ECH4301-Wk5 Application of Thermodynamics in process engineering

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    Application of Thermodynamics

    in Solving Process EngineeringProblem

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    Sommerfeld on thermodynamics

    Thermodynamics is a funny subject. The first

    time you go through the subject, you don't

    understand it at all. The second time you go

    through it, you think you understand it, except for

    one or two small points. The third time you go

    through it, you know you don't understand it, but

    by that time you are so used to the subject that itdoesnt bother you any more.

    - Arnold Sommerfeld (1868-1951)

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    THERMODYNAMIC PROPERTY

    MODELING FOR CHEMICAL PROCESS

    AND PRODUCT ENGINEERING : SOME

    PERSPECTIVE

    John P. OConnell; Rafiqul Gani; Paul M. Mathias; Gerd Maurer; James D. Olson;

    Peter A. Crafts; Ind. Eng. Chem. Res. 2009, 48, 4619-4637.DOI: 10.1021/ie801535a

    Copyright 2009 American Chemical Society

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    Introduction - 1

    Chemical tech has broadened & deepened-

    uses of thermodynamic properties much more

    sophisticated

    Process designs developed via computation,

    based on accurate data & complex model

    To reveal the condition need for desired product

    quality

    To optimize efficiency for sustainability

    To suggest alternative molecular structures for novel

    application (health, comfort & defence)

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    As March 2009

    45 000 000 organic & inorganic substances

    61 000 000 chemical sequences in the CAS registry

    Principles model for pure component & mixture PYTxequation of state

    Excess Gibbs free energy

    Introduction - 2

    Stateproperties

    of formation

    Reactionequilibria

    Volume Enthalpies

    Entropies

    Bulkproperties

    Component properties

    Chemical potential

    FugacityEquipment sizing

    Energy analysis

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    Property model and process model

    Process model set of mass and energy

    balance equations, as well as imposed physical,

    chemical and economic constrains, of process

    situation 2 kind of properties i)measurable, ii) conceptual

    Quantitative equilibrium or dynamic behaviour

    Property model requires spec of desired

    behaviour (properties & molecular structure) and

    then establish the process steps

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    Process and property model

    relationships.

    Published in: John P. OConnell; Rafiqul Gani; Paul M. Mathias; Gerd Maurer; James D. Olson; Peter A. Crafts; Ind. Eng. Chem. Res. 2009, 48,

    4619-4637.DOI: 10.1021/ie801535aCopyright 2009 American Chemical Society

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    Roles of property models in Process

    and Product Engineering1. Common service role

    1. A specified set of property values is provided when

    requested

    2. Process simulation

    2. Service plus advice role1. Models provide information about feasibility

    2. Process and product design

    3. Integration role

    1. Contribute to the technique of problem solution2. Developing efficient and flexible integrated simulation

    design strategies

    *Forward design approach vs Reverse approach

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    Singlephase, fixed

    T & P

    T and cchange?

    Multiplephase ?

    Q in/out?Any

    reaction?

    Model SelectionOnly V (density) needed V(T,c) J for equilibrium phase

    Enthalpy H (T, P, c, T)

    Simultaneous chemical &

    physical equilibriumProperties of formation

    * For more complicated situations, model selection may not be straightforward

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    Model Information Sources

    Molecular simulation

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    Estimation Level of empiricism

    Fundamental behavior - unknown

    or excessively complex.

    Continuous variables - by curve-

    fitting sparse experimental data

    using, for e.g. polynomials,

    loglog plots, analysis of variable

    statistical methods (ANOVA), and

    time-series analysis.Restricted to data interpolation.

    Resulting equations with fitted

    parameters should not be

    extrapolated outside the space of

    measured variables.

    Computational

    chemistry -

    calculations from

    first principles

    where it may be

    claimed that no

    data are needed.

    Include quantummechanics and

    applied statistical

    mechanics.

    Uses rigorous equations or

    models from chemical theory.

    Collections of quantities include

    parameters adjusted to fit data.

    E.g. ~ activity coefficients,

    compressibility factors, residual

    enthalpies, and entropies and

    fugacity coefficients.Relations include equations-of-

    state, group-contribution

    methods, and corresponding-

    states formulations

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    Model Development

    Essential element appropriate specification of the

    problem type and expected outcome

    E.g. ~ Develop a model for the estimation of the

    average density of polymers for the pressures andtemperatures encountered in extruding the product

    A clear delineation of model type, application range and

    expected users.

