Homework (Kittel 7.1) Density of orbitals in one and two dimensions.

Size: px
Start display at page:

Download "Homework (Kittel 7.1) Density of orbitals in one and two dimensions."

Transcription

1 Hoework 8.. Kittel 7. esity of orbitals i oe a two iesios. a Sow tat te esity of orbitals of a free eletro i oe iesio is were is te legt of te lie. b. Sow tat i two iesios, for a square of area, iepeet of. a p ±. Hee p { { a so { b p pp Hee {

2 . Kittel 7. Eergy of a relativisti feri gas. or eletros wit a eergy >>, were is te rest ass of te eletro, te eergy is give by p, were p is te oetu. or eletros i a ube of volue te oetu is of te for ultiplie by z y x + +, exatly as for te orelativisti liit. a Sow tat i tis extree relativisti liit te eri eergy of a gas of eletros is give by were /. b Sow tat te total eergy of te grou state of te gas is e geeral proble is treate by. Jutter, Zeitsrift fur Pysik 7, 98. a p. Hee p p 8 b a. Hee Eq Eq

3 Eq a Eq give. Kittel 7. Pressure a etropy of egeerate eri gas. a Sow tat a feri eletro gas i te grou state exerts a pressure p I a uifor erease of te volue of a ube every orbital as its eergy raise: e eergy of a orbital is proportioal to or. b i a expressio for te etropy of a feri eletro gas i te regio τ <<. otie tat σ as τ. a K. Hee p b B k C C S

4 S C k B S k B. Kittel 7. Ceial potetial versus teperature. Explai grapially wy te iitial urvature of µ versus τ is upwar for a ferio gas i oe iesio a owwar i tree iesios igure 7.7. Hit: e a urves are ifferet, were is give i Proble. It will be fou useful to set up te itegral for, te uber of partiles, a to osier fro te graps te beavior of te itegra betwee zero teperature a a fiite teperature. e β µ + µ t K,. or K, below µ will be exite to > µ. µ will sift to esure te uber of partiles reove fro < µ equals te uber of partiles at > µ. If ostat, te sift of µ will be approxiately zero. If ireases as ireases, te uber of partiles is weigte ore for > µ ta < µ. erefore µ ereases. Siilarly, if ereases as ireases, te µ will sift upwar. or -i,, µ > µ. or -i,, µ < µ.. Kittel 7. iqui He as a feri gas. e ato He as spi I a is a ferio. a Calulate as i able 7. te feri spere paraeters v, a for He at absolute zero, viewe as a gas of oiteratig ferios. e esity of te liqui is.8g. b Calulate te eat apaity at low teperatures << a opare wit te experietal value C,89k B as observe for <.K by. C. erso, W.

5 Reese, a J. C. Weatley, Pys. Rev., 9 96; see also igure 7.8. Exellet surveys of te properties of liqui He are give by J. Wilks, Properties of liqui a soli eliu, Oxfor, 967, a by J. C. Weatley, "ilute solutios of He a He at low teperatures," eria Joural of Pysis, 6, e priiples of refrigerators base o He - He are reviewe i Capter o ryogeis; su refrigerators proue steay teperatures ow to.k i otiuously atig operatio. a b.67 7 g. g ρ.8..6 k k erg. k B K v k s. C k B k B.9 k B.k B 6. Kittel 7.6 ass-raius relatiosip for wite warfs. Cosier a wite warf of ass a raius R. et te eletros be egeerate but orelativisti. a Sow tat te orer of agitue of te gravitatioal self-eergy is G R, were G is te gravitatioal ostat. If te ass esity is ostat witi te spere of raius R, te exat potetial eergy is G R. b Sow tat te orer of agitue of te kieti eergy of te eletros i te grou state is

6 8 R H R were is te ass of a eletro a H is te ass of a proto. Sow tat if te gravitatioal a kieti eergies are of te sae orer o agitue as require by te virial teore of eais, R g. If te ass is equal to tat of te Su g, wat is te esity of te wite warf? e It is believe tat pulsars are stars opose of a ol egeerate gas of eutros. Sow tat for a eutro star R 7 g. Wat is te value of te raius for a eutro star wit a ass equal to tat of te Su? Express te result i k. gr r. Hee r < R : gr G R r r > R : gr G r a so r < R : G r R r G R r > R : r G r g ρ r R r G r G r R R R R G R R G R G R R b e e e e H H a R. Hee

7 e H HR R H. R H et g e. e G R. R H R. G H.8 G H g g. Hee R esity: R g, ie R k.. Hee ρ R g e or eutro stars, replae te eletro ass wit te proto ass H. a so G R R G H R H R H R G H H H G H Hee R for a eutro star is H tat for a wite warf. R R g. So R G H H H G H H 7 g k.

