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Thermal Physics 1: Thermodynamics and Statistical Mechanics, Lecture notes of Thermal Physics

Topics include: temperature and the zeroth law of thermodynamics, heat, work, internal energy, the first law, the Carnot cycle, the second law, entropy, the third law, thermodynamic potentials, derivation of thermodynamic relationships, introduction to phase transitions, kinetic theory of gases, introduction to statistical mechanics and the quantum ideal gas.

Typology: Lecture notes

2022/2023

Available from 06/28/2024

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Download Thermal Physics 1: Thermodynamics and Statistical Mechanics and more Lecture notes Thermal Physics in PDF only on Docsity! Therma Phyeics L. THEORY THERMODYNAMICS CHAPTER 1 e BAsic DERWirio~“g TD By: DEFICE THERNODY WamICS,., AS THE INVEsTIGATIO~ oF THE byw amical avd THERMAL PRoPEAr1 FS OF sopies, pEbucED En71 AREY PROM THE 197 ard 27° Lax oF THERMobyrAnice | wirro7 SPECULATION as TO THE Motpeviah coveriTuziew Sn DEScRIBES MaceoscoPic PROPERTIES OF sS7sTEMS - ris Ew TiRELy EMP AL Sie tavs oF THERRODYKAN IES om law a DEFWES TenPeraturRe T Bsc iw DEFINES ErERoy U a2 law a DERMES E~7ROPy S RD - Sa i: baw a GIVES MURERICAL VALYE TO ENTROPY BP epee EXCHANGE BE rWwEEW SYSTEA Ard sURROVH DI WGS Alves 4 OPEV $y7STEXR Slyes CLOSEn SYSTEr ise Qreaz) BxcHavGt perwEer systim Ard suRROUM DINGS “Aves a DilaTnERnar 57STRA “ive a ApIAbAric ()20L07ES) SYSTEM a VER/ 1SOLATED SYSTEM LEFF on 17S OWN wernt REACH AW Fai 1BRium STAZE LL LIDRIum <7ATE 5 SPEciFiBD By STATE VARIABLES fa A simple TD cycrérn REeavits orty 2 STATE VARIABLES Quire EQuitr BRIvM ft 4 i 1 Ko hish oe iS are Two TD cysTEMS ape w THERMAL conTAclh, Tuey wile ABACH THERMAL FevieiBRiUA ‘Tue ees Ae! pel THERES hywabied, a. TWO $ysrems ARE SEPARATELY in THERMAL EQUILIBRIUM wirn A TRD S¥87EM_ THEN THEY MUST ALSO BE IN 7uERMAL EQUILIBRIUM wir FACH OTHER Brus LAw_LEabs TO THE CovcEertT OF TEMPERATURE a T oF A SYSTEM 1s A BULK PHysieAr PRePERTY me i THERMAL EQ@viciBRium vary OwF swoTméR HAVE THE. € ME PERATURE SCALES a LInEAR VARIATION Ti Sat od a O = CONSTANT SAME TErrerarvRE T x 2 Senk PHrsicAu PROPERTx Blas THERMOMETER Bbosevnds GASES ar row T BEnAvE 1DeALLY Th vcrives OO units BETWEEN Ice Ard STFA Points y @ M.. USE FirrteR corstaer PRESssuRE Pon corsra-r vorvné 400 | wee Pre ssuas a i= lvelaavinne V. a S\= $7 £Acs= Pez too Be veuune a TEE pee Pe ieee rele Males Oo |= 6K 3 - 293 18% poe MrteT: TheW- 27545 Araime Tor oF HzO ie UMIQvE Por? AT Wier Sourd, LiQuid, AP GAS PrHAsES cobxit7 Bx. thazs.46 k © 10 lot °o a Pep Sand Na a ICE toler = 273.15K = 0.0°C me te Pome = 37315 k = 1900.0 °C * 3 poe (Or Werle eal re reed las Tin Vs 1293196. +) ee eC ca a 1 Lom poo CPV Yep Havana OF Stare Aree STATE oF A S7STEM Ar F@uniBRivm 1S Furry DETERM web By oust a FE _hacROScoPre VARLABLES. 