Results of Final Exam
|
|
- Darren Harris
- 6 years ago
- Views:
Transcription
1 Results of Fial Exa # of studets Grade Poits A > C C D F < poits
2 Proble 1 (partitio fuctio) The groud level of the eutral lithiu ato is doubly degeerate (that is, d ). The first excited level is 6-fold degeerate (d 1 6) ad is at a eergy 1. ev above the groud level. (a) (1) I the outer atosphere of the Su, which is at a teperature of about 6 K, what fractio of the eutral lithiu is i the excited level? Sice all the other levels of Li are at a uch higher eergy, it is safe to assue that they are ot sigificatly occupied. (b) (5) Fid the average eergy of Li ato at teperature T (agai, cosider oly the groud state ad the first excited level). (c) (15) Fid the cotributio of these levels to the specific heat per ole, C V, ad setch C V as a fuctio of T. If the groud level eergy is defied as zero ad E is the eergy of excited level: ( β ε ) + 6 ( β E) Z d The probability that the ato is i its excited level: P ( E) i 6 i i ( β E) 3( β E) 3 Z 1+ 3( β E) 3 + ( β E) E 1. ev, T 6K (~.5 ev), βe.3, (βe ) 1: P( E). 3
3 .75 1 ε The average eergy per ato: 1 Z Z ε 6 β + 6 The specific heat: ( βε ) 3ε ( βε ) ( βε ) + 3 ε E/ i ε βε x i 1 C V ε T V 3ε ε ( βε ) [ ( βε ) + 3] β T ( βε ) ( βε ) [ ( βε ) + 3] C / Vf i βε x i 1
4 P (a) Proble (blacbody radiatio) Plaet ercury revolves ad rotates at the sae rate, so oe side of the plaet is always facig the Su. ercury is a distace of 5.8 x 1 1 fro the Su, ad has a radius of.44 x 1 6. The radius of the Su is ad its total power output is 4 x 1 6 W. I this proble treat the plaet as if it were a blac body. a) (5) What is the eergy flux of the Su s radiatio at ercury's orbit? b) (5) What is the total power absorbed by ercury? [Hit: Cosider that it appears as a flat dis to the Su ad it absorbs all of the icidet radiatio.] c) (1) If ercury is i therodyaic equilibriu, it will eit the sae total power as it receives fro the Su. Assuig that the teperature of the "hot side of ercury is uifor, fid this teperature. d) (5) What is the pea frequecy of the radiatio absorbed by ercury? e) (5) What is the pea frequecy of the radiatio eitted by ercury? J P 4πR 6 Su W / orbit 4π 4 1 W 1 ( ) (b) P J πr W / π (.44 1 ) W ercury (c) ercury ercury 4 πrercuryσtercury 1/4 1/4 17 ercury W T ercury ercuryσ - hei-sphere P πr π 6 (.44 1 ) W / K K
5 Proble (blacbody radiatio), cot. (d) T 1/ 4 1/ 4 6 Su 4 1 W Su 5, Suσ P 4πR 4π 8 ( 7 1 ) W / K K ν 3 TSu J / K 5,795K h Js received 14 ax 1 Hz (e) ν 3 Tercury J / K 535K h Js eitted 13 ax 1 Hz
6 Proble 3 (oltza) (a) (15) Withi the odel of isotheral atosphere, fid the ratio of the ass of the atosphere to the ass of the plaet. Assue that the gravitatioal field is uifor. The acceleratio of the free fall, g, ad the pressure at the plaet s surface, P, are ow. Calculate this ratio for the Earth. (Hit: gg pl /R pl, where pl ad R pl are the ass of the plaet ad its radius, respectively, the gravitatioal costat G6.67*1-11 N /g ). gh T H # of olecules withi dh: dn( h h dh) ( area) dh the ass of the olecule, pl ad R pl - the ass of the plaet ad its radius, respectively, the desity of olecules at the plaet s surface. + h dh at at gh T 4π Rpl dh 4πR pl ( x) dx T g 4 4πR plt 4πG plp g g 11 5 πgp 4π N / g 1 Pa g 1 / s at pl ( ) The sae result you would get by cosiderig equilibriu coditio: F where F is the total force exerted o the atosphere by the plaet s surface F P 4π G Rpl atg pl P 4π atg g at 4 pl g P G π πr pl at g g T
7 Proble 3 (oltza) cot. (b) (1) Fid the average potetial eergy of the olecules i the atosphere. U gh gh area dh T ( ) gh area dh T ( ) gh T y ( T ) y ( y) ( y) T g T dy g dy T (c) (5) Fid the heat capacity per olecule i the atosphere (do t forget the ietic eergy). E 5 ( T ) K( T ) + U ( T ) T T + de 7 C C P dt
