Chapter 6 : Gibbs Free Energy

Size: px
Start display at page:

Download "Chapter 6 : Gibbs Free Energy"

Transcription

1 Wnter 01 Chem 54: ntrductry hermdynamcs Chapter 6 : Gbbs Free Energy Defntn f G, A Mawell Relatns Gbbs Free Energy G(,) (ure substances) Gbbs Free Energy fr Mtures ΔG f deal mng Chemcal Equlbrum and Equlbrum Cnstant K p emperature Dependence f K Chemcal Equlbrum: Calculatng Equlbrum Cmpstn rncple f LeChateler Use and Sgnfcance f ΔG, ΔA Chapter 6 : Gbbs Free Energy Defntn f G, A Fr sngle substances du q w Fr reversble prcess rev rev du q w du ds d (crrect relatn always) s nternal pressure f gas. du : epressed n term f functns f state,,, U, H, G, A Defne: H U A U S A arbet (wrk): Helmhltz free energy G H S U S G Gbbs free energy Dfferental frms: du ds d dh du d ds d d d ds d da du d S ds d ds Sd Sd d dg dh d S ds d ds Sd Sd d 64

2 Wnter 01 Chem 54: ntrductry hermdynamcs Fr eact dfferentals F F df d dy y y F F y y y y f true then F(, y ) ests U S H S A G S S ; ; ; ; U S H A G S U( S, ) H( S, ) A(, ) G(, ) Mawell Relatns U H A G S S S S S S 1 ; 1 Dervatns usng Mawell: du ds d ds du d 1 ds du d 1 U U ds d d d C 1 U A) ds d d Chapter 6 : Gbbs Free Energy 65

3 Wnter 01 Chem 54: ntrductry hermdynamcs B) S S ds d d S 1 U S U C S usng Mawell relatn OR U S S ds d d C ds d d C d d We have used all f these relatns wthut dervatn befre. A) B) dh ds d ds dh d dh ds d 1 H H ds d d d C 1 H ds d d S S ds d d S C S 1 H (Mawell) Chapter 6 : Gbbs Free Energy 66

4 Wnter 01 Chem 54: ntrductry hermdynamcs H C ds d d Gbbs Free Energy G(,) (ure substances) G ndependent f path, a functn f state, depends nly n, and, f f Changes n Changes n G wth dg Sd d G H S U S G Fr lquds and slds Fr (deal) gases G wth S G changes n and f G f G d d G nr f G nr ln f G f G d Sd f But S always depends n, nt cnvenent, use a trck G 1 G 1 G S 1 1 G S G H G S G 1 H Chapter 6 : Gbbs Free Energy 67

5 Wnter 01 Chem 54: ntrductry hermdynamcs f G f f G f H ( ) H d assume H( ) H( f ) (cnstant H, apprmatn) G f G 1 1 H f f G f G 1 1 H f f retend we have abslute Gbbs free energy, but n thermdynamcs ths s never the case. We always nly cnsder changes n G, H. Calculate G r, analgus t r H G f G r H r fund n tables alng wth abslute S rg r H f assumed t be cnstant (small errr) n real lfe yu need t knw (we wll d t n an eercse) G, dn t use ths frmula, use dependence f H. r Gbbs Free Energy fr Mtures We have varus speces: # f mles fr each: n1, n, n G G G dg d d dn n 1, n, n 1,, n n 1 Chapter 6 : Gbbs Free Energy 68

6 Wnter 01 Chem 54: ntrductry hermdynamcs G G dn n dn n,, n n,, n n dg Sd d dn dn dn dg Sd d dn G n,, n j n dn : the change n G when addng dn mles f speces, whle keep and, n j n cnstant. ( =chemcal ptental f speces and has unts kj/ml) Understand better fr pure substance, mlecule AG ( ), G naga, m (true because G s a functn f,, and, dn t change wth the sze f system) G na, G A, m ure substance A : mlar Gbbs free energy at partcular, A What s the physcal sgnfcance f? dg Sd dg dn dn dn d 1dn1 dn dg 1 mass balance dn dg 0 Always at cnstant, f dn 0 then 0 hases: Matter flws frm phase wth hgh chemcal ptental t phase wth lw chemcal ptental Analgy mlecules flw frm t, dn 0 Chemcal ptental strngly depends n cncentratn At equlbrum fr any speces lume changes (changng between phases) untl pressure s equal (equal ) Chapter 6 : Gbbs Free Energy 69

7 Wnter 01 Chem 54: ntrductry hermdynamcs Chemcal ptental s equal between dfferent cmpnents n a system: Fundamental prncple f chemcal equlbrum, at cnstant, Hw t calculate G fr mtures (deal mtures) deal mtures: deal gases, dlute slutn (n electrlyte), cmpnents d nt nteract substantally deal gas, pure cmpund, change f G(, f ) G(, ) nr ln nr dg d d f G nr ln G(, ) (, ) (, ) R ln n Lkewse fr an deal gas n a mture (artal ) ttal (, ) (, ) R ln ttal (, ) R ln ttal (, ) R ln R ln ttal Snce (, ) (, ) R ln (,, ) (, ) R ln ttal (,, ) (, ) R ln where (, ) s the chemcal ptental f the pure substance Chapter 6 : Gbbs Free Energy 70

8 Wnter 01 Chem 54: ntrductry hermdynamcs ΔG f deal mng G(, ) G, nr ln Fr pure substances Mtures ttal G(, ) G,, G, nr ln G, nr ln Mlar Gbbs free energy = chemcal ptental,,, (,, ), R ln G(,, ) G, nr ln G are chemcal ptentals fr pure substances (cnstant ) Eample at equlbrum H H pure m H, ln pure R H, ln m R H H pure m ln ln H H pure m tal pressure s dfferent n tw cmpartments! pure H m H ttal pure ttal m H m Ar Ar Chapter 6 : Gbbs Free Energy 71

9 Wnter 01 Chem 54: ntrductry hermdynamcs Eample m Ne G m G G n R ln G 0 ln Ne Ne Ar nne nttal Ne nar nttal Ar n R G Ar Ar Ne ln G n R ln R m ttal Ne Ne Ar Ar ln G n R ln general epressn fr mng Gm nttal R ln m ttal Ne Ne Ar Ar G Ar What s Calculate Sm? Smng 0 1; ln 0 lm ln always G m dg Sd d dn G S, n S m nr ln Sm nr ln S m 0 spntaneus drectly: f change : S nr ln at cnstant ttal ttal Sm nner ln nar R ln Nettal Arttal S n R ln ln m ttal Ne Ne Ar Ar Chapter 6 : Gbbs Free Energy 7

