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Lecture 4: Phase Equilibrium

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Lecture 4: Phase Equilibrium Lecture 4: Phase Equilibrium Equation of state for a pure (single component) gas: The pressure expansion form, which tends to be the more convenient form, is often written in terms of the coefficient for the density expansion (B) since the coefficient is easier to predict and is the one generally measured experimentally. The following approximation is therefore often used: Prediction of B: Three parameter correlation of Pitzer and Curl Parameters: Virial equation of state for a multi-component gas: Page 1 Define fugacity (escaping tendency) for a pure gas: it's baaaaaaaaaack.... Relation between and and and So that ln O is the partial molar property associated with ln O and ln Is the partial molar property associated with ln f. Using these relations it can be shown that: However, the above result yields complex results for as a function of composition. To simplify we can often use the "Lewis Fugacity Rule" which states that: so the dependence of O on composition is removed which leads to: We will show later that this is equivalent to assuming an ideal mixture of non-ideal gases. The equation of state approach is not that useful for a liquid. Instead, use the concept of activity. Page 2 Theories for liquid phase activity coefficients: Regular solution theory: Let's apply the idea of an activity coefficient to a gas mixture with the standard state being the pure real gas component at the T and P of the mixture... Now set =1 (ideal mixture) and you get (and again!) the Lewis Fugacity Rule. Lewis Fugacity Rule assumes that we have an ideal mixture of non-ideal gases. Additional relations often needed in phase equilibrium relations: Antoine Equation: Watson Equation Liquid Phase Heat Capacity The above result is the Lee-Kessler "heat capacity departure function." Cp° can be obtained from thermodynamic handbooks. Note that the dependence of Cp on pressure is given by the equation of state: Page 3 Vapor-Liquid Equilibrium (VLE) Statements of equilibrium: Raoult's and Henry's Law Select standard state for liquid so that =1 in the concentration range of intent. General equation: Raoult's Law: Henry's Law: = vapor pressure of i (xi=1) if all intermolecular forces in pure i were identical to an infinitely dilute solution. Page 4 Some simple results: For ideal gases and liquids, Ki is not a function of composition: If we use the Lewis Fugacity Rule and an average value of for each component, we will again get Ki independent of composition. These are the assumptions used to produce a DePriester Chart. Relative Volatility (also term "separation factor" may be 'inherent" or "actual" ( )) Page 5 Phase equilibrium calculations for VLE Consider the case where 5 components are present... Gibbs phase rule: Examples: 1. "Bubble T" problem Determine boiling point temperature and composition of a vapor if pressure and liquid phase composition are specified. 2. "Dew P" problem Determine the pressure and composition of liquid when a liquid is condensed from a vapor at a given temperature. Page 6 Flash Calculations: General approach when ki is a function of composition and when ki is not a function of composition. ! Chapter 2.9 of Wankat describes a simplified approach" Description Rule: Total DOF=2 if feed properties are fixed ! See page 12 for discussion on degree of freedom analysis (DOFA) Specifying product enthalpy and product pressure is equivalent to using the following control system which uses up to the available DOF Page 7 For simplicity, assume that there are no heat of mixing effects so that, if enthalpy of pure liquid i is set = 0 at 298: Page 8 .
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