    Develop a model to predict the activity coefficients ofliquid solutions

    Must put constrain or the model must treat all types of system

    under all conditions

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    Development strategy Iterative steps.

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    Schematic phase equilibrium diagram of thebinary system formaldehyde + water. V =vapor; L = liquid; S = solid. (insert) Lower

    temperatures where an azeotrope exists atdilute formaldehyde.

    Example 1 VLE for Formaldehyde

    with Water

    The liquidvapor phase region is restricted

    to low formaldehyde concentrations since

    solids characterized as oligomers of

    poly(oxymethylene) glycols, formed from

    varying numbers of formaldehyde and watermolecules, precipitate at higher

    concentrations.

    However, even at the low formaldehyde

    concentrations, complicated phase behavior

    arises, as shown in the insert of Figure 4.

    This is attributed to the formation ofoligomers that remain in solution,

    preventing formaldehyde from volatilizing

    as well as complexing to form methylene

    gycol which can appear in the vapor phase.

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    Thermodynamic properties are usually insufficient to

    determine speciation, because there are too many

    different options, with too many parameters, that may

    correlate the data satisfactorily.

    Many of the models based on property data would be

    unreliable for extrapolation.

    The model was established some years ago when

    computational chemistry would not have been adequate

    to explore the most stable species. However, even now,

    it is essential to validate calculations with appropriate

    measurements.

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    Figure 5 shows a schematic of the vaporand liquid species equilibria with

    formaldehyde (FA), water (W), methylene

    glycol (MG = HO(CH2O)H), and its

    oligomers (MGi= HO(CH2O)iH, i> 1)

    The liquid phase, instead of

    being a binary, contains at

    least four species.

    The vapor phase is

    considered as a ternary

    mixture of the volatile species

    FA, W, and MG, since theoligomers should have vapor

    pressures that are extremely

    low.

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    The thermodynamic problem is simultaneous vaporliquid

    equilibrium for FA, W, and MG and chemical-reaction

    equilibrium for the formation of MG in both phases and the

    formation of MGi in the liquid phase.

    For the expected low-pressure distillation, the phase

    equilibrium relation chosen here assumes ideal gas vapor andnon-ideal liquid solution:

    where pis

    is the saturation pressure of the three volatilizingspecies I (i = FA, W, and MG), with xi and yi being the molefractions of volatilizing species i in the liquid phase and in thevapor phase, respectively, and i being the activity coefficient of

    species iin the liquid phase. The total pressure is indicated by p.

    s

    i i i ip x pyK !

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    The chemical reaction in the vapor phase is the formation of methylene

    glycol from formaldehyde and water:

    The species concentrations in the ideal vapor phase are related to the equilibrium

    constant, a function only of temperature, through

    where p(0) = 0.1 MPa is the standard state pressure.For reaction 1, the equilibrium constant in the liquid phase KI can be expressed with K1gas

    and the saturation pressures of the pure components and is related to the liquid phasespecies activities:

    CH2O + H2O HOCH2OH (1)

    (0 )

    1 ( ) (2)gas MG

    FA W

    y pK T

    y y p!

    1 1 (0)( ) ( ) = (3)

    s sgas FA W MG MG

    s

    MG FA W FA W

    p p xK T K T

    p p x x

    K

    K K!

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    The formation of poly(oxymethylene) glycols involves other equilibria:

    The equilibrium constant for the oligomer of degree n is

    The variation with Tofpis(T) was the Antoine form, while that of variousequilibrium constants was the usual parametrized form of

    These were selected because the range ofTwas limited and no more

    complicated relations, i.e., added parameters, could be justified. The form

    for i(T,x)was chosen to be the UNIFAC group contribution approach

    because it is predictive and the number of groups in this system is limited.

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    The vapor pressures of formaldehyde and water are available in the

    literature, but none are found for MG, as it does not exist as a pure

    substance.

    Thus, pMGs(T) for MG was estimated or treated as an adjustable parameter

    when regressing VLE data.

    The parameters for the vapor reaction equilibrium constant, K1gas(T), were

    determined by the correlation of experimental gas phase density data.

    The parameters for the otherKj(T) were found by fitting experimental NMRdata.Some of the UNIFAC parameters for the species were adjusted from

    those in the literature by regression of new VLE data.

    Model Calculation and Development

    The calculations for the simultaneous phase and reaction equilibria were

    straightforward, and no new models needed to be developed.

