Lecture 8. Chapter 7. - Thermodynamic Web - Departure Functions - Review Equations of state (chapter 4, briefly)

Size: px
Start display at page:

Download "Lecture 8. Chapter 7. - Thermodynamic Web - Departure Functions - Review Equations of state (chapter 4, briefly)"

Transcription

1 Lecture 8 Chapter 5 - Thermodynamc Web - Departure Functons - Revew Equatons of state (chapter 4, brefly) Chapter 6 - Equlbrum (chemcal potental) * Pure Component * Mxtures Chapter 7 - Fugacty (chemcal potental fugacty equlbrum calculatons) * Vapor (overvew), lqud, solds - ctvty Coeffcents [Fugacty Coeffcents (overvew)] Chapter 8 - Phase Equlbrum * Dagrams * Vapor Lqud (VLE) * Lqud Lqud (LLE) * Sold Lqud (SLE) Chapter 9 - Reacton Equlbra

2 Fugacty Coeffcent (methods to calculate) ˆ. Data. Equatons of State 3. Generalzed correlatons a. Pure Flud 3. Generalzed correlatons b. Multcomponent system: ˆ a. Pure Flud. Data ln P ln P 0 dp P P dp RT P CO at 38 o C, 3.79 bar P [bar] P data ln CO dp RT P 0

3 Fugacty Coeffcent (methods to calculate) a. Pure Flud. Equatons of State 3 See handout on webste from Kyle for Peng-Robnson EOS 3 ( ) ( 3 ) ( 3 ) 0 ln ln( ) ln CO at 38 o C, 3.79 bar PREOS CO 0.935

4 Fugacty Coeffcent (methods to calculate) 4 ˆ. Data a. Pure Flud. Equatons of State 3. Generalzed correlatons b. Multcomponent system: ˆ vdw EOS RT a a y a y b b RT b P P y f b a b a a mx a mx v a a v a ln ˆ ln ˆ ln c Peng Robnson EOS (see Kyle handout on web) j j j ln ˆ ln ln

5 Fugacty Coeffcent (Contnued) 5

6 Fugacty Coeffcent (Contnued) 6

7 Fugacty Coeffcent (PREOS) 7 c j j j ln ln ˆ ln T P r r P r T r r T c c c j j j k j j j j k 0 ) ( ) 3 ( ) ( ) ( ) 3 ( ) (

8 Fugacty Coeffcent (spenplus Examples) 8. for ethylene at 5 o C and 40 bar ˆ CO. for CO n 50:50 (mole) mxture wth toluene at 45 o C and 40 bar

9 Fugacty Coeffcent (multcomponent approxmaton) 9 Lews fugacty approxmaton (rule) ˆ Vald near deal soluton condtons,.e. y n excess ( >0.9)

10 ) y Fugacty / Equlbrum (SUMMRY) V L f ˆ ˆ f P ˆ V x P ˆ L Vapor phase: good; lqud phase: good for HC or moderate hgh pressures (compressble lqud phase) 0 ˆ Typcally used for lqud phase V sat sat ) y P x P P. C. fugacty calculatons y Pˆ V x H 3) Used for specal cases (lke gases dssolvng nto lqud phase)

11 L fˆ f. Compressble lquds. Ideal and real solutons 3. Dssolved gases Fugacty (Lqud Phase). Compressble lquds (mod hgh P, and hydrocarbons) f ˆ L L x Pˆ L Use EOS for: ˆ & or L L. Ideal lqud soluton f ˆ L f ˆ deal x f deal x f o o f Pure speces fugacty real soluton fˆ L fˆ deal x f ctvty coeffcent o fˆ fˆ Lews/Randall bass L deal fˆ x L o f

12 real soluton o L Fugacty (Lqud Phase) fˆ x f Lews/Randall bass s o o f P L sat sat P exp dp at system T and P sat RT P fˆ L x P sat sat P exp P sat L RT dp

13 Fugacty (Typcal Lqud Phase Models) fˆ real soluton o L sat sat Lews/Randall bass s x P P.C. 3? real soluton behaves deally n the lqud phase then: fˆ L x P sat real soluton behaves non-deally n the lqud phase then: fˆ L x P sat

14 G E G G ctvty Coeffcent (ways to calculate) deal u RT ln fˆ deal u deal fˆ but : fˆ ˆ L f deal 4 G E RT ln G E nt g n E T, P, n j RT ln nt g n E T, P, n j E Now, need models for calculatng g and then can fnd. -suffx Margules (smple, symmetrc) [bnary] g E x x RT ln RT ln x x x x p RT ln exp x ln ln lm 0 0 x x 0 RT exp

15 ctvty Coeffcent ( suffx Margules model). -suffx Margules agues (smple, symmetrc) [bnary] g E x x x x 5 Fnd : take data y P x P sat Example: bnary mx of cyclohexane (a) and dodecane (b) at o C cycloc C lm x 0 RT exp

16 ctvty Coeffcent (Models). -suffx Margules agues (smple, symmetrc) [bnary] g E x x x x 6 symmetrc models:. Three-suffx Margules: (addtonal parameter) 3. Van Laar: (older model but stll good and easy to work wth) 4. Wlson: (not good for lqud-lqud-equlbra) 5. NRTL: (Non-Random-Two-Lqud; R T d good dfrst choce, usually) 6. UNIQUC: (UNIversal QUs-Chemcal; also good) 7. UNIFC: (only predctve model)