8 Proble 4 (Feri-ose) (1) For a syste of particles at roo teperature, how large ust ε-μ be for the Feri- Dirac, oltza, ad ose-eistei distributios agree withi 1%? () Estiate the desity of a syste of obile electros i a seicoductor that ca be treated at roo teperature equally well (with 1% accuracy) usig all three distributios. Assue that the effective electro ass is the sae as a free electro ass, ad that you ca use for this estiate the ressio for μ i a ideal classical gas. The oltza distributio lies betwee the Feri-Dirac ad ose-eistei distributios. It is sufficiet to request: ε μ ε μ T T ε μ T E FD ε μ + 1 T 1.1 ε μ 1 T ε μ > l 5.3 T This iequality ust be satisfied for all ε, icludig ε: Q Q μ > 5.3 T μoltza T l l > 5.3 < Q Q 3/ 3/ 31 3 π / 3 T g J K K h ( ) Js 3 < 6.3 1
9 Proble 5 (D Feri systes) Cosider a o-relativistic Feri gas i two diesios: N electros cofied to a square area AL. (a) (1) The desity of electroic states i two diesios per uit area: g D ε Show how to derive this forula, do t worry about a exact uerical pre-factor, focus o the depedece o eergy ad ass. (b) (5) Fid the Feri eergy (i ters of N ad A). (c) (5) Fid the average eergy per electro at T (i ters of E F ). (d) (5) Calculate E F for the electro desity N/A (a typical desity of electros i a field-effect trasistor), assue that the effective ass is.x(free electro ass). Is the electro gas i a FET degeerate at roo teperature? (a) For quatu particles cofied i a D box : N ( ) 1 4 π π π L L x y ( area) 4π 4π π ( ) G( ε ) G π x y x y x + Lx Ly 1 ε 4π h ( ε ) ( s + 1) ( ) π h - does ot deped o ε y g D π h π h E F π h N F F π h A (b) The Feri eergy: N g( ε )( area) dε A E E (c) The average F eergy per electro: U tot N ε g( ε )( area) E EF ( ) ( area) 1 area ε dε ε dε πh πh E F
10 Proble 5 (D Feri systes) (cot.) U (d) tot E F F A A 1 A 1 N ε ε g( ε )( area) dε ε dε E E F ε E F πh N πh πh E 34 ( Js) J K π h N π EF A g F At 3K, the syste is ot degeerate.
Physical bases of dental material science
Physical bases of detal aterial sciece The ioizatio eergy of the sodiu ato is 496 kj/ol. How large eergy is ecessary i ev to ioize oe ato? The ioizatio eergy of a sigle ato: E i 19 496000 19 8,7 10 ε i
More informationAIT. Blackbody Radiation IAAT
3 1 Blackbody Radiatio Itroductio 3 2 First radiatio process to look at: radiatio i thermal equilibrium with itself: blackbody radiatio Assumptios: 1. Photos are Bosos, i.e., more tha oe photo per phase
More informationPhysical Chemistry I for Biochemists. Lecture 2 (1/12/11) Yoshitaka Ishii. Gas Ch. 1 Non-Ideal Gas (Ch 1 & Raff p21-41) Announcement
Physical Cheistry I for Biocheists Che340 Lecture (1/1/11) Yoshitaka Ishii Gas Ch. 1 No-Ideal Gas (Ch 1 & Raff p1-41) Aouceet HW 1 is due et Wedesday before the class (Fid HW1 at the web site) Attedace
More informationFlight and Orbital Mechanics. Exams
1 Flight ad Orbital Mechaics Exas Exa AE2104-11: Flight ad Orbital Mechaics (2 Noveber 2012, 14.00 17.00) Please put your ae, studet uber ad ALL YOUR INITIALS o your work. Aswer all questios ad put your
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 informationECE Spring Prof. David R. Jackson ECE Dept. Notes 20
ECE 6341 Sprig 016 Prof. David R. Jackso ECE Dept. Notes 0 1 Spherical Wave Fuctios Cosider solvig ψ + k ψ = 0 i spherical coordiates z φ θ r y x Spherical Wave Fuctios (cot.) I spherical coordiates we
More informationpoints Points <40. Results of. Final Exam. Grade C D,F C B
Results of inal Exa 5 6 7 8 9 points Grade C D, Points A 9- + 85-89 7-8 C + 6-69 -59 < # of students Proble (che. equilibriu) Consider the following reaction: CO(g) + H O(g) CO (g) + H (g) In equilibriu
More informationSemiconductor Statistical Mechanics (Read Kittel Ch. 8)