    Information Sources

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    Figure 6 Equilibrium concentrations of methylene glycol (MG) and poly(oxymethylene)

    glycols MG2 and MG3 in aqueous solutions of formaldehyde at 338 and 368 K:

    (experiment) Hahnenstein et al.,(41) Balashov et al.;(42) (calculated) Albert et al.(43)

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    Figure 6 shows the MG species concentrations in

    aqueous formaldehyde mixtures as calculated from the

    model in comparison with the experimental NMR data

    used to obtain the equilibrium constants.

    Since in the liquid phase more than 99% of the

    formaldehyde is converted to methylene glycol and

    poly(oxymethylene) glycols under the conditions shown

    in Figure 6, the mole fraction of (monomeric)formaldehyde is too small to show.

    Results

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    Figure 7 Vaporliquid partitioning of formaldehyde in the system formaldehydewater at 363 and 413 K:

    (experiment) Credali et al.,(45) Kogan,(46) Maurer,(47) Albert et al.,(43) Albert et al.;(44)

    (calculated) Albert et al.(44)

    Figure 7 shows a typical

    comparison betweenexperimental data and

    correlation results for the

    vaporliquid equilibrium of

    the binary system(formaldehyde + water) at

    363 and 413 K.

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    Formaldehyde also reacts with alcohols. - forms hemiformal and

    poly(oxymethylene) hemiformals with methanol.

    The above model was extended in a straightforward manner to the binary

    formaldehyde + methanol, the ternary formaldehyde + water + methanol, and

    to multicomponent systems containing trioxane and some reaction side

    products.

    The model correctly predicts that at low temperatures the presence of

    methanol results (at very low methanol concentrations) in a higher volatility of

    formaldehyde, whereas at higher methanol concentrations the volatility of

    formaldehyde is lowered.

    The thermodynamic model was also extended to describe caloric properties

    of these mixtures.

    This whole framework has been successfully applied by many companies to

    do basic engineering of processes involving aqueous solutions of

    formaldehyde. The important feature is that the species are established by,

    and their predicted amounts under some conditions are compared with,

    molecular measurements such as NMR and/or UV-VIS spectroscopy.

    Extensions

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    Example 2 - VLE for CO2 and H2S in

    Aqueous Amine Solutions over Wide

    Ranges of ConditionsSour gases, e.g., CO2 and H2S, are commonly removed from natural or

    synthesis gas by chemical absorption in aqueous solutions of amines

    (such as, 2,2-methyliminodiethanol = N-methyldiethanolamine =

    MDEA) or amine mixtures (e.g., MDEA + piperazine).

    While the competitive chemical absorption of CO2 and H2S is kinetically

    controlled, departures from equilibrium are the driving forces of such

    processes.

    The reliable design and optimization of the separation equipmentrequires knowing the chemical reaction thermodynamics and the

    vaporliquid equilibria, along with information about the energy to

    vaporize/condense the mixtures.

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    Gas absorption plants - run at ambient T & P up to 4 Mpa,

    whereas solvent regeneration is in a stripper (i.e., gas desorption) at

    elevated temperatures (over 390 K) and low pressures.

    Composition measurements show that the liquids leaving the

    absorption tower contain nearly no neutral amine and very small

    amounts of neutral sour gases, though there are large amounts of

    electrolyte reaction products such as protonated amines, bicarbonate,

    carbonate, and carbamate.

    In contrast, the liquids leaving the regeneration unit contain nearly no

    electrolytes, the sour gases have been stripped off, and the amines

    are mostly neutral.

    The latest references addressing this approach and earlier works are

    by Maurer and co-workers. A recent similar analysis related to

    postcombustion carbon dioxide capture in aqueous ammonia is given

    by Mathias et al.

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    Figure 8 shows a speciation

    scheme for the solubility of

    CO2 in aqueous solutions ofMDEA and piperazine (PIP).

    The vapor phase - have only

    CO2 (C) and water (W),

    though solvent volatilizationmight need to be treated in

    full process design.

    Liquid phase - extremely

    complicated (more than adozen species, neutral and

    ionic).Figure 8 VLE and chemical reactions in theCO2/MDEA/piperazine/H2O system.

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    Broad range of species and compositions requires a model that is able to

    describe phase behavior over a very wide range of T and P & high loading of

    amine and CO2.

