Fermi Gas. separation

Size: px
Start display at page:

Download "Fermi Gas. separation"

Transcription

1 ri Gas Distiguishabl <---> Idistiguishabl Classical <----> dgrat dd o dsity. If th wavlgth siilar to th saratio tha dgrat ri gas articl h saratio largr traturs hav sallr wavlgth d tightr ackig for dgracy to occur dgrat lctro xals - coductors ad sicoductors - rssur at arth s cor (at last so of it) -aids i iitiatig trasitio fro Mai Squc stars to Rd Giats (allows T to grow lctro rssur is iddt of T) - whit dwarvs ad Iro cor of assiv stars Nutro ad roto xals - ucli with ri otu = 5 MV/c - utro stars 1 1/

2 Dgrat vs o-dgrat

3 Coductio lctros Most lctros i a tal ar attachd to idividual atos. But 1- ar fr to ov through th lattic. Ca trat th as a gas (i a D box) or lik a fiit wll but rgy lvls (ad dsity of stats) siilar (ot boud stats but vibratioal stats of lctros i box) dth of wll V = W (rgy dd for lctro to b rovd fro tal s surfac - hotolctric ffct) + ri rgy at T = all stats u to ar filld V illd lvls W

4 Coductio lctros Ca th calculat th ri rgy for T= (ad it dos t usually chag uch for highr T) N ( ) D( ) d T= D( ) d 8V ( h h N 8 V x. Silvr 1 fr lctro/ato / ) 1/ 1/ d or N V atos/ ol 1.5g 18 g / ol c fr lctros / c 4 (6.61 joul sc) kg (14V) 8.511MV ato / 8 / 5.5V 1V J 4

5 Coductio lctros Ca dtri th avrag rgy at T = for silvr. V ca coar to classical statistics T.V k Pauli xclusio forcs lctros to uch highr rgy lvls at low traturs. (why s ot ivolvd i scific hat which is a lattic vibratio/hoos) D( ) ( ) d D( ) ( ) d 1/ 1/ d d.v 8.61 V / K 5 5/ / 5 o 4, 5 K 5

6 Coductio lctros 6

7 Coductio lctros Siilarly, fro T-ddt 1 Nh kt1 5/ /... V (kt) th trs aftr th 1 ar th dgracy trs.larg if dgrat. or silvr atos at T= K ot util th dgracy tr is sall will th lctro act classically. Has at high T Th ri rgy varis slowly with T ad at T= K is alost th sa as at T= You obtai th ri rgy by oralizatio. Quark-gluo lasa (covrd latr) is a xal of a high T ri gas kt 1 ( ) () 8 7

8 ri Gass i Stars quilibriu: balac btw gravitatioal rssur ad gas (ithr oral or dgrat) rssur total gravitatioal rgy: dsity varis i oral stars (i Su: avrag is 1 g/c but at r= is 1 g/c ). Mor of a costat i whit dwarvs or utro stars will hav ithr oral gas rssur of P=kT (P=<>) or rssur du to dgrat articls. Noral dds o T, dgrat (ostly) dos t = articl dsity i this cas GM ( r) Mass( r r) r R ( r) r G 4r dr 4 r ( r) dr r M G if cos ta t rssur 5 R V 8

9 Start with = <> o-rlativistic N P 5 1 P dds ONLY o dsity Dgrat ri Gas Prssur dsity stats : D( ) D( ) 1/ A 1/ / K 1/ / d 1/ d K 1 d / 5/ 4 K rlativistic both A d 1/ d K cass d 1/ 1/ 4 / 9

10 o-rlativistic P 5 1 / K / Dgrat ri Gas Prssur K 1 / 5/ 4 K 1/ rlativistic K 1/ 1/ 4/ P dds ONLY o dsity Prssur dcrass if, for a giv dsity, articls bco rlativistic if shrik star s radius by dsity icrass by 8 gravitatioal icrass by if o-rlativistic. <> icrass by (N/V) / = 4 if rlativistic <> icrass by (N/V) 1/ = o-rlativistic stabl but rlativistic is ot. ca aid i collas of whit dwarf 1

11 Oldr Su-lik Stars SKIP Dsity of cor icrass as HH. H irt (o fusio yt). Cor cotracts lctros bco dgrat. 4 r H ucli. lctros hav logr wavlgth tha H thral quilibriu lctros ov to highr rgy du to Pauli xclusio/dgracy. No logr i thral quilibriu with, H ucli rssur bcos doiatd by lctros. No logr dds o T P total P P H allows T of,h to icras raidly without oral icras i rssur ad chag i star s quilibriu. Ost of HC fusio ad Rd Giat has (hliu flash wh T = 1,, K) P H H P H P H H P H H H 11

12 Whit Dwarvs Lftovr cors of Rd Giats ad (usually) fro C + O ucli ad dgrat lctros cors of vry assiv stars ar ucli lus dgrat lctros ad hav siilar rortis gravitatioal rssur balacd by lctros rssur which icrass as radius dcrass radius dds o Mass of star Dtri aroxiat ri rgy. Assu lctro dsity =.5(+) dsity N V M Su 1 1 volu arth lctros ar i this rag ad oft ot coltly rlativistic or o-rlativistic d to us th corrct = + rlatioshi h N ( o rl) 8 V. MV N 1/ ( rl) hc.8 MV V 8 / 51 5 / 1

13 Whit Dwarvs + Collas If th lctro rgy is > about 1.4 MV ca hav: Thrshold 1. 4MV ay lctros > T disaar. Th lctro rgy distributio dds o T (avrag ) # s T th lost lctros caus th rssur fro th dgrat lctros to dcras th rgy of th utrios is also lost as thy sca cools th star as th ass icrass, radius dcrass, ad ubr of lctros abov thrshold icrass 1