EE30 - Solid State Electroics Semicoductor Statistical Mechaics (Read Kittel Ch. 8) Coductio bad occupatio desity: f( E)gE ( ) de f(e) - occupatio probability - Fermi-Dirac fuctio: g(e) - desity of states
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 informationAnswers to assigned problems from Chapter 1
Answers to assigned probles fro Chapter 1 1.7. a. A colun of ercury 1 in cross-sectional area and 0.001 in height has a volue of 0.001 and a ass of 0.001 1 595.1 kg. Then 1 Hg 0.001 1 595.1 kg 9.806 65
More informationMath 113, Calculus II Winter 2007 Final Exam Solutions
Math, Calculus II Witer 7 Fial Exam Solutios (5 poits) Use the limit defiitio of the defiite itegral ad the sum formulas to compute x x + dx The check your aswer usig the Evaluatio Theorem Solutio: I this
More informationDefine a Markov chain on {1,..., 6} with transition probability matrix P =
Pla Group Work 0. The title says it all Next Tie: MCMC ad Geeral-state Markov Chais Midter Exa: Tuesday 8 March i class Hoework 4 due Thursday Uless otherwise oted, let X be a irreducible, aperiodic Markov
More informationSolution: APPM 1360 Final Spring 2013
APPM 36 Fial Sprig 3. For this proble let the regio R be the regio eclosed by the curve y l( ) ad the lies, y, ad y. (a) (6 pts) Fid the area of the regio R. (b) (6 pts) Suppose the regio R is revolved
More informationSolutions to the problems in Chapter 6 and 7
Solutions to the probles in Chapter 6 and 7 6.3 Pressure of a Feri gas at zero teperature The nuber of electrons N and the internal energy U, inthevoluev,are N = V D(ε)f(ε)dε, U = V εd(ε)f(ε)dε, () The
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 informationECE 901 Lecture 4: Estimation of Lipschitz smooth functions
ECE 9 Lecture 4: Estiatio of Lipschitz sooth fuctios R. Nowak 5/7/29 Cosider the followig settig. Let Y f (X) + W, where X is a rado variable (r.v.) o X [, ], W is a r.v. o Y R, idepedet of X ad satisfyig
More informationRay 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 informationSummer MA Lesson 13 Section 1.6, Section 1.7 (part 1)
Suer MA 1500 Lesso 1 Sectio 1.6, Sectio 1.7 (part 1) I Solvig Polyoial Equatios Liear equatio ad quadratic equatios of 1 variable are specific types of polyoial equatios. Soe polyoial equatios of a higher
More informationMolecular Speeds. Real Gasses. Ideal Gas Law. Reasonable. Why the breakdown? P-V Diagram. Using moles. Using molecules
Kinetic Theory of Gases Connect icroscopic properties (kinetic energy and oentu) of olecules to acroscopic state properties of a gas (teperature and pressure). P v v 3 3 3 But K v and P kt K v kt Teperature
More informationIntegrals of Functions of Several Variables
Itegrals of Fuctios of Several Variables We ofte resort to itegratios i order to deterie the exact value I of soe quatity which we are uable to evaluate by perforig a fiite uber of additio or ultiplicatio
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 informationNonequilibrium Excess Carriers in Semiconductors
Lecture 8 Semicoductor Physics VI Noequilibrium Excess Carriers i Semicoductors Noequilibrium coditios. Excess electros i the coductio bad ad excess holes i the valece bad Ambiolar trasort : Excess electros
More informationPY241 Solutions Set 9 (Dated: November 7, 2002)
PY241 Solutions Set 9 (Dated: Noveber 7, 2002) 9-9 At what displaceent of an object undergoing siple haronic otion is the agnitude greatest for the... (a) velocity? The velocity is greatest at x = 0, the
More information17 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 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 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 informationDirection: This test is worth 250 points. You are required to complete this test within 50 minutes.
