Name Solutions to Test 2 October 14, 2015

Size: px
Start display at page:

Download "Name Solutions to Test 2 October 14, 2015"

Transcription

1 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 4 h J s 5 h 4.60 ev s J s 6 =6.580 ev s kb.8070 J/K 5 kb ev/k k N m / C 9 e.60 0 C 9 ev.60 0 J ke c 7 9 Part I: Multiple Choice [0 poits] For each questio, choose the best aswer ( poits each). Oe of the ucertaity relatios says that A) Et B) Et C) t E D) t E E) oe of these Hydroge-Like Atoms Hydroge Spectrum 4 kez c Z E 9.7 m m.60 ev Z E Black Bodies 4 kt B Wave Reduced Mass U Relatioships 5c mm max T m K m M k Compto Effect Rutherford Scatterig f h kqq T b cot cos mc mv h.46 0 m Ze k mc R E. Why was there a problem i statistical mechaics whe studyig a thermal distributio of electromagetic waves? A) The eergy i each mode could be aythig, so there was o idea how to figure out how much there was B) Log wavelegths had most of the eergy, leadig to the ifrared catastrophe C) Short wavelegths had most of the eergy, leadig to the ultraviolet catastrophe D) The predictios could ot explai the photoelectric effect E) There was already ample evidece that light was made of particles (photos). Whe you have a wave packet, the speed of the etire packet is govered by the velocity, while the speed of idividual waves withi it are govered by the velocity. A) Group, wave B) Wave, group C) Group, phase D) Phase, group E) Phase, wave

2 4. Which hypothesis is attributed to debroglie? A) Electros have wave-like properties B) Electros must satisfy Schrödiger s equatio C) Electros orbit the ucleus o circular paths D) Electros have agular mometum that is a multiple of E) Electros satisfy a ucertaity relatio o their positio ad mometum 5. If 4 i, what is? A) 7 B) 5 C) 7 + 4i D) 5 + 4i E) Noe of these 6. If f xy, Ax y, the f x A) Ax B) Ax C) A(x + y) D) A(x + y) E) Ay 7. I which of the followig ways is a atom very much like the solar system? A) The mai force ivolved is electromagetism i both cases B) The mai force ivolved is gravity i both cases C) The force betwee two of the orbitig objects is egligible compared to the force betwee oe of the orbitig objects ad the cetral object D) The agular mometum for a sigle electro or plaet is usually a small multiple of E) The cetral object (Su or ucleus) is much smaller tha the size of the whole object (solar system or atom) 8. A dispersio relatio is a relatio betwee which two quatities? A) ad k B) ad f C) ad T D) ad k E) f ad T 9. Rutherford scattered alpha particles off of gold atoms, ad discovered, to his surprise, that A) Most of them wet straight through, suggestig the atom was mostly empty space B) The gold atoms were ofte kocked out, suggestig they were loosely boud C) The electros did little to stop them, showig that electros were light D) The alpha particles sometimes scattered at large agles, suggestig there was a lot of mass ad charge cocetrated i the ucleus E) The gold atoms would ofte be trasmuted to other metals, like lead 0. Wave effects i quatum mechaics are ot oticeable i the everyday world because A) Quatum mechaics does t apply to composite objects, like all everyday objects B) Quatum effects oly describe wave packets, which do t apply to particles C) Quatum effects are so slow that you ca t observe them D) The wavelegth is eormous compared to the size of everyday objects E) The wavelegth is tiy compared to the size of everyday objects

3 Part II: Short aswer [0 poits] Choose two of the followig questios ad give a short aswer (- seteces) (0 poits each).. Explai, i the photoelectric effect, why there is a miimum frequecy which suffices to free a electro from a metal. Whe you are above that frequecy, give a formula for the maximum eergy with which a electro ca be ejected. The photos have eergy E = hf. There is a miimum amout of work (called the work fuctio) for ay give metal that must be iput i order to free the electro. If hf <, the o electros ca be freed. If hf >, the electros ca be freed, ad those electros ca have at most a eergy of Emax = hf.. Sice a electro is attracted to the ucleus, it should have a miimum eergy whe it is exactly at the ucleus ad has zero velocity. Explai why this ca t happe i quatum mechaics. You should have at least oe mathematical relatio i your aswer. The miimum eergy would correspod to positio x = 0 ad mometum p = 0. However, specifyig both of these simultaeously is impossible for quatum waves, because the x p. product of the ucertaities are cotraied by the iequality. Whe electros are accelerated through a thi gas, ad the voltage is gradually icreased, at first the curret will icrease, the at certai threshold velocities, the curret will suddely drop ad the gas begis to glow. Explai qualitatively what is happeig. This is a descriptio of the Frack-Hertz experimet. Because atoms have oly certai levels that are eergies, there is a miimum amout of eergy that ca be absorbed by the atoms. Hece whe electros with less tha this eergy collide, they must collide elastically, maitaiig their speed. But whe we reach this threshold eergy, the atoms suddely ca absorb the eergy, slowig dow the electros ad ultimately decreasig the curret. But the atom is ow i a excited state, ad it emits a photo (it glows) whe it falls back to its groud state.