4 STATE. FuNerionw a FuveTIOm THAT DEPENDS onty ow THE srare OF a System (vor om 17S HIS7eRY) Actes’ Pease RULE “Al ror A HOMOGENEOUS, OVE-comPorEn7 3xSTEM AT EQUILIBRIVA, oney Two s7are @ VARIABLES ARE REQUIRED TO PescriPE THE STATE Aa Ard REAL Gases MB joc. cas Law| Ek Pvt a RT Hel =\s. 344 2/ mol-k at $s | DER WAALS a (p+ eV elalhy dR we Dehavee w Ee@uriBRiun SsTaTes j Ar PROCESS 15 A TRAWSITIOM PROM THE LWITIAL STATE TP THE FUvar STATE “dtp PROCESS 15 DESCR\RED AS A PATH ET ISoBARic PRocEssS = CONS TAw7 — PRESSURE Bicocrore PRocess a COWMSTAKT ~— VOLUME Ab isortermac Process = SYSTED AT A ComSraw? TEMPERATURE Civead_cas| Pw %) NO HEAT rRAMSFER BETWEEN SYSTEM AMD SU FROUAPIN OS AbIABATICc PRoc Benn (~ IRREVERSIBLE PROCESS Theanvor BE sotvem BY SAME METHODS oF REVERSI DLE PRocEss @ WORK By Aw ELECTRic FIELD eee een A PARALLEL PLraTE CAPACITOR a A = PLATES AREA ‘4 bt SEPARAtion H V2 vours or covecé o> = EvreetRic DISPLACEMEns a P = Porapiearion =_PERMEZTIvIT7 OF VAcVU Be Recanve PeRmitrivity Tax, = EreeTRic SuseE P71Bie ITY Ap > OVERALL. ELECTRIC piPOrE nomenr WR el ec hetaie pe Mp-c, €,E MBrizte) xe 98 A, S/Vv|P “tw = Edp- BA mond bh pola ewe mecerere Bute BY aA _maceéric Filip Me ce A MAGNETIC MATERIAL BECOMING MAGMETIZED wirtin Soceworh We = _LEWGTH a = CRoss - seetionar AREA fs = NAGAE7IC [nbueTiow a Bo = imduerien tm ApsewcE oF MATERIAL 7] = _APPLiED FIELD “an MAGRETIZATION Mh. = _PERMFABILITY OF Vacuum i an = MAGHET IC SuUScEPrIBIUTY ww. = OVE RAw MR nar af + = 2 3. waslH+M) = BL + men 2 Cins x H Mp = we. Gx JH mart P= Vin fe t “dtw- Betis Ba vcen REQUIRED TO Pela a MAcrEric MATERIAL ThE CER ARA EL ei 3 Ere woRk REQUIRED To CHArGE Ar AblABAz Ic s¥S7F FROM ovE SPECI FeuLIiBRIun stare To Avprien Rains Beiue srAre lis THE SAME HOWEVER THE WORK Ss DOME, a AU =U, = U4 = War noarie er a lebepay ae SYSTEN 15 pOT THERMALLY 1SOLATED “Bau sur -v, = wre Ho: near 3 Pee E~TERS $78TEN a4 Qze ir we ee LEAVES SyS7EN a Qi -.E 4 Naess 16 THE EXCHANGE OF Er ERGY BETWEEN THE SYSTEM And THE SURRovmdin es THAT - -cenwet BE 1PE~7)FiEbD AS wolle a EMERGY OF THE SYSTER can GE IMC REASED iTmER RY ADDING HEAT wre THE SrsTeR maa eRe Nau: wee Bios sesrw | Bu = nat Hear @ Bear CAPACITY Weel darted (at Ar lo bp eae | atnchidha Vad cchsihae) redial eb teslnmtar veel pice mw. MPa doe lier Meise ae reamed phate y hs che trlad Vouulne Mic.. Miso oda Bil: -pdv Au = vlz,v) Bio=-4du+ pdv dui: (3) at ef p ely Mre-i(i)l a7. Ee (3), Jay S. Comstanr V SS. aVizlo @ Mio=(3)ar edu Mola (S)e Miu = fos a7 4 nor constanr V PROCESS Bove (Cea Mi dvijtclan 4 Sal | the) a Bi hk: vw eel Wivear GAS Wo =| VIG) mt) BL WA ic dtl acy ar @ Bitar capscary ar ComsTa nh? PRESSURE i ae ae ‘BouzuG.p) meee My =e) rs (320 1, Mite) ies (aa, do = dur piv har ccm: p ba ict ts Wra: (ea) drislpitz ] dir Mico irra tied, Beeruarey Me eps leer ee ets View Coy Ado Mas lcd °@ Mu susp Mdn-dus,pdv +vdp = datvd, Mi dui vosl=lclar io re o 4 Eo (=). dT + (el dp Bi MOT comTsTanT p | dh = Ceo dT + (2), dp ci en Foran 4 du eu Gas an Bye (ora ° Mduzcar Mausic har Bc arn Cp iw iDdpAL GASES me IE ak Bol Mo e: pulse). 