Using Accurate Models for Process Modeling. Olivier Baudouin (ProSim) Stéphane Déchelotte Alain Vacher

Size: px
Start display at page:

Download "Using Accurate Models for Process Modeling. Olivier Baudouin (ProSim) Stéphane Déchelotte Alain Vacher"

Transcription

1 Usng Accurate Models for Process Modelng Olver Baudoun (ProSm) Stéphane Déchelotte Alan Vacher

2 Outlne What are Steady State Process Smulaton Software? Importance of Thermodynamcs nsde Smulaton Software? Approaches used for Flud Phase Equlbra Homogeneous Approach (Equatons of State) Heterogeneous Approach (G E Models) New Mxng Rules for Equatons of State (EOS / G E ) SAFT Equatons of State Specfc Models Descrpton of a Thermophyscal Propertes Calculaton Server

3 Steady-State Process Smulator Tools performng rgorous mass and energy balances for all the operatng unts of a contnuous process n steady state operaton Calculaton of all process streams characterstcs (flowrate, temperature, pressure, composton, physcal propertes,...) Calculaton of performance of equpments Calculaton of all process data requred for equpment szng Calculaton of data requred for energetc analyss of a process (Pnch )

4 Typcal Process Industres Served Chemcal & Petrochemcal Processng (ammona and fertlzer plants, olefns, ethylene crackers, polymers, fne & specalty chemcals, norganc chemcals, ntermedates, solvent recovery, ) Ol & gas producton (Offshore platforms, on-shore felds and facltes, LNG plants and termnals, gas dehydraton, gas sweetenng, NGL plants, gas processng, ppelnes, ) Petroleum refnng (Crude/vacuum dstllaton, hydrocrackng, FCCU, somerzaton, alkylaton, hydrotreaters, sulfur recovery, reformers, cokers, lube processng ) Energy (Combned cycle/cogeneraton, nuclear, coal processng, gasfcaton combned cycles, water and utltes, ) and many other felds (Ar separaton, carbon capture & storage, bo-fuels, pharmaceutcals, pulp & paper, bochemcals, food and food ntermedates, ) Operatng companes as well as E&C (Engneerng & Constructon) companes n these felds For conceptual desgn, optmzaton, and performance montorng

5 Useful Throughout the Process Lfecycle R&D, lab. Conceptual development Process Engneerng Detaled Engneerng Constructon & Commssonng Operatons from expermental data regresson to optmzaton of a complete process unt or plant

6 Example of a Flash-Unt (wthout chemcal reacton) Feed P T Vapor Flowrate: V Composton: y Enthalpy: H Data: F, z, HF Parameters: P, T, Q Varables: V, L, y, x, H, h Equatons Flowrate: F Composton: z Enthalpy: HF Q Lqud Flowrate: L Composton: x Enthalpy: h Global mass balance: L + V - F = Partal mass balances: L. x + V. y - F. z = Enthalpy balance: L. h(t,p,x) + V. H(T,P,y) - F. HF(T,P,z) - Q = Thermodynamc equlbrum relatons: f v (T,P,y) = f L (T,P,x) or y = K (T,P,x,y). x Constrants: S x = 1 S y = 1 S z = 1 Thermophyscal propertes Numercal algorthms Chemcal reacton models Unt operaton models

7 Software Archtecture Unt operaton models Thermophyscal calculaton server

8 Concepton of a Dstllaton Column Influence of Relatve Volatlty Error % on the number of theoretcal stages requred a = 1.5 A+B? A B 3 25 a = 1.2 a = a = 4 5 a = Error % on the relatve volatlty (a)

9 Relatve volatlty wrt H 2 O Concepton of a dstllaton column Influence of relatve volatlty Relatve volatlty of H 2 O/x (x=hdo, HTO, D 2 O, DTO, T 2 O) W.A. Van Hook, Vapor Pressures of the Isotopc Waters and Ices, The Journal of Physcal Chemstry, 1968, Vol. 72, No 4, p HDO (model) HTO (model) 1.2 D2O (model) DTO (model) T2O (model) An error on thermodynamc model for flud phase equlbra can lead to a too bg column (several meters of packng n excess) or to a too small column (specfcatons wll not be reached) HDO (Van Hook) HTO (Van Hook) D2O (Van Hook) DTO (Van Hook) T2O (Van Hook) Temperature (K)

10 Data Requred For Accurate Results Process smulaton Pure component propertes (Tc, Pc,, P, ) Bnary propertes (VLE, LLE, excess propertes, ) Accuracy of results Basc concept The behavor of a mult-components system can be deducted from the knowledge of the behavor of the pure substances and the bnares Only expermental data of pure substances and bnary systems are requred

11 Smuls Thermodynamcs Software component for computng thermophyscal propertes and phase equlbra on pure substances or mxtures Smuls Thermodynamcs n MS-Excel, MATLAB or other applcatons

12 Smuls Thermodynamcs Thermodynamc Functons To compute thermo-physcal propertes (Transport, Compressblty, Thermodynamc, Non-deal and ther dervatves)

13 Smuls Thermodynamcs Thermodynamc Functons Flashes (LV, LLV, LL,...) To compute phase equlbra (Vapor-lqud, lqud-lqud, vapor-lqud-lqud flashes)