14 Whit Dwarvs+Surovas SKIP aothr rocss - hotodistgratio - also absorbs rgy coolig star. Siilar rgy loss as + cobiatio H H 4 At so oit th ot vry stabl quilibriu btw gravity ad (ostly) lctro rssur dos t hold Whit Dwarf collass ad so fractio (-5%??) of th rotos covrt to utros durig th collas givs Surovas L L SN SN ( light ) 1 9 L Su ( light ) ( utrios ) 1(1?) L SN ( light ) 14

15 Whit Dwarvs+Surovas 15

16 Nutro Stars-arox. ubrs SKIP Surovas ca roduc utro stars - radius ~ 1 k - ass about that of Su. always < ass Su - rlativ :: ~ 99:1:1 gravity suortd by dgrat utros lug ito o-rlativistic forula for ri rgy 14 MV (as ass =94 MV, o-rl OK) look at wavlgth saratio ca dtri radius vs ass (lik WD) N V ca collas ito black hol M Su /.6 / 4 (1k) h 1. h 14MV 94MV 14MV 16

17 Nutro Stars SKIP sarat ri gass: :: + ar i th sa ottial wll du to strog uclar forc assu iddt ad that / =.1 (dds o star s ass) ( ) ( ) so d to us rlativistic for lctros but ot iddt as <---> ( ) ( ) lus ractios with virtual articls N / 145MV V 5 6MV N / 145MV 94 1,MV ( wrog) V fr utros dcay. But i a utro star thy ca oly do so if thr is a availabl ufilld lctro stat. So sursss dcay 5 N 1/ hc MV ( ) 5 V

18 Nutro Stars SKIP Will d u with a quilibriu btw -- which ca bst b s by atchig u th ri rgy of th utros with th - syst utros with > ca th dcay to --u (which raiss lctro dsity ad its ri rgy thus th balac) d to iclud rst ass rgis. Also dsity of lctros is qual to that of rotos ca th solv for / ratio (w ll ski algbra) givs for tyical utro star: 18 / / 1/ ) ( ) ( ) ( c h h c hc / / 1 1 / kg

How many neutrino species?

How many neutrino species? ow may utrio scis? Two mthods for dtrmii it lium abudac i uivrs At a collidr umbr of utrio scis Exasio of th uivrs is ovrd by th Fridma quatio R R 8G tot Kc R Whr: :ubblcostat G :Gravitatioal costat 6.

More information

8(4 m0) ( θ ) ( ) Solutions for HW 8. Chapter 25. Conceptual Questions

8(4 m0) ( θ ) ( ) Solutions for HW 8. Chapter 25. Conceptual Questions Solutios for HW 8 Captr 5 Cocptual Qustios 5.. θ dcrass. As t crystal is coprssd, t spacig d btw t plas of atos dcrass. For t first ordr diffractio =. T Bragg coditio is = d so as d dcrass, ust icras for

More information

LECTURE 13 Filling the bands. Occupancy of Available Energy Levels

LECTURE 13 Filling the bands. Occupancy of Available Energy Levels LUR 3 illig th bads Occupacy o Availabl rgy Lvls W hav dtrmid ad a dsity o stats. W also d a way o dtrmiig i a stat is illd or ot at a giv tmpratur. h distributio o th rgis o a larg umbr o particls ad

More information

They must have different numbers of electrons orbiting their nuclei. They must have the same number of neutrons in their nuclei.

They must have different numbers of electrons orbiting their nuclei. They must have the same number of neutrons in their nuclei. 37 1 How may utros ar i a uclus of th uclid l? 20 37 54 2 crtai lmt has svral isotops. Which statmt about ths isotops is corrct? Thy must hav diffrt umbrs of lctros orbitig thir ucli. Thy must hav th sam

More information

Session : Plasmas in Equilibrium

Session : Plasmas in Equilibrium Sssio : Plasmas i Equilibrium Ioizatio ad Coductio i a High-prssur Plasma A ormal gas at T < 3000 K is a good lctrical isulator, bcaus thr ar almost o fr lctros i it. For prssurs > 0.1 atm, collisio amog

More information

Lecture contents. Transport, scattering Generation/recombination. E c. E t. E v. NNSE508 / NENG452 Lecture #13. Band-to-band recombination

Lecture contents. Transport, scattering Generation/recombination. E c. E t. E v. NNSE508 / NENG452 Lecture #13. Band-to-band recombination Lctur cotts Trasort, scattrig Gratio/rcobiatio E E c E t E v Bad-to-bad rcobiatio Tra-assistd (SRH) rcobiatio ad gratio Augr rcobiatio Elctro trasort: Gral cosidratios How fr carrirs ract o xtral lctric

More information

Narayana IIT Academy

Narayana IIT Academy INDIA Sc: LT-IIT-SPARK Dat: 9--8 6_P Max.Mars: 86 KEY SHEET PHYSIS A 5 D 6 7 A,B 8 B,D 9 A,B A,,D A,B, A,B B, A,B 5 A 6 D 7 8 A HEMISTRY 9 A B D B B 5 A,B,,D 6 A,,D 7 B,,D 8 A,B,,D 9 A,B, A,B, A,B,,D A,B,

More information

Solid State Device Fundamentals

Solid State Device Fundamentals 8 Biasd - Juctio Solid Stat Dvic Fudamtals 8. Biasd - Juctio ENS 345 Lctur Cours by Aladr M. Zaitsv aladr.zaitsv@csi.cuy.du Tl: 718 98 81 4N101b Dartmt of Egirig Scic ad Physics Biasig uiolar smicoductor

More information

Blackbody Radiation. All bodies at a temperature T emit and absorb thermal electromagnetic radiation. How is blackbody radiation absorbed and emitted?