4 Part III: Calculatio: [60 poits] Choose three of the followig four questios ad perform the idicated calculatios (0 poits each). 4. Oe importat evet i the early uiverse is called recombiatio, ad occurred whe the temperature of the uiverse was approximately T = 970 K. The uiverse was filled with almost perfect black body radiatio at this time. (a) Fid the eergy desity of the blackbody radiatio at this time i J/m. The eergy desity is give by.8070 J/K970 K 4 kt B U c J s.9980 m/s J/m. (b) Fid the wavelegth where the blackbody radiatio was strogest at this time, i m. We use Wie s Law, max T m K, to fid max T m K m m. 970K (c) Fid the eergy for a sigle photo correspodig to the wavelegth you foud i part (b). The eergy of a photo is give by E hf, where f ca be foud from f c, so J J s m/s hc E hf m.7 ev.600 J/eV J (d) Usig the eergy desity you foud i part (a) ad the eergy you foud i part (c), estimate the umber of photos per uit volume (i m - ) at this time. The eergy desity is equal to the eergy per photo times the umber desity of photos, so a simple estimate would yield U J/m 9 E.060 J m. There is a flaw i this argumet, i that we used the eergy of the peak wavelegth photo. The 7 actual umber is more like 5. 0 m istead.

5 5. A N +6 io has atomic umber Z = 7, oe electro, ad is i the = 7 state iitially. (a) What is the eergy of this state? The eergy is give by.60 evz.60 ev7 E.60 ev. 7 (b) A photo of eergy E =.056 ev is absorbed by this atom. What is the ew eergy of the atom? What is the value of ow? Sice a photo is absorbed, the eergy icreases to The fial state ca the be foud from E E E.60 ev ev ev f i Z.60 ev.60 ev ev E,.60 ev7 5, ev 5. (c) The same atom, still at = 7, istead emits a photo of eergy E =.056 ev. What is the ew eergy of the atom? What is the value of ow? This time the eergy is lost, so E E E.60 ev.056 ev ev The fial state ca the be foud from f i Z.60 ev.60 ev ev E,.60 ev7 5, ev 5. (d) What is the wavelegth of light correspodig to a eergy of E =.056 ev? The wavelegth ca be foud from f c, ad the frequecy from E hf, so ev s m/s c hc hc f hf E.056 ev m 94.9 m.

6 6. The 05 Nobel Prize i physics wet to experimeters who demostrated that oe of the eutrios has mass. Based o the measured mass, a log wavelegth eutrio would have a dispersio relatio of the form Ak where A 6650 m /s. (a) Fid a formula for the phase velocity ad the group velocity i terms of k. The phase velocity ad group velocity are give by v p Ak Ak, k k w k k vg Ak Ak vp. (b) A typical eutrio left over from the Big Bag might have k 85 m. For this wave, fid the wavelegth, the agular frequecy ad the frequecy f. Each of these quatities is easily computed from the relevat formulas: k 85 m m 7.8 mm, 9 Ak 6650 m /s 85 m s, s f s MHz. (c) Fid the group ad phase velocity for the eutrio from part (b) i m/s. We simply substitute ito the formulas from part (a) to yield v v p g Ak m /s 85 m m/s, 7 Ak 6650 m /s 85 m. 0 m/s. (d) Fid the eergy i ev of the eutrio you foud i part (b). We use the simple formula E hf ev s s.7 0 ev.7 ev.

7 7. The wave fuctio for a particle is give by (x) Nx a x a, a a x Na 0 elsewhere. x a Na where N ad a are positive costats. The wave is Na sketched at right. (a) Where i the allowed regio a x a is the particle most likely to be? Where is it impossible for it to be? You ca rely o the sketch if you wish. It is most likely to be where the wave fuctio has the largest magitude (positive or egative), so this is clearly at x a. It is impossible for it to be where the wave fuctio vaishes, which is at x = 0. (b) What is the ormalizatio costat N? We fid the ormalizatio costat by demadig that the probability that it is somewhere be give by. We therefore have a a x dx N x dx N x N a a N a 8 N a, a a N, a N a We could have chose N egative, but the problem says N is positive. (c) If the particle s positio is measured, what is the probability that it will have x > 0? This is simply give by a a x dx 0 N x dx 0 N x 0 N a a 9.%. a

PHYS-3301 Lecture 10. Wave Packet Envelope Wave Properties of Matter and Quantum Mechanics I CHAPTER 5. Announcement. Sep.