10 Wnter 01 Chem 54: ntrductry hermdynamcs Eample G n R ln 0 m ttal S nr ln 0 m Hm Gm Sm 0 (deal mes nly) G H S H G S G nr ln ln nr ln S n Rln ttal What abut? 1) G nr ln? ) G 0? Mlecules are ndstngushable n prncple. Gbbs parad? G 0, we knw. Gd understandng f ths nly frm Quantum Mechancs Chapter 6 : Gbbs Free Energy 7

11 Wnter 01 Chem 54: ntrductry hermdynamcs Chemcal Equlbrum and Equlbrum Cnstant K p Cnsder a generc reactn n the gas phase G r n A n B n C n D A ( g) B ( g) C ( g) D ( g) G n n n n r C C D D A A A B,, R ln G, r fr reactants; nfr prducts n rg, R ln rg, R ln rg rg R ln, pure substance at ; = prduct f all factrs, analgus t r f G G fr sums. Q Reactns Qutent: change durng a reactn, Q s an nstantaneus quantty Back t ntal reactn A B C D Q nc nd na nb C D A B Q nc C D A B nd na nb Chapter 6 : Gbbs Free Energy 74

12 Wnter 01 Chem 54: ntrductry hermdynamcs G G R lnq r r Rules: - f ntally 0 the reactn wll prceed t the rght, prduct CD, wll ncrease r G G r ncreases untl t s 0 - f ntally 0 reactn wll prceed t reactants, AB, ncreases r G At equlbrum Q Kequlbrum cnstant G G R ln K 0 r r emperature Dependence f K ln K rg R ln K 1 G 1 H R R r r f ln K f 1 r H d d R f rh f 1 ln K d R assume H s ndependent f r rh 1 1 ln K ( f ) ln K ( ) R f Eample: CO H O CO H ( g) ( l) ( g) ( g) Chapter 6 : Gbbs Free Energy 75

13 Wnter 01 Chem 54: ntrductry hermdynamcs R ln K G r n G ( CO ) n G ( H ) n G ( H O) n G ( CO) f f f f H H r f Q : gases nly, lquds and slds has lttle pressure dependence CO H CO at equlbrum Chemcal Equlbrum: Calculatng Equlbrum Cmpstn K ma A mb B mc C md D (reactants) m (prducts) m m : stchmetrc ceffcents (here) n : actual number f mles fr speces Can we calculate n fr each at chemcal equlbrum? Can we calculate r? Hw d we d t? Etent f reactn n n n beng the ntal number f mles fr mlecule Fr any value f yu get number f mles n wth mles f reactn Eample: N H NH Fr any mle f N that reacts, gan mles f NH and lse mles f H ntal # f mles has t be gven, n ths eample, we start wth mles f H, 1 mle f N and 0.1 mles f NH Chapter 6 : Gbbs Free Energy 76

14 Wnter 01 Chem 54: ntrductry hermdynamcs n n ma / mn N H mn NH mn 0.05 n.1 ttal Fr all n 0, fr all n n : (reactants) 0 ma n ma : (prducts) 0 mn n n dn d mn bunded dg Sd d dn at cnstant, dg dn d G, Fr spntaneus pssble prcess: ntally G dg G f rg,,, G r, d 0 0 Always d 0 : t the rght Chapter 6 : Gbbs Free Energy 77

15 Wnter 01 Chem 54: ntrductry hermdynamcs G f rg,, G f rg,, 0 0 d 0 : t the left chemcal equlbrum G, G r,, R ln, R ln G, R ln R ln r,, R ln, R ln G, R ln r rg, R ln G, R lnq r Q Q ; ( ) Chapter 6 : Gbbs Free Energy 78

16 Wnter 01 Chem 54: ntrductry hermdynamcs N H NH D n n 1 ttal Q Q Q NH N H Q 0 as 0.05 Q as mn mn rg, here s always precsely ne pnt at whch ln Q : chemcal equlbrum R ln Q : mathematcally ncreases between mn and ma Chapter 6 : Gbbs Free Energy 79

17 Wnter 01 Chem 54: ntrductry hermdynamcs rncple f LeChateler Easy t understand frm thermdynamcs: dln K Change n : H d R f H 0, K ncreases wth ncreasng prduct, requres heat (lwers ) f H 0, K decreases wth ncreasng reactant, requres heat (lwers ) K K K K K n gas ; K K ngas a) n gas 0 mre gas n prduct sde K decreases, reactn t the left decreases number f gas mlecules, reduces b) n gas 0, K ncreases, prducts ncreases n gas mles f gas decreases, decreases Chapter 6 : Gbbs Free Energy 80

18 Wnter 01 Chem 54: ntrductry hermdynamcs Use and Sgnfcance f ΔG, ΔA dq Clausus 0 rev q q 0 q ds 0 ds q du w du w ds 0 q rev ds Cnsder a cnstant prcess 0 ds d S ds Sd du d S w 0 d U S w A U S da w 0 w da Same reasnng fr G : epansn nn epansn nn epansn d U S w w d U S d w et cnstrant et cnstant nn epansn nn epansn d U S d w 0 d U S w 0 U S G dg w nn epansn Chapter 6 : Gbbs Free Energy 81

19 Wnter 01 Chem 54: ntrductry hermdynamcs Cmbustn f Octane: G = -596 kj/ml A = -585 kj/ml G A, s very small H = kj/ml Heat engne: heat frm burnng ctane cld ht wrk q heat H 1 w H Fuel cell: React ctane t generate electrcty nn Ma w G 0.98 H Mre effcent (knwn snce 1880!!) r 1 Chapter 6 : Gbbs Free Energy 8

_J _J J J J J J J J _. 7 particles in the blue state; 3 particles in the red state: 720 configurations _J J J _J J J J J J J J _

_J _J J J J J J J J _. 7 particles in the blue state; 3 particles in the red state: 720 configurations _J J J _J J J J J J J J _ Dsrder and Suppse I have 10 partcles that can be n ne f tw states ether the blue state r the red state. Hw many dfferent ways can we arrange thse partcles amng the states? All partcles n the blue state:

More information

Thermodynamics of Materials

Thermodynamics of Materials Thermdynamcs f Materals 14th Lecture 007. 4. 8 (Mnday) FUGACITY dg = Vd SdT dg = Vd at cnstant T Fr an deal gas dg = (RT/)d = RT dln Ths s true fr deal gases nly, but t wuld be nce t have a smlar frm fr

More information

Approach: (Equilibrium) TD analysis, i.e., conservation eqns., state equations Issues: how to deal with

Approach: (Equilibrium) TD analysis, i.e., conservation eqns., state equations Issues: how to deal with Schl f Aerspace Chemcal D: Mtvatn Prevus D Analyss cnsdered systems where cmpstn f flud was frzen fxed chemcal cmpstn Chemcally eactng Flw but there are numerus stuatns n prpulsn systems where chemcal

More information

(element) But, we do NOT know G!!! Correct, but not applicable! Free Energy Problems: o r. products. reactants. o f. reactants.