Blackbody Radiation. All bodies at a temperature T emit and absorb thermal electromagnetic radiation. How is blackbody radiation absorbed and emitted? All bodis at a tmpratur T mit ad absorb thrmal lctromagtic radiatio Blackbody radiatio I thrmal quilibrium, th powr mittd quals th powr absorbd How is blackbody radiatio absorbd ad mittd? 1 2 A blackbody

More information

EE 232 Lightwave Devices Lecture 3: Basic Semiconductor Physics and Optical Processes. Optical Properties of Semiconductors

EE 232 Lightwave Devices Lecture 3: Basic Semiconductor Physics and Optical Processes. Optical Properties of Semiconductors 3 Lightwav Dvics Lctur 3: Basic Smicoductor Physics ad Optical Procsss Istructor: Mig C. Wu Uivrsity of Califoria, Brly lctrical girig ad Computr Scics Dpt. 3 Lctur 3- Optical Proprtis of Smicoductors

More information

How many neutrons does this aluminium atom contain? A 13 B 14 C 27 D 40

How many neutrons does this aluminium atom contain? A 13 B 14 C 27 D 40 alumiium atom has a uclo umbr of 7 ad a roto umbr of 3. How may utros dos this alumiium atom cotai? 3 4 7 40 atom of lmt Q cotais 9 lctros, 9 rotos ad 0 utros. What is Q? calcium otassium strotium yttrium

More information

3.1 Atomic Structure and The Periodic Table

3.1 Atomic Structure and The Periodic Table Sav My Exams! Th Hom of Rvisio For mor awsom GSE ad lvl rsourcs, visit us at www.savmyxams.co.uk/ 3. tomic Structur ad Th Priodic Tabl Qustio Par Lvl IGSE Subjct hmistry (060) Exam oard ambridg Itratioal

More information

5.1 The Nuclear Atom

5.1 The Nuclear Atom Sav My Exams! Th Hom of Rvisio For mor awsom GSE ad lvl rsourcs, visit us at www.savmyxams.co.uk/ 5.1 Th Nuclar tom Qustio Papr Lvl IGSE Subjct Physics (0625) Exam oard Topic Sub Topic ooklt ambridg Itratioal

More information

Nuclear Chemistry -- ANSWERS

Nuclear Chemistry -- ANSWERS Hoor Chstry Mr. Motro 5-6 Probl St Nuclar Chstry -- ANSWERS Clarly wrt aswrs o sparat shts. Show all work ad uts.. Wrt all th uclar quatos or th radoactv dcay srs o Urau-38 all th way to Lad-6. Th dcay

More information

The Death of Stars - II.

The Death of Stars - II. Th Dath of Stars - II. Larning Objctivs! How can w us H-R diagrams to masur th ag of star clustrs (and hnc th ag of our Univrs)?! Why do high and low mass stars volv diffrntly? How ar havy lmnts such as

More information

Weights Interpreting W and lnw What is β? Some Endnotes = n!ω if we neglect the zero point energy then ( )

Weights Interpreting W and lnw What is β? Some Endnotes = n!ω if we neglect the zero point energy then ( ) Sprg Ch 35: Statstcal chacs ad Chcal Ktcs Wghts... 9 Itrprtg W ad lw... 3 What s?... 33 Lt s loo at... 34 So Edots... 35 Chaptr 3: Fudatal Prcpls of Stat ch fro a spl odl (drvato of oltza dstrbuto, also

More information

Chp6. pn Junction Diode: I-V Characteristics I

Chp6. pn Junction Diode: I-V Characteristics I 147 C6. uctio Diod: I-V Caractristics I 6.1. THE IDEAL DIODE EQUATION 6.1.1. Qualitativ Drivatio 148 Figur rfrc: Smicoductor Dvic Fudamtals Robrt F. Pirrt, Addiso-Wsly Publicig Comay 149 Figur 6.1 juctio

More information

(Reference: sections in Silberberg 5 th ed.)

(Reference: sections in Silberberg 5 th ed.) ALE. Atomic Structur Nam HEM K. Marr Tam No. Sctio What is a atom? What is th structur of a atom? Th Modl th structur of a atom (Rfrc: sctios.4 -. i Silbrbrg 5 th d.) Th subatomic articls that chmists

More information

Maxwellian Collisions

Maxwellian Collisions Maxwllian Collisions Maxwll ralizd arly on that th particular typ of collision in which th cross-sction varis at Q rs 1/g offrs drastic siplifications. Intrstingly, this bhavior is physically corrct for

More information

Chapter 8: Electron Configurations and Periodicity

Chapter 8: Electron Configurations and Periodicity Elctron Spin & th Pauli Exclusion Principl Chaptr 8: Elctron Configurations and Priodicity 3 quantum numbrs (n, l, ml) dfin th nrgy, siz, shap, and spatial orintation of ach atomic orbital. To xplain how

More information

ln x = n e = 20 (nearest integer)

ln x = n e = 20 (nearest integer) H JC Prlim Solutios 6 a + b y a + b / / dy a b 3/ d dy a b at, d Giv quatio of ormal at is y dy ad y wh. d a b () (,) is o th curv a+ b () y.9958 Qustio Solvig () ad (), w hav a, b. Qustio d.77 d d d.77

More information

Mon. Tues. Wed. Lab Fri Electric and Rest Energy

Mon. Tues. Wed. Lab Fri Electric and Rest Energy Mon. Tus. Wd. Lab Fi. 6.4-.7 lctic and Rst ngy 7.-.4 Macoscoic ngy Quiz 6 L6 Wok and ngy 7.5-.9 ngy Tansf R 6. P6, HW6: P s 58, 59, 9, 99(a-c), 05(a-c) R 7.a bing lato, sathon, ad, lato R 7.b v. i xal

More information

The Death of Stars - I.