14 Smuls Thermodynamcs Databases (pure, BIP) Thermodynamc Functons Flashes (LV, LLV, LL,...)

15 Pure Compound Propertes Suppled wth a database of over 2 compounds based on AIChE's DIPPR database (publc release 25) 125 constant propertes (molar weght, crtcal temperature, ) 16 temperature dependant propertes (Cp, P,, Hvap ) Optonally the last publc verson of the DIPPR database can be suppled All propertes can be edted, modfed, plotted, Pure compound propertes can be estmated Or regressed from expermental data

16 Smuls Thermodynamcs Databases (pure, BIP) Thermodynamc Functons Thermodynamc Modelss Flashes (LV, LLV, LL,...)

17 A Range of Thermodynamc Models Equatons of State Soave-Redlch-Kwong (SRK) Peng-Robnson (PR) Predctve Peng-Robnson (PPR78) Lee-Kesler-Plöcker (LKP) BWRS Nakamura NRTL-PR PPC-SAFT etc Actvty coeffcents models NRTL UNIQUAC UNIFACs (Larsen, Dortmund, ) Wlson etc Combned approach models MHV2 MHV1 PSRK etc Specfc systems Pure Water (NBS/NRC steam tables - IAPS,1984) Chao-Seader, Grayson-Streed Sour-Water Carboxylc acds Formaldehyde etc Electrolytes Edwards UNIQUAC electrolyte ULPDHS Amnes etc

18 Equaton of State Approach Equatons of State derved from van der Waals Theory (1873) 2 V a b V RT P = Repulsve term (volume of molecules, b) Attractve term (nternal pressure, a) P P T 2 2 T = = At crtcal pont (T=T c, P=P c ) : 2a b RT P 3 c 2 c c T = = 6a b 2RT P 4 c 3 c c T 2 2 = = C 2 C 2 P T R a = C C P RT 8 1 b = 8 3 Z C = 2 C C C C V a b V RT P =

19 Equaton of State Approach Redlch and Kwong (1949) : P = RT V b V aa V b a = 1 T Soave (1972) : RT P = V b V a = aa V b.5 1 m 1 2 T r Peng-Robnson (1976) : a = RT P = V b V 2 aa 2 2 bv b T.5 2 Improvements: new alpha functons (Boston-Mathas, Mathas-Coppeman, Twu-Bluck-Cunnngham-Coon ), volume translaton (Peneloux) r

20 Equaton of State Approach Some other Classcal Equatons of State: Z - Z Z Z r r = Lee-Kesler (1975) : Benedct-Webb-Rubbn (194) : = = V - exp V V T c V D V C V B 1 T P V Z 2 r 2 r 2 r 3 r 4 5 r 2 r r r r r 2 e 1 T T h T g T c T f T e T d a T f T e T d a brt T E T D T C A RT B RT P 2 3 S E 3 2 A a =

21 Equaton of State Approach Equlbrum constant (vapor-lqud): K T, P, x, y = L V T, P, x T, P, y Applcaton range: «Systems composed of normal gases, rare gases, ntrogen, oxygen, carbon monoxde, hydrocarbons and some hydrocarbons dervatves. Carbon doxde, hydrogen sulfde, hydrogen and wth some lmts, some lght polar substances can be ncluded». L. Oellrch, U. Plöcker, J.M. Prausntz and H. Knapp, «Equaton of State Methods for Computng Phase Equlbra and Enthalpes, Int. Chem. Eng., 21, 1, pp 1-16 (1981)

22 Methane Pressure (atm) Equaton of State Approach Phase Envelope of a Methane Benzene (,25-,75 mol/mol) mxture mole % Methane + 75 mole % Benzene Methane vapor pressure Benzene Vapor pressure Methane Crtcal Pont Benzene Crtcal Pont Mxture Dew Curve Mxture Bubble Curve Mxture Crtcal Pont Benzene Temperature ( C)

23 Pressure (bar) Equaton of State Approach Phase envelopes for mxtures of mole % C1 and,1 mole % of nc9, dmethylcyclohexane and ethylbenzene wth NRTL-PR EoS 8 n-nonane Ethyl benzene Dmethylcyclohexane Temperatute ( C)

24 Acetone vapor mole fracton Equaton of State Approach Vapor - Lqud equlbrum curve of Acetone - Water 76 mmhg Othmer, D.F., M. M. Chdgar, Sh. L. Levy, Ind. Eng. Chem., 44, 1872 (1952) Exp. SRK Acetone lqud mole fracton

25 Heterogeneous Approach (-) Based on an actvty coeffcents model n order to take care about the non dealty of the lqud phase: Margules Scatchard Hldebrand (Regular solutons) Wlson NRTL Unquac UNIFAC Models And based on a equaton of state usable for vapor phase: Ideal gas Soave Redlch Kwong Peng Robnson Lee Kessler Plöcker

26 Acetone vapor mole fracton Heterogeneous Approach (-) Vapor - Lqud equlbrum curve of Acetone - Water 76 mmhg Othmer, D.F., M. M. Chdgar, Sh. L. Levy, Ind. Eng. Chem., 44, 1872 (1952) Exp. NRTL SRK Acetone lqud mole fracton