(element) But, we do NOT know G!!! Correct, but not applicable! Free Energy Problems: o r. products. reactants. o f. reactants. SANDARD fr hemcal Rxns prducts G p G reactants r But, we d NO knw G!!! rrect, but nt applcable! prducts G f G reactants f f (element) 0 f standard Gbbs free energy f frmatn Free Energy Prblems: 5. Prf.

More information

Chem 204A, Fall 2004, Mid-term (II)

Chem 204A, Fall 2004, Mid-term (II) Frst tw letters f yur last name Last ame Frst ame McGll ID Chem 204A, Fall 2004, Md-term (II) Read these nstructns carefully befre yu start tal me: 2 hurs 50 mnutes (6:05 PM 8:55 PM) 1. hs exam has ttal

More information

Physic 231 Lecture 33

Physic 231 Lecture 33 Physc 231 Lecture 33 Man pnts f tday s lecture: eat and heat capacty: Q cm Phase transtns and latent heat: Q Lm ( ) eat flw Q k 2 1 t L Examples f heat cnductvty, R values fr nsulatrs Cnvectn R L / k Radatn

More information

V. Electrostatics Lecture 27a: Diffuse charge at electrodes

V. Electrostatics Lecture 27a: Diffuse charge at electrodes V. Electrstatcs Lecture 27a: Dffuse charge at electrdes Ntes by MIT tudent We have talked abut the electrc duble structures and crrespndng mdels descrbng the n and ptental dstrbutn n the duble layer. Nw

More information

Lecture 12. Heat Exchangers. Heat Exchangers Chee 318 1

Lecture 12. Heat Exchangers. Heat Exchangers Chee 318 1 Lecture 2 Heat Exchangers Heat Exchangers Chee 38 Heat Exchangers A heat exchanger s used t exchange heat between tw fluds f dfferent temperatures whch are separated by a sld wall. Heat exchangers are

More information

Chapter 7. Systems 7.1 INTRODUCTION 7.2 MATHEMATICAL MODELING OF LIQUID LEVEL SYSTEMS. Steady State Flow. A. Bazoune

Chapter 7. Systems 7.1 INTRODUCTION 7.2 MATHEMATICAL MODELING OF LIQUID LEVEL SYSTEMS. Steady State Flow. A. Bazoune Chapter 7 Flud Systems and Thermal Systems 7.1 INTODUCTION A. Bazune A flud system uses ne r mre fluds t acheve ts purpse. Dampers and shck absrbers are eamples f flud systems because they depend n the

More information

Phys 344 Ch 5 Lect 4 Feb 28 th,

Phys 344 Ch 5 Lect 4 Feb 28 th, hys 44 Ch 5 Lect 4 Feb 8 th, 009 1 Wed /4 Fr /6 Mn /9 Wed /11 Fr / 1 55 Dlute Slutn 56 Chemcal Equlbrum Revew Exam (C 107 S 60, 61 Bltzmann Statstcs Bnus: hys Sr hess resentatns @ 4pm HW17: 7,76,8 HW18:8,84,86,88,89,91

More information

Chemical Equilibrium. Chapter 6 Spontaneity of Reactive Mixtures (gases) Taking into account there are many types of work that a sysem can perform

Chemical Equilibrium. Chapter 6 Spontaneity of Reactive Mixtures (gases) Taking into account there are many types of work that a sysem can perform Ths chapter deals wth chemcal reactons (system) wth lttle or no consderaton on the surroundngs. Chemcal Equlbrum Chapter 6 Spontanety of eactve Mxtures (gases) eactants generatng products would proceed

More information

( ) 1/ 2. ( P SO2 )( P O2 ) 1/ 2.

( ) 1/ 2. ( P SO2 )( P O2 ) 1/ 2. Chemstry 360 Dr. Jean M. Standard Problem Set 9 Solutons. The followng chemcal reacton converts sulfur doxde to sulfur troxde. SO ( g) + O ( g) SO 3 ( l). (a.) Wrte the expresson for K eq for ths reacton.

More information

Conduction Heat Transfer

Conduction Heat Transfer Cnductn Heat Transfer Practce prblems A steel ppe f cnductvty 5 W/m-K has nsde and utsde surface temperature f C and 6 C respectvely Fnd the heat flw rate per unt ppe length and flux per unt nsde and per

More information

CHEM Thermodynamics. Change in Gibbs Free Energy, G. Review. Gibbs Free Energy, G. Review

CHEM Thermodynamics. Change in Gibbs Free Energy, G. Review. Gibbs Free Energy, G. Review Review Accrding t the nd law f Thermdynamics, a prcess is spntaneus if S universe = S system + S surrundings > 0 Even thugh S system

More information

University of Washington Department of Chemistry Chemistry 452/456 Summer Quarter 2014

University of Washington Department of Chemistry Chemistry 452/456 Summer Quarter 2014 Lecture 12 7/25/14 ERD: 7.1-7.5 Devoe: 8.1.1-8.1.2, 8.2.1-8.2.3, 8.4.1-8.4.3 Unversty o Washngton Department o Chemstry Chemstry 452/456 Summer Quarter 2014 A. Free Energy and Changes n Composton: The

More information

Chemistry 1A Fall 2000

Chemistry 1A Fall 2000 Chemistry 1A Fall 2000 Midterm Exam III, versin B Nvember 14, 2000 (Clsed bk, 90 minutes, 155 pints) Name: SID: Sectin Number: T.A. Name: Exam infrmatin, extra directins, and useful hints t maximize yur

More information

Chapter 17: Thermodynamics: Spontaneous and Nonspontaneous Reactions and Processes

Chapter 17: Thermodynamics: Spontaneous and Nonspontaneous Reactions and Processes Chapter 17: hermdynamics: Spntaneus and Nnspntaneus Reactins and Prcesses Learning Objectives 17.1: Spntaneus Prcesses Cmparing and Cntrasting the hree Laws f hermdynamics (1 st Law: Chap. 5; 2 nd & 3

More information

AP CHEMISTRY CHAPTER 6 NOTES THERMOCHEMISTRY

AP CHEMISTRY CHAPTER 6 NOTES THERMOCHEMISTRY AP CHEMISTRY CHAPTER 6 NOTES THERMOCHEMISTRY Energy- the capacity t d wrk r t prduce heat 1 st Law f Thermdynamics: Law f Cnservatin f Energy- energy can be cnverted frm ne frm t anther but it can be neither

More information

Chapter 17 Free Energy and Thermodynamics

Chapter 17 Free Energy and Thermodynamics Chemistry: A Mlecular Apprach, 1 st Ed. Nivald Tr Chapter 17 Free Energy and Thermdynamics Ry Kennedy Massachusetts Bay Cmmunity Cllege Wellesley Hills, MA 2008, Prentice Hall First Law f Thermdynamics

More information

15-69C Under the conditions of complete combustion with stoichiometric amount of air.