The Death of Stars - I. Th Dath of Stars - I. Larning Objctivs! B abl to sktch th H-R diagram and includ stars by siz, sctral ty, liftim, color, mass, magnitud, tmratur and luminosity, rlativ to our Sun! Comar Rd Dwarfs to our

More information

fiziks Institute for NET/JRF, GATE, IIT JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics

fiziks Institute for NET/JRF, GATE, IIT JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics Atoic and olcular Physics JEST Q. Th binding nrgy of th hydrogn ato (lctron bound to proton) is.6 V. Th binding nrgy of positroniu (lctron bound to positron) is (a).6 / V (b).6 / 8 V (c).6 8 V (d).6 V.6

More information

Ideal crystal : Regulary ordered point masses connected via harmonic springs

Ideal crystal : Regulary ordered point masses connected via harmonic springs Statistical thrmodyamics of crystals Mooatomic crystal Idal crystal : Rgulary ordrd poit masss coctd via harmoic sprigs Itratomic itractios Rprstd by th lattic forc-costat quivalt atom positios miima o

More information

Principles of Humidity Dalton s law

Principles of Humidity Dalton s law Principls of Humidity Dalton s law Air is a mixtur of diffrnt gass. Th main gas componnts ar: Gas componnt volum [%] wight [%] Nitrogn N 2 78,03 75,47 Oxygn O 2 20,99 23,20 Argon Ar 0,93 1,28 Carbon dioxid

More information

Today s topic 2 = Setting up the Hydrogen Atom problem. Schematic of Hydrogen Atom

Today s topic 2 = Setting up the Hydrogen Atom problem. Schematic of Hydrogen Atom Today s topic Sttig up th Hydog Ato pobl Hydog ato pobl & Agula Motu Objctiv: to solv Schödig quatio. st Stp: to dfi th pottial fuctio Schatic of Hydog Ato Coulob s aw - Z 4ε 4ε fo H ato Nuclus Z What

More information

The real E-k diagram of Si is more complicated (indirect semiconductor). The bottom of E C and top of E V appear for different values of k.

The real E-k diagram of Si is more complicated (indirect semiconductor). The bottom of E C and top of E V appear for different values of k. Modr Smcoductor Dvcs for Itgratd rcuts haptr. lctros ad Hols Smcoductors or a bad ctrd at k=0, th -k rlatoshp ar th mmum s usually parabolc: m = k * m* d / dk d / dk gatv gatv ffctv mass Wdr small d /

More information

Motivation. We talk today for a more flexible approach for modeling the conditional probabilities.

Motivation. We talk today for a more flexible approach for modeling the conditional probabilities. Baysia Ntworks Motivatio Th coditioal idpdc assuptio ad by aïv Bays classifirs ay s too rigid spcially for classificatio probls i which th attributs ar sowhat corrlatd. W talk today for a or flibl approach

More information

Chapter 2 Infinite Series Page 1 of 11. Chapter 2 : Infinite Series

Chapter 2 Infinite Series Page 1 of 11. Chapter 2 : Infinite Series Chatr Ifiit Sris Pag of Sctio F Itgral Tst Chatr : Ifiit Sris By th d of this sctio you will b abl to valuat imror itgrals tst a sris for covrgc by alyig th itgral tst aly th itgral tst to rov th -sris

More information

Washington State University

Washington State University he 3 Ktics ad Ractor Dsig Sprg, 00 Washgto Stat Uivrsity Dpartmt of hmical Egrg Richard L. Zollars Exam # You will hav o hour (60 muts) to complt this xam which cosists of four (4) problms. You may us

More information

1985 AP Calculus BC: Section I

1985 AP Calculus BC: Section I 985 AP Calculus BC: Sctio I 9 Miuts No Calculator Nots: () I this amiatio, l dots th atural logarithm of (that is, logarithm to th bas ). () Ulss othrwis spcifid, th domai of a fuctio f is assumd to b

More information

coulombs or esu charge. It s mass is about 1/1837 times the mass of hydrogen atom. Thus mass of electron is

coulombs or esu charge. It s mass is about 1/1837 times the mass of hydrogen atom. Thus mass of electron is 1 ATOMIC STRUCTURE Fudamtal Particls: Mai Fudamtal Particl : (a) Elctro: It is a fudamtal particl of a atom which carris a uit gativ charg. It was discovrd by J.J. Thomso (1897) from th studis carrid out

More information

Digital Signal Processing, Fall 2006

Digital Signal Processing, Fall 2006 Digital Sigal Procssig, Fall 6 Lctur 9: Th Discrt Fourir Trasfor Zhg-Hua Ta Dpartt of Elctroic Systs Aalborg Uivrsity, Dar zt@o.aau.d Digital Sigal Procssig, I, Zhg-Hua Ta, 6 Cours at a glac MM Discrt-ti

More information

Exam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator.

Exam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator. Exam N a m : _ S O L U T I O N P U I D : I n s t r u c t i o n s : It is important that you clarly show your work and mark th final answr clarly, closd book, closd nots, no calculator. T i m : h o u r

More information

Probability & Statistics,

Probability & Statistics, Probability & Statistics, BITS Pilai K K Birla Goa Campus Dr. Jajati Kshari Sahoo Dpartmt of Mathmatics BITS Pilai, K K Birla Goa Campus Poisso Distributio Poisso Distributio: A radom variabl X is said

More information

GRAPHS IN SCIENCE. drawn correctly, the. other is not. Which. Best Fit Line # one is which?

GRAPHS IN SCIENCE. drawn correctly, the. other is not. Which. Best Fit Line # one is which? 5 9 Bt Ft L # 8 7 6 5 GRAPH IN CIENCE O of th thg ot oft a rto of a xrt a grah of o k. A grah a vual rrtato of ural ata ollt fro a xrt. o of th ty of grah you ll f ar bar a grah. Th o u ot oft a l grah,

More information

CIVE322 BASIC HYDROLOGY Hydrologic Science and Engineering Civil and Environmental Engineering Department Fort Collins, CO (970)

CIVE322 BASIC HYDROLOGY Hydrologic Science and Engineering Civil and Environmental Engineering Department Fort Collins, CO (970) CVE322 BASC HYDROLOGY Hydrologic Scic ad Egirig Civil ad Evirotal Egirig Dpartt Fort Collis, CO 80523-1372 (970 491-7621 MDERM EXAM 1 NO. 1 Moday, Octobr 3, 2016 8:00-8:50 AM Haod Auditoriu You ay ot cosult

More information

signal amplification; design of digital logic; memory circuits

signal amplification; design of digital logic; memory circuits hatr Th lctroc dvc that s caabl of currt ad voltag amlfcato, or ga, cojucto wth othr crcut lmts, s th trasstor, whch s a thr-trmal dvc. Th dvlomt of th slco trasstor by Bard, Bratta, ad chockly at Bll

More information

APPENDIX: STATISTICAL TOOLS

APPENDIX: STATISTICAL TOOLS I. Nots o radom samplig Why do you d to sampl radomly? APPENDI: STATISTICAL TOOLS I ordr to masur som valu o a populatio of orgaisms, you usually caot masur all orgaisms, so you sampl a subst of th populatio.