27 Heterogeneous Approach (-) Vapor Phase: Lqud phase: f f V L f V T, P, y = T, P, y.y. P L T, P, x = T, x.x.f T, P L L V v T,P = T, P (T ) P T exp P P T RT Equlbrum constant: K T, P, x, y = L T, X f T, P V T, P, y P Applcaton doman: Chemcal systems where complex chemcal or polar nteractons take place; low pressure and temperature (far above the crtcal pont)

28 Equaton of State Approach wth Complex Mxng Rules (EoS/G E ) Use of a unque equaton of state for the whole flud zone ncludng sophstcated mxng rules based on actvty coeffcent models: Equatons of state (cubc) Soave Redlch Kwong Peng Robnson Actvty coeffcents models Wlson NRTL UNIQUAC UNIFACs Mxng rules MHV1 MHV2 PSRK f H T, P, z = T, P, z * * T, P, z = z H T, P = H - H z P T, P

29 Equaton of State Approach wth Complex Mxng Rules (EoS/G E ) Acetone vapour molar fracton Vapor - Lqud equlbrum curve of Acetone - Water 76 mmhg Othmer, D.F., M. M. Chdgar, Sh. L. Levy, Ind. Eng. Chem., 44, 1872 (1952) Exp. NRTL SRK_MHV2_NRTL Acetone lqud molar fracton

30 Pressure (Ps) Equaton of State Approach wth Complex Mxng Rules (EoS/G E ) Acetone - Water SRK - MHV2 MR - NRTL Grswold, J. Wong, S.Y, Chem. Eng. Prog. Symp. Seres, 48, N 3 (1952) Bubble curve at 15 C Dew curve at 15 C Bubble curve at 2 C Dew curve at 2 C Bubble curve 25 C Dew curve at 25 C Expermental bubble curves Expermental dew curves Acetone molar fracton

31 log P [bar] Equaton of State Approach wth Complex Mxng Rules (EoS/G E ) 2,5 Ethanol (1) / water(2) Comparson of MHV2 n SmulsThermodynamcs TM wth expermental results Barr-Davd,F. and B.F.Dodge, J.Chem.Eng.Data, 4, 17 (1959) 2 3 C 25 C 1,5 2 C 1 15 C,5,1,2,3,4,5,6,7,8,9 1 x1, y1

32 PPC-SAFT Statstcal Assocatng Flud Theory (Chapman et al. 199) Z resdual = Z SAFT 1 = m (Z rep + Z dsp ) + Z chan + Z assoc + Polar extenson (Z pol ) µ or Q Z rep = Z réference HS = f(, ε) Dspersve-attractve f(, ε) Gubbns et Twu 1978 ε Chan f (m,) ln Z chan = ( 1 - m ) HS g ( d ) ρ Assocaton assoc, ε assooc assoc Z = ρ A 1 X A 1 2 A X ρ, X A = f ( assoc ε assooc ) µ, Q Modeled as a chan of m sphercal segments assoc ε assooc Assocaton stes

33 Pressure, MPa PPC-SAFT VLE of Hydrogen - Methane system exp [ K] exp [ K] exp [ K] exp [ K] exp [ K] exp [ K] exp [123.5 K] PPC-SAFT [ K] PPC-SAFT [ K] PPC-SAFT [ K] PPC-SAFT [ K] PPC-SAFT [ K] PPC-SAFT [ K] PPC-SAFT [123.5 K] mole fracton Hydrogen

34 P, atm PPC-SAFT VLE of Hydrogen - Toluene exp [188.7 C] PPR78 [188.7 C] exp [229 C] PPR78 [229 C] exp [269 C] PPR78 [269 C] exp [32 C] PPR78 [32 C] mole fracton Hydrogen

35 P / bar P / bar PPC-SAFT 2 VLE of polystyrene (PS) - ethylbenzene mxture (PS: M = 93 kg/mol) 1,5 1 T=14 C T=16 C Exp. Data (T=14 C) Exp. Data (T=16 C),5,1,2,3,4,5,6,7,8,9 1 w PS 2,5 VLE of polystyrene (PS) - monochlorobenzene mxture (PS: M = 93 kg/mol) 2 GROSS J., SADOWSKI G., Modelng Polymer Systems Usng the Perturbed-Chan Statstcal Assocatng Flud Theory Equaton of State, Ind. Eng. Chem. Res., 41, (22) 1,5 1,5 T=14 C T=16 C Exp. Data (T=14 C) Exp. Data (T=16 C),1,2,3,4,5,6,7,8,9 1 w PS

36 Temperature (K) PPC-SAFT VLLE of Water - 1-Butanol mxture at atmospherc pressure Exp. Bubble Exp. Dew Exp. LLE PPC-SAFT x, y 1-butanol

37 Temperature (K) PPC-SAFT VLLE of Methanol - n-heptane mxture at atmospherc pressure LLE data VLE data PPC-SAFT x, y Methanol

38 HNO3 n vapour, wt fr. Specfc models: Electrolytes H 2 O-HNO 3 : vapour-lqud composton dagram on bnary bass wt% H2SO4 n lqud (calc) 7 wt% H2SO4 n lqu (calc) 2 wt% H2SO4 n lqud (calc) 37 wt% H2SO4 n lqud (calc) 5 wt% H2SO4 n lqud (calc) 7 wt% H2SO4 n lqud (calc) 8 wt% H2SO4 n lqud (calc) wt% H2SO4 n lqud (exp) 7 wt% H2SO4 n lqud (exp) 2 wt% H2SO4 n lqud (exp) 37 wt% H2SO4 n lqud (exp) 5 wt% H2SO4 n lqud (exp) 7 wt% H2SO4 n lqud (exp) 8 wt% H2SO4 n lqud (exp) HNO3 (H2SO4 free) n lqud, wt fr.