Results of Final Exam

Results of Final Exam Results of Fial Exa # of studets 1 3 4 5 6 7 8 9 Grade Poits A >15 + 1-14 75-94 C + 7-74 C 45-69 D 35-44 F

More information

Integrals of Functions of Several Variables

Integrals 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 information

Chapter 3. Problem Solutions

Chapter 3. Problem Solutions Capter. Proble Solutions. A poton and a partile ave te sae wavelengt. Can anyting be said about ow teir linear oenta opare? About ow te poton's energy opares wit te partile's total energy? About ow te

More information

10/ Statistical Machine Learning Homework #1 Solutions

10/ Statistical Machine Learning Homework #1 Solutions Caregie Mello Uiversity Departet of Statistics & Data Sciece 0/36-70 Statistical Macie Learig Hoework # Solutios Proble [40 pts.] DUE: February, 08 Let X,..., X P were X i [0, ] ad P as desity p. Let p

More information

Homework 6: Forced Vibrations Due Friday April 6, 2018

Homework 6: Forced Vibrations Due Friday April 6, 2018 EN40: Dyais ad Vibratios Hoework 6: Fored Vibratios Due Friday April 6, 018 Shool of Egieerig Brow Uiversity 1. The vibratio isolatio syste show i the figure has 0kg, k 19.8 kn / 1.59 kns / If the base

More information

Absorption and Emission of Radiation: Time Dependent Perturbation Theory Treatment

Absorption and Emission of Radiation: Time Dependent Perturbation Theory Treatment Absorptio ad Eissio of Radiatio: Tie Depedet Perturbatio Theory Treatet Wat Hailtoia for Charged Partile i E & M Field Need the potetial U. Fore o Charged Partile: 1 F e E V B Fore (geeralized for i Lagragia

More information

Statistics for Applications Fall Problem Set 7

Statistics 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 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

The Hypergeometric Coupon Collection Problem and its Dual

The 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 information

An Insight into Differentiation and Integration

An Insight into Differentiation and Integration Differetiatio A Isigt ito Differetiatio a Itegratio Differetiatio is basically a task to fi out ow oe variable is cagig i relatio to aoter variable, te latter is usually take as a cause of te cage. For

More information

5.1 The derivative or the gradient of a curve. Definition and finding the gradient from first principles

5.1 The derivative or the gradient of a curve. Definition and finding the gradient from first principles Capter 5: Dierentiation In tis capter, we will study: 51 e derivative or te gradient o a curve Deinition and inding te gradient ro irst principles 5 Forulas or derivatives 5 e equation o te tangent line

More information

MATH CALCULUS I 2.1: Derivatives and Rates of Change

MATH CALCULUS I 2.1: Derivatives and Rates of Change MATH 12002 - CALCULUS I 2.1: Derivatives and Rates of Cange Professor Donald L. Wite Department of Matematical Sciences Kent State University D.L. Wite (Kent State University) 1 / 1 Introduction Our main

More information

X. Perturbation Theory

X. 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 information

DEGENERACY AND ALL THAT

DEGENERACY AND ALL THAT DEGENERACY AND ALL THAT Te Nature of Termodyamics, Statistical Mecaics ad Classical Mecaics Termodyamics Te study of te equilibrium bulk properties of matter witi te cotext of four laws or facts of experiece

More information

Physical Chemistry I for Biochemists. Lecture 2 (1/12/11) Yoshitaka Ishii. Gas Ch. 1 Non-Ideal Gas (Ch 1 & Raff p21-41) Announcement

Physical 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 information

GAUTENG DEPARTMENT OF EDUCATION SENIOR SECONDARY INTERVENTION PROGRAMME. PHYSICAL SCIENCE Grade 11 SESSION 11 (LEARNER NOTES)

GAUTENG DEPARTMENT OF EDUCATION SENIOR SECONDARY INTERVENTION PROGRAMME. PHYSICAL SCIENCE Grade 11 SESSION 11 (LEARNER NOTES) PYSICAL SCIENCE Grade 11 SESSION 11 (LEARNER NOTES) MOLE CONCEPT, STOICIOMETRIC CALCULATIONS Learner Note: The ole concept is carried forward to calculations in the acid and base section, as well as in

More information

c hc h c h. Chapter Since E n L 2 in Eq. 39-4, we see that if L is doubled, then E 1 becomes (2.6 ev)(2) 2 = 0.65 ev.

c hc h c h. Chapter Since E n L 2 in Eq. 39-4, we see that if L is doubled, then E 1 becomes (2.6 ev)(2) 2 = 0.65 ev. Capter 39 Since n L in q 39-4, we see tat if L is doubled, ten becoes (6 ev)() = 065 ev We first note tat since = 666 0 34 J s and c = 998 0 8 /s, 34 8 c6 66 0 J sc 998 0 / s c 40eV n 9 9 60 0 J / ev 0