4 Cp > Cv t+ mR Bue CAPACITY OF A SYSTEM (assecere) @ Mase: cur [an] a SPEQ\FI€ MovAR PEAT cAPAciTy Mit@ieles dn ilk! ja HEAT caPaci77Y PER Ke (Hee pede vapadiey) BM dalle aes ke gd iron A MOWwATOMIE cas aR * ‘ fp ssa t a Mc: 2 pea Move. icp = 2 pee move Qc, RYE CeY Be abiapene EXPArSi0~n OF \DEAL GAS 2 [Bto-o0 Milage lo clit till ° =) évdT + mlRtoe =o fic Ba 4 deel 20 az. (cea Bhima kh vl: od | Me: F Mirvac ay isch a, Werle lek saws he IDEAL Gas a Ys PA pisronie IDPAL GAs rth Weew 3 |THE LAW OF TD lata ENTROPy eo SEcovs LAW oF THERMobyNAMICS Mr iest raw (du: dal+ dw A FIRST LAw FOR C¥ctie process Mavic } ‘42 ow ier = lw = Mw za} a! By) =)4/- |S B.. ErGive OPERATING BE TWEE. (Two | RESERVOIRS Caw RE More EPFici Rr? —THAN~ A CARM OF Freire OPERAN rr 6 ow FE sAME RESERVOIRS =) A roe A REAL ENGINE a m-< ne a THER MODY KAA IC TE PERATURE Q at Pi beats Th i [ a | ee 7} aS | Me =| ot Qs Tr a EFFic.ewery n= a = ee gEeicipely | |= |t-) er FF 2) Wy pt raickndron Or Qz a5 - 2 . et + Wel = lag Fa >: ze - 4 MEAT Pump 3 B a) - Bee CYCLE Sole dk ae Le eet eee _ a PSS Se icoh Fe Igual 1Qer 2 halls los ele clol | Fiat = 1Qel + Iywt_ a ke air et a LQ Ty Bu ee —t ee i ae pS C4 fais |= Vag te Pr eed dR I as YL TN, a Mysto eS eee 2 Beas Gureodadia) | eh 3 as : pees Le P : pee es Be te eee ah ic ea Awl cLosED everk $ = \</o wine | THE BQvALiry NECESSAR My Hobs e ze FoR A REVERSI PLE cy eR _ ies ca etme sorte et ere ba z AW ear EXCAIANGE tH 3 RBobiks ee eee fete acy a 2! wer | ponies! (Ts, Te!) doup bory |CTe)| A. caRvoT peFRiertarons (A, 8), 4 prerre CE) Bao), eee ele NASI eee We eee eI HEAT Flowire TO AND sehees cod reser Qoa + Qop Bw wor Ww > (%, 4 Wp) 8 Avzo Bio.) + Oo,)-Q. > Ww - (wy + Wp) Uw < : 4 @ nt My Wi ol lzlol eo Ora Qon Te Qry av Be a> Fe S10 qo g. @ BS sce Te Te S001 51 Ma,, 0) | PAU Wwe auAUTy ale v ~ fake mp \F_ srBPs OF B ADEN AAR SMALL Awd Maw y Pett ot FoR REvERS: Bie Crees tou Boas |. Pe THEOREM We eo ladsletatads bbe da @ i \RREVERSIGLE PROCESS § f toe ree REVERSIBLE PRocEss =o “Ferory a Wide = 3@e Abo pees > REVERSIBLE process Bas [7s “AD proverries OF Er7Roly w S2-S1 i (7 1s A STATE FUKerionw ™” Umi Query DEFi rE FoR EVERY $7476 OF A sySTEN =D a AS 1s PATH In~DEPEWDENT (Bop A REVERSIDUE cy CLE DB eteory IX A CARWOT CYCLE all ISOTHERMAL ExPAXS 10x Aube dealer ay AdIABATIC ExPansionw Alsii= 1 Bese (Aso rurenar| comberssiow AS dE tory OR pamaparie Con Pressi ow ZV) Sa @ rt Sy oe WE ier levee JAS a Te | eo a) To Ruder (We rropy 1 A REVERS\OLE PROCESS e@ Mien ¢plar rr TF us - paeaes 1 c {las pha. i cy as mlep sdb tl Bhai Mais: bp ] Wheel Al peokess = HAT AbsoRBeD /RELRAStA BY S7STEN rROCESS “Tevrnopy (WM \anB VE RSIBLE CHAMGES Bt tio Ww: i = af | tel do Ay inr 8 mei se ‘Ae Ayrey 7 a eae {| 2a mi! IZ IAS = Sale Sa \4 Min S AS. dQ (Alas > = Bf plreopy lv Am 1SOLATED S7*7En iy. Ar (SevarEd s7stem , $ carror | pECREASE (wer EXTRoPy cHan~oeE zo) as 70° 8 IWcREASE iv 1RREVERSIBLE PROCESS AS =0 a COMSTAAT IN REVEASIDLD PROcESS [a As <¢o a InPOssiBLE , PROCESS Witt co te OPPOsiTE DikREcTION De abel OF _En7ROPY cup~r~ Ge Mol ete sate Gieinh Qu Mas te Se Berto CHAMGE (7 FREE EXPArsLor ff ag eis! ts, 2 fe L a REVERSIBLE |SOTHERRAL ExPArsio~ (vz = 2¥2) de = du + pay Mast & . 