39 Na 2 SO 4 n lqud phase (g / 1 g of water) Specfc models: Electrolytes Solublty of Sodum Sulfate n water wth respect to temperature Smulaton Exp Temperature ( C)

40 (y /x) FA / mol.mol -1 x / mol.mol -1 Specfc Models: Reactve Systems Partton coeffcent of formaldehyde at 333K and 383 K and ξ FA =.1 g.g -1 ( 383 K, 333 K). Concentraton of hemformal (HF) and poly(oxymethylene) hemformals HF 2 and HF 3 n chemcal equlbra at 276 K. 2,6 HF 1,5,4 1,2,5 HF 2 HF 3,25,5,75 1 x * ME / mol.mol -1 Partton coeffcent of FA n the FA-water-methanol system,1,2,3,4,5 x FA / mol.mol -1 Concentraton of HF, HF2 and HF3 n chemcal equlbra at 276 K

41 Temperature ( C) Mole fracton (y1) Vapor mole fracton [Y1] Specfc Models: Reactve Systems WATER (1) / FORMIC ACID (2) - Comparsons between expermental / calculated equlbrum data, pressure = 1 atm 1,9,8,7,6 [RIC6] [MEL56] [CON6] Calc. Water (1) / Formc acd (2) - Azeotropc data: Comparson expermental data / smulaton,5,4 16,8,3 14,7,2 12,6,1 1,5 8,4,2,4,6,8 1 Lqud mole fracton [X1] Azeotrope temperature [GME4] Smulaton Azeotrope composton [GME4] Smulaton,3,2,1, Pressure (kpa)

42 Smuls Thermodynamcs Compounds selecton (from databases, modfcatons, comparsons ) Graphcal User Interface Confguraton of the property model Databases (pure, BIP) Thermodynamc Functons Thermodynamc Modelss Flashes (LV, LLV, LL,...)

43 Smuls Thermodynamcs Graphcal User Interface Databases (pure, BIP) Set of Servces Thermodynamc Functons Thermodynamc Modelss Flashes (LV, LLV, LL,...)

44 A Range of Servces Avalable An nteractve calculaton servce Graphcal dsplay of propertes on temperature, pressure or composton ranges Calculaton of petroleum fractons propertes Management of group contrbuton predctve models Estmaton of pure component propertes Data regresson of pure components expermental propertes Unt conversons management tool etc Provde user wth qute all tools requred for thermodynamcs analyss

45 Smuls Thermodynamcs Graphcal User Interface Databases (BIP, Compounds) Thermodynamc functons Set of servces Thermodynamc Models Smuls Thermodynamcs Flashs (LV, LLV, LL,...)

46 Smuls Thermodynamcs Can Be Used n a Number of Ways ProSm Software Sute MS-Excel Add-In Smuls MATLAB Toolbox Thermodynamcs CAPE- OPEN "plug" Modelng tool mplementng CO Thermo Socket Aspen Plus, ProII, Aspen HYSYS, HTRI, gproms Export Usng Smuls Thermodynamcs, fles A.P.I. thermodynamc calculaton Tabulated results to : consstency between software s automatcally ensured MS-Excel Aspen TASC (PSF fle) OLGA (PVT fle) Your software (C++, VB, FORTRAN, )

47 Thank you for your attenton! Usng Accurate Models for Process Modellng Olver Baudoun (ProSm) Stéphane Déchelotte Alan Vacher

48 Equaton of State Approach wth Complex Mxng Rules (EoS/G E ) Huron Vdal (Reference state: nfnte pressure) Huron Vdal Modfed by Mchelsen (Reference state: null pressure) ex Ln x - Ln RT G = * e e ex b x b C x T, G b a x b a mod G G b V P = = e ex mod G G P MHV2 b b Ln x RT x, T, P G x - q x - q e = = a a a a MHV1,PSRK b b Ln x RT x, P T, G q 1 x e 1 = a = a

49 A Range of Servces Avalable An nteractve calculaton servce

50 A Range of Servces Avalable An nteractve calculaton servce Graphcal dsplay of propertes on temperature, pressure or composton ranges

51 A Range of Servces Avalable An nteractve calculaton servce Graphcal dsplay of propertes on temperature, pressure or composton ranges Calculaton of petroleum fractons propertes D 2887 Smulated dstllaton Results of ASTM D86 dstllaton ASTM D86 corrected Smulaton results TBP at 76 mmhg Set of components, weght composton ASTM D116 at low pressure TBP at 1 mmhg Propertes estmaton ASTM D116 at 76 mmhg ASTM D116 at 1 mmhg

52 A Range of Servces Avalable An nteractve calculaton servce Graphcal dsplay of propertes on temperature, pressure or composton ranges Calculaton of petroleum fractons propertes Management of group contrbuton methods versons Several versons are supported: UNIFAC orgnal UNIFAC (Dortmund) modfed UNIFAC (Dortmund) LL UNIFAC (Lyngby) modfed Larsen UNIFAC formaldehyde PPR78 NRTL-PR A group contrbuton models edtor s suppled