More information

Conditions Within The Nucleus Nadi, Nagi,mdi, m gi And Nuclear Energy Density And The Electric Field Parameters

Conditions Within The Nucleus Nadi, Nagi,mdi, m gi And Nuclear Energy Density And The Electric Field Parameters Aerica Joural of Eeerig esearch (AJE 3 w w w. a j e r. o r g Page 79 Aerica Joural of Eeerig esearch (AJE e-ss : 3-847 p-ss : 3-936 Volue-, ssue-, pp-4-43 www.ajer.org esearch Paper Ope Access Coitios

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

Computational Methods CMSC/AMSC/MAPL 460. Quadrature: Integration

Computational Methods CMSC/AMSC/MAPL 460. Quadrature: Integration Computatioal Metods CMSC/AMSC/MAPL 6 Quadrature: Itegratio Ramai Duraiswami, Dept. o Computer Siee Some material adapted rom te olie slides o Eri Sadt ad Diae O Leary Numerial Itegratio Idea is to do itegral

More information

2. SCHWARZSCHILD GEOMETRY REVISITED The metric for Schwarzschild Geometry is given by, ) (1) For constant values of time we have, c r

2. SCHWARZSCHILD GEOMETRY REVISITED The metric for Schwarzschild Geometry is given by, ) (1) For constant values of time we have, c r urved Spae-Tie ad the Speed of Light aitra Palit uthor/teaher, P-54 Motijheel veue, Motijheel Housig ooperative soiety, Flat- 4, Kolkata-700074, Idia, Eail: palit.aaitra@gail.o Keywords: Shwarzshild Geoetry,

More information

Given: Hot fluid oil, Cold fluid - water (T 1, T 2 ) (t 1, t 2 ) Water

Given: Hot fluid oil, Cold fluid - water (T 1, T 2 ) (t 1, t 2 ) Water . In a counter flow double pipe eat excanger, oil is cooled fro 85 to 55 by water entering at 5. Te ass flow rate of oil is 9,800 kg/ and specific eat f oil is 000 J/kg K. Te ass flow rate of water is

More information

Bob Brown Math 251 Calculus 1 Chapter 3, Section 1 Completed 1 CCBC Dundalk

Bob Brown Math 251 Calculus 1 Chapter 3, Section 1 Completed 1 CCBC Dundalk Bob Brown Mat 251 Calculus 1 Capter 3, Section 1 Completed 1 Te Tangent Line Problem Te idea of a tangent line first arises in geometry in te context of a circle. But before we jump into a discussion of

More information

CPT 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 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 information

THE ESSENCE OF QUANTUM MECHANICS

THE ESSENCE OF QUANTUM MECHANICS THE ESSENCE OF QUANTUM MECHANICS Capter belongs to te "Teory of Spae" written by Dariusz Stanisław Sobolewski. Http: www.tsengines.o ttp: www.teoryofspae.info E-ail: info@tsengines.o All rigts resered.

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

1. State whether the function is an exponential growth or exponential decay, and describe its end behaviour using limits.

1. State whether the function is an exponential growth or exponential decay, and describe its end behaviour using limits. Questions 1. State weter te function is an exponential growt or exponential decay, and describe its end beaviour using its. (a) f(x) = 3 2x (b) f(x) = 0.5 x (c) f(x) = e (d) f(x) = ( ) x 1 4 2. Matc te

More information

SOLUTION TO CHAPTER 4 EXERCISES: SLURRY TRANSPORT

SOLUTION TO CHAPTER 4 EXERCISES: SLURRY TRANSPORT SOLUTION TO CHAPTER 4 EXERCISES: SLURRY TRANSPORT EXERCISE 4.1 Sales o a osate slurry ixture are aalyzed i a lab. Te ollowig data describe te relatiosi betwee te sear stress ad te sear rate: 1 Sear Rate,γ&

More information

Chapter 2 Solutions. Prob. 2.1 (a&b) Sketch a vacuum tube device. Graph photocurrent I versus retarding voltage V for several light intensities.

Chapter 2 Solutions. Prob. 2.1 (a&b) Sketch a vacuum tube device. Graph photocurrent I versus retarding voltage V for several light intensities. Chapter Solutios Prob..1 (a&b) Sketh a vauum tube devie. Graph photourret I versus retardig voltage V for several light itesities. I light itesity V o V Note that V o remais same for all itesities. ()

More information

The Advection-Diffusion equation!

The Advection-Diffusion equation! ttp://www.d.edu/~gtryggva/cf-course/! Te Advectio-iffusio equatio! Grétar Tryggvaso! Sprig 3! Navier-Stokes equatios! Summary! u t + u u x + v u y = P ρ x + µ u + u ρ y Hyperbolic part! u x + v y = Elliptic

More information

NURTURE COURSE TARGET : JEE (MAIN) Test Type : ALL INDIA OPEN TEST TEST DATE : ANSWER KEY HINT SHEET. 1. Ans.

