Aspen Physical Property System - Physical Property Models

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Model Model name Phase(s) BinaryMixture Chapman-Enskog-Wilke-Lee Mixture Dawson-Khoury-Kobayashi Binary Dawson-Khoury-Kobayashi Mixture Nernst-Hartley Electrolytes DL0NST, DL1NST 246 3 Transport Property Models DV1CEWL V — X DV1DKK V X — DV1DKK V — X L X X Wilke-Chang Binary DL0WC2 L X — Wilke-Chang Mixture DL1WC L — X Surface tension models These models calculate SIGL (pure) and/or SIGLMX (mixture). Model Model name Phase(s) Pure Mixture Liquid Mixture Surface Tension SIG2IDL L — X API Surface Tension SIG2API L — X General Pure Component Liquid Surface Tension SIG0HSS, SIG2HSS L X — IAPS surface tension SIG0H2O L X — Onsager-Samaras Electrolyte Correction SIG2ONSG L — X Modified MacLeod-Sugden SIG2MS L — X Viscosity Models The Aspen Physical Property System has the following built-in viscosity models: Model Type Andrade Liquid Mixture Viscosity Liquid General Pure Component Liquid Viscosity Pure component liquid API liquid viscosity Liquid API 1997 liquid viscosity Liquid General Pure Component Vapor Viscosity Low pressure vapor, pure components Chapman-Enskog-Brokaw-Wilke Mixing Rule Low pressure vapor, mixture Chung-Lee-Starling Low Pressure Low pressure vapor Chung-Lee-Starling Liquid or vapor Dean-Stiel Pressure correction Vapor IAPS viscosity Water or steam Jones-Dole Electrolyte Correction Electrolyte Letsou-Stiel High temperature liquid Lucas Vapor TRAPP viscosity Vapor or liquid
Model Type Aspen Liquid Mixture Viscosity Liquid ASTM Liquid Mixture Viscosity Liquid Twu liquid viscosity Liquid Viscosity quadratic mixing rule Liquid Andrade Liquid Mixture Viscosity The liquid mixture viscosity is calculated by the modified Andrade equation: Where: kij mij 3 Transport Property Models 247 = = fi depends on the option code for the model MUL2ANDR. If first option code of Then fi is MUL2ANDR is 0 (Default) Mole fraction of component i 1 Mass fraction of component i Note that the Andrade liquid mixture viscosity model is called from other models. The first option codes of these models cause fi to be mole or mass fraction when Andrade is used in the respective models. To maintain consistency across models, if you set the first option code for MUL2ANDR to 1, you should also the set the first option code of the other models to 1, if they are used in your simulation. Model Model Name MUL2JONS Jones-Dole Electrolyte Viscosity model DL0WCA Wilke-Chang Diffusivity model (binary) DL1WCA Wilke-Chang Diffusivity model (mixture) DL0NST Nernst-Hartley Electrolyte Diffusivity model (binary) DL1NST Nernst-Hartley Electrolyte Diffusivity model (mixture) The binary parameters kij and mij allow accurate representation of complex liquid mixture viscosity. Both binary parameters default to zero. Parameter Symbol Default MDS Lower Upper Units Name/Element Limit Limit ANDKIJ/1 a ij 0 — — — — ANDKIJ/2 b ij 0 — — — — ANDMIJ/1 c ij 0 — — — — ANDMIJ/2 d ij 0 — — — — The pure component liquid viscosity �i *,l is calculated by the General Pure Component Liquid Viscosity model.
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Aspen Physical Property System Phys
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Contents Contents..................
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General Pure Component Solid Molar
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1 Introduction This manual describe
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Pure Component Temperature- Depende
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the Properties Parameters Pure-Comp
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2 Thermodynamic Property Models Thi
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Property Model Model Name Phase(s)P
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Property Model Model Name 2 Thermod
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Where: Parameter Name/Element 2 The
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critical temperature, the critical
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Where the ideal-gas contribution
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, where � For polar, associating
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Parameter Name/ Element 2 Thermodyn
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The denominator of equation 8 is gi
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V. V. De Leeuw and S. Watanasiri, "
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References M. Benedict, G. B. Webb,
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References L. Haar, J.S. Gallagher,
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Parameter Name/Element NTHDDH 0 †
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Gibbs free energy departure: The fo
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For a block copolymer, there is onl
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Copolymer PC-SAFT Dispersion Term T
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The association-site number of the
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Then I2(�) and I3(�) are comput
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A databank called PC-SAFT contains
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Parameter Name/Element PRKBV/1 k ij
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Predictive SRK (PSRK) This model us
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ka,ij kb,ij = = For best results, b
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J. Schwartzentruber and H. Renon, "
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Redlich-Kwong-Soave-MHV2 This equat
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‡ RKUC0, RKUC1, and RKUC2 are tre
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Parameter Name/ Element SRKLIJ/3 l
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Parameter Name/ Element Symbol Defa
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Association Equilibria Every associ
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and respectively. For the reactions
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R. W. Long, J. H. Hildebrand, and W
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Where the L, M, and N are parameter
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Alpha function Model name First Opt
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mi = Computed by equation 6 Equatio
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Parameter Name/Element 2 Thermodyna
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standard RKS alpha function, except
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These mixing rules are discussed se
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Where both Ai* and Am are calculate
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Like Huron and Vidal, the limiting
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Model Type Wilson Local composition
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Therefore, the simplified Pitzer eq
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Parameter Name/Element Symbol Defau
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Where: �i 2 Thermodynamic Propert
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The electrolyte NRTL model uses the
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Parameter Symbol No. of Name Elemen
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with Where: xi = Mole fraction of c
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It should be understood that equati
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The reference Gibbs energy is deter
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Where: j and k can be any species (
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The pure component dielectric const
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2 Thermodynamic Property Models 109
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�I *PDH = Pitzer-Debye-Hückel te
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Where: �i Vi = Activity coefficie
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Recommended cij Values for Differen
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Parameter Name/ Element 2 Thermodyn
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NRTL-SAC Reference States The NRTL-
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For an anionic component, we have M
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For a molecular segment, the activi
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Specifically, The long range intera
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where and are activity coefficients
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and Y+, are used to reflect the wid
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Parameter Name/ Element Symbol Defa
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Reference C.-C. Chen and Y. Song, "
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Parameter Name GMPTPS, GMPTP1, GMPT
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zi = Charge of ion i Subscripts c,
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For option code = 0 (default), the
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and for n-m electrolytes: 2 Thermod
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= 0.00979 Perform the necessary con
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Pitzer, K.S., J.R. Peterson, and L.