15-69C Under the conditions of complete combustion with stoichiometric amount of air. 15-43 Adabatc Flame emperature 15-68C Fr the case f stchmetrc amunt f pure xy snce we have the same amunt f chemcal energy released but a smaller amunt f mass t absrb t. 15-69C Under the cndtns f cmplete

More information

Part One: Heat Changes and Thermochemistry. This aspect of Thermodynamics was dealt with in Chapter 6. (Review)

Part One: Heat Changes and Thermochemistry. This aspect of Thermodynamics was dealt with in Chapter 6. (Review) CHAPTER 18: THERMODYNAMICS AND EQUILIBRIUM Part One: Heat Changes and Thermchemistry This aspect f Thermdynamics was dealt with in Chapter 6. (Review) A. Statement f First Law. (Sectin 18.1) 1. U ttal

More information

Find this material useful? You can help our team to keep this site up and bring you even more content consider donating via the link on our site.

Find this material useful? You can help our team to keep this site up and bring you even more content consider donating via the link on our site. Find this material useful? Yu can help ur team t keep this site up and bring yu even mre cntent cnsider dnating via the link n ur site. Still having truble understanding the material? Check ut ur Tutring

More information

Gibbs-Duhem Equation

Gibbs-Duhem Equation Gbbs-Duhem Equtn rvdes reltnshp (cnstrnt) between prtl mlr prpertes es f dfferent speces n mture. V V (,, n, n,... n,... n m ) dv V d V d m V n, n n,,, n j j dn dv At cnstnt nd : m V n,, n j j dn ut: dv

More information

...Thermodynamics. If Clausius Clapeyron fails. l T (v 2 v 1 ) = 0/0 Second order phase transition ( S, v = 0)

...Thermodynamics. If Clausius Clapeyron fails. l T (v 2 v 1 ) = 0/0 Second order phase transition ( S, v = 0) If Clausus Clapeyron fals ( ) dp dt pb =...Thermodynamcs l T (v 2 v 1 ) = 0/0 Second order phase transton ( S, v = 0) ( ) dp = c P,1 c P,2 dt Tv(β 1 β 2 ) Two phases ntermngled Ferromagnet (Excess spn-up

More information

Transient Conduction: Spatial Effects and the Role of Analytical Solutions

Transient Conduction: Spatial Effects and the Role of Analytical Solutions Transent Cnductn: Spatal Effects and the Rle f Analytcal Slutns Slutn t the Heat Equatn fr a Plane Wall wth Symmetrcal Cnvectn Cndtns If the lumped capactance apprxmatn can nt be made, cnsderatn must be

More information

Spring 2002 Lecture #17

Spring 2002 Lecture #17 1443-51 Sprng 22 Lecture #17 r. Jaehn Yu 1. Cndtns fr Equlbrum 2. Center f Gravty 3. Elastc Prpertes f Slds Yung s dulus Shear dulus ulk dulus Tday s Hmewrk Assgnment s the Hmewrk #8!!! 2 nd term eam n

More information

Thermodynamics Partial Outline of Topics

Thermodynamics Partial Outline of Topics Thermdynamics Partial Outline f Tpics I. The secnd law f thermdynamics addresses the issue f spntaneity and invlves a functin called entrpy (S): If a prcess is spntaneus, then Suniverse > 0 (2 nd Law!)

More information

TEST 5 (phy 240) 2. Show that the volume coefficient of thermal expansion for an ideal gas at constant pressure is temperature dependent and given by

TEST 5 (phy 240) 2. Show that the volume coefficient of thermal expansion for an ideal gas at constant pressure is temperature dependent and given by ES 5 (phy 40). a) Wrte the zeroth law o thermodynamcs. b) What s thermal conductvty? c) Identyng all es, draw schematcally a P dagram o the arnot cycle. d) What s the ecency o an engne and what s the coecent

More information

Advanced Chemistry Practice Problems

Advanced Chemistry Practice Problems Advanced Chemistry Practice Prblems Thermdynamics: Gibbs Free Energy 1. Questin: Is the reactin spntaneus when ΔG < 0? ΔG > 0? Answer: The reactin is spntaneus when ΔG < 0. 2. Questin: Fr a reactin with

More information

Thermodynamics Second Law Entropy

Thermodynamics Second Law Entropy Thermodynamcs Second Law Entropy Lana Sherdan De Anza College May 8, 2018 Last tme the Boltzmann dstrbuton (dstrbuton of energes) the Maxwell-Boltzmann dstrbuton (dstrbuton of speeds) the Second Law of

More information

ALE 21. Gibbs Free Energy. At what temperature does the spontaneity of a reaction change?

ALE 21. Gibbs Free Energy. At what temperature does the spontaneity of a reaction change? Name Chem 163 Sectin: Team Number: ALE 21. Gibbs Free Energy (Reference: 20.3 Silberberg 5 th editin) At what temperature des the spntaneity f a reactin change? The Mdel: The Definitin f Free Energy S

More information

Lecture 12: Chemical reaction equilibria

Lecture 12: Chemical reaction equilibria 3.012 Fundamentals f Materials Science Fall 2005 Lecture 12: 10.19.05 Chemical reactin equilibria Tday: LAST TIME...2 EQUATING CHEMICAL POTENTIALS DURING REACTIONS...3 The extent f reactin...3 The simplest

More information

Design of Analog Integrated Circuits

Design of Analog Integrated Circuits Desgn f Analg Integrated Crcuts I. Amplfers Desgn f Analg Integrated Crcuts Fall 2012, Dr. Guxng Wang 1 Oerew Basc MOS amplfer structures Cmmn-Surce Amplfer Surce Fllwer Cmmn-Gate Amplfer Desgn f Analg

More information

CIRCLE YOUR DIVISION: Div. 1 (9:30 am) Div. 2 (11:30 am) Div. 3 (2:30 pm) Prof. Ruan Prof. Naik Mr. Singh