Term Test October 3, 003 Name Math 56 Studet Number Directio: This test is worth 50 poits. You are required to complete this test withi 50 miutes. I order to receive full credit, aswer each problem completely
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 informationLecture 14. Review for Exam 1.
Lecture 4. Review for Exa. Eectroagetic radiatio exhibits the dua ature: wave properties ad particuate properties Wave ature of radiatio: Eectroagetic waves are characterized by waveegth or frequecy ~,or
More informationThe Hypergeometric Coupon Collection Problem and its Dual
Joural of Idustrial ad Systes Egieerig Vol., o., pp -7 Sprig 7 The Hypergeoetric Coupo Collectio Proble ad its Dual Sheldo M. Ross Epstei Departet of Idustrial ad Systes Egieerig, Uiversity of Souther
More informationRAYLEIGH'S METHOD Revision D
RAYGH'S METHOD Revisio D B To Irvie Eail: toirvie@aol.co Noveber 5, Itroductio Daic sstes ca be characterized i ters of oe or ore atural frequecies. The atural frequec is the frequec at which the sste
More informationA PROBABILITY PROBLEM
A PROBABILITY PROBLEM A big superarket chai has the followig policy: For every Euros you sped per buy, you ear oe poit (suppose, e.g., that = 3; i this case, if you sped 8.45 Euros, you get two poits,
More informationfiziks Forum for CSIR-UGC JRF/NET, GATE, IIT-JAM, GRE in PHYSICAL SCIENCES
IIT-JAM-8(HYSICS) IMORTAN NOTE FOR CANDIDTES Attept A 5 questios. uestios -5(objective questios) carr si ars each ad questios 6-5(subjective questios) carr twet oe ars each.. The product of a two real,
More informationLecture 20 - Wave Propagation Response
.09/.093 Fiite Eleet Aalysis of Solids & Fluids I Fall 09 Lecture 0 - Wave Propagatio Respose Prof. K. J. Bathe MIT OpeCourseWare Quiz #: Closed book, 6 pages of otes, o calculators. Covers all aterials
More informationPhys 6303 Final Exam Solutions December 19, 2012
Phys 633 Fial Exam s December 19, 212 You may NOT use ay book or otes other tha supplied with this test. You will have 3 hours to fiish. DO YOUR OWN WORK. Express your aswers clearly ad cocisely so that
More informationJacobi symbols. p 1. Note: The Jacobi symbol does not necessarily distinguish between quadratic residues and nonresidues. That is, we could have ( a
Jacobi sybols efiitio Let be a odd positive iteger If 1, the Jacobi sybol : Z C is the costat fuctio 1 1 If > 1, it has a decopositio ( as ) a product of (ot ecessarily distict) pries p 1 p r The Jacobi
More informationHW 6 - Solutions Due November 20, 2017
Conteporary Physics I HW 6 HW 6 - Solutions Due Noveber 20, 2017 1. A 4 kg block is attached to a spring with a spring constant k 200N/, and is stretched an aount 0.2 [5 pts each]. (a) Sketch the potential
More informationLet us give one more example of MLE. Example 3. The uniform distribution U[0, θ] on the interval [0, θ] has p.d.f.
Lecture 5 Let us give oe more example of MLE. Example 3. The uiform distributio U[0, ] o the iterval [0, ] has p.d.f. { 1 f(x =, 0 x, 0, otherwise The likelihood fuctio ϕ( = f(x i = 1 I(X 1,..., X [0,
More informationPerturbation Theory, Zeeman Effect, Stark Effect
Chapter 8 Perturbatio Theory, Zeea Effect, Stark Effect Ufortuately, apart fro a few siple exaples, the Schrödiger equatio is geerally ot exactly solvable ad we therefore have to rely upo approxiative
More informationPhysics 556 Stellar Astrophysics Prof. James Buckley. Lecture 5
Physics 556 Stellar Astrophysics Prof. James Buckley Lecture 5 Thermodyamics Equatio of State of Radiatio The mometum flux ormal to a surface (mometum per uit area per uit time) is the same as the ormal
More informationProbability Theory. Exercise Sheet 4. ETH Zurich HS 2017
ETH Zurich HS 2017 D-MATH, D-PHYS Prof. A.-S. Szita Coordiator Yili Wag Probability Theory Exercise Sheet 4 Exercise 4.1 Let X ) N be a sequece of i.i.d. rado variables i a probability space Ω, A, P ).
