Aspen Physical Property System - Physical Property Models

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The apparent fugacities and partial molar enthalpies, Gibbs energies and entropies of H2S and CO2 are calculated by standard thermodynamic relationships. The chemical reactions are always considered. The values of the coefficients for the seven equilibrium constants (A1i, ... A5i) and for the two Henry's constants B1i and B2i are built into the Aspen Physical Property System. The coefficients for the equilibrium constants were determined by regression. All available data for the four amines were used: monoethanolamine, diethanolamine, disopropanolamine and diglycolamine. You are not required to enter any parameters for this model. References R.L. Kent and B. Eisenberg, Hydrocarbon Processing, (February 1976), pp. 87-92. Maxwell-Bonnell Vapor Pressure Model The Maxwell-Bonnell model calculates vapor pressure using the Maxwell- Bonnell vapor pressure correlation for all hydrocarbon pseudo-components as a function of temperature. This is an empirical correlation based on API procedure 5A1.15, 5A1.13. This model is used in property method MXBONNEL for calculating vapor pressure and liquid fugacity coefficients (K-values). References API procedure 5A1.15 and 5A1.13. Solid Antoine Vapor Pressure Model The vapor pressure of a solid can be calculated using the Antoine equation. Parameters for some components are available for the extended Antoine equation from the Aspen Physical Property System pure component databank. This equation can be used whenever the parameter PSANT is available. The equation for the solid Antoine vapor pressure model is: Extrapolation of ln pi *,s versus 1/T occurs outside of temperature bounds. Parameter Name/ Element 190 2 Thermodynamic Property Models Symbol Default MDS Lower Limit Upper Limit Units PSANT/1 C 1i — x — — PRESSURE, TEMPERATURE PSANT/2 C 2i — x — — TEMPERATURE PSANT/3 C 3i 0 x — — TEMPERATURE PSANT/4 C 4i 0 x — — TEMPERATURE PSANT/5 C 5i 1000 x — — TEMPERATURE
General Pure Component Heat of Vaporization The Aspen Physical Property System has several submodels for calculating pure component heat of vaporization. It uses parameter THRSWT/4 to determine which submodel is used. See Pure Component Temperature- Dependent Properties for details. If THRSWT/4 is 2 Thermodynamic Property Models 191 Then this equation is used And this parameter is used 0 Watson DHVLWT 106 DIPPR DHVLDP 301 PPDS DHVLDS 401 IK-CAPE DHVLPO 505 NIST TDE Watson equation DHVLTDEW DIPPR Heat of Vaporization Equation The DIPPR equation is used to calculate heat of vaporization when THRSWT/4 is set to 106. (Other DIPPR equations may sometimes be used. See Pure Component Temperature-Dependent Properties for details.) The equation for the DIPPR heat of vaporization model is: Where: Tri = T / Tci Note: Reduced temperature Tr is always calculated using absolute temperature units. Linear extrapolation of �vapHi * versus T occurs outside of temperature bounds, using the slope at the temperature bound, except that �vapHi * is zero for . Parameter Symbol Default MDS Lower Name/Element Limit Upper Limit Units DHVLDP/1 C 1i — x — — MOLE-ENTHALPY DHVLDP/2, ..., 5 C 2i, ..., C 5i 0 x — — — DHVLDP/6 C 6i 0 x — — TEMPERATURE DHVLDP/7 C 7i 1000 x — — TEMPERATURE TC T ci — — 5.0 2000.0 TEMPERATURE Watson Heat of Vaporization Equation The Watson equation is used to calculate heat of vaporization when THRSWT/4 is set to 0. See Pure Component Temperature-Dependent Properties for details.
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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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2 Thermodynamic Property Models 121
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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
Page 141 and 142: zi = Charge of ion i Subscripts c,
Page 143 and 144: For option code = 0 (default), the
Page 145 and 146: and for n-m electrolytes: 2 Thermod
Page 147 and 148: = 0.00979 Perform the necessary con
Page 149 and 150: Pitzer, K.S., J.R. Peterson, and L.
Page 151 and 152: A4,ij = gij / T + hij A5,ij = mij /
Page 153 and 154: Symmetric and Unsymmetric Electroly
Page 155 and 156: Parameter Symbol No. of Name Elemen
Page 157 and 158: Reference state for ionic component
Page 159 and 160: with 2 Thermodynamic Property Model
Page 161 and 162: G for these pairs is calculated the
Page 163 and 164: with 2 Thermodynamic Property Model
Page 165 and 166: 2 Thermodynamic Property Models 163
Page 167 and 168: Activity Coefficient Basis for Henr
Page 169 and 170: Where is the liquid Gibbs free ener
Page 171 and 172: Ionic components 2 Thermodynamic Pr
Page 173 and 174: the pure fused salts. Applying Eq.
Page 175 and 176: �k is the activity coefficient of
Page 177 and 178: References U. Weidlich and J. Gmehl
Page 179 and 180: ti' = �ij 2 Thermodynamic Propert
Page 181 and 182: Wagner Interaction Parameter The Wa
Page 183 and 184: References G.M. Wilson, J. Am. Chem
Page 185 and 186: Extended Antoine Equation Parameter
Page 187 and 188: IK-CAPE Vapor Pressure Equation The
Page 189 and 190: Harlacher and Braun, "A Four-Parame
Page 191: Parameter Name/Element 2 Thermodyna
Page 195 and 196: 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
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Where: 2 Thermodynamic Property Mod
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Correlation algorithms for ionic sp
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Model Model name Phase(s) Pure Mixt
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Model Type Aspen Liquid Mixture Vis
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(Other DIPPR equations may sometime
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Parameter Symbol Default MDS Lower
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�i = Viscosity of component i (N-
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Parameter Name/Element 3 Transport
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Where: The Stockmayer or Lennard-Jo
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Where: Vcij = �ij = 0 (in almost
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Where: Vcij = �ij = 0 (in almost
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Jones-Dole Electrolyte Correction T
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Letsou-Stiel The Letsou-Stiel model
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Where: The parameter is the mole fr
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Reference C.H. Twu, "Internally Con
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Vcij 3 Transport Property Models 27
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You must provide parameters for the
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Linear extrapolation of � *,l ver
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If TRNSWT/4 is This equation is use
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Parameter Symbol Default MDS Lower
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References R.C. Reid, J.M. Prausnit
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The mixture surface tension is then
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Where: �solv = Dielectric constan
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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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