (ev) is a measure of: A)
More informationPhysics 232 Gauge invariance of the magnetic susceptibilty
Physics 232 Gauge ivariace of the magetic susceptibilty Peter Youg (Dated: Jauary 16, 2006) I. INTRODUCTION We have see i class that the followig additioal terms appear i the Hamiltoia o addig a magetic
More informationQuantum Annealing for Heisenberg Spin Chains
LA-UR # - Quatum Aealig for Heiseberg Spi Chais G.P. Berma, V.N. Gorshkov,, ad V.I.Tsifriovich Theoretical Divisio, Los Alamos Natioal Laboratory, Los Alamos, NM Istitute of Physics, Natioal Academy of
More informationLecture #1 Nasser S. Alzayed.
Lecture #1 Nasser S. Alzayed alzayed@ksu.edu.sa Chapter 6: Free Electro Fermi Gas Itroductio We ca uderstad may physical properties of metals, ad ot oly of the simple metals, i terms of the free electro
More informationNumerical Methods in Fourier Series Applications
Numerical Methods i Fourier Series Applicatios Recall that the basic relatios i usig the Trigoometric Fourier Series represetatio were give by f ( x) a o ( a x cos b x si ) () where the Fourier coefficiets
More informationMIXED REVIEW of Problem Solving
MIXED REVIEW of Problem Solvig STATE TEST PRACTICE classzoe.com Lessos 2.4 2.. MULTI-STEP PROBLEM A ball is dropped from a height of 2 feet. Each time the ball hits the groud, it bouces to 70% of its previous
More informationLecture 3-7 Semiconductor Lasers.
Laser LED Stimulated emissio Spotaeous emissio Laser I th I Typical output optical power vs. diode curret (I) characteristics ad the correspodig output spectrum of a laser diode.?1999 S.O. Kasap, Optoelectroics
More informationThe Quantum Oscillatory Modulated Potential I The Hydrogen Atom
Joural of Moder Physics 3 597-63 http://dx.doi.org/.436/jmp..378 Published Olie July (http://www.scirp.org/joural/jmp) The Quatum Oscillatory Modulated Potetial I The Hydroge Atom Waldemar Woley Filho
More informationPHYS 321 Solutions to Practice Final (December 2002).
PHYS Solutios to Practice Fial (December ) Two masses, m ad m are coected by a sprig of costat k, leadig to the potetial V( r) = k( r ) r a) What is the Lagragia for this system? (Assume -dimesioal motio)
More information5. Quantum Nature of the Nano-world ( Fundamental of. Quantum mechanics)
5. Quatu Nature of the Nao-world Fudaetal of What is the defiitio of aoaterials?? Quatu echaics i Origial: quatu size effect where the electroic properties of solids are altered with great reductios i
More informationMihai V. Putz: Undergraduate Structural Physical Chemistry Course, Lecture 6 1
Mihai V. Putz: Udergraduate Structural Physical Chemistry Course, Lecture 6 Lecture 6: Quatum-Classical Correspodece I. Bohr s Correspodece Priciple Turig back to Bohr atomic descriptio it provides the
More information: ) 9) 6 PM, 6 PM
Physics 101 Sectio 3 Mar. 1 st : Ch. 7-9 review Ch. 10 Aoucemets: Test# (Ch. 7-9) will be at 6 PM, March 3 (6) Lockett) Study sessio Moday eveig at 6:00PM at Nicholso 130 Class Website: http://www.phys.lsu.edu/classes/sprig010/phys101-3/
More informationEngineering Mechanics Dynamics & Vibrations. Engineering Mechanics Dynamics & Vibrations Plane Motion of a Rigid Body: Equations of Motion
1/5/013 Egieerig Mechaics Dyaics ad Vibratios Egieerig Mechaics Dyaics & Vibratios Egieerig Mechaics Dyaics & Vibratios Plae Motio of a Rigid Body: Equatios of Motio Motio of a rigid body i plae otio is
More informationUnit 5. Gases (Answers)
Uit 5. Gases (Aswers) Upo successful completio of this uit, the studets should be able to: 5. Describe what is meat by gas pressure.. The ca had a small amout of water o the bottom to begi with. Upo heatig
More informationATOMIC STRUCTURE (ADVANCED) FOUNDATION BUILDER (OBJECTIVE) By law of conservation of mass and change the missing particle in neutron
. (A) Li? e 6 ATOMIC STRUCTURE (ADVANCED) FOUNDATION BUILDER (OBJECTIVE) By law of coservatio of mass ad cage te missig particle i eutro. (D) e ratio lies i te sequece p l M Particle Cage Mass + + + p
More information1. Hydrogen Atom: 3p State
7633A QUANTUM MECHANICS I - solutio set - autum. Hydroge Atom: 3p State Let us assume that a hydroge atom is i a 3p state. Show that the radial part of its wave fuctio is r u 3(r) = 4 8 6 e r 3 r(6 r).