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A4,ij = gij / T + hij A5,ij = mij /
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Symmetric and Unsymmetric Electroly
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Parameter Symbol No. of Name Elemen
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Reference state for ionic component
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with 2 Thermodynamic Property Model
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G for these pairs is calculated the
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with 2 Thermodynamic Property Model
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Activity Coefficient Basis for Henr
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Where is the liquid Gibbs free ener
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Ionic components 2 Thermodynamic Pr
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the pure fused salts. Applying Eq.
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�k is the activity coefficient of
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References U. Weidlich and J. Gmehl
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ti' = �ij 2 Thermodynamic Propert
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Wagner Interaction Parameter The Wa
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References G.M. Wilson, J. Am. Chem
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Extended Antoine Equation Parameter
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IK-CAPE Vapor Pressure Equation The
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Harlacher and Braun, "A Four-Parame
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Parameter Name/Element 2 Thermodyna
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General Pure Component Heat of Vapo
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IK-CAPE Heat of Vaporization Equati
Page 197 and 198: Where: xp = Mole fraction of pseudo
Page 199 and 200: Parameter Name/Element VLBROC/1 V i
Page 201 and 202: Where: Vm l,t = Liquid volume per n
Page 203 and 204: Debye-Hückel Volume The Debye-Hüc
Page 205 and 206: DIPPR DIPPR equation 105 is the def
Page 207 and 208: Rackett The Rackett equation is: Wh
Page 209 and 210: Rackett/Campbell-Thodos Mixture Liq
Page 211 and 212: Zm RA Zi *,RA Vcm 2 Thermodynamic P
Page 213 and 214: General Pure Component Solid Molar
Page 215 and 216: Liquid Volume Quadratic Mixing Rule
Page 217 and 218: If THRSWT/6 is This equation is use
Page 219 and 220: Parameter Symbol Default MDS Lower
Page 221 and 222: General Pure Component Ideal Gas He
Page 223 and 224: (Other DIPPR equations may sometime
Page 225 and 226: General Pure Component Solid Heat C
Page 227 and 228: Parameter Name/Element 2 Thermodyna
Page 229 and 230: The expression for the liquid mole
Page 231 and 232: � Entropy: � Heat capacity: �
Page 233 and 234: Parameter Name † /Element CPIXPn/
Page 235 and 236: Option Codes for Electrolyte NRTL E
Page 237 and 238: Parameter Name Applicable Component
Page 239 and 240: For subcritical components: Hm l -H
Page 241 and 242: The vapor enthalpy is calculated fr
Page 243 and 244: Where: 2 Thermodynamic Property Mod
Page 245 and 246: Correlation algorithms for ionic sp
Page 247: Model Model name Phase(s) Pure Mixt
Page 251 and 252: (Other DIPPR equations may sometime
Page 255 and 256: �i = Viscosity of component i (N-
Page 257 and 258: Parameter Name/Element 3 Transport
Page 259 and 260: Where: The Stockmayer or Lennard-Jo
Page 261 and 262: Where: Vcij = �ij = 0 (in almost
Page 263 and 264: Where: Vcij = �ij = 0 (in almost
Page 265 and 266: Jones-Dole Electrolyte Correction T
Page 267 and 268: Letsou-Stiel The Letsou-Stiel model
Page 269 and 270: Where: The parameter is the mole fr
Page 271 and 272: Reference C.H. Twu, "Internally Con
Page 273 and 274: Vcij 3 Transport Property Models 27
Page 275 and 276: You must provide parameters for the
Page 277 and 278: Linear extrapolation of � *,l ver
Page 279 and 280: If TRNSWT/4 is This equation is use
Page 289 and 290: References R.C. Reid, J.M. Prausnit
Page 291 and 292: The mixture surface tension is then
Page 295 and 296: Where: �solv = Dielectric constan
Page 297 and 298: 4 Nonconventional Solid Property Mo
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wij = Mass fraction of the jth cons
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The oxygen and organic sulfur conte
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The complete oxidation of carbon is
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The equation for �i dm is good fo
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5 Property Model Option Codes The f
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Model Name Option Code 5 Property M
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Model Name Option Code 5 Property M
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Soave-Redlich-Kwong Option Codes Th
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Model Name Option Code HLRELNRT and
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Model Name Option Code GLRELNRT, GL
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Index A activity coefficient models
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ideal gas/DIPPR heat capacity model
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S Sato-Riedel/DIPPR thermal conduct
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Aspen Physical Property System - Physical Property Models

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