PHYS-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 information

PHYS-3301 Lecture 7. CHAPTER 4 Structure of the Atom. Rutherford Scattering. Sep. 18, 2018

PHYS-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 information

Development of QM. What do we know from classical physics? 1. Energy can take any continuous value.

Development 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 information

True Nature of Potential Energy of a Hydrogen Atom

True 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 information

Phys 102 Lecture 25 The quantum mechanical model of light

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 information

PHYS-3301 Lecture 5. CHAPTER 3 The Experimental Basis of Quantum. 3.8: Compton Effect. 3.8: Compton Effect. Sep. 11, 2018

PHYS-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 information

PHYS-3301 Lecture 3. EM- Waves behaving like Particles. CHAPTER 3 The Experimental Basis of Quantum. CHAPTER 3 The Experimental Basis of Quantum

PHYS-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 information

Exercises and Problems

Exercises 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 information

Experimental Fact: E = nhf

Experimental 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 information

The power of analytical spectroscopy

The 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 information

Lecture 36 (Atomic Spectra) Physics Spring 2018 Douglas Fields

Lecture 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 information

Physics 201 Final Exam December

Physics 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 information

Polynomial Functions and Their Graphs

Polynomial Functions and Their Graphs Polyomial Fuctios ad Their Graphs I this sectio we begi the study of fuctios defied by polyomial expressios. Polyomial ad ratioal fuctios are the most commo fuctios used to model data, ad are used extesively

More information

Things you should know when you leave Discussion today for one-electron atoms:

Things 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 information

Math 116 Second Midterm November 13, 2017

Math 116 Second Midterm November 13, 2017 Math 6 Secod Midterm November 3, 7 EXAM SOLUTIONS. Do ot ope this exam util you are told to do so.. Do ot write your ame aywhere o this exam. 3. This exam has pages icludig this cover. There are problems.

More information

17 Phonons and conduction electrons in solids (Hiroshi Matsuoka)

17 Phonons and conduction electrons in solids (Hiroshi Matsuoka) 7 Phoos ad coductio electros i solids Hiroshi Matsuoa I this chapter we will discuss a miimal microscopic model for phoos i a solid ad a miimal microscopic model for coductio electros i a simple metal.

More information

PHYS-3301 Lecture 9. CHAPTER 5 Wave Properties of Matter and Quantum Mechanics I. 5.3: Electron Scattering. Bohr s Quantization Condition

PHYS-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 information

Quantum Mechanics I. 21 April, x=0. , α = A + B = C. ik 1 A ik 1 B = αc.

Quantum Mechanics I. 21 April, x=0. , α = A + B = C. ik 1 A ik 1 B = αc. Quatum Mechaics I 1 April, 14 Assigmet 5: Solutio 1 For a particle icidet o a potetial step with E < V, show that the magitudes of the amplitudes of the icidet ad reflected waves fuctios are the same Fid

More information

TMA4245 Statistics. Corrected 30 May and 4 June Norwegian University of Science and Technology Department of Mathematical Sciences.

TMA4245 Statistics. Corrected 30 May and 4 June Norwegian University of Science and Technology Department of Mathematical Sciences. Norwegia Uiversity of Sciece ad Techology Departmet of Mathematical Scieces Corrected 3 May ad 4 Jue Solutios TMA445 Statistics Saturday 6 May 9: 3: Problem Sow desity a The probability is.9.5 6x x dx

More information

Physics Methods in Art and Archaeology

Physics 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 information

Infinite Sequences and Series

Infinite Sequences and Series Chapter 6 Ifiite Sequeces ad Series 6.1 Ifiite Sequeces 6.1.1 Elemetary Cocepts Simply speakig, a sequece is a ordered list of umbers writte: {a 1, a 2, a 3,...a, a +1,...} where the elemets a i represet

More information

MIDTERM 3 CALCULUS 2. Monday, December 3, :15 PM to 6:45 PM. Name PRACTICE EXAM SOLUTIONS

MIDTERM 3 CALCULUS 2. Monday, December 3, :15 PM to 6:45 PM. Name PRACTICE EXAM SOLUTIONS MIDTERM 3 CALCULUS MATH 300 FALL 08 Moday, December 3, 08 5:5 PM to 6:45 PM Name PRACTICE EXAM S Please aswer all of the questios, ad show your work. You must explai your aswers to get credit. You will