More information

5.62 Physical Chemistry II Spring 2008

5.62 Physical Chemistry II Spring 2008 MIT OpnCoursWar http://ocw.mit.du 5.62 Physical Chmistry II Spring 2008 For information about citing ths matrials or our Trms of Us, visit: http://ocw.mit.du/trms. 5.62 Lctur #7: Translational Part of

More information

Worksheet: Taylor Series, Lagrange Error Bound ilearnmath.net

Worksheet: Taylor Series, Lagrange Error Bound ilearnmath.net Taylor s Thorm & Lagrag Error Bouds Actual Error This is th ral amout o rror, ot th rror boud (worst cas scario). It is th dirc btw th actual () ad th polyomial. Stps:. Plug -valu ito () to gt a valu.

More information

Problem Set 4 Solutions Distributed: February 26, 2016 Due: March 4, 2016

Problem Set 4 Solutions Distributed: February 26, 2016 Due: March 4, 2016 Probl St 4 Solutions Distributd: Fbruary 6, 06 Du: March 4, 06 McQuarri Probls 5-9 Ovrlay th two plots using Excl or Mathatica. S additional conts blow. Th final rsult of Exapl 5-3 dfins th forc constant

More information

Chemistry 432 Problem Set 11 Spring 2018 Solutions

Chemistry 432 Problem Set 11 Spring 2018 Solutions 1. Show that for an ideal gas Cheistry 432 Proble Set 11 Spring 2018 Solutions P V 2 3 < KE > where is the average kinetic energy of the gas olecules. P 1 3 ρ v2 KE 1 2 v2 ρ N V P V 1 3 N v2 2 3 N

More information

Lecture contents. Semiconductor statistics. NNSE508 / NENG452 Lecture #12

Lecture contents. Semiconductor statistics. NNSE508 / NENG452 Lecture #12 Ltur otts Sioutor statistis S58 / G45 Ltur # illig th pty bas: Distributio futio ltro otratio at th rgy (Dsity of stats) (istributio futio): ( ) ( ) f ( ) Pauli lusio Priipl: o two ltros (frios) a hav

More information

Collisions. In had on lastic collision of two bodis of qual ass ) Th fastr body spds up furthr and th slowr body slows down. ) Th fastr body slows down and th slowr body spds up. 3) Both of th abov. 4)

More information

If we integrate the given modulating signal, m(t), we arrive at the following FM signal:

If we integrate the given modulating signal, m(t), we arrive at the following FM signal: Part b If w intgrat th givn odulating signal, (, w arriv at th following signal: ( Acos( πf t + β sin( πf W can us anothr trigonotric idntity hr. ( Acos( β sin( πf cos( πf Asin( β sin( πf sin( πf Now,

More information

Option 3. b) xe dx = and therefore the series is convergent. 12 a) Divergent b) Convergent Proof 15 For. p = 1 1so the series diverges.

Option 3. b) xe dx = and therefore the series is convergent. 12 a) Divergent b) Convergent Proof 15 For. p = 1 1so the series diverges. Optio Chaptr Ercis. Covrgs to Covrgs to Covrgs to Divrgs Covrgs to Covrgs to Divrgs 8 Divrgs Covrgs to Covrgs to Divrgs Covrgs to Covrgs to Covrgs to Covrgs to 8 Proof Covrgs to π l 8 l a b Divrgt π Divrgt

More information

Blackbody Radiation. All bodies at a temperature T emit and absorb thermal electromagnetic radiation. How is blackbody radiation absorbed and emitted?

Blackbody Radiation. All bodies at a temperature T emit and absorb thermal electromagnetic radiation. How is blackbody radiation absorbed and emitted? All bodis at a tmpratur T mit ad absorb thrmal lctromagtic radiatio Blackbody radiatio I thrmal quilibrium, th powr mittd quals th powr absorbd How is blackbody radiatio absorbd ad mittd? 1 2 A blackbody

More information

Superfluid Liquid Helium

Superfluid Liquid Helium Surfluid Liquid Hlium:Bo liquid ad urfluidity Ladau thory: two fluid modl Bo-iti Codatio ad urfluid ODLRO, otaou ymmtry brakig, macrocoic wafuctio Gro-Pitakii GP quatio Fyma ictur Rfrc: Thory of quatum

More information

III.5. THE THERMISTOR

III.5. THE THERMISTOR III.5. H HRMISOR 1. Wor uros o cc t law dscribig t tratur ddc of t lctrical rsistac of sicoductor atrials ad to valuat tir ga.. ory Quatu caics stats tat isolatd icrosysts (lctros, olculs, ios) av oly

More information

Astronomy 210. Outline. Life of a Low Mass Star. Evolutionary Path of a Solar-Mass Star. Solar Observing & HW9 due Friday Stardial 2 is available.