NURTURE 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 information

SOLUTIONS for Homework #3

SOLUTIONS for Homework #3 SOLUTIONS for Hoework #3 1. In the potential of given for there is no unboun states. Boun states have positive energies E n labele by an integer n. For each energy level E, two syetrically locate classical

More information

Optimal Estimator for a Sample Set with Response Error. Ed Stanek

Optimal Estimator for a Sample Set with Response Error. Ed Stanek Optial Estiator for a Saple Set wit Respose Error Ed Staek Itroductio We develop a optial estiator siilar to te FP estiator wit respose error tat was cosidered i c08ed63doc Te first 6 pages of tis docuet

More information

Answers to assigned problems from Chapter 1

Answers 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 information

Orthogonal Function Solution of Differential Equations

Orthogonal Function Solution of Differential Equations Royal Holloway Uiversity of Loo Departet of Physics Orthogoal Fuctio Solutio of Differetial Equatios trouctio A give oriary ifferetial equatio will have solutios i ters of its ow fuctios Thus, for eaple,

More information

1 Proving the Fundamental Theorem of Statistical Learning

1 Proving the Fundamental Theorem of Statistical Learning THEORETICAL MACHINE LEARNING COS 5 LECTURE #7 APRIL 5, 6 LECTURER: ELAD HAZAN NAME: FERMI MA ANDDANIEL SUO oving te Fundaental Teore of Statistical Learning In tis section, we prove te following: Teore.

More information

Example A1: Preparation of a Calibration Standard

Example A1: Preparation of a Calibration Standard Suary Goal A calibration standard is prepared fro a high purity etal (cadiu) with a concentration of ca.1000 g l -1. Measureent procedure The surface of the high purity etal is cleaned to reove any etal-oxide

More information

Perturbation Theory, Zeeman Effect, Stark Effect

Perturbation 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 information

(b) The heat transfer can be determined from an energy balance on the system

(b) The heat transfer can be determined from an energy balance on the system 8-5 Heat is transferred to a iston-cylinder device wit a set of stos. e work done, te eat transfer, te exergy destroyed, and te second-law efficiency are to be deterined. Assutions e device is stationary

More information

ECE 6560 Chapter 2: The Resampling Process

ECE 6560 Chapter 2: The Resampling Process Capter 2: e Resaplig Process Dr. Bradley J. Bazui Wester iciga Uiversity College of Egieerig ad Applied Scieces Departet of Electrical ad Coputer Egieerig 1903 W. iciga Ave. Kalaazoo I, 49008-5329 Capter

More information

Differentiation Techniques 1: Power, Constant Multiple, Sum and Difference Rules

Differentiation Techniques 1: Power, Constant Multiple, Sum and Difference Rules Differetiatio Teciques : Power, Costat Multiple, Sum ad Differece Rules 97 Differetiatio Teciques : Power, Costat Multiple, Sum ad Differece Rules Model : Fidig te Equatio of f '() from a Grap of f ()

More information

Solve exponential equations in one variable using a variety of strategies. LEARN ABOUT the Math. What is the half-life of radon?

Solve exponential equations in one variable using a variety of strategies. LEARN ABOUT the Math. What is the half-life of radon? 8.5 Solving Exponential Equations GOAL Solve exponential equations in one variable using a variety of strategies. LEARN ABOUT te Mat All radioactive substances decrease in mass over time. Jamie works in

More information

5.1 We will begin this section with the definition of a rational expression. We

5.1 We will begin this section with the definition of a rational expression. We Basic Properties and Reducing to Lowest Terms 5.1 We will begin tis section wit te definition of a rational epression. We will ten state te two basic properties associated wit rational epressions and go

More information

EXAM 3 REVIEW: hardest problems

EXAM 3 REVIEW: hardest problems PHYS 17: oern echanics Spring 011 xa 3 results: ultiple choice: 4.5/70 = 60.7% Hanwritten: XXX FINAL XA: 1. Coprehensie. About 0-5 ultiple choice questions only. If you hae Final xa conflict: 1. Notify

More information

. Compute the following limits.