17 ctvty Coeffcent (nary Models) 7 Koretsky, 004

18 ctvty Coeffcent (nary Models) 8

19 ctvty Coeffcent (nary Models) 9 Prausntz, et.al., 999

20 ctvty Coeffcent (nary Models) 0 Prausntz, et.al., 999

21 ctvty Coeffcent (nary Models) Prausntz, et.al., 999

22 ctvty Coeffcent (nary Models) Prausntz, et.al., 999

23 ctvty Coeffcent (nary Models) 3 Prausntz, et.al., 999

24 ctvty Coeffcent (nary Models) 4 Prausntz, et.al., 999

25 ctvty Coeffcent (nary Models) 5 r and q depend on molecular sze (volume) and external surface areas of pure components. Prausntz, et.al., 999

26 ctvty Coeffcent (nary Models) 6 Prausntz, et.al., 999

27 ctvty Coeffcent (Example) 7 Temperature-composton dagram at.03 bar ( atm) pressure for system: formc acd () and acetc acd () Prausntz, et.al., 999

28 Lecture 8 Chapter 5 - Thermodynamc Web - Departure Functons - Revew Equatons of state (chapter 4, brefly) Chapter 6 - Equlbrum (chemcal potental) * Pure Component * Mxtures Chapter 7 - Fugacty (chemcal potental fugacty equlbrum calculatons) * Vapor (overvew), lqud, solds - ctvty Coeffcents [Fugacty Coeffcents (overvew)] Chapter 8 - Phase Equlbrum * Dagrams * Vapor Lqud (VLE) * Lqud Lqud (LLE) * Sold Lqud (SLE) Chapter 9 - Reacton Equlbra 8

Energy, Entropy, and Availability Balances Phase Equilibria. Nonideal Thermodynamic Property Models. Selecting an Appropriate Model

Energy, Entropy, and Availability Balances Phase Equilibria. Nonideal Thermodynamic Property Models. Selecting an Appropriate Model Lecture 4. Thermodynamcs [Ch. 2] Energy, Entropy, and Avalablty Balances Phase Equlbra - Fugactes and actvty coeffcents -K-values Nondeal Thermodynamc Property Models - P-v-T equaton-of-state models -

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

General Thermodynamics for Process Simulation. Dr. Jungho Cho, Professor Department of Chemical Engineering Dong Yang University

General Thermodynamics for Process Simulation. Dr. Jungho Cho, Professor Department of Chemical Engineering Dong Yang University General Thermodynamcs for Process Smulaton Dr. Jungho Cho, Professor Department of Chemcal Engneerng Dong Yang Unversty Four Crtera for Equlbra μ = μ v Stuaton α T = T β α β P = P l μ = μ l1 l 2 Thermal

More information

PETE 310 Lectures # 24 & 25 Chapter 12 Gas Liquid Equilibrium

PETE 310 Lectures # 24 & 25 Chapter 12 Gas Liquid Equilibrium ETE 30 Lectures # 24 & 25 Chapter 2 Gas Lqud Equlbrum Thermal Equlbrum Object A hgh T, Object B low T Intal contact tme Intermedate tme. Later tme Mechancal Equlbrum ressure essels Vale Closed Vale Open

More information

Supplementary Notes for Chapter 9 Mixture Thermodynamics

Supplementary Notes for Chapter 9 Mixture Thermodynamics Supplementary Notes for Chapter 9 Mxture Thermodynamcs Key ponts Nne major topcs of Chapter 9 are revewed below: 1. Notaton and operatonal equatons for mxtures 2. PVTN EOSs for mxtures 3. General effects

More information

Solution Thermodynamics

Solution Thermodynamics CH2351 Chemcal Engneerng Thermodynamcs II Unt I, II www.msubbu.n Soluton Thermodynamcs www.msubbu.n Dr. M. Subramanan Assocate Professor Department of Chemcal Engneerng Sr Svasubramanya Nadar College of

More information

The ChemSep Book. Harry A. Kooijman Consultant. Ross Taylor Clarkson University, Potsdam, New York University of Twente, Enschede, The Netherlands

The ChemSep Book. Harry A. Kooijman Consultant. Ross Taylor Clarkson University, Potsdam, New York University of Twente, Enschede, The Netherlands The ChemSep Book Harry A. Koojman Consultant Ross Taylor Clarkson Unversty, Potsdam, New York Unversty of Twente, Enschede, The Netherlands Lbr Books on Demand www.bod.de Copyrght c 2000 by H.A. Koojman

More information

Gasometric Determination of NaHCO 3 in a Mixture

Gasometric Determination of NaHCO 3 in a Mixture 60 50 40 0 0 5 15 25 35 40 Temperature ( o C) 9/28/16 Gasometrc Determnaton of NaHCO 3 n a Mxture apor Pressure (mm Hg) apor Pressure of Water 1 NaHCO 3 (s) + H + (aq) Na + (aq) + H 2 O (l) + CO 2 (g)

More information

y i x P vap 10 A T SOLUTION TO HOMEWORK #7 #Problem

y i x P vap 10 A T SOLUTION TO HOMEWORK #7 #Problem SOLUTION TO HOMEWORK #7 #roblem 1 10.1-1 a. In order to solve ths problem, we need to know what happens at the bubble pont; at ths pont, the frst bubble s formed, so we can assume that all of the number

More information

If two volatile and miscible liquids are combined to form a solution, Raoult s law is not obeyed. Use the experimental data in Table 9.