Astronomy 210. Outline. Life of a Low Mass Star. Evolutionary Path of a Solar-Mass Star. Solar Observing & HW9 due Friday Stardial 2 is available. Astronomy 210 Outlin This Class (Lctur 32): Lif and Dath of th Sun Nxt Class: Lif and Dath of Othr Stars Solar Obsrving & HW9 du Friday Stardial 2 is availabl. Dath of a solar mass star! Burning m u. Whit

More information

H2 Mathematics Arithmetic & Geometric Series ( )

H2 Mathematics Arithmetic & Geometric Series ( ) H Mathmatics Arithmtic & Gomtric Sris (08 09) Basic Mastry Qustios Arithmtic Progrssio ad Sris. Th rth trm of a squc is 4r 7. (i) Stat th first four trms ad th 0th trm. (ii) Show that th squc is a arithmtic

More information

Gases and Vapour Mixtures

Gases and Vapour Mixtures 9 Gass and aour Mixturs 9.. Introduction. 9.. Dalton s law and Gibbs-Dalton law. 9.. olutric analysis of a gas ixtur. 9.4. h aarnt olcular wight and gas constant. 9.. Scific hats of a gas ixtur. 9.6. Adiabatic

More information

Chapter 6. pn-junction diode: I-V characteristics

Chapter 6. pn-junction diode: I-V characteristics Chatr 6. -jucto dod: -V charactrstcs Tocs: stady stat rsos of th jucto dod udr ald d.c. voltag. ucto udr bas qualtatv dscusso dal dod quato Dvatos from th dal dod Charg-cotrol aroach Prof. Yo-S M Elctroc

More information

Ch. 6 Free Electron Fermi Gas

Ch. 6 Free Electron Fermi Gas Ch. 6 lcto i Gas Coductio lctos i a tal ov fl without scattig b io cos so it ca b cosidd as if walitactig o f paticls followig idiac statistics. hfo th coductio lctos a fqutl calld as f lcto i gas. Coductio

More information

orbiting electron turns out to be wrong even though it Unfortunately, the classical visualization of the

orbiting electron turns out to be wrong even though it Unfortunately, the classical visualization of the Lctur 22-1 Byond Bohr Modl Unfortunatly, th classical visualization of th orbiting lctron turns out to b wrong vn though it still givs us a simpl way to think of th atom. Quantum Mchanics is ndd to truly

More information

MONTGOMERY COLLEGE Department of Mathematics Rockville Campus. 6x dx a. b. cos 2x dx ( ) 7. arctan x dx e. cos 2x dx. 2 cos3x dx

MONTGOMERY COLLEGE Department of Mathematics Rockville Campus. 6x dx a. b. cos 2x dx ( ) 7. arctan x dx e. cos 2x dx. 2 cos3x dx MONTGOMERY COLLEGE Dpartmt of Mathmatics Rockvill Campus MATH 8 - REVIEW PROBLEMS. Stat whthr ach of th followig ca b itgratd by partial fractios (PF), itgratio by parts (PI), u-substitutio (U), or o of

More information

School of Aerospace Engineering Origins of Quantum Theory. Measurements of emission of light (EM radiation) from (H) atoms found discrete lines

School of Aerospace Engineering Origins of Quantum Theory. Measurements of emission of light (EM radiation) from (H) atoms found discrete lines Ogs of Quatu Thoy Masuts of sso of lght (EM adato) fo (H) atos foud dsct ls 5 4 Abl to ft to followg ss psso ν R λ c λwavlgth, νfqucy, cspd lght RRydbg Costat (~09,7677.58c - ),,, +, +,..g.,,.6, 0.6, (Lya

More information

Mixed Mode Oscillations as a Mechanism for Pseudo-Plateau Bursting

Mixed Mode Oscillations as a Mechanism for Pseudo-Plateau Bursting Mixd Mod Oscillatios as a Mchaism for Psudo-Platau Burstig Richard Brtram Dpartmt of Mathmatics Florida Stat Uivrsity Tallahass, FL Collaborators ad Support Thodor Vo Marti Wchslbrgr Joël Tabak Uivrsity

More information

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches.

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches. Subjct Chmistry Papr No and Titl Modul No and Titl Modul Tag 8/ Physical Spctroscopy / Brakdown of th Born-Oppnhimr approximation. Slction ruls for rotational-vibrational transitions. P, R branchs. CHE_P8_M

More information

ECE594I Notes set 6: Thermal Noise

ECE594I Notes set 6: Thermal Noise C594I ots, M. odwll, copyrightd C594I Nots st 6: Thrmal Nois Mark odwll Uivrsity of Califoria, ata Barbara rodwll@c.ucsb.du 805-893-344, 805-893-36 fax frcs ad Citatios: C594I ots, M. odwll, copyrightd

More information

Homework 1: Solutions

Homework 1: Solutions Howo : Solutos No-a Fals supposto tst but passs scal tst lthouh -f th ta as slowss [S /V] vs t th appaac of laty alty th path alo whch slowss s to b tat to obta tavl ts ps o th ol paat S o V as a cosquc

More information

ME 300 Exam 1 October 9, :30 p.m. to 7:30 p.m.

ME 300 Exam 1 October 9, :30 p.m. to 7:30 p.m. CIRCLE YOUR LECTURE BELOW: First Na Last Na 10:0 a.. 1:0 p.. Naik Gor ME 00 Exa 1 Octobr 9, 014 6:0 p.. to 7:0 p.. INSTRUCTIONS 1. This is a closd book and closd nots xaination. You ar providd with an

More information

Acoustomagnetoelectric effect in a degenerate semiconductor with nonparabolic energy dispersion law.

Acoustomagnetoelectric effect in a degenerate semiconductor with nonparabolic energy dispersion law. Acoustoatolctric ct i a drat sicoductor it oarabolic ry disrsio la. N. G. Msa Dartt o Matatics ad Statistics Uirsity o Ca Coast Gaa. Abstract: Surac D acoustoatolctric ct SAM ad bul D acoustoatolctric

More information

Outline. Ionizing Radiation. Introduction. Ionizing radiation

Outline. Ionizing Radiation. Introduction. Ionizing radiation Outli Ioizig Radiatio Chaptr F.A. Attix, Itroductio to Radiological Physics ad Radiatio Dosimtry Radiological physics ad radiatio dosimtry Typs ad sourcs of ioizig radiatio Dscriptio of ioizig radiatio

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

Chem/Biochem 471 Exam 3 12/18/08 Page 1 of 7 Name:

Chem/Biochem 471 Exam 3 12/18/08 Page 1 of 7 Name: Che/Bioche 47 Exa /8/08 Pae of 7 Please leave the exa paes stapled toether. The forulas are on a separate sheet. This exa has 5 questions. You ust answer at least 4 of the questions. You ay answer ore

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

Neutrinos are chargeless, nearly massless particles Most abundant particle in the Universe Interact with matter via weak nuclear force

Neutrinos are chargeless, nearly massless particles Most abundant particle in the Universe Interact with matter via weak nuclear force By Wndi Wamlr Nutrinos ar charglss, narly masslss articls Most abundant articl in th Univrs Intract with mattr via wak nuclar forc Narly transarnt to mattr Only known ty of articl that can sca from th

More information

pn Junction Under Reverse-Bias Conditions 3.3 Physical Operation of Diodes

pn Junction Under Reverse-Bias Conditions 3.3 Physical Operation of Diodes 3.3 Physcal Orato of os Jucto Ur vrs-bas Cotos rft Currt S : ato to th ffuso Currt comot u to majorty carrr ffuso, caus by thrmally grat morty carrrs, thr ar two currt comots lctros mov by rft from to

More information

The probability of Riemann's hypothesis being true is. equal to 1. Yuyang Zhu 1

The probability of Riemann's hypothesis being true is. equal to 1. Yuyang Zhu 1 Th robablty of Ra's hyothss bg tru s ual to Yuyag Zhu Abstract Lt P b th st of all r ubrs P b th -th ( ) lt of P ascdg ordr of sz b ostv tgrs ad s a rutato of wth Th followg rsults ar gv ths ar: () Th

More information

ME311 Machine Design

ME311 Machine Design ME311 Machin Dsign Lctur 4: Strss Concntrations; Static Failur W Dornfld 8Sp017 Fairfild Univrsit School of Enginring Strss Concntration W saw that in a curvd bam, th strss was distortd from th uniform

More information

All Excuses must be taken to 233 Loomis before 4:15, Monday, April 30.

All Excuses must be taken to 233 Loomis before 4:15, Monday, April 30. Miscellaneous Notes he end is near don t get behind. All Excuses ust be taken to 233 Loois before 4:15, Monday, April 30. he PHYS 213 final exa ties are * 8-10 AM, Monday, May 7 * 8-10 AM, uesday, May

More information

9 Kinetic Theory of Gases

9 Kinetic Theory of Gases Contnt 9 Kintic hory of Gass By Liw Sau oh 9. Ial gas quation 9. rssur of a gas 9. Molcular kintic nrgy 9.4 h r..s. sp of olculs 9.5 Dgrs of fro an law of quipartition of nrgy 9.6 Intrnal nrgy of an ial

More information

A 1 A 2. a) Find the wavelength of the radio waves. Since c = f, then = c/f = (3x10 8 m/s) / (30x10 6 Hz) = 10m.

A 1 A 2. a) Find the wavelength of the radio waves. Since c = f, then = c/f = (3x10 8 m/s) / (30x10 6 Hz) = 10m. 1. Young s doubl-slit xprint undrlis th instrunt landing syst at ost airports and is usd to guid aircraft to saf landings whn th visibility is poor. Suppos that a pilot is trying to align hr plan with

More information

CHAPTER 4. The First Law of Thermodynamics for Control Volumes

CHAPTER 4. The First Law of Thermodynamics for Control Volumes CHAPTER 4 T Frst Law of Trodynacs for Control olus CONSERATION OF MASS Consrvaton of ass: Mass, lk nrgy, s a consrvd proprty, and t cannot b cratd or dstroyd durng a procss. Closd systs: T ass of t syst

More information

Queueing Theory II. Summary. M/M/1 Output process Networks of Queue Method of Stages. General Distributions

Queueing Theory II. Summary. M/M/1 Output process Networks of Queue Method of Stages. General Distributions Queueig Theory II Suary M/M/1 Output process Networks of Queue Method of Stages Erlag Distributio Hyperexpoetial Distributio Geeral Distributios Ebedded Markov Chais 1 M/M/1 Output Process Burke s Theore:

More information

Chemical Physics II. More Stat. Thermo Kinetics Protein Folding...

Chemical Physics II. More Stat. Thermo Kinetics Protein Folding... Chmical Physics II Mor Stat. Thrmo Kintics Protin Folding... http://www.nmc.ctc.com/imags/projct/proj15thumb.jpg http://nuclarwaponarchiv.org/usa/tsts/ukgrabl2.jpg http://www.photolib.noaa.gov/corps/imags/big/corp1417.jpg

More information

5. Equation of state for high densities

5. Equation of state for high densities 5 1 5. Equation of stat for high dnsitis Equation of stat for high dnsitis 5 Vlocity distribution of lctrons Classical thrmodynamics: 6 dimnsional phas spac: (x,y,z,px,py,pz) momntum: p = p x+p y +p z

More information

Chapter 11 Solutions ( ) 1. The wavelength of the peak is. 2. The temperature is found with. 3. The power is. 4. a) The power is

Chapter 11 Solutions ( ) 1. The wavelength of the peak is. 2. The temperature is found with. 3. The power is. 4. a) The power is Chapt Solutios. Th wavlgth of th pak is pic 3.898 K T 3.898 K 373K 885 This cospods to ifad adiatio.. Th tpatu is foud with 3.898 K pic T 3 9.898 K 50 T T 5773K 3. Th pow is 4 4 ( 0 ) P σ A T T ( ) ( )

More information

Physics 302 Exam Find the curve that passes through endpoints (0,0) and (1,1) and minimizes 1

Physics 302 Exam Find the curve that passes through endpoints (0,0) and (1,1) and minimizes 1 Physis Exam 6. Fid th urv that passs through dpoits (, ad (, ad miimizs J [ y' y ]dx Solutio: Si th itgrad f dos ot dpd upo th variabl of itgratio x, w will us th sod form of Eulr s quatio: f f y' y' y

More information

Pair (and Triplet) Production Effect:

Pair (and Triplet) Production Effect: Pair (and riplt Production Effct: In both Pair and riplt production, a positron (anti-lctron and an lctron (or ngatron ar producd spontanously as a photon intracts with a strong lctric fild from ithr a

More information

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

Chapter Five. More Dimensions. is simply the set of all ordered n-tuples of real numbers x = ( x 1

Chapter Five. More Dimensions. is simply the set of all ordered n-tuples of real numbers x = ( x 1 Chatr Fiv Mor Dimsios 51 Th Sac R W ar ow rard to mov o to sacs of dimsio gratr tha thr Ths sacs ar a straightforward gralizatio of our Euclida sac of thr dimsios Lt b a ositiv itgr Th -dimsioal Euclida

More information

CHEM 305 Solutions for assignment #2

CHEM 305 Solutions for assignment #2 CHEM 05 Solutions for assignent #. (a) Starting fro C C show that C C Substitute the result into the original expression for C C : C C (b) Using the result fro (a), evaluate C C for an ideal gas. a. Both

More information

DFT: Discrete Fourier Transform

DFT: Discrete Fourier Transform : Discrt Fourir Trasform Cogruc (Itgr modulo m) I this sctio, all lttrs stad for itgrs. gcd m, = th gratst commo divisor of ad m Lt d = gcd(,m) All th liar combiatios r s m of ad m ar multils of d. a b

More information

Brief Introduction to Statistical Mechanics

Brief Introduction to Statistical Mechanics Brif Introduction to Statistical Mchanics. Purpos: Ths nots ar intndd to provid a vry quick introduction to Statistical Mchanics. Th fild is of cours far mor vast than could b containd in ths fw pags.

More information

The tight-binding method

The tight-binding method Th tight-idig thod Wa ottial aoach: tat lcto a a ga of aly f coductio lcto. ow aout iulato? ow aout d-lcto? d Tight-idig thod: gad a olid a a collctio of wa itactig utal ato. Ovla of atoic wav fuctio i

More information

Chapter 4: Exponential and Logarithmic Functions

Chapter 4: Exponential and Logarithmic Functions Erciss. 7 EXERCISES. Chatr : Eotial a Logarithmic Fuctios. a. c.. a. c. 7.89. a. 0.5 /.69 c. 5 5 + ( ). a. 5 5 5 5 5 + ( ) 5 c. + 0.086 0.050 /.96 5 ( ) + 5 + 6 + ( ) 5. 6. 7. 8. 9. 5.697 0. 0.9. a.. a.

More information

Physics of the Interstellar and Intergalactic Medium

Physics of the Interstellar and Intergalactic Medium PYA0 Sior Sophistr Physics of th Itrstllar ad Itrgalactic Mdium Lctur 7: II gios Dr Graham M. arpr School of Physics, TCD Follow-up radig for this ad t lctur Chaptr 5: Dyso ad Williams (lss dtaild) Chaptr

More information

Estimating the Variance in a Simulation Study of Balanced Two Stage Predictors of Realized Random Cluster Means Ed Stanek

Estimating the Variance in a Simulation Study of Balanced Two Stage Predictors of Realized Random Cluster Means Ed Stanek Etatg th Varac a Sulato Study of Balacd Two Stag Prdctor of Ralzd Rado Clutr Ma Ed Stak Itroducto W dcrb a pla to tat th varac copot a ulato tudy N ( µ µ W df th varac of th clutr paratr a ug th N ulatd

More information

Exam 2 Thursday (7:30-9pm) It will cover material through HW 7, but no material that was on the 1 st exam.

Exam 2 Thursday (7:30-9pm) It will cover material through HW 7, but no material that was on the 1 st exam. Exam 2 Thursday (7:30-9pm) It will covr matrial through HW 7, but no matrial that was on th 1 st xam. What happns if w bash atoms with lctrons? In atomic discharg lamps, lots of lctrons ar givn kintic

More information

Lecture Outline. Skin Depth Power Flow 8/7/2018. EE 4347 Applied Electromagnetics. Topic 3e

Lecture Outline. Skin Depth Power Flow 8/7/2018. EE 4347 Applied Electromagnetics. Topic 3e 8/7/018 Cours Instructor Dr. Raymond C. Rumpf Offic: A 337 Phon: (915) 747 6958 E Mail: rcrumpf@utp.du EE 4347 Applid Elctromagntics Topic 3 Skin Dpth & Powr Flow Skin Dpth Ths & Powr nots Flow may contain

More information

points Points <40. Results of. Final Exam. Grade C D,F C B

points 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 information

Spin(calori)tronics = spin+heat+electronics

Spin(calori)tronics = spin+heat+electronics Spi(calori)troic = pi+hat+lctroic Grrit aur Sdai 仙台 Populatio:.046 illio Grrit E.W. aur Grrit aur Tohoku Uivrity ( 東北 学 ) Udrgraduat,094 Potgraduat 7,704 itratioal tudt,346 ctur DC Magtolctroic i. dfiitio

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

CHAPTER 5 FREE ELECTRON THEORY

CHAPTER 5 FREE ELECTRON THEORY CHAPTER 5 REE ELECTRON THEORY r Elctron Thory Many solids conduct lctricity. Thr ar lctrons that ar not bound to atos but ar abl to ov through th whol crystal. Conducting solids fall into two ain classs;

More information

Davisson Germer experiment Announcements:

Davisson Germer experiment Announcements: Davisson Grmr xprimnt Announcmnts: Homwork st 7 is du Wdnsday. Problm solving sssions M3-5, T3-5. Th 2 nd midtrm will b April 7 in MUEN E0046 at 7:30pm. BFFs: Davisson and Grmr. Today w will go ovr th

More information

Chapter Taylor Theorem Revisited

Chapter Taylor Theorem Revisited Captr 0.07 Taylor Torm Rvisitd Atr radig tis captr, you sould b abl to. udrstad t basics o Taylor s torm,. writ trascdtal ad trigoomtric uctios as Taylor s polyomial,. us Taylor s torm to id t valus o

More information