53 A Range of Servces Avalable An nteractve calculaton servce Graphcal dsplay of propertes on temperature, pressure or composton ranges Calculaton of petroleum fractons propertes Management of UNIFAC versons Estmaton of pure component propertes Data regresson of pure components expermental propertes Unt conversons management tool etc Provde user wth qute all tools requred for thermodynamcs analyss

54 Smuls Thermodynamcs Can Be Used n ProSm Software Sute Snce Smuls Thermodynamcs s a software component t must be embedded n another applcaton ProSm Software Sute Smuls Thermodynamcs Smuls Thermodynamcs s the thermodynamc "heart" of all ProSm software sute

55 Smuls Thermodynamcs Can Be Used Wthn MS-Excel MS-Excel Add-In Thermodynamc functons are added to Mcrosoft Excel and used n spreadsheets as natve functons ProSm Software Sute Smuls Thermodynamcs to perform more or less complex engneerng calculatons (wth rgorous thermodynamcs) to ft BIP of models

56 Smuls Thermodynamcs Can Be Used Wthn MATLAB Smuls Thermodynamcs s provded as a toolbox n MATLAB MS-Excel Add-In MATLAB Toolbox ProSm Software Sute Smuls Thermodynamcs Rgorous thermodynamcs become avalable n MATLAB wthout further programmng effort

57 Smuls Thermodynamcs Can Export Result Fles to Other Packages MS-Excel Add-In MATLAB Toolbox ProSm Software Sute Smuls Thermodynamcs Tabulated results to : MS-Excel Aspen TASC (PSF fle) Export fles OLGA (PVT fle)

58 Smuls Thermodynamcs Can Be Used Wthn Your Software A complete Applcaton Programmng Interface (API) s also provded Vsual Basc C++ Delph FORTRAN C# etc ProSm Software Sute MS-Excel Add-In Smuls MATLAB Toolbox Thermodynamcs Smuls Thermodynamcs can be easly embedded n any applcaton supportng the COM/DCOM technology Export fles A.P.I. However, the nterface between the embeddng applcaton and Smuls Thermodynamcs must be coded Your software (C++, VB, FORTRAN, )

59 Smuls Thermodynamcs Can Be Used Wthn CO Complant Packages ProSm Software Sute MS-Excel Add-In Export fles Smuls MATLAB Toolbox Thermodynamcs A.P.I. CAPE- OPEN "plug" Modelng tool mplementng CO Thermo Socket Aspen Plus, ProII, Aspen HYSYS, HTRI, gproms

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

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

SIMULIS THERMODYNAMICS

SIMULIS THERMODYNAMICS 2007 AIChE Annual Meeting Salt Lake City, Utah #459e CAPE-OPEN Thermodynamic & Physical Properties Interface (TD002) SIMULIS THERMODYNAMICS A CAPE-OPEN COMPLIANT FRAMEWORK FOR USERS AND DEVELOPERS Olivier

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

SIMULIS THERMODYNAMICS, JUST ONE MORE THERMODYNAMIC PACKAGE?

SIMULIS THERMODYNAMICS, JUST ONE MORE THERMODYNAMIC PACKAGE? SIMULIS THERMODYNAMICS, JUST ONE MORE THERMODYNAMIC PACKAGE? APPLICATION: MODELING OF FORMALDEHYDE-WATER-METHANOL SYSTEM AND PROPERTIES PREDICTION WITH IMPLEMENTED EoS/G E MODELS "Thermodynamik-Kolloquium"

More information

CAPE-OPEN and Simulis Thermodynamics enable you to use rigorous thermodynamics in MATLAB

CAPE-OPEN and Simulis Thermodynamics enable you to use rigorous thermodynamics in MATLAB Alain VACHER Stratège Bâtiment A BP 2738 F-31312 LABEGE Cedex FRANCE www.prosim.net Dr Michel PONS CAPE-OPEN Laboratories Network 32 rue Raulin F-69007 LYON FRANCE www.colan.org CAPE-OPEN and Simulis Thermodynamics

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

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

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

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

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

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

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

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

Method of Measuring the Vapor Pressure and Concentration of Fluids using VLE and Vibrating Tube Densitometer Apparatuses

Method of Measuring the Vapor Pressure and Concentration of Fluids using VLE and Vibrating Tube Densitometer Apparatuses Method of Measurng the Vapor Pressure and Concentraton of Fluds usng VLE and Vbratng Tube Denstometer Apparatuses Momn Elhad Abdalla Assstant Professor,Chemcal Engneerng Department, Unversty of Khartoum;

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

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

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

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

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

CALCULATION OF ACID GAS DENSITY IN THE VAPOR, LIQUID, AND DENSE-PHASE REGIONS

CALCULATION OF ACID GAS DENSITY IN THE VAPOR, LIQUID, AND DENSE-PHASE REGIONS CALCULATION OF ACID GAS DENSITY IN THE VAPOR, LIQUID, AND DENSE-PHASE REGIONS Tm B. Boyle PanCanadan Petroleum Ltd. 150-9 Avenue SW Calgary, Alberta TP 1S John J. Carroll Gas Lquds Engneerng Ltd. #300,