4) -slav 4 Misia Pe ete ie) vw = ZR = : | | DW isemone PROcE £3 Be vind iole ADA BAT IC Ghs =|0 i: = ConstTaneT WEEK a - Tbe Beeb a yataml PoreuriAls | Avd ue Maxweve RELATIoxs CEv7RAr Fevarionw OF} Tu eRH6 syvanie Ss BR elroy caw BE USE To Revisit 1" Law oF Tb Bi rieteiva oF ye du- dQi dw Tih coe REVERSIBLE CHArGES Maw: - pay Aso: tds WA diul-| tas + Pav Milras adult poy a FOUNDANExTAL Eavario~w oF TD bel tO dsl hal cledade | reese Bdo-tis -pav + rda 9 Mide= va, -sdt + eda Bit Constant p = | dGlzl=S$ dr it eda w- (4), = GE), M, tons rawr TT Blac ¢ Vdpl+ eda a(S), = GP), Feddsbebe ComDITIONS a PECHAMICS STABLE FQvieiBun 1s wee EQ = mini at TD Sysrenc Ted TO EOuunRiwn @ Mesias DEPEXPS or PourbARy combiner’ ees) alee Pe tee meeting (to ls peseabinpel a SIMCLE S¥Sren THERE 15 comPLET THERMO DIVAMIC EQVILIBRI vn See obs laa alacta ” 1S wor iwinAciy Ww A~ EQULIBRIUM STATE 4 1S Compurx @.. IRREVERS Pie PROCESS witn @ TAA-SFER USUALLY OCeURS WHF SySri TExDS Fo EQULIRRIUN Deeds SYSTEMS ExamPres 3 A, MULTI — PHASE SYSTEM Pee eal ek woe A SYSTEM AT CorsrarT Vi Coerberes wire a RESERVO.R ar To Beh ue IsoL are» Bae VY, To Ber eur oF Faun BRivm (commer) TW ecevore Te = Censrart a SysTEA T, V = cosracs BF avebeo a when) T= TS. Ge. ISOLATED COMBINED SYSTEM Q g Ba: 7O B DSc + ASnss % O a Ades ree, MHo- Tas, <0 a Av -T.e AS £@ Bo w-alzs) ¢o MPalu-ts) <0 [4 Ar, = OF <0 Jar co ma. CHarck Towarbt EQuiuintiun ner REDUCE Foye | Febs_1$ Eauivareer ye! mactmizinie | $1 4 Sines a. Mueri- conPoneer s7eTEn 4 CorcinER a SYSTEM AT comSTAn? Pin Con7ae7r wirh a RESERVOIR Ar To elas ror ar Eauiidaiun pe and Te MotrAsislo a AU = Q@- pe AV A nua pav- Tas £6 Pau + alpv) atts) £0 AY Alot py-ts) co [A aago Bacicio Ma, CHANGE TewaRrS Four iBRiun usr RERYCE Gs Mae a. Gry 18 | BOvivaceer po paximzire 1Ssy5 + Sass 4 MP atrdicladrolwe TO CHEnICA REACTIONS _ ee tee BR pad pot wit. PROCEED sPo~TanFausry iF AG <O Be Oubariow C lO. 14 16 O, | = 1G CO|+ CHO x | Bo : | Fe 2554) Pac == 2900 K) mel "| (sromtanrous) BP eho deletal | lected, eleho) | ld bl ol beol B este Se de 4 #0| KS bel" (Yer cpokbaeaie IS BF dg alul-ts tipv SW Ts | Ft pv bo ! s Pha = AH! = TAS x Bac = lan 4 Alpv) : Biehl ch hs BP aval bile Furero~ | =P Vas + as. > 0 Mas. sl | ale pile Bas. 2 ple Belt dslelo Wale h- ee aus o- pray a DU + po AV - To AS £0 ale AVAL CABIEITY A(S,Y, Po, Te) = V+ p¥-TeS Wala <o (spot Tale lut CHAMGES Iw A. ARE noe) Bas AT £Quict BRium «HERE SYSTEM Ard SURROUADIMGS APE AT EQviu BRUM i Pot pare Te = T @ DA-AG LO B- constant V ay 46 = AF ¢<o BTL de Week 5 - Hea CAPACITIES, JOULE An Joule Kevin ExPawsiow Hear CAPACITIES e* USEFUL MATH RE LATIONSHIPS Bie ACs. %, %) Owe aety 2 vaRABLRS ARB IAD EP DEAT Mx] kG 2) dy syle) Me = 2 (sy) Boy - ner: le p= /p(v,7) WW = vly7) Ar- rp, V) Wx: 2 (See MW ear Lenaclnes|. desarionsees ll wp ane ea spake @ Bc eee MS Woe Ey Mich cpa (oes as!) Ma ely gus Tas a... eR orem Pr a inoeraisl| Bete Bea (Sy Ms s(t Vv). Bogs: (ey dint (yay Wc, = cv +7 (3), (%), BCG: Ce) > cy +r (3%), (3) @ “ IsoPARic ExParSiiry as +) a He -comPerssipieity K=-Y¥ (%), a a aots estat 1 MW tocar lcs) CAPE SUS Ae e Pp Be ANd Cp VARIATIO~S wiTH Vv amd P 2s t aC Ea ees * ae BGS): Taal Solel x4) 3 ocx | awe/r = O FoR 4m Idea. cas Uc, sg: (ar A CW s karen S it =a) a 2p Dy SIOMEF OR Als hEALLGAS rane OF HEar CAPACITIES \ , Cote (arate = (Ap), CPAr). = (ov/ap), Bie ly sya st (assy ie Ca¥ 7 a7), QQv/ap)s a (= 8 Die rose nd ComPRESS pity Ky =~ Vv lip ie at (5) Wa asses COMPRESSIBILITY Ki Ss TV Mo ase Spake Cy - Ks Wri Pow? Typ 5 FAT wetien Au THREE Plases coex!sT Michi TEMPERATURE Tp, = APOVE \r, 1s0THERMAL Con PRESsion pRabucES wo SHAAP Ligvib- VaPovR TRAW Si TIOw eer Fuurp 9 Bre raic DREAM Ie ehonecl le