More information

Lecture 6. Semiconductor physics IV. The Semiconductor in Equilibrium

Lecture 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 information

Lecture 6 Simple alternatives and the Neyman-Pearson lemma

Lecture 6 Simple alternatives and the Neyman-Pearson lemma STATS 00: Itroductio to Statistical Iferece Autum 06 Lecture 6 Simple alteratives ad the Neyma-Pearso lemma Last lecture, we discussed a umber of ways to costruct test statistics for testig a simple ull

More information

SPEC/4/PHYSI/SPM/ENG/TZ0/XX PHYSICS PAPER 1 SPECIMEN PAPER. 45 minutes INSTRUCTIONS TO CANDIDATES

SPEC/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 information

Kinetics of Complex Reactions

Kinetics 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 information

The Born-Oppenheimer approximation

The Born-Oppenheimer approximation The Bor-Oppeheimer approximatio 1 Re-writig the Schrödiger equatio We will begi from the full time-idepedet Schrödiger equatio for the eigestates of a molecular system: [ P 2 + ( Pm 2 + e2 1 1 2m 2m m

More information

6.3 Testing Series With Positive Terms

6.3 Testing Series With Positive Terms 6.3. TESTING SERIES WITH POSITIVE TERMS 307 6.3 Testig Series With Positive Terms 6.3. Review of what is kow up to ow I theory, testig a series a i for covergece amouts to fidig the i= sequece of partial

More information

( ) = p and P( i = b) = q.

( ) = p and P( i = b) = q. MATH 540 Radom Walks Part 1 A radom walk X is special stochastic process that measures the height (or value) of a particle that radomly moves upward or dowward certai fixed amouts o each uit icremet of

More information

4.3 Growth Rates of Solutions to Recurrences

4.3 Growth Rates of Solutions to Recurrences 4.3. GROWTH RATES OF SOLUTIONS TO RECURRENCES 81 4.3 Growth Rates of Solutios to Recurreces 4.3.1 Divide ad Coquer Algorithms Oe of the most basic ad powerful algorithmic techiques is divide ad coquer.

More information

Physics 324, Fall Dirac Notation. These notes were produced by David Kaplan for Phys. 324 in Autumn 2001.

Physics 324, Fall Dirac Notation. These notes were produced by David Kaplan for Phys. 324 in Autumn 2001. Physics 324, Fall 2002 Dirac Notatio These otes were produced by David Kapla for Phys. 324 i Autum 2001. 1 Vectors 1.1 Ier product Recall from liear algebra: we ca represet a vector V as a colum vector;

More information

Math 116 Final Exam December 19, 2016

Math 116 Final Exam December 19, 2016 Math 6 Fial Exam December 9, 06 UMID: EXAM SOLUTIONS Iitials: Istructor: Sectio:. Do ot ope this exam util you are told to do so.. Do ot write your ame aywhere o this exam. 3. This exam has 3 pages icludig

More information

Lecture 4. Random variable and distribution of probability

Lecture 4. Random variable and distribution of probability Itroductio to theory of probability ad statistics Lecture. Radom variable ad distributio of probability dr hab.iż. Katarzya Zarzewsa, prof.agh Katedra Eletroii, AGH e-mail: za@agh.edu.pl http://home.agh.edu.pl/~za

More information

Mihai V. Putz: Undergraduate Structural Physical Chemistry Course, Lecture 6 1

Mihai 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

Assignment 2 Solutions SOLUTION. ϕ 1 Â = 3 ϕ 1 4i ϕ 2. The other case can be dealt with in a similar way. { ϕ 2 Â} χ = { 4i ϕ 1 3 ϕ 2 } χ.

Assignment 2 Solutions SOLUTION. ϕ 1  = 3 ϕ 1 4i ϕ 2. The other case can be dealt with in a similar way. { ϕ 2 Â} χ = { 4i ϕ 1 3 ϕ 2 } χ. PHYSICS 34 QUANTUM PHYSICS II (25) Assigmet 2 Solutios 1. With respect to a pair of orthoormal vectors ϕ 1 ad ϕ 2 that spa the Hilbert space H of a certai system, the operator  is defied by its actio

More information

Shedding light on atomic energy levels (segment of Hydrogen spectrum)

Shedding light on atomic energy levels (segment of Hydrogen spectrum) 3.0 ev.85 ev.55 ev.69 ev Fri. 8.4-.7 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)

More information

Name: Math 10550, Final Exam: December 15, 2007

Name: Math 10550, Final Exam: December 15, 2007 Math 55, Fial Exam: December 5, 7 Name: Be sure that you have all pages of the test. No calculators are to be used. The exam lasts for two hours. Whe told to begi, remove this aswer sheet ad keep it uder