. Compute the following limits. Today: Tangent Lines and te Derivative at a Point Warmup:. Let f(x) =x. Compute te following limits. f( + ) f() (a) lim f( +) f( ) (b) lim. Let g(x) = x. Compute te following limits. g(3 + ) g(3) (a) lim

More information

Derivative at a point

Derivative at a point Roberto s Notes on Differential Calculus Capter : Definition of derivative Section Derivative at a point Wat you need to know already: Te concept of liit and basic etods for coputing liits. Wat you can

More information

MAT 1339-S14 Class 2

MAT 1339-S14 Class 2 MAT 1339-S14 Class 2 July 07, 2014 Contents 1 Rate of Cange 1 1.5 Introduction to Derivatives....................... 1 2 Derivatives 5 2.1 Derivative of Polynomial function.................... 5 2.2 Te

More information

d dx where k is a spring constant

d dx where k is a spring constant Vorlesug IX Harmoic Oscillator 1 Basic efiitios a properties a classical mechaics Oscillator is efie as a particle subject to a liear force fiel The force F ca be epresse i terms of potetial fuctio V F

More information

Function Composition and Chain Rules

Function Composition and Chain Rules Function Composition an Cain Rules James K. Peterson Department of Biological Sciences an Department of Matematical Sciences Clemson University November 2, 2018 Outline Function Composition an Continuity

More information

distinct distinct n k n k n! n n k k n 1 if k n, identical identical p j (k) p 0 if k > n n (k)

distinct distinct n k n k n! n n k k n 1 if k n, identical identical p j (k) p 0 if k > n n (k) THE TWELVEFOLD WAY FOLLOWING GIAN-CARLO ROTA How ay ways ca we distribute objects to recipiets? Equivaletly, we wat to euerate equivalece classes of fuctios f : X Y where X = ad Y = The fuctios are subject

More information

Chapter 5 Problem Solutions

Chapter 5 Problem Solutions Capter 5 Proble Solutios Wic of te wave fuctios i Fig 55 caot ave psical sigificace i te iterval sow? W ot? Figure b is double valued ad is ot a fuctio at all ad caot ave psical sigificace Figure c as

More information

of conduction electrons

of conduction electrons Dr. Fritz Wilhel, Physics 3 E:\Excel files\3 lecture\ch7 current.ocx Last save: /3/8 :53:; Last printe:/3/8 :53: of 9 Hoework: See website. Table of Contents: Ch. 7 Electric Current an esistance, 7. Electric

More information

Some Nonlinear Equations with Double Solutions: Soliton and Chaos

Some Nonlinear Equations with Double Solutions: Soliton and Chaos Some Noliear Equatios with Double Solutios: Solito a Chaos Yi-Fag Chag Departmet of Physics, Yua Uiversity, Kumig, 659, Chia (E-mail: yifagchag@hotmail.com) Abstract The fuametal characteristics of solito

More information

232 Calculus and Structures

232 Calculus and Structures 3 Calculus and Structures CHAPTER 17 JUSTIFICATION OF THE AREA AND SLOPE METHODS FOR EVALUATING BEAMS Calculus and Structures 33 Copyrigt Capter 17 JUSTIFICATION OF THE AREA AND SLOPE METHODS 17.1 THE

More information

158 Calculus and Structures

158 Calculus and Structures 58 Calculus and Structures CHAPTER PROPERTIES OF DERIVATIVES AND DIFFERENTIATION BY THE EASY WAY. Calculus and Structures 59 Copyrigt Capter PROPERTIES OF DERIVATIVES. INTRODUCTION In te last capter you

More information

MTH-112 Quiz 1 Name: # :

MTH-112 Quiz 1 Name: # : MTH- Quiz Name: # : Please write our name in te provided space. Simplif our answers. Sow our work.. Determine weter te given relation is a function. Give te domain and range of te relation.. Does te equation

More information

Chemistry Department Al-kharj, October Prince Sattam Bin Abdulaziz University First semester (1437/1438)

Chemistry 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 information

Summer MA Lesson 13 Section 1.6, Section 1.7 (part 1)

Summer 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 information

Research on Fuzzy Clustering Image Segmentation Algorithm based on GA and Gray Histogram Baoyi Wang1, a, Long Kang1, b, Shaomin Zhang1, c

Research on Fuzzy Clustering Image Segmentation Algorithm based on GA and Gray Histogram Baoyi Wang1, a, Long Kang1, b, Shaomin Zhang1, c 3rd Iteratioal Coferee o Mahiery, Materials ad Iforatio Tehology Appliatios (ICMMITA 05 Researh o Fuzzy Clusterig Iage Segetatio Algorith based o GA ad Gray Histogra Baoyi Wag, a, Log Kag, b, Shaoi Zhag,

More information

I. Existence of photon

I. Existence of photon I. Existee of photo MUX DEMUX 1 ight is a eletromageti wave of a high frequey. Maxwell s equatio H t E 0 E H 0 t E 0 H 0 1 E E E Aos( kzt ) t propagatig eletrial field while osillatig light frequey (Hz)

More information

Problem T1. Main sequence stars (11 points)

Problem 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 information

Uncertainty Principle of Mathematics

Uncertainty Principle of Mathematics Septeber 27 Ucertaity Priciple of Matheatics Shachter Mourici Israel, Holo ourici@walla.co.il Preface This short paper prove that atheatically, Reality is ot real. This short paper is ot about Heiseberg's