METALLIC HYDROGEW Puasel | TRAMSiziows | 2 Be rou helud Te Wess AT Thee tHASES EL .t SYSTER COMTAIPING Two PHASES (5 KEPT A? core%anT P= Par And T= arenes BP eb tulad, ve wen G18 Ar fininun Ain sy |t Ma ‘4n = TetTac pass ; | cl: Magi tM ge Wicls|toral © lor me ssren © | Weise SYSTEN B dn Elder + dm lalo 4 dn, = - dz ~ = | War pet a dG = 02 9,dM,+ 4, dn, ed 41=g2 Weekes OF Two PHaSeS ww Fahad 1s THAT THEIR SPECPI€ GIBDS FuncTio~w ARE Eauay Me ae ot leaded a EQuarto~ Me ded G1 =-G2— Swoued DE_SarisriEh Fok 6VERY PotwT Op THE coExisTivce CURVE We elite Ak [nb |e ee lal BP rib lah rly May a) 4. (radr| psdp) = gel THdr, prde) 8 114.0) 2 5. )tdgs MO let ta dg Ws ay ia : = et Bor (eo Cel Gp et @( (202: ee WB dclelvas dor mes 4 MG, - 5.) 37 = (=v) de mie te | Dentrory CHAMYGE \¥ PHASE TRAYS ITION ) tQmy Godt Grey BL Con STAMT pp Tidhs A Te Gas: Ea Ban = au +pav = oH ff FUSiOw = f Chew ahi alie VAHL, AS pus = Mire. 4 Qapvaaele pet AH an a3 Side Bienes = Lawes e 4 Se asta Tete tai a EtAapsl= TAS nas 2P L L aw Bala SL ie(ve = V0) fs TA a Crausius ~ CLAPEYROX~ Favariow Be slece OF PHASE BouwbaRy 4 WIEGRATIOn OF CLAUSIUS - CLAPEYROr EQvATIOW Bon. A LLQUIB= VAPOUR TRAPSITION, ASSUME VAPOUR BEHAVES Ad Aw IDEAL GAS Wasa. THAT Var 2? Vira Baye Vee ee Ase: aan Diplelebsar une. a 42 (4): S bear (= - t) PHASE TRANSITION, 3 eee OF GIBBS Fuweriow in 1°" oRDER TRarSiTIoKs My (oD Sada ss clit : ‘ Bw. COrsSTarT p ake ” (52), =\=/5 ‘i a. 2 ° Pens g a) HAs weearive Stohr sf (3), ETS). = me <o° ie | Cp 20 Aways a gt) berds town 10 T Ams | THAT 15. STABLE a3 HiGHER T. HAS GkeareR S 2 a. constant T a =) V1 210 a a (p) LAS A POSTIVE SLOPE (33), = (le <o 4 gl) pews down Te rahe ibs 4 have Via Vel = pe = Beinsx ORDER PHASE TRArSITIONS A. CluanGE IM sheewrie GIBBS Furcrio~ r (colezmvers) | 1X SPECIFIC Volume V Bc nc tw srEeiFle ExTRopy § or ORDER. PHASE TRarsirions 2 Wc,': Plse lh m2 tl my 2-2 (3). “| AI< — > af eheee) (ur Te B eevreer CLASS\ FicATIOM OF PUASE TRArSITIO~S Gu. ORDER Sl DERIWATIVES of g WITH RESPECT TO Tard p me biscontmvous 2°? opPER PHASE 7TRersiT1Ons BB ieonees FRUATIO~“~S FOR moO sys 6G. : Tey eo cikvl Mier) = av Maes cls iat dr Cp2-- Cer av > Tv (ee -Bs) a PIRST EHREY FEST FavaTion a 2 - Ay mS r mats Ss SEco~p EMRE FEST EQvarionw Wee 2 - Twits raw of Ib Amd Kiwirie THEORY of GASES ABso. TE ENTROPY AND | 3" Law oF | THERMObY NAMICS FD iwreopy OF tbEAL Gas iE Mirds sau tpdv = Cvdt-+ pdy > Cvdt + ~ydyv Mas. co B+ Mav Ms 2 eek a nk bn v4 8 DB bsh eure eumory wire venrowe coms rane BD eariow OF ErtRoPy with TEMPERATURE S.- CowstT Aart p Wde, = dH d d d Mais |=| Ses Se ir fey May th earl Sin pA; Ab yap Mi Asielce C=) ae Ber rropy AnD PHASE CHANGES la S Uresxt Es Ab tews QS tows > Trrars Trans - — (Wevreory INCREASES AS Sorib — Liauib ™ GAs Baiscrare INCREASES with EMrROPy (PHASE SrADLE AT HIGHER T HAS HIGHER EX7RoPY) @ osscavarions FoR DIFFEREYT PHASES i Ran MOMATOMIC GASES SHowd DE EQ@varry DISORDERED AT SANE a EXCEPTIOw a TROVUTOM’S RULE |: HAVE SAME ~ DS var FOR MOBLE GASES AT THEIR Bowe Ports (85 tkmel? on 10.5R) | Caan DISTRIBUTION OF NorEcULAR SPEEDS f iy) BF eon Fim TESimAtcry SMALL iv TRRVALS amy? aT 34, @ Mya): ae Ga av: Os Wb atalirarwe, Comenepations dmlv) a Qi SS OF asl EB Sol lan | als | =. 