If two volatile and miscible liquids are combined to form a solution, Raoult s law is not obeyed. Use the experimental data in Table 9. 9.9 Real Solutons Exhbt Devatons from Raoult s Law If two volatle and mscble lquds are combned to form a soluton, Raoult s law s not obeyed. Use the expermental data n Table 9.3: Physcal Chemstry 00 Pearson

More information

Vapor-Liquid Equilibria for Water+Hydrochloric Acid+Magnesium Chloride and Water+Hydrochloric Acid+Calcium Chloride Systems at Atmospheric Pressure

Vapor-Liquid Equilibria for Water+Hydrochloric Acid+Magnesium Chloride and Water+Hydrochloric Acid+Calcium Chloride Systems at Atmospheric Pressure Chnese J. Chem. Eng., 4() 76 80 (006) RESEARCH OES Vapor-Lqud Equlbra for Water+Hydrochlorc Acd+Magnesum Chlorde and Water+Hydrochlorc Acd+Calcum Chlorde Systems at Atmospherc Pressure ZHAG Yng( 张颖 ) and

More information

Name: SID: Discussion Session:

Name: SID: Discussion Session: Name: SID: Dscusson Sesson: Chemcal Engneerng Thermodynamcs 141 -- Fall 007 Thursday, November 15, 007 Mdterm II SOLUTIONS - 70 mnutes 110 Ponts Total Closed Book and Notes (0 ponts) 1. Evaluate whether

More information

I wish to publish my paper on The International Journal of Thermophysics. A Practical Method to Calculate Partial Properties from Equation of State

I wish to publish my paper on The International Journal of Thermophysics. A Practical Method to Calculate Partial Properties from Equation of State I wsh to publsh my paper on The Internatonal Journal of Thermophyscs. Ttle: A Practcal Method to Calculate Partal Propertes from Equaton of State Authors: Ryo Akasaka (correspondng author) 1 and Takehro

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 16 8/4/14 Unversty o Washngton Department o Chemstry Chemstry 452/456 Summer Quarter 214. Real Vapors and Fugacty Henry s Law accounts or the propertes o extremely dlute soluton. s shown n Fgure

More information

Department of Physical Chemistry, Faculty of Chemistry, University of Bucharest, Bd. Regina Elisabeta 4-12, , Bucharest, Romania

Department of Physical Chemistry, Faculty of Chemistry, University of Bucharest, Bd. Regina Elisabeta 4-12, , Bucharest, Romania ISOTHERMAL LIQUID-VAOR EQUILIBRIUM IN ACETONITRILE-WATER SYSTEM Rodca Vlcu, Zoca Cenuse abstact: The study of ths system started from the mportance that acetontrle has as the component of some mxtures

More information

Non-Commercial Use Only

Non-Commercial Use Only Plottng P-x-y dagram for bnary system Acetone/water at temperatures 25,100,and 200 C usng UNIFAC method and comparng t wth expermental results. Unfac Method: The UNIFAC method s based on the UNIQUAC equaton,

More information

Chapter 8 Solutions Engineering and Chemical Thermodynamics 2e

Chapter 8 Solutions Engineering and Chemical Thermodynamics 2e Chapter 8 Solutons Engneerng and Chemcal Thermodynamcs e Mlo Koretsky Wyatt Tenhaeff School of Chemcal, Bologcal, and Envronmental Engneerng Oregon State Unversty mlo.koretsky@oregonstate.edu 8. No ths

More information

Equation of State Modeling of Phase Equilibrium in the Low-Density Polyethylene Process

Equation of State Modeling of Phase Equilibrium in the Low-Density Polyethylene Process Equaton of State Modelng of Phase Equlbrum n the Low-Densty Polyethylene Process H. Orbey, C. P. Boks, and C. C. Chen Ind. Eng. Chem. Res. 1998, 37, 4481-4491 Yong Soo Km Thermodynamcs & Propertes Lab.

More information

(1) The saturation vapor pressure as a function of temperature, often given by the Antoine equation:

(1) The saturation vapor pressure as a function of temperature, often given by the Antoine equation: CE304, Sprng 2004 Lecture 22 Lecture 22: Topcs n Phase Equlbra, part : For the remander of the course, we wll return to the subject of vapor/lqud equlbrum and ntroduce other phase equlbrum calculatons

More information

INTRODUCTION TO CHEMICAL PROCESS SIMULATORS

INTRODUCTION TO CHEMICAL PROCESS SIMULATORS INTRODUCTION TO CHEMICAL PROCESS SIMULATORS DWSIM Chemcal Process Smulator A. Carrero, N. Qurante, J. Javaloyes October 2016 Introducton to Chemcal Process Smulators Contents Monday, October 3 rd 2016

More information

Thermodynamics II. Department of Chemical Engineering. Prof. Kim, Jong Hak

Thermodynamics II. Department of Chemical Engineering. Prof. Kim, Jong Hak Thermodynamcs II Department of Chemcal Engneerng Prof. Km, Jong Hak Soluton Thermodynamcs : theory Obectve : lay the theoretcal foundaton for applcatons of thermodynamcs to gas mxture and lqud soluton

More information

PREDICTION OF GAS HYDRATE PHASE BEHAVIOR IN THE PRESENCE OF ALCOLHOLS AND GLYCOLS WITH PRSV EQUATION OF STATE AND THE VDW-P MODEL

PREDICTION OF GAS HYDRATE PHASE BEHAVIOR IN THE PRESENCE OF ALCOLHOLS AND GLYCOLS WITH PRSV EQUATION OF STATE AND THE VDW-P MODEL Proceedngs of the 7th Internatonal Conference on Gas Hydrates (ICGH 2011), Ednburgh, Scotland, Unted Kngdom, July 1721, 2011. PREDICTION OF GAS HYDRATE PHASE BEHAVIOR IN THE PRESENCE OF ALCOLHOLS AND GLYCOLS