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

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

(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

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

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

Prediction of steady state input multiplicities for the reactive flash separation using reactioninvariant composition variables

Prediction of steady state input multiplicities for the reactive flash separation using reactioninvariant composition variables Insttuto Tecnologco de Aguascalentes From the SelectedWorks of Adran Bonlla-Petrcolet 2 Predcton of steady state nput multplctes for the reactve flash separaton usng reactonnvarant composton varables Jose

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

( ) 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

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

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

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

DETERMINATION OF CO 2 MINIMUM MISCIBILITY PRESSURE USING SOLUBILITY PARAMETER

DETERMINATION OF CO 2 MINIMUM MISCIBILITY PRESSURE USING SOLUBILITY PARAMETER DETERMINATION OF CO 2 MINIMUM MISCIBILITY PRESSURE USING SOLUBILITY PARAMETER Rocha, P. S. 1, Rbero, A. L. C. 2, Menezes, P. R. F. 2, Costa, P. U. O. 2, Rodrgues, E. A. 2, Costa, G. M. N. 2 *, glora.costa@unfacs.br,

More information

PREDICTIVE MODELING OF METAL-CATALYZED POLYOLEFIN PROCESSES

PREDICTIVE MODELING OF METAL-CATALYZED POLYOLEFIN PROCESSES PREDICTIVE MODELING OF METAL-CATALYZED POLYOLEFIN PROCESSES Neeraj Prasad Khare Dssertaton submtted to the Faculty of the Vrgna Polytechnc Insttute and State Unversty n partal fulfllment of the requrements

More information

BINARY VAPOUR-LIQUID EQUILIBRIUM FOR SYSTEMS OF INDUSTRIAL IMPORTANCE

BINARY VAPOUR-LIQUID EQUILIBRIUM FOR SYSTEMS OF INDUSTRIAL IMPORTANCE BINARY VAPOUR-LIQUID EQUILIBRIUM FOR SYSTEMS OF INDUSTRIAL IMPORTANCE By Funmlola Elzabeth Avoseh B.Sc. Chemcal and Polymer Engneerng Lagos State Unversty, Lagos state, Ngera. 2015 PREFACE The work presented

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

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

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

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

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

New Perturbation Model for Prediction of Amino Acid and Peptide Activity Coefficients

New Perturbation Model for Prediction of Amino Acid and Peptide Activity Coefficients Iranan Journal of Chemcal Engneerng Vol. 9, No. 2 (Sprng), 2012, IAChE Resea rch note New Perturbaton Model for Predcton of Amno Acd and Peptde Actvty Coeffcents M. R. Dehghan 1, E. Saleh 1,2, A. R. Fazlal

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

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

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

Investigation of High-Pressure Phase Equilibrium with the Observation of the Cloud Point

Investigation of High-Pressure Phase Equilibrium with the Observation of the Cloud Point Investgaton of Hgh-Pressure Phase Equlbrum wth the Observaton of the Cloud Pont Introducton In the last 2 decades supercrtcal solvents have had a more sgnfcant role as the solvents n chemcal reactons.

More information

McCabe-Thiele Diagrams for Binary Distillation

McCabe-Thiele Diagrams for Binary Distillation McCabe-Thele Dagrams for Bnary Dstllaton Tore Haug-Warberg Dept. of Chemcal Engneerng August 31st, 2005 F V 1 V 2 L 1 V n L n 1 V n+1 L n V N L N 1 L N L 0 VN+1 Q < 0 D Q > 0 B FIGURE 1: Smplfed pcture

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

Simulation of a steady state flash

Simulation of a steady state flash Smulaton of a steady state flash Descrpton: Statonary flash smulaton of an Ethanol(1) - Water(2) - mxture Wth followng assumptons: Apart from heater and mass flows, no energy s transferred across the system

More information

modeling of equilibrium and dynamic multi-component adsorption in a two-layered fixed bed for purification of hydrogen from methane reforming products

modeling of equilibrium and dynamic multi-component adsorption in a two-layered fixed bed for purification of hydrogen from methane reforming products modelng of equlbrum and dynamc mult-component adsorpton n a two-layered fxed bed for purfcaton of hydrogen from methane reformng products Mohammad A. Ebrahm, Mahmood R. G. Arsalan, Shohreh Fatem * Laboratory

More information

Adiabatic Sorption of Ammonia-Water System and Depicting in p-t-x Diagram

Adiabatic Sorption of Ammonia-Water System and Depicting in p-t-x Diagram Adabatc Sorpton of Ammona-Water System and Depctng n p-t-x Dagram J. POSPISIL, Z. SKALA Faculty of Mechancal Engneerng Brno Unversty of Technology Techncka 2, Brno 61669 CZECH REPUBLIC Abstract: - Absorpton

More information

Thermodynamics General

Thermodynamics General Thermodynamcs General Lecture 1 Lecture 1 s devoted to establshng buldng blocks for dscussng thermodynamcs. In addton, the equaton of state wll be establshed. I. Buldng blocks for thermodynamcs A. Dmensons,