00. (ea) We ie fle) + decemswo fle) WP eialid Sim FuKeTions 7? anf WeREASIMG Ar smart E. oy Oo Ie a dn(v) BE | DEcREASwe Ar raRee E ay eos daxtvs Sep aE : av. = AE @ = goat | daly? r -BY a t 2 epi et v7 le MAXWELL DISTRIBU rion vz00 va. per ith eek er NUMBER oF mMocscutes N = sl dn(v) = ), #v*e dv = avd 7 3 a = iia Wa = 4nn (Ge 2 Azizi dnlyy (= my? 4 sq SON 2 or i Ter ft Bovténanr Factor = Sc te Poisranurion Or MoOrEcuL AR SPEEDS Biassune WE CAr~ DEFINE SOME CrHAkAcTERIST Ie SPEED Vans @ PS Ale noveeues Wourd MevE witig Vans Aeoor Pear SsavaRE SPERD { By elie ee ee BR alecrct SPEED | vie ete) 2 | Wa: I. v a = Sep Wp 2 eae yer. [err Bivo = lim = Aer os; TRoDA pie sherD as Peerol ec 4 Pave ted RELAT LOM PeLrWwEE AM | Vin} of YP. mcd Vams BR vb: vn. Sl patel Sala S42 -4.13-5-1.22 Ve aL Grok al mpd i fhe ell del abe pa eto bede be tel | | | Kinetic MOLECULAR THEeRY OF GASES 2 BB ete Uae BY AN IDEAL GAS W,- $ p<v*? 3 Mv: tNm vi? > KT (ileal asl (al nicdoabapel blenune) Baka! FREE PATH >» Mi lect DISTAWEE TRAVELLED By A molBeutE fErwher 2 CowsBcurivE corrisians rear FREE mn Pea cleshe TIME BETWEEN Covvisions a As hyp Ble _ FREE Pate! kT i: Az dp a: DIAM AZER OF GAS MerecuLR e a 4 % AT Constant p AX~ > x GB. pie At 8,.-+ 8 a DULKIER NMorecure LEADS TO SuerTER DISTArCE BETWEEN Corrl Sio~s Beds. VAwWES oF Are bance e y = ae 3e +10 &.. Ts2e%c | awd Belt, ER > ite ae EG) te ey Faiernsront PRePERTIES OF GASES : Bi ceveic. Be raac lon fase (coerFiciexr Db) mL. TRAMSFER 4 TRarsporr OF Kiwerie Ewe RGY (coerricierr «) = BAe coche) a TRArSPORT OF birEAR MomEnrTUM eles nee 7 ) = | EAT CAPACITIES OF GASES We eerste gs Wc. .% Mic, = a | a, = ae = > 142 Ms 4 Mic) | Bc BS seal ee cuieaati mn oe OF ErEray ab a. Some = fi + my? dn(y)= = an v <v*> ZNwr |. A eles Mewerey EQuUIPARTITIOo~ THEOAEN st ra cu DEGREE or) FRaston! (V. Vv, \ve|,.|)-|-Polss bam comrAlbume Skt” yo (ue reac enERGy cr AS¥srEM G Way ee Rs x ‘4 Be Fa fll Bh m1 = DEGREES OF PREEDOM Pose ee Ne dad abemcbalel q — leet la 2 2 2) {4 EVERGY OF AW WwDIVIDYAL ATOM E=ymvt =z mlvitvi+vi e@ ie 3M DEGREES OF FREEDOR Pa rdral. yeimEric EXERGY oF N Arons 4 Biatomie MovEcuLe Me Ce lk + hoy ) aa Me el ket Pes Sm vit dk (eren) Wi visceelodal Morton BECOMES SiGwIFICEAMT OnLy Ar VERY HioH T a Porry Atomie nore cures (w ATons 1% A horecutc) @ ‘4 LIMEAR Orecuens = | By 7 5 vieranons ae LIMEAR MoLvecuL ES oy 3M > 6 vignarions \ Weex @ - Rear Gaees avs Iwrobucriow To Smristiae Mecrames REAL GASES Bo GAS el p= a RT Pe A CompRESs:o~ FACTOR Z = mk : p Von | By zl: 45 WA Vi rl laals sod arate “Aven WRAL GaASES., 2 = 1 Arwarys REAL GASES ‘a 23 a= raed “a Bact ff: As atpt 0 4 Tye Lal FOR HIGHER vatvct of 2 (Vn LARGER Tun. ik dss) 4 Zig FoR INTERMEDIATE (Von SraLeE A THEM BAL Gases) Wvievae EQuatior OF STATE Be sa Bie + Cpt... PY v2 nar (tse p scp...) Me, C, ++. ARE vita, COEFFICIENT ec avcinen The Slope OF 2 v3 p_ Pror (zcp vs p) dz he ME palate) 4 chp +) dab AS pO dz dz | ae GAS ap =o Shrew GAS a de12 |B) ib reoreenies OF REAL GaSES po wor ALWAYS COINCIDE WITH IbFAL GAS DEMAVIOUR EvEw AT Low Perssuar | | ee es Oe 4 packostares iene. op erassiear TD Ree KvMOWLEDGE OF MiCRosTATES 18 UMFASIBLR e Wl edoctcke Ape COMSIETEAT WITH A GivE™ mMAcROSTATE (carved acceSsiDLR Ff avarrizins ane fect) N, A... pate |pacRosrare THERe ank Usvarey | 2? 