More information

A Self-Consistent Gibbs Excess Mixing Rule for Cubic Equations of State: derivation and fugacity coefficients

A Self-Consistent Gibbs Excess Mixing Rule for Cubic Equations of State: derivation and fugacity coefficients A Self-Consstent Gbbs Excess Mxng Rule for Cubc Equatons of State: dervaton and fugacty coeffcents Paula B. Staudt, Rafael de P. Soares Departamento de Engenhara Químca, Escola de Engenhara, Unversdade

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

( ) 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

MODELING THE HIGH-PRESSURE BEHAVIOR OF BINARY MIXTURES OF CARBON DIOXIDE+ALKANOLS USING AN EXCESS FREE ENERGY MIXING RULE

MODELING THE HIGH-PRESSURE BEHAVIOR OF BINARY MIXTURES OF CARBON DIOXIDE+ALKANOLS USING AN EXCESS FREE ENERGY MIXING RULE Brazlan Journal of Chemcal Engneerng ISSN 0104-6632 Prnted n Brazl Vol. 21, No. 04, pp. 659-666, October - December 04 MODELING THE HIGH-PRESSURE BEHAVIOR OF BINARY MIXTURES OF CARBON DIOXIDE+ALKANOLS

More information

applied to a single-phase fluid in a closed system wherein no chemical reactions occur.

applied to a single-phase fluid in a closed system wherein no chemical reactions occur. The basc relaton connectng the Gbbs energy to the temperature and pressure n any closed system: (ng) (ng) d(ng) d dt (nv)d (ns)dt T T,n appled to a sngle-phase flud n a closed system wheren no chemcal

More information

CHEMICAL REACTIONS AND DIFFUSION

CHEMICAL REACTIONS AND DIFFUSION CHEMICAL REACTIONS AND DIFFUSION A.K.A. NETWORK THERMODYNAMICS BACKGROUND Classcal thermodynamcs descrbes equlbrum states. Non-equlbrum thermodynamcs descrbes steady states. Network thermodynamcs descrbes

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

VAPOR LIQUID EQUILIBRIUM DATA GENERATION FOR ACETIC ACID AND p-xylene AT ATMOSPHERIC PRESSURE

VAPOR LIQUID EQUILIBRIUM DATA GENERATION FOR ACETIC ACID AND p-xylene AT ATMOSPHERIC PRESSURE Int. J. Chem. Sc.: 14(3), 2016, 1511-1519 ISSN 0972-768X www.sadgurupublcatons.com VAPOR LIQUID EQUILIBRIUM DATA GENERATION FOR ACETIC ACID AND p-xylene AT ATMOSPHERIC PRESSURE PAWAN KIRAN MALI *,a and

More information

Appendix II Summary of Important Equations

Appendix II Summary of Important Equations W. M. Whte Geochemstry Equatons of State: Ideal GasLaw: Coeffcent of Thermal Expanson: Compressblty: Van der Waals Equaton: The Laws of Thermdynamcs: Frst Law: Appendx II Summary of Important Equatons

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

10.34 Numerical Methods Applied to Chemical Engineering Fall Homework #3: Systems of Nonlinear Equations and Optimization

10.34 Numerical Methods Applied to Chemical Engineering Fall Homework #3: Systems of Nonlinear Equations and Optimization 10.34 Numercal Methods Appled to Chemcal Engneerng Fall 2015 Homework #3: Systems of Nonlnear Equatons and Optmzaton Problem 1 (30 ponts). A (homogeneous) azeotrope s a composton of a multcomponent mxture

More information

Experimental and Modeling Studies for a Reactive Batch Distillation Column

Experimental and Modeling Studies for a Reactive Batch Distillation Column Expermental and Modelng Studes for a Reactve Batch Dstllaton Column Almıla Bahar*. Canan Özgen** Department of Chemcal Engneerng, Mddle East Techncal Unversty, Ankara, 0653, Turkey e-mal: *abahar@metu.edu.tr,

More information

UNIFAC. Documentation. DDBSP Dortmund Data Bank Software Package

UNIFAC. Documentation. DDBSP Dortmund Data Bank Software Package UNIFAC Documentaton DDBSP Dortmund Data Ban Software Pacage DDBST Dortmund Data Ban Software & Separaton Technology GmbH Mare-Cure-Straße 10 D-26129 Oldenburg Tel.: +49 441 361819 0 Fax: +49 441 361819

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

Non-Ideality Through Fugacity and Activity

Non-Ideality Through Fugacity and Activity Non-Idealty Through Fugacty and Actvty S. Patel Deartment of Chemstry and Bochemstry, Unversty of Delaware, Newark, Delaware 19716, USA Corresondng author. E-mal: saatel@udel.edu 1 I. FUGACITY In ths dscusson,

More information

a for save as PDF Chemistry 163B Introduction to Multicomponent Systems and Partial Molar Quantities

a for save as PDF Chemistry 163B Introduction to Multicomponent Systems and Partial Molar Quantities a for save as PDF Chemstry 163B Introducton to Multcomponent Systems and Partal Molar Quanttes 1 the problem of partal mmolar quanttes mx: 10 moles ethanol C 2 H 5 OH (580 ml) wth 1 mole water H 2 O (18

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

Lecture 11. Chapter 7. - Thermodynamic Web - Departure Functions - Review Equations of state (chapter 4, briefly)