More information

Section 5.2: Calorimetry and Enthalpy Tutorial 1 Practice, page 297

Section 5.2: Calorimetry and Enthalpy Tutorial 1 Practice, page 297 Sectio 52: Calorietry ad Ethalpy Tutorial 1 Practice, page 297 1 Give: V 60 L ; T iitial 25 C ; T fial 75 C; d H2O(l) H2O(l) 100 g/l Required: theral eergy required, q Aalysis: q cδt Solutio: Step 1: Deterie

More information

Lecture #3. Math tools covered today

Lecture #3. Math tools covered today Toay s Program:. Review of previous lecture. QM free particle a particle i a bo. 3. Priciple of spectral ecompositio. 4. Fourth Postulate Math tools covere toay Lecture #3. Lear how to solve separable

More information

Partial Differential Equations

Partial Differential Equations EE 84 Matematical Metods i Egieerig Partial Differetial Eqatios Followig are some classical partial differetial eqatios were is assmed to be a fctio of two or more variables t (time) ad y (spatial coordiates).

More information

Data Analysis and Statistical Methods Statistics 651

Data Analysis and Statistical Methods Statistics 651 Data Aalysis ad Statistical Methods Statistics 651 http://www.stat.tau.edu/~suhasii/teachig.htl Suhasii Subba Rao Exaple The itroge cotet of three differet clover plats is give below. 3DOK1 3DOK5 3DOK7

More information

Newton's Laws. Lecture 2 Key Concepts. Newtonian mechanics and relation to Kepler's laws The Virial Theorem Tidal forces Collision physics

Newton's Laws. Lecture 2 Key Concepts. Newtonian mechanics and relation to Kepler's laws The Virial Theorem Tidal forces Collision physics Lecture 2 Key Concepts Newtonian echanics and relation to Kepler's laws The Virial Theore Tidal forces Collision physics Newton's Laws 1) An object at rest will reain at rest and an object in otion will

More information

Solution: APPM 1360 Final Spring 2013

Solution: 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 information

Chapters 19 & 20 Heat and the First Law of Thermodynamics

Chapters 19 & 20 Heat and the First Law of Thermodynamics Capters 19 & 20 Heat and te First Law of Termodynamics Te Zerot Law of Termodynamics Te First Law of Termodynamics Termal Processes Te Second Law of Termodynamics Heat Engines and te Carnot Cycle Refrigerators,

More information

Solutions to the Multivariable Calculus and Linear Algebra problems on the Comprehensive Examination of January 31, 2014

Solutions to the Multivariable Calculus and Linear Algebra problems on the Comprehensive Examination of January 31, 2014 Solutions to te Multivariable Calculus and Linear Algebra problems on te Compreensive Examination of January 3, 24 Tere are 9 problems ( points eac, totaling 9 points) on tis portion of te examination.

More information

! " * (x,t) " (x,t) dx =! #(x,t) dx = 1 all space

!  * (x,t)  (x,t) dx =! #(x,t) dx = 1 all space Chapter-4 Formalism 4- Schroiger Equatio Durig the early ays of i evelopmet of QM Schroiger a Heiseberg le the charge. Schroiger evelope a QM theory Schroiger Picture base o his famous equato. Heiseberg

More information

PHY 171. Lecture 14. (February 16, 2012)

PHY 171. Lecture 14. (February 16, 2012) PHY 171 Lecture 14 (February 16, 212) In the last lecture, we looked at a quantitative connection between acroscopic and icroscopic quantities by deriving an expression for pressure based on the assuptions

More information

Problem Set 2. Chapter 1 Numerical:

Problem Set 2. Chapter 1 Numerical: Chapter 1 Nuerical: roble Set 16. The atoic radius of xenon is 18 p. Is that consistent with its b paraeter of 5.15 1 - L/ol? Hint: what is the volue of a ole of xenon atos and how does that copare to

More information

Mathematics 105 Calculus I. Exam 1. February 13, Solution Guide

Mathematics 105 Calculus I. Exam 1. February 13, Solution Guide Matematics 05 Calculus I Exam February, 009 Your Name: Solution Guide Tere are 6 total problems in tis exam. On eac problem, you must sow all your work, or oterwise torougly explain your conclusions. Tere

More information

Problem. Consider the sequence a j for j N defined by the recurrence a j+1 = 2a j + j for j > 0

Problem. Consider the sequence a j for j N defined by the recurrence a j+1 = 2a j + j for j > 0 GENERATING FUNCTIONS Give a ifiite sequece a 0,a,a,, its ordiary geeratig fuctio is A : a Geeratig fuctios are ofte useful for fidig a closed forula for the eleets of a sequece, fidig a recurrece forula,