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

Aspen Dr. Ziad Abuelrub

Aspen Dr. Ziad Abuelrub Aspen Plus Lab Pharmaceutical Plant Design Aspen Dr. Ziad Abuelrub OUTLINE 1. Introduction 2. Getting Started 3. Thermodynamic Models & Physical Properties 4. Pressure Changers 5. Heat Exchangers 6. Flowsheet

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

Three-Phase Distillation in Packed Towers: Short-Cut Modelling and Parameter Tuning

Three-Phase Distillation in Packed Towers: Short-Cut Modelling and Parameter Tuning European Symposum on Computer Arded Aded Process Engneerng 15 L. Pugjaner and A. Espuña (Edtors) 2005 Elsever Scence B.V. All rghts reserved. Three-Phase Dstllaton n Packed Towers: Short-Cut Modellng and

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

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

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

UNIVERSITY OF CALGARY. Recovery Processes. Bita Bayestehparvin A THESIS SUBMITTED TO THE FACULTY OF GRADUATE STUDIES

UNIVERSITY OF CALGARY. Recovery Processes. Bita Bayestehparvin A THESIS SUBMITTED TO THE FACULTY OF GRADUATE STUDIES UNIVERSITY OF CALGARY Phase Behavor Modelng of Complex Hydrocarbon Systems Applcable to Solvent Asssted Recovery Processes by Bta Bayestehparvn A THESIS SUBMITTED TO THE FACULTY OF GRADUATE STUDIES IN

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

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

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

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

Prediction of Ultrasonic Velocity in Binary Mixtures of a Nuclear Extractant and Monocarboxylic Acids using Several Theoretical Models

Prediction of Ultrasonic Velocity in Binary Mixtures of a Nuclear Extractant and Monocarboxylic Acids using Several Theoretical Models Predcton of ltrasonc Velocty n Bnary Mxtures of a Nuclear Extractant and Monocarboxylc Acds usng Several Theoretcal Models R. K. Mshra 1, B. Dala 1*, N. Swan 2 and S.K. Dash 3 1 BSH, Gandh Insttute of

More information

is the calculated value of the dependent variable at point i. The best parameters have values that minimize the squares of the errors

is the calculated value of the dependent variable at point i. The best parameters have values that minimize the squares of the errors Multple Lnear and Polynomal Regresson wth Statstcal Analyss Gven a set of data of measured (or observed) values of a dependent varable: y versus n ndependent varables x 1, x, x n, multple lnear regresson

More information

Reliable Phase Stability Analysis for Asymmetric Models

Reliable Phase Stability Analysis for Asymmetric Models Relable Phase Stablty Analyss for Asymmetrc Models Gang Xu 1, Wllam D. Haynes 2* and Mark A. Stadtherr 2 1 Invensys/SmSc-Esscor, 26561 Rancho Parkway South, Sute 1, Lake Forest, CA 9263 USA 2 Department

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

Calculation of Interfacial Properties of Binary Mixtures Containing Polar and Non-polar Components

Calculation of Interfacial Properties of Binary Mixtures Containing Polar and Non-polar Components Calculaton of Interfacal Propertes of nary Mxtures Contanng Polar and Non-polar Components STRCT Oscar Gabrel Nño mézquta 1, Sabne Enders 1 * 1 TU erln, Ernst Reuter Platz 1, D-157 erln, Germany * Correspondng

More information

Research Article Extension of LIR Equation of State to Alkylamines Using Group Contribution Method

Research Article Extension of LIR Equation of State to Alkylamines Using Group Contribution Method ISRN Physcal Chemstry Volume 013, Artcle ID 804576, 9 pages http://dx.do.org/10.1155/013/804576 Research Artcle Extenson of LIR Equaton of State to Alkylamnes Usng Group Contrbuton Method Zahra Kalantar,

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

Thermo-Calc Software. Modelling Multicomponent Precipitation Kinetics with CALPHAD-Based Tools. EUROMAT2013, September 8-13, 2013 Sevilla, Spain

Thermo-Calc Software. Modelling Multicomponent Precipitation Kinetics with CALPHAD-Based Tools. EUROMAT2013, September 8-13, 2013 Sevilla, Spain Modellng Multcomponent Precptaton Knetcs wth CALPHAD-Based Tools Kasheng Wu 1, Gustaf Sterner 2, Qng Chen 2, Åke Jansson 2, Paul Mason 1, Johan Bratberg 2 and Anders Engström 2 1 Inc., 2 AB EUROMAT2013,

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

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

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

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

Ph.D. Qualifying Examination in Kinetics and Reactor Design

Ph.D. Qualifying Examination in Kinetics and Reactor Design Knetcs and Reactor Desgn Ph.D.Qualfyng Examnaton January 2006 Instructons Ph.D. Qualfyng Examnaton n Knetcs and Reactor Desgn January 2006 Unversty of Texas at Austn Department of Chemcal Engneerng 1.