Lecture 11. Chapter 7. - Thermodynamic Web - Departure Functions - Review Equations of state (chapter 4, briefly) Lecture 11 Chpter 5 - Thermodnmc We - Deprture unctons - Revew Equtons of stte (chpter 4, refl) Chpter 6 - Equlrum (chemcl potentl) * ure Component * Mtures Chpter 7 - ugct (chemcl potentl fugct equlrum

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

Multicomponent Vaporization Modeling of Petroleum-Biofuel Mixture at High-Pressure Conditions

Multicomponent Vaporization Modeling of Petroleum-Biofuel Mixture at High-Pressure Conditions ILASS Amercas, 3 rd Annual Conference on Lqud Atomzaton and Spray Systems, Ventura, CA, May 011 Multcomponent Vaporzaton Modelng of Petroleum-Bofuel Mxture at Hgh-Pressure Condtons L. Zhang and Song-Charng

More information

Outlet temperature of a WGS reactor (Stage I) for the conversion of CO, applied for the abatement of CO to a fixed value.

Outlet temperature of a WGS reactor (Stage I) for the conversion of CO, applied for the abatement of CO to a fixed value. Department of Energy Poltecnco d Mlano Va Lambruschn 56 MILAN Exercses of Fundamentals of Chemcal Processes Prof. Ganpero Gropp Exercse utlet temperature of a WGS reactor (Stage I for the converson of

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

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

A Modulated Hydrothermal (MHT) Approach for the Facile. Synthesis of UiO-66-Type MOFs

A Modulated Hydrothermal (MHT) Approach for the Facile. Synthesis of UiO-66-Type MOFs Supplementary Informaton A Modulated Hydrothermal (MHT) Approach for the Facle Synthess of UO-66-Type MOFs Zhgang Hu, Yongwu Peng, Zx Kang, Yuhong Qan, and Dan Zhao * Department of Chemcal and Bomolecular

More information

Determination of Structure and Formation Conditions of Gas Hydrate by Using TPD Method and Flash Calculations

Determination of Structure and Formation Conditions of Gas Hydrate by Using TPD Method and Flash Calculations nd atonal Iranan Conference on Gas Hydrate (ICGH) Semnan Unersty Determnaton of Structure and Formaton Condtons of Gas Hydrate by Usng TPD Method and Flash Calculatons H. Behat Rad, F. Varamnan* Department

More information

4.2 Chemical Driving Force

4.2 Chemical Driving Force 4.2. CHEMICL DRIVING FORCE 103 4.2 Chemcal Drvng Force second effect of a chemcal concentraton gradent on dffuson s to change the nature of the drvng force. Ths s because dffuson changes the bondng n a

More information

ARTICLE IN PRESS. Fluid Phase Equilibria 275 (2008) Contents lists available at ScienceDirect. Fluid Phase Equilibria

ARTICLE IN PRESS. Fluid Phase Equilibria 275 (2008) Contents lists available at ScienceDirect. Fluid Phase Equilibria Flud Phase Equlbra 275 (2008) 33 38 Contents lsts avalable at ScenceDrect Flud Phase Equlbra journal homepage: www.elsever.com/locate/flud Solubltes of cnnamc acd, phenoxyacetc acd and 4-methoxyphenylacetc

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

Mass Transfer Processes

Mass Transfer Processes Mass Transfer Processes S. Majd Hassanzadeh Department of Earth Scences Faculty of Geoscences Utrecht Unversty Outlne: 1. Measures of Concentraton 2. Volatlzaton and Dssoluton 3. Adsorpton Processes 4.

More information

Modelling of Phase Equilibria for Supercritical Carbon Dioxide System by Hole-Theory Equation of State with Local Composition Model

Modelling of Phase Equilibria for Supercritical Carbon Dioxide System by Hole-Theory Equation of State with Local Composition Model Modellng of Phase Equlbra for Supercrtcal Carbon Doxde System by Hole-Theory Equaton of State wth Local Composton Model Yusuke Shmoyama*, Yuta Yokozak Department of Chemcal Scence and Engneerng, Tokyo

More information

Electrochemical Equilibrium Electromotive Force

Electrochemical Equilibrium Electromotive Force CHM465/865, 24-3, Lecture 5-7, 2 th Sep., 24 lectrochemcal qulbrum lectromotve Force Relaton between chemcal and electrc drvng forces lectrochemcal system at constant T and p: consder Gbbs free energy

More information

ChE 512: Topic 1 Reactions at a fluid non-porous solid interface. P.A. Ramachandran

ChE 512: Topic 1 Reactions at a fluid non-porous solid interface. P.A. Ramachandran he 512: Topc 1 Reactons at a flud non-porous sold nterface P.. Ramachandran rama@wustl.edu OUTLIE External Transport: Flm oncept Mass transfer coeffcents Effect of transport on reacton multaneous heat

More information

Solution Thermodynamics

Solution Thermodynamics Soluton hermodynamcs usng Wagner Notaton by Stanley. Howard Department of aterals and etallurgcal Engneerng South Dakota School of nes and echnology Rapd Cty, SD 57701 January 7, 001 Soluton hermodynamcs

More information

1) Silicon oxide has a typical surface potential in an aqueous medium of ϕ,0

1) Silicon oxide has a typical surface potential in an aqueous medium of ϕ,0 1) Slcon oxde has a typcal surface potental n an aqueous medum of ϕ, = 7 mv n 5 mm l at ph 9. Whch concentraton of catons do you roughly expect close to the surface? What s the average dstance between