CIRCLE YOUR DIVISION: Div. 1 (9:30 am) Div. 2 (11:30 am) Div. 3 (2:30 pm) Prof. Ruan Prof. Naik Mr. Singh Frst CIRCLE YOUR DIVISION: Dv. 1 (9:30 am) Dv. (11:30 am) Dv. 3 (:30 m) Prf. Ruan Prf. Na Mr. Sngh Schl f Mechancal Engneerng Purdue Unversty ME315 Heat and Mass ransfer Eam #3 Wednesday Nvember 17 010

More information

Entropy, Free Energy, and Equilibrium

Entropy, Free Energy, and Equilibrium Nv. 26 Chapter 19 Chemical Thermdynamics Entrpy, Free Energy, and Equilibrium Nv. 26 Spntaneus Physical and Chemical Prcesses Thermdynamics: cncerned with the questin: can a reactin ccur? A waterfall runs

More information

Thermodynamics and Equilibrium

Thermodynamics and Equilibrium Thermdynamics and Equilibrium Thermdynamics Thermdynamics is the study f the relatinship between heat and ther frms f energy in a chemical r physical prcess. We intrduced the thermdynamic prperty f enthalpy,

More information

NAME and Section No. it is found that 0.6 mol of O

NAME and Section No. it is found that 0.6 mol of O NAME and Secton No. Chemstry 391 Fall 7 Exam III KEY 1. (3 Ponts) ***Do 5 out of 6***(If 6 are done only the frst 5 wll be graded)*** a). In the reacton 3O O3 t s found that.6 mol of O are consumed. Fnd

More information

Unit 14 Thermochemistry Notes

Unit 14 Thermochemistry Notes Name KEY Perid CRHS Academic Chemistry Unit 14 Thermchemistry Ntes Quiz Date Exam Date Lab Dates Ntes, Hmewrk, Exam Reviews and Their KEYS lcated n CRHS Academic Chemistry Website: https://cincchem.pbwrks.cm

More information

Thermochemistry. Thermochemistry

Thermochemistry. Thermochemistry Thermchemistry Petrucci, Harwd and Herring: Chapter 7 CHEM 1000A 3.0 Thermchemistry 1 Thermchemistry The study energy in chemical reactins A sub-discipline thermdynamics Thermdynamics studies the bulk

More information

Lucas Imperfect Information Model

Lucas Imperfect Information Model Lucas Imerfect Infrmatn Mdel 93 Lucas Imerfect Infrmatn Mdel The Lucas mdel was the frst f the mdern, mcrfundatns mdels f aggregate suly and macrecnmcs It bult drectly n the Fredman-Phels analyss f the

More information

BME 5742 Biosystems Modeling and Control

BME 5742 Biosystems Modeling and Control BME 5742 Bsystems Mdeln and Cntrl Cell Electrcal Actvty: In Mvement acrss Cell Membrane and Membrane Ptental Dr. Zv Rth (FAU) 1 References Hppensteadt-Peskn, Ch. 3 Dr. Rbert Farley s lecture ntes Inc Equlbra

More information

CinChE Problem-Solving Strategy Chapter 4 Development of a Mathematical Model. formulation. procedure

CinChE Problem-Solving Strategy Chapter 4 Development of a Mathematical Model. formulation. procedure nhe roblem-solvng Strategy hapter 4 Transformaton rocess onceptual Model formulaton procedure Mathematcal Model The mathematcal model s an abstracton that represents the engneerng phenomena occurrng n

More information

Chem 112, Fall 05 (Weis/Garman) Exam 4A, December 14, 2005 (Print Clearly) +2 points

Chem 112, Fall 05 (Weis/Garman) Exam 4A, December 14, 2005 (Print Clearly) +2 points +2 pints Befre yu begin, make sure that yur exam has all 7 pages. There are 14 required prblems (7 pints each) and tw extra credit prblems (5 pints each). Stay fcused, stay calm. Wrk steadily thrugh yur

More information

Find this material useful? You can help our team to keep this site up and bring you even more content consider donating via the link on our site.

Find this material useful? You can help our team to keep this site up and bring you even more content consider donating via the link on our site. Find this material useful? Yu can help ur team t keep this site up and bring yu even mre cntent cnsider dnating via the link n ur site. Still having truble understanding the material? Check ut ur Tutring

More information

V T for n & P = constant

V T for n & P = constant Pchem 365: hermodynamcs -SUMMARY- Uwe Burghaus, Fargo, 5 9 Mnmum requrements for underneath of your pllow. However, wrte your own summary! You need to know the story behnd the equatons : Pressure : olume

More information

Chemistry 163B Free Energy and Equilibrium E&R ( ch 6)

Chemistry 163B Free Energy and Equilibrium E&R ( ch 6) Chemstry 163B Free Energy and Equlbrum E&R ( ch 6) 1 ΔG reacton and equlbrum (frst pass) 1. ΔG < spontaneous ( natural, rreversble) ΔG = equlbrum (reversble) ΔG > spontaneous n reverse drecton. ΔG = ΔHΔS

More information

Solutions to the Extra Problems for Chapter 14

Solutions to the Extra Problems for Chapter 14 Slutins t the Extra Prblems r Chapter 1 1. The H -670. T use bnd energies, we have t igure ut what bnds are being brken and what bnds are being made, s we need t make Lewis structures r everything: + +

More information

Edexcel IGCSE Chemistry. Topic 1: Principles of chemistry. Chemical formulae, equations and calculations. Notes.

Edexcel IGCSE Chemistry. Topic 1: Principles of chemistry. Chemical formulae, equations and calculations. Notes. Edexcel IGCSE Chemistry Tpic 1: Principles f chemistry Chemical frmulae, equatins and calculatins Ntes 1.25 write wrd equatins and balanced chemical equatins (including state symbls): fr reactins studied

More information

6. ELUTRIATION OF PARTICLES FROM FLUIDIZED BEDS

6. ELUTRIATION OF PARTICLES FROM FLUIDIZED BEDS 6. ELUTRIATION OF PARTICLES FROM FLUIDIZED BEDS Elutratn s the prcess n whch fne partcles are carred ut f a fludzed bed due t the flud flw rate passng thrugh the bed. Typcally, fne partcles are elutrated

More information

CTN 2/23/16. EE 247B/ME 218: Introduction to MEMS Design Lecture 11m2: Mechanics of Materials. Copyright 2016 Regents of the University of California

CTN 2/23/16. EE 247B/ME 218: Introduction to MEMS Design Lecture 11m2: Mechanics of Materials. Copyright 2016 Regents of the University of California Vlume Change fr a Unaxal Stress Istrpc lastcty n 3D Istrpc = same n all drectns The cmplete stress-stran relatns fr an strpc elastc Stresses actng n a dfferental vlume element sld n 3D: (.e., a generalzed

More information

Chapters 29 and 35 Thermochemistry and Chemical Thermodynamics

Chapters 29 and 35 Thermochemistry and Chemical Thermodynamics Chapters 9 and 35 Thermchemistry and Chemical Thermdynamics 1 Cpyright (c) 011 by Michael A. Janusa, PhD. All rights reserved. Thermchemistry Thermchemistry is the study f the energy effects that accmpany

More information

Chapter 3, Solution 1C.