More information

Machine Learning Brett Bernstein

Machine Learning Brett Bernstein Machie Learig Brett Berstei Week 2 Lecture: Cocept Check Exercises Starred problems are optioal. Excess Risk Decompositio 1. Let X = Y = {1, 2,..., 10}, A = {1,..., 10, 11} ad suppose the data distributio

More information

Lecture 9: Diffusion, Electrostatics review, and Capacitors. Context

Lecture 9: Diffusion, Electrostatics review, and Capacitors. Context EECS 5 Sprig 4, Lecture 9 Lecture 9: Diffusio, Electrostatics review, ad Capacitors EECS 5 Sprig 4, Lecture 9 Cotext I the last lecture, we looked at the carriers i a eutral semicoductor, ad drift currets

More information

Lecture 5. Random variable and distribution of probability

Lecture 5. Random variable and distribution of probability Itroductio to theory of probability ad statistics Lecture 5. Radom variable ad distributio of probability prof. dr hab.iż. Katarzya Zarzewsa Katedra Eletroii, AGH e-mail: za@agh.edu.pl http://home.agh.edu.pl/~za

More information

There are 7 crystal systems and 14 Bravais lattices in 3 dimensions.

There are 7 crystal systems and 14 Bravais lattices in 3 dimensions. EXAM IN OURSE TFY40 Solid State Physics Moday 0. May 0 Time: 9.00.00 DRAFT OF SOLUTION Problem (0%) Itroductory Questios a) () Primitive uit cell: The miimum volume cell which will fill all space (without

More information

Physics Oct Reading

Physics 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 information

Section 1.1. Calculus: Areas And Tangents. Difference Equations to Differential Equations

Section 1.1. Calculus: Areas And Tangents. Difference Equations to Differential Equations Differece Equatios to Differetial Equatios Sectio. Calculus: Areas Ad Tagets The study of calculus begis with questios about chage. What happes to the velocity of a swigig pedulum as its positio chages?

More information

CEE 522 Autumn Uncertainty Concepts for Geotechnical Engineering

CEE 522 Autumn Uncertainty Concepts for Geotechnical Engineering CEE 5 Autum 005 Ucertaity Cocepts for Geotechical Egieerig Basic Termiology Set A set is a collectio of (mutually exclusive) objects or evets. The sample space is the (collectively exhaustive) collectio

More information

sessions lectures 3-4

sessions 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 information

Today. Homework 4 due (usual box) Center of Mass Momentum

Today. 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 information

Topic 9: Sampling Distributions of Estimators

Topic 9: Sampling Distributions of Estimators Topic 9: Samplig Distributios of Estimators Course 003, 2018 Page 0 Samplig distributios of estimators Sice our estimators are statistics (particular fuctios of radom variables), their distributio ca be

More information

Physics 232 Gauge invariance of the magnetic susceptibilty

Physics 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 information

Limitation of Applicability of Einstein s. Energy-Momentum Relationship

Limitation of Applicability of Einstein s. Energy-Momentum Relationship Limitatio of Applicability of Eistei s Eergy-Mometum Relatioship Koshu Suto Koshu_suto19@mbr.ifty.com Abstract Whe a particle moves through macroscopic space, for a isolated system, as its velocity icreases,

More information

ENGI 4421 Probability and Statistics Faculty of Engineering and Applied Science Problem Set 1 Solutions Descriptive Statistics. None at all!

ENGI 4421 Probability and Statistics Faculty of Engineering and Applied Science Problem Set 1 Solutions Descriptive Statistics. None at all! ENGI 44 Probability ad Statistics Faculty of Egieerig ad Applied Sciece Problem Set Solutios Descriptive Statistics. If, i the set of values {,, 3, 4, 5, 6, 7 } a error causes the value 5 to be replaced

More information

PRACTICE PROBLEMS FOR THE FINAL

PRACTICE 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 information

MID-YEAR EXAMINATION 2018 H2 MATHEMATICS 9758/01. Paper 1 JUNE 2018

MID-YEAR EXAMINATION 2018 H2 MATHEMATICS 9758/01. Paper 1 JUNE 2018 MID-YEAR EXAMINATION 08 H MATHEMATICS 9758/0 Paper JUNE 08 Additioal Materials: Writig Paper, MF6 Duratio: hours DO NOT OPEN THIS BOOKLET UNTIL YOU ARE TOLD TO DO SO READ THESE INSTRUCTIONS FIRST Write

More information

Section A assesses the Units Numerical Analysis 1 and 2 Section B assesses the Unit Mathematics for Applied Mathematics

Section A assesses the Units Numerical Analysis 1 and 2 Section B assesses the Unit Mathematics for Applied Mathematics X0/70 NATIONAL QUALIFICATIONS 005 MONDAY, MAY.00 PM 4.00 PM APPLIED MATHEMATICS ADVANCED HIGHER Numerical Aalysis Read carefully. Calculators may be used i this paper.. Cadidates should aswer all questios.