More informationEE415/515 Fundamentals of Semiconductor Devices Fall 2012
090 EE4555 Fudaetals of Seicoductor evices Fall 0 ecture : MOSFE hapter 0.3, 0.4 090 J. E. Morris Reider: Here is what the MOSFE looks like 090 N-chael MOSFEs: Ehaceet & epletio odes 090 J. E. Morris 3
More informationCPT 17. XI-LJ (Date: ) PHYSICS CHEMISTRY MATHEMATICS 1. (B) 31. (A) 61. (A) 2. (B) 32. (B) 62. (C) 3. (D) 33. (D) 63. (B) 4. (B) 34.
CPT-7 / XI-LJ / NARAYANA I I T A C A D E M Y CPT 7 XI-LJ (Date:.0.7) CODE XI-LJ PHYSICS CHEMISTRY MATHEMATICS. (B). (A) 6. (A). (B). (B) 6. (C). (D). (D) 6. (B). (B). (C) 6. (C) 5. (D) 5. (C) 65. (A) 6.
More informationNURTURE COURSE TARGET : JEE (MAIN) Test Type : ALL INDIA OPEN TEST TEST DATE : ANSWER KEY HINT SHEET. 1. Ans.
Test Type : LL INDI OPEN TEST Paper Code : 0000CT005 00 CLSSROOM CONTCT PROGRMME (cadeic Sessio : 05-06) NURTURE COURSE TRGET : JEE (MIN) 07 TEST DTE : - 0-06 NSWER KEY HINT SHEET Corporate Office : CREER
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 information8.3 Perturbation theory
8.3 Perturbatio theory Slides: Video 8.3.1 Costructig erturbatio theory Text referece: Quatu Mechaics for Scietists ad gieers Sectio 6.3 (u to First order erturbatio theory ) Perturbatio theory Costructig
More informationEN40: Dynamics and Vibrations. Final Examination Friday May : 2pm-5pm
EN4: Dyaics ad Vibratios Fial Exaiatio Friday May 8 15: p-5p School of Egieerig Brow Uiversity NAME: Geeral Istructios No collaboratio of ay kid is peritted o this exaiatio. You ay brig double sided pages
More informationJ 10 J W W W W
PHYS 54 Practice Test 3 Solutios Sprig 8 Q: [4] A costat force is applied to a box, cotributig to a certai displaceet o the floor. If the agle betwee the force ad displaceet is 35, the wor doe b this force
More informationECONOMETRIC THEORY. MODULE XIII Lecture - 34 Asymptotic Theory and Stochastic Regressors
ECONOMETRIC THEORY MODULE XIII Lecture - 34 Asymptotic Theory ad Stochastic Regressors Dr. Shalabh Departmet of Mathematics ad Statistics Idia Istitute of Techology Kapur Asymptotic theory The asymptotic
More informationChapter 2 Motion and Recombination of Electrons and Holes
Chapter 2 Motio ad Recombiatio of Electros ad Holes 2.1 Thermal Motio 3 1 2 Average electro or hole kietic eergy kt mv th 2 2 v th 3kT m eff 23 3 1.38 10 JK 0.26 9.1 10 1 31 300 kg K 5 7 2.310 m/s 2.310
More informationIntroduction to Astrophysics Tutorial 2: Polytropic Models
Itroductio to Astrophysics Tutorial : Polytropic Models Iair Arcavi 1 Summary of the Equatios of Stellar Structure We have arrived at a set of dieretial equatios which ca be used to describe the structure
More informationRatio of Two Random Variables: A Note on the Existence of its Moments
Metodološki zvezki, Vol. 3, o., 6, -7 Ratio of wo Rado Variables: A ote o the Existece of its Moets Ato Cedilik, Kataria Košel, ad Adre Bleec 3 Abstract o eable correct statistical iferece, the kowledge
More informationMetric Space Properties
Metric Space Properties Math 40 Fial Project Preseted by: Michael Brow, Alex Cordova, ad Alyssa Sachez We have already poited out ad will recogize throughout this book the importace of compact sets. All
More informationChemistry Department Al-kharj, October Prince Sattam Bin Abdulaziz University First semester (1437/1438)
Exercise 1 Exercises- chapter-1- Properties of gases (Part-2- Real gases Express the van der Waals paraeters a = 1.32 at d 6 ol 2 and b = 0.0436 d 3 ol 1 in SI base units? * The SI unit of pressure is
More informationX. Perturbation Theory
X. Perturbatio Theory I perturbatio theory, oe deals with a ailtoia that is coposed Ĥ that is typically exactly solvable of two pieces: a referece part ad a perturbatio ( Ĥ ) that is assued to be sall.