101° | accrscip ee michostAre APRS OF Fava. A_ PRIOR: PROBABIUNES .. ISOLATED. Sy STEA A Given MACROSTATE MAY BE Found Wirn Bau PRaBABILITY I ACY oF THE micRosrATES Altowkb &Y THAT MacRos TATE Bi aicncholia DEFIMITIOW OF FATROPY As =k gw Mw = crazertcar weigur Petar ISTICAL WE tGeir - © “tw: “an 2 yum BER oF OBaccTS iE | mt m= N mitnil i. = Opweerts tw stare 1 a! OBoEcTs ww Stare 2 a eee Hed a Murti MomaAr DISTRIBUTION = on, ehtest Im: shel 6's APPRoxim ATION TYAN! = New -N MM Jessaloh Iw STATISTICAL MECHANICS be Bub: AVERAGING. Coe tose Fi 4 Ake 2 Xo, 2 en {J X(v) de a InPessiBLe Iw PRACTICE Pi aleda dive By pisTai Buriew (exsenpie AvERAGiwe) LU g | OS = 2 ps Xe Bp. = PRoBaDIeinies Wer 9 - . Rowrznanm Dis7eiputiow | avs tHe Paesition BovtenAnm DistR Burien 4 STATISTICAL EWSEMBLES | 2 ©F nary coPlES oF THE S7S7EM), EACH In OWE OF THE MLOWED fiCROs7ATES bl ckodan orien. EVSErBe & a CLOSED SYSTEA wire, FixER EXERGY Wena ENSEMBLE 4 SYSTEM AT CorSTArnT TEAPERATVAE Bic, Caroricae ErSEnPte 4 OPEN $7S7TEM AT EQu LiPRIUM e PBnicaccmoneae evsennce. (VE ersenaie) Mae Eeoehe a COMPLETELY — 1S0LATED Mhussen Te Sew PrePamumes of STATfme dee re coms runs Breasewtea eastnme (ver tesenacs) e 2 Fixe N,v Tt Wainer OF PARMERES DFRAISED OF Bartnave MSR OUT! ow Wy preesunire @F A SPSTER Mines esha Predbabiure sre demon -= B.. = ie, S w.. > PARTIELES WW Srar€ wire, feeRer = E > BR arnt TMAT A PARrCCE vena BE Fourd w srare wim ErFAsr E TM =” RN Bae. ToPvLanes ~ E ¢ xr Bw Pepucarier - E> «Tr Os: DISTR BvTen Wo. DV mercEeveEs wire EERGIES Ey ann Es 4 PROSa mares Ps Ces) ane Pa (Ed) ee BY L cH Ce; Baa Paopamanty by Cert Fs) > Pile Pyles) = e€ er | B.. > TePaanen of Er€RGY revi ES . eS : Re I —- Ba a Mui = = wT DEGEMERATE fr S*Gy LEVERS ler = tea Ramen Fure toe ae vores Ee Gz: a si e Cae 2 TOT, PAR Nee Furcriem Wes OF YrearAuy ACCESSIDE ExRey LEVELS OF TLE whorE System at a Givew TT er eter 7 t z Mu 22 e = ate Wane) =. Wu -o. = kT ar]. Buu, (a= U-Ve treat = KTM ae ly tm RT Fo > -kt bn z Go 2 > kt kn 2 + WRT (=). wer Car St & sale xr CPF) aan (==) = Seon Sa dy + eT oa ly Paaetetae Fusextbw | le RT 'Tiow Furerior pu vevees A E+ 3 Ete 2 Tages el. fer] flodirbeks | Messe FActoR |= @ Fem eg | EL w.. Ey og) es sy 1 as EN Scie eae aeee led TF Eb i er <1 a avy POPULATED , (THERMALLY. Access! Me STATES is.) | Ey yr? 7 i Excited ENERGY Levers ARE MOT THERMALLY ACCESSI PLE i coake avd MorecuAR PApri tion | Fureriows | Ae TOTAL PARTITION Furctiow 2 in TERMS oF siwcer PARTICLES PARTINIew FuteTions 2 e We, > | EX Epa, LE VELs |OF A Siwock| paaricuk eal lede ae x eels eet E> LE Tora, For oas with norrtereRacrmng PARricL es mas Ei: | 2) &: Tera, _E— (For tremrienr paerrcers | im 7HE GAS Au REVELS OF ei? Nekevees, a = pees to}. eet grranv2 [| 4 Zi =1|4) Giese ys teT) a e. coe, é } | (az: ASB Ot 2 ES Jha Pr tek takelies Bale le T Na w (ele MpervRE For PaaticcES A AMD B_ iS eet a eee Ee 3 edn IMDISTIMGUISu ABLE PARTICLES a ZS le " a (Glee ian ame PARnCL eS b.e_ ei |) din tite aol oe Ne Ne Mal Mar IDEA Gas a” Gels et! Bees 4 Z|) Binate Zetad Me ee PAaRTitiow FurcTions | JADE Ie Mesias Gielen eee ns n 5 N A disrmoursuane PARTICES