More information

Solutions to Final Exam Review Problems

Solutions to Final Exam Review Problems . Let f(x) 4+x. Solutios to Fial Exam Review Problems Math 5C, Witer 2007 (a) Fid the Maclauri series for f(x), ad compute its radius of covergece. Solutio. f(x) 4( ( x/4)) ( x/4) ( ) 4 4 + x. Sice the

More information

Random Variables, Sampling and Estimation

Random Variables, Sampling and Estimation Chapter 1 Radom Variables, Samplig ad Estimatio 1.1 Itroductio This chapter will cover the most importat basic statistical theory you eed i order to uderstad the ecoometric material that will be comig

More information

Math 116 Second Exam

Math 116 Second Exam Math 6 Secod Exam November, 6 Name: Exam Solutios Istructor: Sectio:. Do ot ope this exam util you are told to do so.. This exam has 9 pages icludig this cover. There are 8 problems. Note that the problems

More information

PROBABILITY AMPLITUDE AND INTERFERENCE

PROBABILITY AMPLITUDE AND INTERFERENCE PROILITY MPLITUDE ND INTERFERENCE I. Probability amplitude Suppose that particle is placed i the ifiite square well potetial. Let the state of the particle be give by ϕ ad let the system s eergy eigestates

More information

5. Quantum Nature of the Nano-world ( Fundamental of. Quantum mechanics)

5. 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 information

Lecture 1 Probability and Statistics

Lecture 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 information

University of Washington Department of Chemistry Chemistry 453 Winter Quarter 2015

University 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 information

Application to Random Graphs

Application to Random Graphs A Applicatio to Radom Graphs Brachig processes have a umber of iterestig ad importat applicatios. We shall cosider oe of the most famous of them, the Erdős-Réyi radom graph theory. 1 Defiitio A.1. Let

More information

1 of 7 7/16/2009 6:06 AM Virtual Laboratories > 6. Radom Samples > 1 2 3 4 5 6 7 6. Order Statistics Defiitios Suppose agai that we have a basic radom experimet, ad that X is a real-valued radom variable

More information

On a Smarandache problem concerning the prime gaps

On a Smarandache problem concerning the prime gaps O a Smaradache problem cocerig the prime gaps Felice Russo Via A. Ifate 7 6705 Avezzao (Aq) Italy felice.russo@katamail.com Abstract I this paper, a problem posed i [] by Smaradache cocerig the prime gaps

More information

1 Review of Probability & Statistics

1 Review of Probability & Statistics 1 Review of Probability & Statistics a. I a group of 000 people, it has bee reported that there are: 61 smokers 670 over 5 960 people who imbibe (drik alcohol) 86 smokers who imbibe 90 imbibers over 5

More information

Ray Optics Theory and Mode Theory. Dr. Mohammad Faisal Dept. of EEE, BUET

Ray Optics Theory and Mode Theory. Dr. Mohammad Faisal Dept. of EEE, BUET Ray Optics Theory ad Mode Theory Dr. Mohammad Faisal Dept. of, BUT Optical Fiber WG For light to be trasmitted through fiber core, i.e., for total iteral reflectio i medium, > Ray Theory Trasmissio Ray

More information

Nernst Equation. Nernst Equation. Electric Work and Gibb's Free Energy. Skills to develop. Electric Work. Gibb's Free Energy

Nernst Equation. Nernst Equation. Electric Work and Gibb's Free Energy. Skills to develop. Electric Work. Gibb's Free Energy Nerst Equatio Skills to develop Eplai ad distiguish the cell potetial ad stadard cell potetial. Calculate cell potetials from kow coditios (Nerst Equatio). Calculate the equilibrium costat from cell potetials.