More information

The influence of non-ideal vapor-liquid-equilibrium on vaporization of multicomponent hydrocarbon fuels

The influence of non-ideal vapor-liquid-equilibrium on vaporization of multicomponent hydrocarbon fuels ICLASS 202, 2 th Trennal Internatonal Conference on Lqud Atomzaton and Spray Systems, Hedelberg, Germany, September 2-6, 202 The nfluence of non-deal vapor-lqud-equlbrum on vaporzaton of multcomponent

More information

Q e E i /k B. i i i i

Q e E i /k B. i i i i Water and Aqueous Solutons 3. Lattce Model of a Flud Lattce Models Lattce models provde a mnmalst, or coarse-graned, framework for descrbng the translatonal, rotatonal, and conformatonal degrees of freedom

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

Solutions Review Worksheet

Solutions Review Worksheet Solutons Revew Worksheet NOTE: Namng acds s ntroduced on pages 163-4 and agan on pages 208-9.. You learned ths and were quzzed on t, but snce acd names are n the Data Booklet you wll not be tested on ths

More information

A New Thermodynamic Function for Phase-Splitting at Constant Temperature, Moles, and Volume

A New Thermodynamic Function for Phase-Splitting at Constant Temperature, Moles, and Volume A New Thermodynamc Functon for Phase-Splttng at Constant Temperature, Moles, and olume Jří Mkyška Dept. of Mathematcs, Faculty of Nuclear Scences and Physcal Engneerng, Czech Techncal Unversty n Prague,

More information

Modeling of Phase and Chemical Equilibria for Systems Involved in Biodiesel Production

Modeling of Phase and Chemical Equilibria for Systems Involved in Biodiesel Production 855 A publcaton of CHEMICAL ENGINEERING TRANSACTIONS VOL. 43, 205 Chef Edtors: Sauro Perucc, Jří J. Klemeš Copyrght 205, AIDIC Servz S.r.l., ISBN 978-88-95608-34-; ISSN 2283-926 The Italan Assocaton of

More information

Lecture 7: Boltzmann distribution & Thermodynamics of mixing

Lecture 7: Boltzmann distribution & Thermodynamics of mixing Prof. Tbbtt Lecture 7 etworks & Gels Lecture 7: Boltzmann dstrbuton & Thermodynamcs of mxng 1 Suggested readng Prof. Mark W. Tbbtt ETH Zürch 13 März 018 Molecular Drvng Forces Dll and Bromberg: Chapters

More information

5.60 Thermodynamics & Kinetics Spring 2008

5.60 Thermodynamics & Kinetics Spring 2008 MIT OpenCourseWare http://ocw.mt.edu 5.60 Thermodynamcs & Knetcs Sprng 2008 For nformaton about ctng these materals or our Terms of Use, vst: http://ocw.mt.edu/terms. 5.60 Sprng 2008 Lecture #29 page 1

More information

CALCULATION OF VAPOUR - LIQUID - LIQUID EQUILIBRIA

CALCULATION OF VAPOUR - LIQUID - LIQUID EQUILIBRIA Chemcal and Process Engneerng 202, 33 (3), 463-477 DOI: 0.2478/v076-02-0039-5 CALCULATIO OF VAPOUR - LIQUID - LIQUID EQUILIBRIA I QUATERARY SYSTEMS Andrzej Wyczesany * Unversty of Technology, Insttute

More information

KINETICS OF GAS HYDRATE FORMATION FROM PYROLYSIS GAS IN WATER-IN-OIL EMULSION SYSTEM

KINETICS OF GAS HYDRATE FORMATION FROM PYROLYSIS GAS IN WATER-IN-OIL EMULSION SYSTEM Proceedngs of the 7th Internatonal Conference on Gas Hydrates (ICGH 211), Ednburgh, Scotland, Unted Kngdom, July 17-21, 211. KINETICS OF GAS HYDRATE FORMATION FROM PYROLYSIS GAS IN WATER-IN-OIL EMULSION

More information

Diffusion Mass Transfer

Diffusion Mass Transfer Dffuson Mass Transfer General onsderatons Mass transfer refers to mass n transt due to a speces concentraton gradent n a mture. Must have a mture of two or more speces for mass transfer to occur. The speces

More information

MODELING OF ASSOCIATION EFFECTS IN MIXTURES OF CARBOXYLIC ACIDS WITH ASSOCIATING AND NON-ASSOCIATING COMPONENTS

MODELING OF ASSOCIATION EFFECTS IN MIXTURES OF CARBOXYLIC ACIDS WITH ASSOCIATING AND NON-ASSOCIATING COMPONENTS Latn Amercan Appled Research 33:307-31 (003) MODELING OF ASSOCIATION EFFECTS IN MIXTURES OF CARBOXYLIC ACIDS WITH ASSOCIATING AND NON-ASSOCIATING COMPONENTS O. FERREIRA, T. FORNARI, E. A. BRIGNOLE and

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

V. Electrostatics. Lecture 25: Diffuse double layer structure

V. Electrostatics. Lecture 25: Diffuse double layer structure V. Electrostatcs Lecture 5: Dffuse double layer structure MIT Student Last tme we showed that whenever λ D L the electrolyte has a quas-neutral bulk (or outer ) regon at the geometrcal scale L, where there

More information

Phase equilibria Introduction General equilibrium conditions

Phase equilibria Introduction General equilibrium conditions .5 hase equlbra.5. Introducton A gven amount of matter (usually called a system) can be characterzed by unform ntensve propertes n ts whole volume or only n some of ts parts; a porton of matter wth unform

More information

Adsorption: A gas or gases from a mixture of gases or a liquid (or liquids) from a mixture of liquids is bound physically to the surface of a solid.