More information

CHAPTER ONE. Physics and the Life Sciences

CHAPTER ONE. Physics and the Life Sciences Solution anual for Physics for the Life Sciences 2nd Edition by Allang Link download full: http://testbankair.co/download/solution-anual-forphysics-for-the-life-sciences-2nd-edition-by-allang/ CHAPTER

More information

PhyzExamples: Advanced Electrostatics

PhyzExamples: Advanced Electrostatics PyzExaples: Avance Electrostatics Pysical Quantities Sybols Units Brief Definitions Carge or Q coulob [KOO lo]: C A caracteristic of certain funaental particles. Eleentary Carge e 1.6 10 19 C Te uantity

More information

Tutorial 2 (Solution) 1. An electron is confined to a one-dimensional, infinitely deep potential energy well of width L = 100 pm.

Tutorial 2 (Solution) 1. An electron is confined to a one-dimensional, infinitely deep potential energy well of width L = 100 pm. Seester 007/008 SMS0 Modern Pysics Tutorial Tutorial (). An electron is confined to a one-diensional, infinitely deep potential energy well of widt L 00 p. a) Wat is te least energy te electron can ave?

More information

Study on Solution of Non-homogeneous Linear Equation based on Ordinary Differential Equation Driving Jing Zhang

Study on Solution of Non-homogeneous Linear Equation based on Ordinary Differential Equation Driving Jing Zhang Iteratioal Coeree o Automatio Meaial Cotrol ad Computatioal Egieerig AMCCE 05 Stud o Solutio o No-omogeeous Liear Equatio based o Ordiar Dieretial Equatio Drivig Jig Zag Meaial ad Eletrial Egieerig College

More information

2.11 That s So Derivative

2.11 That s So Derivative 2.11 Tat s So Derivative Introduction to Differential Calculus Just as one defines instantaneous velocity in terms of average velocity, we now define te instantaneous rate of cange of a function at a point

More information

Application of Homotopy Analysis Method for Solving various types of Problems of Ordinary Differential Equations

Application of Homotopy Analysis Method for Solving various types of Problems of Ordinary Differential Equations Iteratioal Joural o Recet ad Iovatio Treds i Coputig ad Couicatio IN: 31-8169 Volue: 5 Issue: 5 16 Applicatio of Hootopy Aalysis Meod for olvig various types of Probles of Ordiary Differetial Equatios

More information

11. Ideal Gas Mixture

11. Ideal Gas Mixture . Ideal Ga xture. Geeral oderato ad xture of Ideal Gae For a geeral xture of N opoet, ea a pure ubtae [kg ] te a for ea opoet. [kol ] te uber of ole for ea opoet. e al a ( ) [kg ] N e al uber of ole (

More information

International Journal of Advance Engineering and Research Development OSCILLATION AND STABILITY IN A MASS SPRING SYSTEM

International Journal of Advance Engineering and Research Development OSCILLATION AND STABILITY IN A MASS SPRING SYSTEM Scientific Journal of Ipact Factor (SJIF): 5.71 International Journal of Advance Engineering and Researc Developent Volue 5, Issue 06, June -018 e-issn (O): 348-4470 p-issn (P): 348-6406 OSCILLATION AND

More information

REVIEW LAB ANSWER KEY

REVIEW LAB ANSWER KEY REVIEW LAB ANSWER KEY. Witout using SN, find te derivative of eac of te following (you do not need to simplify your answers): a. f x 3x 3 5x x 6 f x 3 3x 5 x 0 b. g x 4 x x x notice te trick ere! x x g

More information

Information entropy of isospectral Pöschl-Teller potential

Information entropy of isospectral Pöschl-Teller potential Iia Joural of Pure & Applie Physics Vol. 43 December 5 pp. 958-963 Iformatio etropy of isospectral Pöschl-Teller potetial Ail Kumar Departmet of Physics Pajab Uiversity Chaigarh 6 4 Receive April 5; accepte

More information

CS 70 Second Midterm 7 April NAME (1 pt): SID (1 pt): TA (1 pt): Name of Neighbor to your left (1 pt): Name of Neighbor to your right (1 pt):

CS 70 Second Midterm 7 April NAME (1 pt): SID (1 pt): TA (1 pt): Name of Neighbor to your left (1 pt): Name of Neighbor to your right (1 pt): CS 70 Secod Midter 7 April 2011 NAME (1 pt): SID (1 pt): TA (1 pt): Nae of Neighbor to your left (1 pt): Nae of Neighbor to your right (1 pt): Istructios: This is a closed book, closed calculator, closed

More information

Logarithmic functions

Logarithmic functions Roberto s Notes on Differential Calculus Capter 5: Derivatives of transcendental functions Section Derivatives of Logaritmic functions Wat ou need to know alread: Definition of derivative and all basic