More informationToday. Homework 4 due (usual box) Center of Mass Momentum
Today Homework 4 due (usual box) Ceter of Mass Mometum Physics 40 - L 0 slide review Coservatio of Eergy Geeralizatio of Work-Eergy Theorem Says that for ay isolated system, the total eergy is coserved
More informationThis exam is formed of four exercises in four pages numbered from 1 to 4 The use of non-programmable calculator is recommended
وزارة التربية والتعلين العالي الوديرية العاهة للتربية دائرة االهتحانات اهتحانات الشهادة الثانىية العاهة الفرع : علىم عاهة مسابقة في مادة الفيزياء المدة ثالث ساعات االسن: الرقن: الدورة العادية للعام This
More informationmx bx kx F t. dt IR I LI V t, Q LQ RQ V t,
Lecture 5 omplex Variables II (Applicatios i Physics) (See hapter i Boas) To see why complex variables are so useful cosider first the (liear) mechaics of a sigle particle described by Newto s equatio
More informationProbability, Expectation Value and Uncertainty
Chapter 1 Probability, Expectatio Value ad Ucertaity We have see that the physically observable properties of a quatum system are represeted by Hermitea operators (also referred to as observables ) such
More informationEE 485 Introduction to Photonics Photon Optics and Photon Statistics
Itroductio to Photoics Photo Optics ad Photo Statistics Historical Origi Photo-electric Effect (Eistei, 905) Clea metal V stop Differet metals, same slope Light I Slope h/q ν c/λ Curret flows for λ < λ
More information567. Research of Dynamics of a Vibration Isolation Platform
567. Research of Dyamics of a Vibratio Isolatio Platform A. Kilikevičius, M. Jurevičius 2, M. Berba 3 Vilius Gedimias Techical Uiversity, Departmet of Machie buildig, J. Basaavičiaus str. 28, LT-03224
More informationMiscellaneous Notes. Lecture 19, p 1
Miscellaeous Notes The ed is ear do t get behid. All Excuses must be take to 233 Loomis before oo, Thur, Apr. 25. The PHYS 213 fial exam times are * 8-10 AM, Moday, May 6 * 1:30-3:30 PM, Wed, May 8 The
More informationSequences I. Chapter Introduction
Chapter 2 Sequeces I 2. Itroductio A sequece is a list of umbers i a defiite order so that we kow which umber is i the first place, which umber is i the secod place ad, for ay atural umber, we kow which
More informationECE 442. Spring, Lecture - 4
ECE 44 Power Semicoductor Devices ad Itegrated circuits Srig, 6 Uiversity of Illiois at Chicago Lecture - 4 ecombiatio, geeratio, ad cotiuity equatio 1. Geeratio thermal, electrical, otical. ecombiatio
More informationPART I: MULTIPLE CHOICE (60 POINTS) A m/s B m/s C m/s D m/s E. The car doesn t make it to the top.
Uit II Test (practice test for fall ) (Ch. 6 8, 0) Name: Physics Notes: the actual test will hae 0 m/c ad - writte problems. Also the test will coer ch. 9 (static equilibrium), which was ot coered o this
More informationSOLUTIONS: ECE 606 Homework Week 7 Mark Lundstrom Purdue University (revised 3/27/13) e E i E T
SOUIONS: ECE 606 Homework Week 7 Mark udstrom Purdue Uiversity (revised 3/27/13) 1) Cosider a - type semicoductor for which the oly states i the badgap are door levels (i.e. ( E = E D ). Begi with the
More informationLecture 1 Probability and Statistics
Wikipedia: Lecture 1 Probability ad Statistics Bejami Disraeli, British statesma ad literary figure (1804 1881): There are three kids of lies: lies, damed lies, ad statistics. popularized i US by Mark
More informationOffice: JILA A709; Phone ;
Office: JILA A709; Phoe 303-49-7841; email: weberjm@jila.colorado.edu Problem Set 5 To be retured before the ed of class o Wedesday, September 3, 015 (give to me i perso or slide uder office door). 1.