Adsorption: A gas or gases from a mixture of gases or a liquid (or liquids) from a mixture of liquids is bound physically to the surface of a solid. Searatons n Chemcal Engneerng Searatons (gas from a mxture of gases, lquds from a mxture of lquds, solds from a soluton of solds n lquds, dssolved gases from lquds, solvents from gases artally/comletely

More information

CHEMICAL ENGINEERING

CHEMICAL ENGINEERING Postal Correspondence GATE & PSUs -MT To Buy Postal Correspondence Packages call at 0-9990657855 1 TABLE OF CONTENT S. No. Ttle Page no. 1. Introducton 3 2. Dffuson 10 3. Dryng and Humdfcaton 24 4. Absorpton

More information

Estimation of the composition of the liquid and vapor streams exiting a flash unit with a supercritical component

Estimation of the composition of the liquid and vapor streams exiting a flash unit with a supercritical component Department of Energ oltecnco d Mlano Va Lambruschn - 05 MILANO Eercses of Fundamentals of Chemcal rocesses rof. Ganpero Gropp Eercse 8 Estmaton of the composton of the lqud and vapor streams etng a unt

More information

Thermodynamic Analysis of Supercritical Water Gasification of Microalgae Biomass for Hydrogen and Syngas Production

Thermodynamic Analysis of Supercritical Water Gasification of Microalgae Biomass for Hydrogen and Syngas Production 553 A publcaton of VOL. 32, 203 CHEMICAL ENGINEERING TRANSACTIONS Chef Edtors: Sauro Perucc, Jří J. Klemeš Copyrght 203, AIDIC Servz S.r.l., ISBN 978-88-95608-23-5; ISSN 974-979 The Italan Assocaton of

More information

Process Modeling. Improving or understanding chemical process operation is a major objective for developing a dynamic process model

Process Modeling. Improving or understanding chemical process operation is a major objective for developing a dynamic process model Process Modelng Improvng or understandng chemcal process operaton s a major objectve for developng a dynamc process model Balance equatons Steady-state balance equatons mass or energy mass or energy enterng

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

3) Thermodynamic equation to characterize interfaces

3) Thermodynamic equation to characterize interfaces 3) Thermodynamc equaton to characterze nterfaces 3.1) Gbbs Model Realty: rapd contnuous change of chemcal and thermodynamc propertes Replaced by model (constant propertes up to the surface) uv bulk uv

More information

Thermodynamic Analysis for Fischer-Tropsch Synthesis Using Biomass

Thermodynamic Analysis for Fischer-Tropsch Synthesis Using Biomass A publcaton of CHEMICAL ENGINEERING TRANSACTIONS VOL. 65, 2018 Guest Edtors: Elseo Ranz, Maro Costa Copyrght 2018, AIDIC Servz S.r.l. ISBN 978-88-95608-62-4; ISSN 2283-9216 The Italan Assocaton of Chemcal

More information

Modified Redlich-Kwong and Peng-Robinson Equations of State for Solubility Calculation of Solid Compounds in Supercritical Carbon dioxide

Modified Redlich-Kwong and Peng-Robinson Equations of State for Solubility Calculation of Solid Compounds in Supercritical Carbon dioxide Indan Journal of Scence and Technology, Vol 9(16), DOI: 10.1745/jst/2016/v916/52344, Aprl 2016 ISSN (Prnt) : 0974-646 ISSN (Onlne) : 0974-5645 Modfed Redlch-Kwong and Peng-Robnson Equatons of State for

More information

( ) Phase equilibrium Some basic principles for phase calculations

( ) Phase equilibrium Some basic principles for phase calculations Chapter From Fundamentals to Propertes 6 Table. Total propertes from an excess approach V U H A G S Pure component Real mxture Ideal mxture Mxng contrbuton Excess property = * v + 0 + * v v (.0) = * u

More information

Determination of activity coefficients of dimethyl ether in butyl acetate and 2-propanol

Determination of activity coefficients of dimethyl ether in butyl acetate and 2-propanol Determnaton of actvty coeffcents of dmethyl ether n butyl acetate and 2-propanol Petar Petrov Determnaton of actvty coeefcents of dmethyl ether n butyl acetate and 2-propanol: The paper presents expermental

More information

Name ID # For relatively dilute aqueous solutions the molality and molarity are approximately equal.

Name ID # For relatively dilute aqueous solutions the molality and molarity are approximately equal. Name ID # 1 CHEMISTRY 212, Lect. Sect. 002 Dr. G. L. Roberts Exam #1/Sprng 2000 Thursday, February 24, 2000 CLOSED BOOK EXM No notes or books allowed. Calculators may be used. tomc masses of nterest are

More information

Phase equilibria for the oxygen-water system up to elevated temperatures and pressures

Phase equilibria for the oxygen-water system up to elevated temperatures and pressures Phase equlbra for the oxygen-water system up to elevated temperatures and pressures Xaoyan J 1, 2, Xaohua Lu 2, Jnyue Yan 1,3* 1 Department of Chemcal Engneerng and Technology / Energy Processes, Royal

More information

G.M.N. Costa, V.J. Pereira, R.L. Matos, G.L. Santana, A. São Pedro, E.C.M. Cabral-Albuquerque, S.A.B. Vieira de Melo *

G.M.N. Costa, V.J. Pereira, R.L. Matos, G.L. Santana, A. São Pedro, E.C.M. Cabral-Albuquerque, S.A.B. Vieira de Melo * PREDICTION OF SOLID-LIQUID-VAPOR EQUILIBRIUM FOR SUPERCRITICAL PROCESSING OF PHARMACEUTICALS USING A CUBIC EQUATION OF STATE AND GROUP CONTRIBUTION METHODS G.M.N. Costa, V.J. Perera, R.L. Matos, G.L. Santana,

More information

ME 300 Exam 2 November 18, :30 p.m. to 7:30 p.m.