More information

Function Composition and Chain Rules

Function Composition and Chain Rules Function Composition and s James K. Peterson Department of Biological Sciences and Department of Matematical Sciences Clemson University Marc 8, 2017 Outline 1 Function Composition and Continuity 2 Function

More information

Rules of Differentiation

Rules of Differentiation LECTURE 2 Rules of Differentiation At te en of Capter 2, we finally arrive at te following efinition of te erivative of a function f f x + f x x := x 0 oing so only after an extene iscussion as wat te

More information

The total error in numerical differentiation

The total error in numerical differentiation AMS 147 Computational Metods and Applications Lecture 08 Copyrigt by Hongyun Wang, UCSC Recap: Loss of accuracy due to numerical cancellation A B 3, 3 ~10 16 In calculating te difference between A and

More information

1. Which two values of temperature are equivalent to the nearest degree when measured on the Kelvin and on the

1. Which two values of temperature are equivalent to the nearest degree when measured on the Kelvin and on the . Whih two values of teperature are equivalent to the nearest degree when easured on the Kelvin and on the Celsius sales of teperature? Kelvin sale Celsius sale A. 40 33 B. 273 00 C. 33 40 D. 373 0 2.

More information

SOLUTION. The reactor thermal output is related to the maximum heat flux in the hot channel by. Z( z ). The position of maximum heat flux ( z max

SOLUTION. The reactor thermal output is related to the maximum heat flux in the hot channel by. Z( z ). The position of maximum heat flux ( z max Te verpwer trip set pit i PWRs is desiged t isure te iu fuel eterlie teperature reais belw a give value T, ad te iiu rati reais abve a give value MR. Fr te give ifrati give a step by step predure, iludig

More information

Define a Markov chain on {1,..., 6} with transition probability matrix P =

Define 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 information

( ) Ce, 1 System with Mass, Spring, and Viscous Damper = (2) s are unknown constants. Substituting (2) into (1), we get. Ce ms cs k. ms cs k.

( ) Ce, 1 System with Mass, Spring, and Viscous Damper = (2) s are unknown constants. Substituting (2) into (1), we get. Ce ms cs k. ms cs k. Syste with Mass, Sprig, a Visous Daper by We ow fro Lesso that the visous apig fore F is give F =, where is the apig ostat or oeffiiet of visous apig Vibratig systes are all subjet to apig to soe egree

More information

Physics 6C. De Broglie Wavelength Uncertainty Principle. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Physics 6C. De Broglie Wavelength Uncertainty Principle. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB Pyic 6C De Broglie Wavelengt Uncertainty Principle De Broglie Wavelengt Bot ligt and atter ave bot particle and wavelike propertie. We can calculate te wavelengt of eiter wit te ae forula: p v For large

More information

d y f f dy Numerical Solution of Ordinary Differential Equations Consider the 1 st order ordinary differential equation (ODE) . dx

d y f f dy Numerical Solution of Ordinary Differential Equations Consider the 1 st order ordinary differential equation (ODE) . dx umerical Solutio o Ordiar Dieretial Equatios Cosider te st order ordiar dieretial equatio ODE d. d Te iitial coditio ca be tae as. Te we could use a Talor series about ad obtai te complete solutio or......!!!

More information

Hee = ~ dxdy\jj+ (x) 'IJ+ (y) u (x- y) \jj (y) \jj (x), V, = ~ dx 'IJ+ (x) \jj (x) V (x), Hii = Z 2 ~ dx dy cp+ (x) cp+ (y) u (x- y) cp (y) cp (x),

Hee = ~ dxdy\jj+ (x) 'IJ+ (y) u (x- y) \jj (y) \jj (x), V, = ~ dx 'IJ+ (x) \jj (x) V (x), Hii = Z 2 ~ dx dy cp+ (x) cp+ (y) u (x- y) cp (y) cp (x), SOVIET PHYSICS JETP VOLUME 14, NUMBER 4 APRIL, 1962 SHIFT OF ATOMIC ENERGY LEVELS IN A PLASMA L. E. PARGAMANIK Khar'kov State University Subitted to JETP editor February 16, 1961; resubitted June 19, 1961

More information

What we learned last time

What we learned last time Wat we learned last time Value-function approximation by stocastic gradient descent enables RL to be applied to arbitrarily large state spaces Most algoritms just carry over Targets from tabular case Wit

More information

Acoustic Field inside a Rigid Cylinder with a Point Source

Acoustic 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 information

7.1 Using Antiderivatives to find Area

7.1 Using Antiderivatives to find Area 7.1 Using Antiderivatives to find Area Introduction finding te area under te grap of a nonnegative, continuous function f In tis section a formula is obtained for finding te area of te region bounded between

More information