More information

SOLUTIONS: ECE 606 Homework Week 7 Mark Lundstrom Purdue University (revised 3/27/13) e E i E T

SOLUTIONS: 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 information

Topic 9: Sampling Distributions of Estimators

Topic 9: Sampling Distributions of Estimators Topic 9: Samplig Distributios of Estimators Course 003, 2018 Page 0 Samplig distributios of estimators Sice our estimators are statistics (particular fuctios of radom variables), their distributio ca be

More information

Topic 9: Sampling Distributions of Estimators

Topic 9: Sampling Distributions of Estimators Topic 9: Samplig Distributios of Estimators Course 003, 2016 Page 0 Samplig distributios of estimators Sice our estimators are statistics (particular fuctios of radom variables), their distributio ca be

More information

Holistic Approach to the Periodic System of Elements

Holistic Approach to the Periodic System of Elements Holistic Approach to the Periodic System of Elemets N.N.Truov * D.I.Medeleyev Istitute for Metrology Russia, St.Peterburg. 190005 Moskovsky pr. 19 (Dated: February 20, 2009) Abstract: For studyig the objectivity

More information

Math 116 Practice for Exam 3

Math 116 Practice for Exam 3 Math 6 Practice for Exam Geerated October 0, 207 Name: SOLUTIONS Istructor: Sectio Number:. This exam has 7 questios. Note that the problems are ot of equal difficulty, so you may wat to skip over ad retur

More information

w (1) ˆx w (1) x (1) /ρ and w (2) ˆx w (2) x (2) /ρ.

w (1) ˆx w (1) x (1) /ρ and w (2) ˆx w (2) x (2) /ρ. 2 5. Weighted umber of late jobs 5.1. Release dates ad due dates: maximimizig the weight of o-time jobs Oce we add release dates, miimizig the umber of late jobs becomes a sigificatly harder problem. For

More information

CHAPTER 8 SYSTEMS OF PARTICLES

CHAPTER 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 information

Hilbert Space Methods Used in a First Course in Quantum Mechanics

Hilbert Space Methods Used in a First Course in Quantum Mechanics Hilbert Space Methods Used i a First Course i Quatum Mechaics Victor Poliger Physics/Mathematics Bellevue College 03/07/3-04//3 Outlie The Ifiite Square Well: A Follow-Up Timelie of basic evets Statistical

More information

The Riemann Zeta Function

The Riemann Zeta Function Physics 6A Witer 6 The Riema Zeta Fuctio I this ote, I will sketch some of the mai properties of the Riema zeta fuctio, ζ(x). For x >, we defie ζ(x) =, x >. () x = For x, this sum diverges. However, we

More information

Introduction to Signals and Systems, Part V: Lecture Summary

Introduction to Signals and Systems, Part V: Lecture Summary EEL33: Discrete-Time Sigals ad Systems Itroductio to Sigals ad Systems, Part V: Lecture Summary Itroductio to Sigals ad Systems, Part V: Lecture Summary So far we have oly looked at examples of o-recursive

More information

Position Time Graphs 12.1

Position Time Graphs 12.1 12.1 Positio Time Graphs Figure 3 Motio with fairly costat speed Chapter 12 Distace (m) A Crae Flyig Figure 1 Distace time graph showig motio with costat speed A Crae Flyig Positio (m [E] of pod) We kow

More information

The Pendulum. Purpose

The 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 information

CS / MCS 401 Homework 3 grader solutions

CS / MCS 401 Homework 3 grader solutions CS / MCS 401 Homework 3 grader solutios assigmet due July 6, 016 writte by Jāis Lazovskis maximum poits: 33 Some questios from CLRS. Questios marked with a asterisk were ot graded. 1 Use the defiitio of

More information

(c) Write, but do not evaluate, an integral expression for the volume of the solid generated when R is

(c) Write, but do not evaluate, an integral expression for the volume of the solid generated when R is Calculus BC Fial Review Name: Revised 7 EXAM Date: Tuesday, May 9 Remiders:. Put ew batteries i your calculator. Make sure your calculator is i RADIAN mode.. Get a good ight s sleep. Eat breakfast. Brig:

More information

Chapter 6 Infinite Series

Chapter 6 Infinite Series Chapter 6 Ifiite Series I the previous chapter we cosidered itegrals which were improper i the sese that the iterval of itegratio was ubouded. I this chapter we are goig to discuss a topic which is somewhat

More information

PH 425 Quantum Measurement and Spin Winter SPINS Lab 1

PH 425 Quantum Measurement and Spin Winter SPINS Lab 1 PH 425 Quatum Measuremet ad Spi Witer 23 SPIS Lab Measure the spi projectio S z alog the z-axis This is the experimet that is ready to go whe you start the program, as show below Each atom is measured

More information

Preliminary Examination - Day 1 Thursday, May 12, 2016

Preliminary Examination - Day 1 Thursday, May 12, 2016 UNL - Departmet of Physics ad Astroomy Prelimiary Examiatio - Day Thursday, May, 6 This test covers the topics of Quatum Mechaics (Topic ) ad Electrodyamics (Topic ). Each topic has 4 A questios ad 4 B