Chapter 3, Solution 1C. COSMOS: Cmplete Onlne Slutns Manual Organzatn System Chapter 3, Slutn C. (a If the lateral surfaces f the rd are nsulated, the heat transfer surface area f the cylndrcal rd s the bttm r the tp surface

More information

Higher. Specimen NAB Assessment

Higher. Specimen NAB Assessment hsn.uk.net Higher Mathematics UNIT Specimen NAB Assessment HSN50 This dcument was prduced speciall fr the HSN.uk.net website, and we require that an cpies r derivative wrks attribute the wrk t Higher Still

More information

Open Systems: Chemical Potential and Partial Molar Quantities Chemical Potential

Open Systems: Chemical Potential and Partial Molar Quantities Chemical Potential Open Systems: Chemcal Potental and Partal Molar Quanttes Chemcal Potental For closed systems, we have derved the followng relatonshps: du = TdS pdv dh = TdS + Vdp da = SdT pdv dg = VdP SdT For open systems,

More information

Introduction to Statistical Methods

Introduction to Statistical Methods Introducton to Statstcal Methods Physcs 4362, Lecture #3 hermodynamcs Classcal Statstcal Knetc heory Classcal hermodynamcs Macroscopc approach General propertes of the system Macroscopc varables 1 hermodynamc

More information

Analysis The characteristic length of the junction and the Biot number are

Analysis The characteristic length of the junction and the Biot number are -4 4 The temerature f a gas stream s t be measured by a thermule. The tme t taes t regster 99 erent f the ntal ΔT s t be determned. Assumtns The juntn s sheral n shae wth a dameter f D 0.00 m. The thermal

More information

A Chemical Reaction occurs when the of a substance changes.

A Chemical Reaction occurs when the of a substance changes. Perid: Unit 8 Chemical Reactin- Guided Ntes Chemical Reactins A Chemical Reactin ccurs when the f a substance changes. Chemical Reactin: ne r mre substances are changed int ne r mre new substances by the

More information

A brief overview of the principles of thermobarometry Cin-Ty Lee (2009)

A brief overview of the principles of thermobarometry Cin-Ty Lee (2009) A bref vervew f the prncples f thermbarmetry Cn-y Lee (2009) Hmgeneus tem Fr a ne phase tem (hmgeneus tem) characterzed by a fxed cmpstn, the state varable knwn as Gbbs Free energy G s defned as fllws:

More information

Review of Classical Thermodynamics

Review of Classical Thermodynamics Revew of Classcal hermodynamcs Physcs 4362, Lecture #1, 2 Syllabus What s hermodynamcs? 1 [A law] s more mpressve the greater the smplcty of ts premses, the more dfferent are the knds of thngs t relates,

More information

Types of Energy COMMON MISCONCEPTIONS CHEMICAL REACTIONS INVOLVE ENERGY

Types of Energy COMMON MISCONCEPTIONS CHEMICAL REACTIONS INVOLVE ENERGY CHEMICAL REACTIONS INVOLVE ENERGY The study energy and its transrmatins is knwn as thermdynamics. The discussin thermdynamics invlve the cncepts energy, wrk, and heat. Types Energy Ptential energy is stred

More information

How can standard heats of formation be used to calculate the heat of a reaction?

How can standard heats of formation be used to calculate the heat of a reaction? Name Chem 161, Sectin: Grup Number: ALE 28. Hess s Law and Standard Enthalpies Frmatin (Reerence: Chapter 6 - Silberberg 5 th editin) Imprtant!! Fr answers that invlve a calculatin yu must shw yur wrk

More information

Chapter Outline 4/28/2014. P-V Work. P-V Work. Isolated, Closed and Open Systems. Exothermic and Endothermic Processes. E = q + w

Chapter Outline 4/28/2014. P-V Work. P-V Work. Isolated, Closed and Open Systems. Exothermic and Endothermic Processes. E = q + w Islated, Clsed and Open Systems 9.1 Energy as a Reactant r a Prduct 9.2 Transferring Heat and Ding Wrk 9.5 Heats f Reactin and Calrimetry 9.6 Hess s Law and Standard Heats f Reactin 9.7 Heats f Reactin

More information

Chemical Equilibrium

Chemical Equilibrium 0.110/5.60 Fall 005 Lecture #10 age 1 Chemical Equilibrium Ideal Gases Questin: What is the cmsitin f a reacting miture f ideal gases? e.g. ½ N (g, T, ) + 3/ H (g, T, ) = NH 3 (g, T, ) What are N,, and

More information

How can standard heats of formation be used to calculate the heat of a reaction?

How can standard heats of formation be used to calculate the heat of a reaction? Answer Key ALE 28. ess s Law and Standard Enthalpies Frmatin (Reerence: Chapter 6 - Silberberg 4 th editin) Imprtant!! Fr answers that invlve a calculatin yu must shw yur wrk neatly using dimensinal analysis

More information

Feedback Principle :-

Feedback Principle :- Feedback Prncple : Feedback amplfer s that n whch a part f the utput f the basc amplfer s returned back t the nput termnal and mxed up wth the nternal nput sgnal. The sub netwrks f feedback amplfer are:

More information

3. Be able to derive the chemical equilibrium constants from statistical mechanics.

3. Be able to derive the chemical equilibrium constants from statistical mechanics. Lecture #17 1 Lecture 17 Objectves: 1. Notaton of chemcal reactons 2. General equlbrum 3. Be able to derve the chemcal equlbrum constants from statstcal mechancs. 4. Identfy how nondeal behavor can be

More information

A quote of the week (or camel of the week): There is no expedience to which a man will not go to avoid the labor of thinking. Thomas A.

A quote of the week (or camel of the week): There is no expedience to which a man will not go to avoid the labor of thinking. Thomas A. A quote of the week (or camel of the week): here s no expedence to whch a man wll not go to avod the labor of thnkng. homas A. Edson Hess law. Algorthm S Select a reacton, possbly contanng specfc compounds

More information

between standard Gibbs free energies of formation for products and reactants, ΔG! R = ν i ΔG f,i, we

between standard Gibbs free energies of formation for products and reactants, ΔG! R = ν i ΔG f,i, we hermodynamcs, Statstcal hermodynamcs, and Knetcs 4 th Edton,. Engel & P. ed Ch. 6 Part Answers to Selected Problems Q6.. Q6.4. If ξ =0. mole at equlbrum, the reacton s not ery far along. hus, there would

More information

Circuits Op-Amp. Interaction of Circuit Elements. Quick Check How does closing the switch affect V o and I o?