More informationVector Quantization: a Limiting Case of EM
. Itroductio & defiitios Assume that you are give a data set X = { x j }, j { 2,,, }, of d -dimesioal vectors. The vector quatizatio (VQ) problem requires that we fid a set of prototype vectors Z = { z
More informationME 440 Intermediate Vibrations
ME 440 Itermediate Vibratios Th, Jauary 29, 2009 Sectio 1.11 Da Negrut, 2009 ME440, UW-Madiso Before we get started Last Time: Discussed about periodic fuctios Covered the Fourier Series Expasio Wet through
More informationThe Transition Dipole Moment
The Trasitio Dipole Momet Iteractio of Light with Matter The probability that a molecule absorbs or emits light ad udergoes a trasitio from a iitial to a fial state is give by the Eistei coefficiet, B
More informationLecture 6. Semiconductor physics IV. The Semiconductor in Equilibrium
Lecture 6 Semicoductor physics IV The Semicoductor i Equilibrium Equilibrium, or thermal equilibrium No exteral forces such as voltages, electric fields. Magetic fields, or temperature gradiets are actig
More informationThe Transition Dipole Moment
The Trasitio Dipole Momet Iteractio of Light with Matter The probability that a molecule absorbs or emits light ad udergoes a trasitio from a iitial to a fial state is give by the Eistei coefficiet, B
More informationParticle nature of light & Quantization
Particle nature of light & Quantization A quantity is quantized if its possible values are limited to a discrete set. An example from classical physics is the allowed frequencies of standing waves on a
More informationECEN Microelectronics. Semiconductor Physics and P/N junctions 2/05/19
ECEN 3250 Microelectroics Semicoductor Physics ad P/N juctios 2/05/19 Professor J. Gopiath Professor J. Gopiath Uiversity of Colorado at Boulder Microelectroics Sprig 2014 Overview Eergy bads Atomic eergy
More informationACCESS TO SCIENCE, ENGINEERING AND AGRICULTURE: MATHEMATICS 1 MATH00030 SEMESTER / Statistics
ACCESS TO SCIENCE, ENGINEERING AND AGRICULTURE: MATHEMATICS 1 MATH00030 SEMESTER 1 018/019 DR. ANTHONY BROWN 8. Statistics 8.1. Measures of Cetre: Mea, Media ad Mode. If we have a series of umbers the
More informationMIT Department of Chemistry 5.74, Spring 2005: Introductory Quantum Mechanics II Instructor: Professor Andrei Tokmakoff
MIT Departmet of Chemistry 5.74, Sprig 5: Itroductory Quatum Mechaics II Istructor: Professor Adrei Tomaoff p. 97 ABSORPTION SPECTRA OF MOLECULAR AGGREGATES The absorptio spectra of periodic arrays of
More informationPRACTICE PROBLEMS FOR THE FINAL
PRACTICE PROBLEMS FOR THE FINAL Math 36Q Fall 25 Professor Hoh Below is a list of practice questios for the Fial Exam. I would suggest also goig over the practice problems ad exams for Exam ad Exam 2 to
More informationreactions / Fission Classification of nuclear reactions
Classiicatio o uclear reactios reactios / Fissio Geeralities Liquid-drop picture Chai reactios Mass distributio Fissio barrier Double issio barrier Ater the scissio poit Time scale i issio Neutro-iduced
More informationMA131 - Analysis 1. Workbook 2 Sequences I
MA3 - Aalysis Workbook 2 Sequeces I Autum 203 Cotets 2 Sequeces I 2. Itroductio.............................. 2.2 Icreasig ad Decreasig Sequeces................ 2 2.3 Bouded Sequeces..........................
More informationPROBLEM Copyright McGraw-Hill Education. Permission required for reproduction or display. SOLUTION. v 1 = 4 km/hr = 1.
PROLEM 13.119 35,000 Mg ocea lier has a iitial velocity of 4 km/h. Neglectig the frictioal resistace of the water, determie the time required to brig the lier to rest by usig a sigle tugboat which exerts
More informationFIR Filter Design: Part II
EEL335: Discrete-Time Sigals ad Systems. Itroductio I this set of otes, we cosider how we might go about desigig FIR filters with arbitrary frequecy resposes, through compositio of multiple sigle-peak
More information(4 pts.) (4 pts.) (4 pts.) b) y(x,t) = 1/(ax 2 +b) This function has no time dependence, so cannot be a wave.
12. For each of the possible wave forms below, idicate which satisf the wave equatio, ad which represet reasoable waveforms for actual waves o a strig. For those which do represet waves, fid the speed
More informationNARAYANA. XI-REG (Date: ) Physics Chemistry Mathematics
CPT-5 / XI-REG / 0..07 / Hits & Solutio CODE NARAYANA I I T / N E E T A C A D E M Y XI-REG XI-REG (Date: 0..07) Physics Chemistry Mathematics. 3. 6.. 3 3. 6. 3. 33. 63.. 3. 6. 5. 35. 65. 6. 3 36. 66. 7.
More information