More information

Quantum Annealing for Heisenberg Spin Chains

Quantum 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 information

Bohr s Atomic Model Quantum Mechanical Model

Bohr 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 information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION DOI: 10.1038/NPHYS309 O the reality of the quatum state Matthew F. Pusey, 1, Joatha Barrett, ad Terry Rudolph 1 1 Departmet of Physics, Imperial College Lodo, Price Cosort Road, Lodo SW7 AZ, Uited Kigdom

More information

NICK DUFRESNE. 1 1 p(x). To determine some formulas for the generating function of the Schröder numbers, r(x) = a(x) =

NICK DUFRESNE. 1 1 p(x). To determine some formulas for the generating function of the Schröder numbers, r(x) = a(x) = AN INTRODUCTION TO SCHRÖDER AND UNKNOWN NUMBERS NICK DUFRESNE Abstract. I this article we will itroduce two types of lattice paths, Schröder paths ad Ukow paths. We will examie differet properties of each,

More information

Similarity between quantum mechanics and thermodynamics: Entropy, temperature, and Carnot cycle

Similarity between quantum mechanics and thermodynamics: Entropy, temperature, and Carnot cycle Similarity betwee quatum mechaics ad thermodyamics: Etropy, temperature, ad Carot cycle Sumiyoshi Abe 1,,3 ad Shiji Okuyama 1 1 Departmet of Physical Egieerig, Mie Uiversity, Mie 514-8507, Japa Istitut

More information

Optimally Sparse SVMs

Optimally Sparse SVMs A. Proof of Lemma 3. We here prove a lower boud o the umber of support vectors to achieve geeralizatio bouds of the form which we cosider. Importatly, this result holds ot oly for liear classifiers, but

More information

HE ATOM & APPROXIMATION METHODS MORE GENERAL VARIATIONAL TREATMENT. Examples:

HE 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 information

5.61 Fall 2013 Problem Set #3

5.61 Fall 2013 Problem Set #3 5.61 Fall 013 Problem Set #3 1. A. McQuarrie, page 10, #3-3. B. McQuarrie, page 10, #3-4. C. McQuarrie, page 18, #4-11.. McQuarrie, pages 11-1, #3-11. 3. A. McQuarrie, page 13, #3-17. B. McQuarrie, page

More information

Question 1: The magnetic case

Question 1: The magnetic case September 6, 018 Corell Uiversity, Departmet of Physics PHYS 337, Advace E&M, HW # 4, due: 9/19/018, 11:15 AM Questio 1: The magetic case I class, we skipped over some details, so here you are asked to

More information

Module 1 Fundamentals in statistics

Module 1 Fundamentals in statistics Normal Distributio Repeated observatios that differ because of experimetal error ofte vary about some cetral value i a roughly symmetrical distributio i which small deviatios occur much more frequetly

More information

EXPERIMENT OF SIMPLE VIBRATION

EXPERIMENT 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 information

Quadratic Functions. Before we start looking at polynomials, we should know some common terminology.

Quadratic Functions. Before we start looking at polynomials, we should know some common terminology. Quadratic Fuctios I this sectio we begi the study of fuctios defied by polyomial expressios. Polyomial ad ratioal fuctios are the most commo fuctios used to model data, ad are used extesively i mathematical

More information

Algebra of Least Squares

Algebra of Least Squares October 19, 2018 Algebra of Least Squares Geometry of Least Squares Recall that out data is like a table [Y X] where Y collects observatios o the depedet variable Y ad X collects observatios o the k-dimesioal

More information

The Growth of Functions. Theoretical Supplement

The Growth of Functions. Theoretical Supplement The Growth of Fuctios Theoretical Supplemet The Triagle Iequality The triagle iequality is a algebraic tool that is ofte useful i maipulatig absolute values of fuctios. The triagle iequality says that

More information

3.2 Properties of Division 3.3 Zeros of Polynomials 3.4 Complex and Rational Zeros of Polynomials

3.2 Properties of Division 3.3 Zeros of Polynomials 3.4 Complex and Rational Zeros of Polynomials Math 60 www.timetodare.com 3. Properties of Divisio 3.3 Zeros of Polyomials 3.4 Complex ad Ratioal Zeros of Polyomials I these sectios we will study polyomials algebraically. Most of our work will be cocered

More information

Atomic 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.

Atomic 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 information

Feedback in Iterative Algorithms

Feedback in Iterative Algorithms Feedback i Iterative Algorithms Charles Byre (Charles Byre@uml.edu), Departmet of Mathematical Scieces, Uiversity of Massachusetts Lowell, Lowell, MA 01854 October 17, 2005 Abstract Whe the oegative system

More information