Circuits Op-Amp. Interaction of Circuit Elements. Quick Check How does closing the switch affect V o and I o? Crcuts Op-Amp ENGG1015 1 st Semester, 01 Interactn f Crcut Elements Crcut desgn s cmplcated by nteractns amng the elements. Addng an element changes vltages & currents thrughut crcut. Example: clsng a

More information

A New Method for Solving Integer Linear. Programming Problems with Fuzzy Variables

A New Method for Solving Integer Linear. Programming Problems with Fuzzy Variables Appled Mathematcal Scences, Vl. 4, 00, n. 0, 997-004 A New Methd fr Slvng Integer Lnear Prgrammng Prblems wth Fuzzy Varables P. Pandan and M. Jayalakshm Department f Mathematcs, Schl f Advanced Scences,

More information

55:041 Electronic Circuits

55:041 Electronic Circuits 55:04 Electrnc Crcuts Feedback & Stablty Sectns f Chapter 2. Kruger Feedback & Stablty Cnfguratn f Feedback mplfer S S S S fb Negate feedback S S S fb S S S S S β s the feedback transfer functn Implct

More information

More Tutorial at

More Tutorial at Answer each questin in the space prvided; use back f page if extra space is needed. Answer questins s the grader can READILY understand yur wrk; nly wrk n the exam sheet will be cnsidered. Write answers,

More information

CHAPTER Read Chapter 17, sections 1,2,3. End of Chapter problems: 25

CHAPTER Read Chapter 17, sections 1,2,3. End of Chapter problems: 25 CHAPTER 17 1. Read Chapter 17, sectins 1,2,3. End f Chapter prblems: 25 2. Suppse yu are playing a game that uses tw dice. If yu cunt the dts n the dice, yu culd have anywhere frm 2 t 12. The ways f prducing

More information

CHEM 1032 FALL 2017 Practice Exam 4 1. Which of the following reactions is spontaneous under normal and standard conditions?

CHEM 1032 FALL 2017 Practice Exam 4 1. Which of the following reactions is spontaneous under normal and standard conditions? 1 CHEM 1032 FALL 2017 Practice Exam 4 1. Which f the fllwing reactins is spntaneus under nrmal and standard cnditins? A. 2 NaCl(aq) 2 Na(s) + Cl2(g) B. CaBr2(aq) + 2 H2O(aq) Ca(OH)2(aq) + 2 HBr(aq) C.

More information

Hess Law - Enthalpy of Formation of Solid NH 4 Cl

Hess Law - Enthalpy of Formation of Solid NH 4 Cl Hess Law - Enthalpy f Frmatin f Slid NH 4 l NAME: OURSE: PERIOD: Prelab 1. Write and balance net inic equatins fr Reactin 2 and Reactin 3. Reactin 2: Reactin 3: 2. Shw that the alebraic sum f the balanced

More information

Physical Chemistry I for Biochemists. Chem340. Lecture 16 (2/18/11)

Physical Chemistry I for Biochemists. Chem340. Lecture 16 (2/18/11) hyscal Chemstry I or Bochemsts Chem34 Lecture 16 (/18/11) Yoshtaka Ish Ch4.6, Ch5.1-5.5 & HW5 4.6 Derental Scannng Calormetry (Derental hermal Analyss) sample = C p, s d s + dh uson = ( s )Kdt, [1] where

More information

CHEM 116 Concentrations and Colligative Properties

CHEM 116 Concentrations and Colligative Properties UMass stn, Chem 116 CHEM 116 Cncentratins and Clligative Prperties FSG is Mndays 11:00 am Lecture 10 Prf. Sevian and Tuesdays 3:30 pm bth in S-1-89 Tday s agenda Ways f expressing cncentratin Clligative

More information

Lecture 3 Examples and Problems

Lecture 3 Examples and Problems Lecture 3 Examles and Problems Mechancs & thermodynamcs Equartton Frst Law of Thermodynamcs Ideal gases Isothermal and adabatc rocesses Readng: Elements Ch. 1-3 Lecture 3, 1 Wllam Thomson (1824 1907) a.k.a.

More information

Unit 9: The Mole- Guided Notes What is a Mole?

Unit 9: The Mole- Guided Notes What is a Mole? Unit 9: The Mle- Guided Ntes What is a Mle? A mle is a name fr a specific f things Similar t a r a One mle is equal t 602 602,000,000,000,000,000,000,000 That s 602 with zers A mle is NOT an abbreviatin

More information

Chemistry 114 First Hour Exam

Chemistry 114 First Hour Exam Chemistry 114 First Hur Exam Please shw all wrk fr partial credit Name: (4 pints) 1. (12 pints) Espress is made by frcing very ht water under high pressure thrugh finely grund, cmpacted cffee. (Wikipedia)

More information

Nomenclature: number of electrons e -1. electron charge F constant number, (columbs/moles of e -1 ) atomic number g

Nomenclature: number of electrons e -1. electron charge F constant number, (columbs/moles of e -1 ) atomic number g Quanttatve Analyss f Irreversbltes Causes Vltage Drp n Fuel cell (Smulatn) Hssen Ghadaman*, Dr. Yadlah Sabh** Department f Energy Engneerng, Scence and Research Branch Azad Unversty, Islamc Republc f IRAN

More information

Chapter 5 rd Law of Thermodynamics

Chapter 5 rd Law of Thermodynamics Entropy and the nd and 3 rd Chapter 5 rd Law o hermodynamcs homas Engel, hlp Red Objectves Introduce entropy. Derve the condtons or spontanety. Show how S vares wth the macroscopc varables,, and. Chapter

More information

SIMULATION OF THREE PHASE THREE LEG TRANSFORMER BEHAVIOR UNDER DIFFERENT VOLTAGE SAG TYPES

SIMULATION OF THREE PHASE THREE LEG TRANSFORMER BEHAVIOR UNDER DIFFERENT VOLTAGE SAG TYPES SIMULATION OF THREE PHASE THREE LEG TRANSFORMER BEHAVIOR UNDER DIFFERENT VOLTAGE SAG TYPES Mhammadreza Dlatan Alreza Jallan Department f Electrcal Engneerng, Iran Unversty f scence & Technlgy (IUST) e-mal:

More information

Problem Set 5 Solutions - McQuarrie Problems 3.20 MIT Dr. Anton Van Der Ven

Problem Set 5 Solutions - McQuarrie Problems 3.20 MIT Dr. Anton Van Der Ven Prblem Set 5 Slutns - McQuarre Prblems 3.0 MIT Dr. Antn Van Der Ven Fall Fall 003 001 Prblem 3-4 We have t derve the thermdynamc prpertes f an deal mnatmc gas frm the fllwng: = e q 3 m = e and q = V s

More information

What determines how matter behaves? Thermodynamics.