More informationSupplementary Information
Suppleetary Iforatio -Breakdow of cotiuu fracture echaics at the aoscale- Takahiro Shiada,,* Keji Ouchi, Yuu Chihara, ad Takayuki Kitaura Departet of echaical Egieerig ad Sciece, Kyoto Uiversity, Nishikyo-ku,
More information1.3 Convergence Theorems of Fourier Series. k k k k. N N k 1. With this in mind, we state (without proof) the convergence of Fourier series.
.3 Covergece Theorems of Fourier Series I this sectio, we preset the covergece of Fourier series. A ifiite sum is, by defiitio, a limit of partial sums, that is, a cos( kx) b si( kx) lim a cos( kx) b si(
More informationMATH Exam 1 Solutions February 24, 2016
MATH 7.57 Exam Solutios February, 6. Evaluate (A) l(6) (B) l(7) (C) l(8) (D) l(9) (E) l() 6x x 3 + dx. Solutio: D We perform a substitutio. Let u = x 3 +, so du = 3x dx. Therefore, 6x u() x 3 + dx = [
More information7.1 Convergence of sequences of random variables
Chapter 7 Limit Theorems Throughout this sectio we will assume a probability space (, F, P), i which is defied a ifiite sequece of radom variables (X ) ad a radom variable X. The fact that for every ifiite
More informationChapter 2 Motion and Recombination of Electrons and Holes
Chapter 2 Motio ad Recombiatio of Electros ad Holes 2.1 Thermal Eergy ad Thermal Velocity Average electro or hole kietic eergy 3 2 kt 1 2 2 mv th v th 3kT m eff 3 23 1.38 10 JK 0.26 9.1 10 1 31 300 kg
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 informationAnswer Key, Problem Set 1, Written
Cheistry 1 Mies, Sprig, 018 Aswer Key, Proble Set 1, Writte 1. 14.3;. 14.34 (add part (e): Estiate / calculate the iitial rate of the reactio); 3. NT1; 4. NT; 5. 14.37; 6. 14.39; 7. 14.41; 8. NT3; 9. 14.46;
More informationStatistics and Data Analysis in MATLAB Kendrick Kay, February 28, Lecture 4: Model fitting
Statistics ad Data Aalysis i MATLAB Kedrick Kay, kedrick.kay@wustl.edu February 28, 2014 Lecture 4: Model fittig 1. The basics - Suppose that we have a set of data ad suppose that we have selected the
More informationLecture 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 informationABOUT CHAOS AND SENSITIVITY IN TOPOLOGICAL DYNAMICS
ABOUT CHAOS AND SENSITIVITY IN TOPOLOGICAL DYNAMICS EDUARD KONTOROVICH Abstract. I this work we uify ad geeralize some results about chaos ad sesitivity. Date: March 1, 005. 1 1. Symbolic Dyamics Defiitio
More informationPRELIMINARY EXAMINATION Department of Physics University of Florida Part A, January, 2016, 09:00 12:00. Instructions
Studet ID Number: PRELIMINRY EXMINTION Part, Jauary, 6, 9: : Istructios. You may use a calculator ad CRC Math tables or equivalet. No other tables or aids are allowed or required. You may NOT use programmable
More information19.1 The dictionary problem
CS125 Lecture 19 Fall 2016 19.1 The dictioary proble Cosider the followig data structural proble, usually called the dictioary proble. We have a set of ites. Each ite is a (key, value pair. Keys are i
More informationDETERMINATION OF NATURAL FREQUENCY AND DAMPING RATIO
Hasa G Pasha DETERMINATION OF NATURAL FREQUENCY AND DAMPING RATIO OBJECTIVE Deterie the atural frequecy ad dapig ratio for a aluiu catilever bea, Calculate the aalytical value of the atural frequecy ad
More informationLecture 5-2: Polytropes. Literature: MWW chapter 19
Lecture 5-2: Polytropes Literature: MWW chapter 9!" Preamble The 4 equatios of stellar structure divide ito two groups: Mass ad mometum describig the mechaical structure ad thermal equilibrium ad eergy
More informationStatistics for Applications Fall Problem Set 7