ME 300 Exam 2 November 18, :30 p.m. to 7:30 p.m. CICLE YOU LECTUE BELOW: Frst Name Last Name 1:3 a.m. 1:3 p.m. Nak Gore ME 3 Exam November 18, 14 6:3 p.m. to 7:3 p.m. INSTUCTIONS 1. Ths s a closed book and closed notes examnaton. You are provded wth

More information

Assignment 4. Adsorption Isotherms

Assignment 4. Adsorption Isotherms Insttute of Process Engneerng Assgnment 4. Adsorpton Isotherms Part A: Compettve adsorpton of methane and ethane In large scale adsorpton processes, more than one compound from a mxture of gases get adsorbed,

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

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

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

Shortcut Design Method for Multistage Binary Distillation via MS-Excel

Shortcut Design Method for Multistage Binary Distillation via MS-Excel RESERCH RTICE OPEN CCESS Shortcut Desgn Method for Multstage Bnary Dstllaton a MS-Excel Mr. S. B. Dongare a, Mr..C.Shende a, Dr.V.N.Ganr a, Dr. G.M.Deshmukh a a axmnarayan Insttute of Technology, Rashtrasant

More information

Computation of Phase Equilibrium and Phase Envelopes

Computation of Phase Equilibrium and Phase Envelopes Downloaded from orbt.dtu.dk on: Sep 24, 2018 Computaton of Phase Equlbrum and Phase Envelopes Rtschel, Tobas Kasper Skovborg; Jørgensen, John Bagterp Publcaton date: 2017 Document Verson Publsher's PDF,

More information

Exercises of Fundamentals of Chemical Processes

Exercises of Fundamentals of Chemical Processes Department of Energ Poltecnco d Mlano a Lambruschn 4 2056 MILANO Exercses of undamentals of Chemcal Processes Prof. Ganpero Gropp Exercse 7 ) Estmaton of the composton of the streams at the ext of an sothermal

More information

Application of Activity Coefficient Models in VLE Determination for Azeotropic System Using Othmer Type Ebulliometer

Application of Activity Coefficient Models in VLE Determination for Azeotropic System Using Othmer Type Ebulliometer Applcaton of Actvty Coeffcent Models n VLE Determnaton for Azeotropc System Usng Othmer Type Ebullometer Manojumar M.S, B. Svapraash 2 Department of Chemcal Engneerng, Annamala Unversty, Annamala Nagar-

More information

Chemical Reaction Engineering

Chemical Reaction Engineering Lecture 19 hemcal Reacton Engneerng (RE) s the feld that studes the rates and mechansms of chemcal reactons and the desgn of the reactors n whch they take place. Web Lecture 19 lass Lecture 17 uesday 3/19/2013

More information

Available online at Energy Procedia 4 (2011) Energy Procedia 00 (2010) GHGT-10

Available online at   Energy Procedia 4 (2011) Energy Procedia 00 (2010) GHGT-10 Avalable onlne at www.scencedrect.com Energy Proceda 4 (011) 179 186 Energy Proceda 00 (010) 000 000 Energy Proceda www.elsever.com/locate/xxx www.elsever.com/locate/proceda GHGT10 Solublty of Carbon Doxde

More information

Chapter 3 Thermochemistry of Fuel Air Mixtures

Chapter 3 Thermochemistry of Fuel Air Mixtures Chapter 3 Thermochemstry of Fuel Ar Mxtures 3-1 Thermochemstry 3- Ideal Gas Model 3-3 Composton of Ar and Fuels 3-4 Combuston Stochometry t 3-5 The1 st Law of Thermodynamcs and Combuston 3-6 Thermal converson

More information

Journal of Polytechnic, 2017; 20 (1) : Journal of Polytechnic, 2017; 20 (1) :

Journal of Polytechnic, 2017; 20 (1) : Journal of Polytechnic, 2017; 20 (1) : Journal of Polytechnc, 2017; 20 (1) : 129-135 Journal of Polytechnc, 2017; 20 (1) : 129-135 Modelng Of Lqud-Lqud Equlbrum Data and Estmaton of New Bnary Interacton Parameters for NRTL Model for the Quaternary

More information

Thermodynamics. Section 4

Thermodynamics. Section 4 Secton 4 Thermodynamcs Hendrck C. Van Ness, D.Eng., Howard. Isermann Department of Chemcal Engneerng, Rensselaer olytechnc Insttute; Fellow, Amercan Insttute of Chemcal Engneers; Member, Amercan Chemcal

More information

Modeling Interfacial Tension in Liquid Liquid Systems Containing Electrolytes

Modeling Interfacial Tension in Liquid Liquid Systems Containing Electrolytes Artcle pubs.acs.org/iecr Modelng Interfacal Tenson n Lqud Lqud Systems Contanng Electrolytes Pemng Wang* and Andrzej Anderko OLI Systems Inc., 240 Cedar Knolls Road, Sute 3, Cedar Knolls, New Jersey 07927,

More information