What determines how matter behaves? Thermodynamics. What determines hw matter ehaves? hermdynamics.. What determines hw matter ehaves? Final Stale State Equilirium State Gis free energy: Minimum (at specific, ). Classical thermdynamics Macrscpic phenmena.

More information

TP A SOLUTION. For an ideal monatomic gas U=3/2nRT, Since the process is at constant pressure Q = C. giving ) =1000/(5/2*8.31*10)

TP A SOLUTION. For an ideal monatomic gas U=3/2nRT, Since the process is at constant pressure Q = C. giving ) =1000/(5/2*8.31*10) T A SOLUTION For an deal monatomc gas U/nRT, Snce the process s at constant pressure Q C pn T gvng a: n Q /( 5 / R T ) /(5/*8.*) C V / R and C / R + R 5 / R. U U / nr T (/ ) R T ( Q / 5 / R T ) Q / 5 Q

More information

Lecture. Polymer Thermodynamics 0331 L Chemical Potential

Lecture. Polymer Thermodynamics 0331 L Chemical Potential Prof. Dr. rer. nat. habl. S. Enders Faculty III for Process Scence Insttute of Chemcal Engneerng Department of Thermodynamcs Lecture Polymer Thermodynamcs 033 L 337 3. Chemcal Potental Polymer Thermodynamcs

More information

Chapter 18, Part 1. Fundamentals of Atmospheric Modeling

Chapter 18, Part 1. Fundamentals of Atmospheric Modeling Overhead Sldes for Chapter 18, Part 1 of Fundamentals of Atmospherc Modelng by Mark Z. Jacobson Department of Cvl & Envronmental Engneerng Stanford Unversty Stanford, CA 94305-4020 January 30, 2002 Types

More information

An Extended Regular Solution Model with Local Volume Fraction

An Extended Regular Solution Model with Local Volume Fraction () An Etended Regular Slutn Mdel wth cal Vlume Fractn Shgetsh KOBUCHI, Ken ISHIGE (Department f Enrnmental Scence and Engneerng, Graduate Schl f Scence and Engneerng, Yamaguch Unersty) Setsuk YONEZAWA

More information

G4023 Mid-Term Exam #1 Solutions

G4023 Mid-Term Exam #1 Solutions Exam1Solutons.nb 1 G03 Md-Term Exam #1 Solutons 1-Oct-0, 1:10 p.m to :5 p.m n 1 Pupn Ths exam s open-book, open-notes. You may also use prnt-outs of the homework solutons and a calculator. 1 (30 ponts,

More information

Find this material useful? You can help our team to keep this site up and bring you even more content consider donating via the link on our site.

Find this material useful? You can help our team to keep this site up and bring you even more content consider donating via the link on our site. Find this material useful? Yu can help ur team t keep this site up and bring yu even mre cntent cnsider dnating via the link n ur site. Still having truble understanding the material? Check ut ur Tutring

More information

On the concentration dependence of the surface tension of liquid metallic alloys Theoretical basis Hungary, Miskolc, Egyetemvaros.

On the concentration dependence of the surface tension of liquid metallic alloys Theoretical basis Hungary, Miskolc, Egyetemvaros. On the cncentratn dependence the surace tensn lqud metallc allys heretcal bass 1 G.Kaptay, kmkap@gld.un-msklc.hu 2 Z.Papp zltanp@da.ed.ac.uk 1 Pressr at the Department Physcal Chemstry the Unversty Msklc

More information

and Statistical Mechanics Material Properties

and Statistical Mechanics Material Properties Statstcal Mechancs and Materal Propertes By Kuno TAKAHASHI Tokyo Insttute of Technology, Tokyo 15-855, JAPA Phone/Fax +81-3-5734-3915 takahak@de.ttech.ac.jp http://www.de.ttech.ac.jp/~kt-lab/ Only for

More information

Shell Stiffness for Diffe ent Modes

Shell Stiffness for Diffe ent Modes Engneerng Mem N 28 February 0 979 SUGGESTONS FOR THE DEFORMABLE SUBREFLECTOR Sebastan vn Herner Observatns wth the present expermental versn (Engneerng Dv nternal Reprt 09 July 978) have shwn that a defrmable

More information

Introduction to Vapor/Liquid Equilibrium, part 2. Raoult s Law:

Introduction to Vapor/Liquid Equilibrium, part 2. Raoult s Law: CE304, Sprng 2004 Lecture 4 Introducton to Vapor/Lqud Equlbrum, part 2 Raoult s Law: The smplest model that allows us do VLE calculatons s obtaned when we assume that the vapor phase s an deal gas, and

More information

A Few Basic Facts About Isothermal Mass Transfer in a Binary Mixture

A Few Basic Facts About Isothermal Mass Transfer in a Binary Mixture Few asic Facts but Isthermal Mass Transfer in a inary Miture David Keffer Department f Chemical Engineering University f Tennessee first begun: pril 22, 2004 last updated: January 13, 2006 dkeffer@utk.edu

More information

Wp/Lmin. Wn/Lmin 2.5V

Wp/Lmin. Wn/Lmin 2.5V UNIVERITY OF CALIFORNIA Cllege f Engneerng Department f Electrcal Engneerng and Cmputer cences Andre Vladmrescu Hmewrk #7 EEC Due Frday, Aprl 8 th, pm @ 0 Cry Prblem #.5V Wp/Lmn 0.0V Wp/Lmn n ut Wn/Lmn.5V

More information

Introduction to Electronic circuits.

Introduction to Electronic circuits. Intrductn t Electrnc crcuts. Passve and Actve crcut elements. Capactrs, esstrs and Inductrs n AC crcuts. Vltage and current dvders. Vltage and current surces. Amplfers, and ther transfer characterstc.

More information

Temperature. Chapter Heat Engine

Temperature. Chapter Heat Engine Chapter 3 Temperature In prevous chapters of these notes we ntroduced the Prncple of Maxmum ntropy as a technque for estmatng probablty dstrbutons consstent wth constrants. In Chapter 9 we dscussed the

More information

CHEM 1001 Problem Set #3: Entropy and Free Energy

CHEM 1001 Problem Set #3: Entropy and Free Energy CHEM 1001 Prblem Set #3: Entry and Free Energy 19.7 (a) Negative; A liquid (mderate entry) cmbines with a slid t frm anther slid. (b)psitive; One mle f high entry gas frms where n gas was resent befre.

More information