a Ze EL 2 eaaeale pret clan le etal z cE In Dist lw GulSHABE PARTICLES =| 2i=lMwy PRariti bk Fowedrlad | 9 2 Be arom PARTITIo~ FurcTionws (evectRonte PARTITION pees AS) K ey dedle Re pee = cai) t= = = r ea. vE_ POPULATION PS eet ie Bee ReTATIO~AL PAATITIO~ Furecrionw ez . Zee ae ° Thea 9 4 T= 1 FoR HETEROMYCLEAR DiATONIc MorECUES a. >t For HomonvercarR | FOR N Movecuces wa <r Be ie! ean) Me eee wie (Ge ur vt dn Zacr = Rt Rte feces Oy. TEMPERATURE ob Me.) a Foe, HiGu T | | T >? Oro, c a AEM cr Dros Oy. jth ce [tobelabuas Paantion Fuveriows 4 2 7 Bivisrarionad ENERGY LEVELS a 2 [ TM povenriay Ereney Vz 2k (t-te) a K = FORCE corstac? . 4 8 Ml F-Fe = DISPLACEMEXT From EQviiitRium poad ter etn te a HAR Meme OSerLcATOR APPROXIMATION 4 re SES Ee E(v) 2 he ® (vt 2) @ = viprarioma. wavemunser a v= vIBRATI On~aL QuaeTum MUmBER (v: Ort Eads ) Bel. Bavaccy spaced By he ® vic a £(o)|=|\s hea (zero porer ErFRay, zp.e.) |. ae OSci.caTok a LEvVErs MoT EQUAWY sPackb (purtrien ear BE monewen ) | Lé (b= be) 7% | e@ | Bv: dbel+-e ] Bo. 5 pissociatio~m EXERGY a VIBRATIorAL PARTITION Fuséerion MB atl de THE VIBRATION CAH BE APPROMmMarED AS AM HARMOAIE OSceL ATOR Mecpt ves iG ls) 2 Mo Eel ee) Mieled cl LEVELS ARE | MOr - DEGERERATE 4 = Mcleler) -letes os hev® MAG. =lvanew iepoeecheny, | gy e eee ee eee ec. hes) | ———————_ Na —]- = iW Ziseleat ZN) ic)..! al Kr (es ar}? | PO a — Nah a Se ae ear cael 2+ + Kr%_[e-sae 4 (.. PAS ee PaARTIMe& Furerior i host cases Pietra. Gis: af |. Fe FoR VERY low ErERGy exeitéb srazEs Were Fie Denys Hanh Wiksle bor wlll Quawrun | Sraig rics. Vauwity oF Bourenavw Distaipyzionw ed: ewsembre (eecare) | Wo Lee | a. SYSTEM Ar Cowstan? Te conpaer wir ren ae asernvore (NYT Erserme | FXED Nur) ProBABiLiTyY oF A SYS7EM In a $TArE mite ExERGr E —— | | Mau. oe bet F™ a PoPULAriow I @ p Ee | Ap: te “> eee | - waa Ahr veny tow T, RBOLTEMArn DISTRIBYTIO~ (. Dk) shislb on Vadan } H 4 ER D, ASSUMES crassicar BEHAVIOUR wirn po RESTRIcrIo~ oO Occ¥PATIO~ OF EwERGy LEVELS | | | tT a2) Ds VERY AccuRATE | WHE THE WUnBER oF Er€RGY SrATFS >> NUnBER OF PARTICLES yal } - t t Be. APPROACHER I CLASSICAL ard Quanristicar | | | Bolas. STATISTICS | | | | | ele On inpiviDU AL Qvarvn STATE | witicel cour DE coPiED By VARIOUS NUMBERS OF Te & ¢ bh = tes ae a if De BRocue Apn =P ia ion wes hl Eg aia Fenedes Smut 1 Nw aa rhte BeTWEEW taRTICLES a WO | | Bh ctireniow bon lerdsslemn eb Anaua_|-Nvul Sot 4 CLASSICAL IDEAL GAS Sy Hor Arb Diwv7e @ af avanrrur (OFAL GAS a coup AWD bDEWwsE BD eeniaet Abn pesons S| posors Mave wreerR she rumpees (01,2, Lo) babe lusvel sy nner ale wave rucerions a Feenion~g mAYE HACE - 1~TEGER SPie (172 4 3a, we) AMD AeTisyank TRie WArE Furenors ‘A BOSE-E\rS7Bir DistRiBUTIon FoR Boso~S He bs Bosow$ Ba: i ee DiRac DesraiByrier foR FEAMION~S Qe B... 2 pi 41 FERA Lor S @. FD Pisrarbyrier De ee waverurerion Y= (1) ¥o(2) ~ Yal2)%oar) Bo PUMBER OF PARTICLES otcupyhn eet | (lodevParom renner) We abek led esl eld codes Let |! Crecewenne,) a Paver Excevsier primeiPLe B ni <i ge Whe) cee) encece B. Cet fle) Fi? Kr a CrAssicAl DISTAIBUTIOR. ‘4 BOSE -EiwSrei~ DisrRiBeTiow @ a DeURM eae POTERTIAL | wreobueTiow To. QUAMTUM NiSTRiBUTION
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