18.650. Statistics for Applicatios Fall 016. Proble Set 7 Due Friday, Oct. 8 at 1 oo Proble 1 QQ-plots Recall that the Laplace distributio with paraeter λ > 0 is the cotiuous probaλ bility easure with
More information1 (40) Gravitational Systems Two heavy spherical (radius 0.05R) objects are located at fixed positions along
(40) Gravitational Systes Two heavy spherical (radius 0.05) objects are located at fixed positions along 2M 2M 0 an axis in space. The first ass is centered at r = 0 and has a ass of 2M. The second ass
More informationMath 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 informationPhysics 219 Summary of linear response theory
1 Physics 219 Suary of liear respose theory I. INTRODUCTION We apply a sall perturbatio of stregth f(t) which is switched o gradually ( adiabatically ) fro t =, i.e. the aplitude of the perturbatio grows
More informationROSE WONG. f(1) f(n) where L the average value of f(n). In this paper, we will examine averages of several different arithmetic functions.
AVERAGE VALUES OF ARITHMETIC FUNCTIONS ROSE WONG Abstract. I this paper, we will preset problems ivolvig average values of arithmetic fuctios. The arithmetic fuctios we discuss are: (1)the umber of represetatios
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 informationThis exam contains 19 pages (including this cover page) and 10 questions. A Formulae sheet is provided with the exam.
Probability ad Statistics FS 07 Secod Sessio Exam 09.0.08 Time Limit: 80 Miutes Name: Studet ID: This exam cotais 9 pages (icludig this cover page) ad 0 questios. A Formulae sheet is provided with the
More informationPhys102 First Major-131 Zero Version Coordinator: xyz Saturday, October 26, 2013 Page: 1
Phys10 First Major-131 Zero Version Coordinator: xyz Saturday, October 6, 013 Page: 1 Q1. Under a tension τ, it takes s for a pulse to travel the length of a stretched wire. What tension is required for
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 informationAcoustic Field inside a Rigid Cylinder with a Point Source
Acoustic Field iside a Rigid Cylider with a Poit Source 1 Itroductio The ai objectives of this Deo Model are to Deostrate the ability of Coustyx to odel a rigid cylider with a poit source usig Coustyx
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 informationx a x a Lecture 2 Series (See Chapter 1 in Boas)
Lecture Series (See Chapter i Boas) A basic ad very powerful (if pedestria, recall we are lazy AD smart) way to solve ay differetial (or itegral) equatio is via a series expasio of the correspodig solutio
More information(5x 7) is. 63(5x 7) 42(5x 7) 50(5x 7) BUSINESS MATHEMATICS (Three hours and a quarter)
BUSINESS MATHEMATICS (Three hours ad a quarter) (The first 5 miutes of the examiatio are for readig the paper oly. Cadidate must NOT start writig durig this time). ------------------------------------------------------------------------------------------------------------------------
More informationPHY4905: Nearly-Free Electron Model (NFE)
PHY4905: Nearly-Free Electro Model (NFE) D. L. Maslov Departmet of Physics, Uiversity of Florida (Dated: Jauary 12, 2011) 1 I. REMINDER: QUANTUM MECHANICAL PERTURBATION THEORY A. No-degeerate eigestates
More informationSECTION 2 Electrostatics
SECTION Electrostatics This sectio, based o Chapter of Griffiths, covers effects of electric fields ad forces i static (timeidepedet) situatios. The topics are: Electric field Gauss s Law Electric potetial
More informationy X F n (y), To see this, let y Y and apply property (ii) to find a sequence {y n } X such that y n y and lim sup F n (y n ) F (y).
