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Aspen Physical Property System - Physical Property Models

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Ti con,ig<br />

240 2 Thermodynamic <strong>Property</strong> <strong>Models</strong><br />

= The temperature at which one crosses from vapor<br />

state to liquid state. This is a user defined<br />

temperature that defaults to the system temperature<br />

T. Ti con,ig may be selected such that heat of<br />

vaporization of component i at the temperature is<br />

most accurate.<br />

The ideal gas enthalpy is calculated as follows:<br />

The vapor enthalpy is calculated as follows:<br />

The liquid heat capacity and the ideal gas heat capacity can be calculated<br />

from the General Pure Component Liquid Heat Capacity and General Pure<br />

Component Ideal Gas Heat Capacity, or other available models. The heat of<br />

vaporization can be calculated from the General Pure Component Heat of<br />

Vaporization, or other available models. The enthalpy departure is obtained<br />

from an equation of state that is being used in the property method. For<br />

WILS-LR and WILS-GLR, the ideal gas equation of state is used.<br />

Parameter Symbol Default MDS Lower<br />

Name/Element<br />

Limit<br />

Upper<br />

Limit<br />

RSTATE — 1 † — — — —<br />

TREFHI T i ref,ig<br />

DHFORM H i ref,ig<br />

TCONHI T i con,ig<br />

Units<br />

†† — — — TEMPERATURE<br />

— — — — MOLE ENTHALPY<br />

T — — — TEMPERATURE<br />

† Enthalpy reference state RSTATE for a component. Value of 1 denotes ideal<br />

gas.<br />

††For components with TB � 298.15 K, RSTATE defaults to 1 (ideal gas).<br />

TREFHI defaults to 298.15 K. For components with TB > 298.15 K, RSTATE<br />

defaults to 2 (liquid) and TREFHI does not apply to these components. See<br />

the Saturated Liquid as Reference State section for more details.<br />

Helgeson Equations of State<br />

The Helgeson equations of state for standard volume , heat capacity ,<br />

entropy , enthalpy of formation , and Gibbs energy of formation<br />

at infinite dilution in aqueous phase are:

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