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

4.3 CONCLUSION: HOW TO CHOOSE A MODEL The right questions Ionic liquids What is the property of interest?

4.3 CONCLUSION: HOW TO CHOOSE A MODEL The right questions Ionic liquids What is the property of interest? Chapter 4 From Phases to Method (Models) Selection 325 4.2.7.2 Ionic liquids Ionic liquids are a new kind of solvent receiving considerable attention in the research community. These solvents are in fact

More information

ADSORPTION EQUILIBRIUM OF LIGHT HYDROCARBON MIXTURES BY MONTE CARLO SIMULATION

ADSORPTION EQUILIBRIUM OF LIGHT HYDROCARBON MIXTURES BY MONTE CARLO SIMULATION Brazlan Journal of Chemcal Engneerng ISSN 0104-6632 Prnted n Brazl www.abeq.org.br/bjche Vol. 24, No. 04, pp. 597-610 October - December, 2007 ADSORPTION EQUILIBRIUM OF LIGHT HYDROCARBON MIXTURES BY MONTE

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

Module 3: The Whole-Process Perspective for Thermochemical Hydrogen

Module 3: The Whole-Process Perspective for Thermochemical Hydrogen "Thermodynamc Analyss of Processes for Hydrogen Generaton by Decomposton of Water" by John P. O'Connell Department of Chemcal Engneerng Unversty of Vrgna Charlottesvlle, VA 2294-4741 A Set of Energy Educaton

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

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

Thermodynamic Models & Physical Properties

Thermodynamic Models & Physical Properties Thermodynamic Models & Physical Properties When building a simulation, it is important to ensure that the properties of pure components and mixtures are being estimated appropriately. In fact, selecting

More information

Parametric fractional imputation for missing data analysis. Jae Kwang Kim Survey Working Group Seminar March 29, 2010

Parametric fractional imputation for missing data analysis. Jae Kwang Kim Survey Working Group Seminar March 29, 2010 Parametrc fractonal mputaton for mssng data analyss Jae Kwang Km Survey Workng Group Semnar March 29, 2010 1 Outlne Introducton Proposed method Fractonal mputaton Approxmaton Varance estmaton Multple mputaton

More information

Prediction of the flash point of ternary ideal mixtures

Prediction of the flash point of ternary ideal mixtures Electronc Journal of New Materals, Energy and Envronment Volume No. (25), -5 url: http://ejnmee.eu/ eissn: 2367-6868 redcton of the flash pont of ternary deal mxtures M. Hrstova Unversty of Chemcal Technology

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

Assessing the use of NMR chemical shifts for prediction of VLE in nonideal binary liquid mixtures

Assessing the use of NMR chemical shifts for prediction of VLE in nonideal binary liquid mixtures Assessng the use of NMR chemcal shfts for predcton of VLE n nondeal bnary lqud mtures Q. Zhu, G. D. Moggrdge, T. Dalton, J. Cooper, M.D. Mantle, L. F. Gladden, C. D Agostno* *Correspondng Author: Dr Carmne

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

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

Chemical Engineering 160/260 Polymer Science and Engineering. Lecture 10 - Phase Equilibria and Polymer Blends February 7, 2001

Chemical Engineering 160/260 Polymer Science and Engineering. Lecture 10 - Phase Equilibria and Polymer Blends February 7, 2001 Checal Engneerng 60/60 Polyer Scence and Engneerng Lecture 0 - Phase Equlbra and Polyer Blends February 7, 00 Therodynacs of Polyer Blends: Part Objectves! To develop the classcal Flory-Huggns theory for

More information

Polymer Solution Thermodynamics. 5. Polymer Blends. Flory-Huggins Model

Polymer Solution Thermodynamics. 5. Polymer Blends. Flory-Huggins Model Polymer Soluton Thermodynamcs 5. Polymer Blends Flory-Huggns Model Up to ths pont we have consdered polymer chans n solvent at varous concentratons. In dlute soluton, we observed that the segmental densty

More information

Uncertainty in measurements of power and energy on power networks

Uncertainty in measurements of power and energy on power networks Uncertanty n measurements of power and energy on power networks E. Manov, N. Kolev Department of Measurement and Instrumentaton, Techncal Unversty Sofa, bul. Klment Ohrdsk No8, bl., 000 Sofa, Bulgara Tel./fax:

More information

LNG CARGO TRANSFER CALCULATION METHODS AND ROUNDING-OFFS

LNG CARGO TRANSFER CALCULATION METHODS AND ROUNDING-OFFS CARGO TRANSFER CALCULATION METHODS AND ROUNDING-OFFS CONTENTS 1. Method for determnng transferred energy durng cargo transfer. Calculatng the transferred energy.1 Calculatng the gross transferred energy.1.1

More information

APPLICATION OF AN ADAPTIVE NEURO INFERENCE SYSTEM FOR CONTINUOUS MONITORING AND CONTROL OF AN EXTRACTIVE DISTILLATION PLANT

APPLICATION OF AN ADAPTIVE NEURO INFERENCE SYSTEM FOR CONTINUOUS MONITORING AND CONTROL OF AN EXTRACTIVE DISTILLATION PLANT Journal of Chemcal Bahman Technology ZareNezhad, and Metallurgy, Al Amnan 48,, 203, 99-03 APPLICATION OF AN ADAPTIVE NEURO INFERENCE SYSTEM FOR CONTINUOUS MONITORING AND CONTROL OF AN EXTRACTIVE DISTILLATION

More information

Pure Component Equations

Pure Component Equations Pure Component Equatons Fttng of Pure Component Equaton Parameters DDBSP Dortmund Data Bank Software Package DDBST Software & Separaton Technology GmbH Mare-Cure-Straße 10 D-26129 Oldenburg Tel.: +49 441

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

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

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

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