Modica Mortola Fuctioal 2 Γ-Covergece Let X, d) be a metric space ad cosider a sequece {F } of fuctioals F : X [, ]. We say that {F } Γ-coverges to a fuctioal F : X [, ] if the followig properties hold:
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 informationThe Binomial Multi-Section Transformer
4/15/2010 The Bioial Multisectio Matchig Trasforer preset.doc 1/24 The Bioial Multi-Sectio Trasforer Recall that a ulti-sectio atchig etwork ca be described usig the theory of sall reflectios as: where:
More informationProblem T1. Main sequence stars (11 points)
Proble T1. Main sequence stars 11 points Part. Lifetie of Sun points i..7 pts Since the Sun behaves as a perfectly black body it s total radiation power can be expressed fro the Stefan- Boltzann law as
More informationTHERMODYNAMICS (SPA5219) Detailed Solutions to Coursework 1 ISSUE: September 26 th 2017 HAND-IN: October 3 rd 2017
HERMODYNAMICS (SPA519) Detailed s to Coursework 1 ISSUE: Septeber 6 th 017 HAND-IN: October rd 017 QUESION 1: (5 arks) he siple kinetic theory arguent sketched in the lectures and in Feynan's lecture notes
More informationMTH 142 Exam 3 Spr 2011 Practice Problem Solutions 1
MTH 42 Exam 3 Spr 20 Practice Problem Solutios No calculators will be permitted at the exam. 3. A pig-pog ball is lauched straight up, rises to a height of 5 feet, the falls back to the lauch poit ad bouces
More informationBertrand s postulate Chapter 2
Bertrad s postulate Chapter We have see that the sequece of prie ubers, 3, 5, 7,... is ifiite. To see that the size of its gaps is ot bouded, let N := 3 5 p deote the product of all prie ubers that are
More informationCalculus 2 Test File Fall 2013
Calculus Test File Fall 013 Test #1 1.) Without usig your calculator, fid the eact area betwee the curves f() = 4 - ad g() = si(), -1 < < 1..) Cosider the followig solid. Triagle ABC is perpedicular to
More informationBirth-Death Processes. Outline. EEC 686/785 Modeling & Performance Evaluation of Computer Systems. Relationship Among Stochastic Processes.
EEC 686/785 Modelig & Perforace Evaluatio of Couter Systes Lecture Webig Zhao Deartet of Electrical ad Couter Egieerig Clevelad State Uiversity webig@ieee.org based o Dr. Raj jai s lecture otes Relatioshi
More informationSequences and Series of Functions
Chapter 6 Sequeces ad Series of Fuctios 6.1. Covergece of a Sequece of Fuctios Poitwise Covergece. Defiitio 6.1. Let, for each N, fuctio f : A R be defied. If, for each x A, the sequece (f (x)) coverges
More informationAVERAGE MARKS SCALING
TERTIARY INSTITUTIONS SERVICE CENTRE Level 1, 100 Royal Street East Perth, Wester Australia 6004 Telephoe (08) 9318 8000 Facsiile (08) 95 7050 http://wwwtisceduau/ 1 Itroductio AVERAGE MARKS SCALING I
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 informationBernoulli Polynomials Talks given at LSBU, October and November 2015 Tony Forbes
Beroulli Polyoials Tals give at LSBU, October ad Noveber 5 Toy Forbes Beroulli Polyoials The Beroulli polyoials B (x) are defied by B (x), Thus B (x) B (x) ad B (x) x, B (x) x x + 6, B (x) dx,. () B 3
More informationExtreme Value Theory in Civil Engineering
Extreme Value Theory i Civil Egieerig Baidurya Bhattacharya Dept of Civil Egieerig IIT Kharagpur December 2016 Homepage: www.facweb.iitkgp.eret.i/~baidurya/ Prelimiaries: Retur period IID radom variables
More informationQuiz. Use either the RATIO or ROOT TEST to determine whether the series is convergent or not.
Quiz. Use either the RATIO or ROOT TEST to determie whether the series is coverget or ot. e .6 POWER SERIES Defiitio. A power series i about is a series of the form c 0 c a c a... c a... a 0 c a where
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 information