    The VLE relation includes vapor-phase non-ideality and the effect of pressure

    on the liquid phase. For water, the phase equilibrium relation is

    while the extended Henrys law standard state on the molality scale

    is used for carbon dioxide because it is supercritical at most conditions

    of interest here. Consistent treatment of pressure and non-ideality withEqn 6 must be implemented

    Model Relations and Selection

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    The fugacity coefficients of saturated water vapor, water in

    the vapor mixture, and CO2 in the vapor are

    and respectively.

    Predicted by the 2nd virial equation of state (since P were

    not extremely high and the coefficients are generally more

    reliable for aqueous systems than cubic equations of state

    based on corresponding states

    The Poynting factors for liquid phase pressure effects use

    the pure liquid molar volume for water, vW, and the partialmolar volume at infinite dilution for CO2 in water, vCW

    ,

    since these are good estimates and the effects on them

    of composition and pressure can be ignored.

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    For liquid phase properties - Chemical reactions dominate (see Fig 8).

    Chemical equilibrium for reaction Rk is expressed using activities:

    where the activity of a solute species i(i.e., all species except water)is the product of its stoichiometric molality and its activity coefficient

    appropriate for the Henrys Law standard state, denoted with *:

    For water, the activity, aw, is calculated via integration of theGibbsDuhem equation using the activities of all the solutes.

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    The temperature-dependence of the chemical

    equilibrium constant

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    The scheme shown in Figure 8 involves extensive information.Parameters for the equilibrium constants were provided from the literature

    cited above.

    The Henrys law constant is that for unreacted carbon dioxide in water, which

    along with pWs, vW, and the second virial coefficients, which, along with the

    estimation method forvCW were taken from in the literature.

    The Pitzer model for Gibbs excess energy requires binary and ternary

    parameters to describe the interactions between solute species from low gas

    loadings (i.e., at low partial pressures of carbon dioxide) to high gas loadings

    (i.e., at high partial pressures of carbon dioxide).

    The only source for obtaining reliably the most important parameter values is

    experimental data of the solubility of CO2 in aqueous solutions of MDEA and of

    piperazine at low, as well as at high, CO2 partial pressures.

    Such investigations were performed with two different types of experimental

    equipment.(50, 51, 60)

    Information Sources

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    Figure 9 Partial pressure of carbon dioxide (left diagram) and total pressure (right diagram) above

    liquid mixtures of (CO2 + MDEA + H2O), mMDEA 2 molkg1: (experiment)(60) 313, 353, 393 K; (experiment)(61) 313, 333, 373, 393, 413 K; (calculation) correlation from all

    data, - - - from only high pressure data.(60)

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    Figure 10 Carbon dioxide partial pressure (left) and total pressure (right) above liquid mixtures of

    (CO2 + MDEA + H2O), mMDEA 8 molkg1: (experiment)(59) 313, 353, 393 K;(experiment)(60, 61) 313.7, 354.4, 395 K; (calculations) correlation from all data, - - - from

    only high pressure data.(60)

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    The solid lines in Figure 9 and 10 show the excellent comparisons

    between experimental(60, 61) and model results(60) for CO2 solubility

    in aqueous solutions at low (Figure 9) and high (Figure 10) MDEA

    molalities.

    In addition, the broken lines in both figures show predictions at lowpartial pressures of carbon dioxide when all interaction parameters

    were estimated by using only high-pressure gas solubility data.

    These predictions agree well with low pressure experimental data at

    low and moderate amine concentrations (high C/MDEA values) but are

    less accurate at higher amine concentrations where parameters

    characterizing important interactions between molecular MDEA and

    other solute species were not included, as they cannot be determined

    from high pressure gas solubility data.

    Results

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    This example illustrates the very great range of data thatmust be assembled in order to reliably develop a full model

    for a truly complex system.

    Note that every aspect was compared with data and

    sensitivity to parameters was tested.

    Compared to the first case, fewer molecular

    measurements were available, though the speciation was

    generally known.

    It is possible that computational chemistry methods could

    apply here, but this work was done before they were ready

    for implementation.

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    Example 3 LLE of carboxylic Acid from

    Aqueous Solution Many carboxylic acid products are produced by fermentation. Product

    recovery from the dilute aqueous solutions is achieved by reaction with

    a hydrophobic component, e.g. tri-n-octylamine (TnOA), with theresulting complexes extracted into an organic phase.

    Subsequently, the carboxylic acid must be separated and the auxiliary

    component regenerated. The design of such extraction and recovery processes requires a

    thermodynamic model for liquidliquid equilibria that accounts for

    electrolytes in both aqueous and organic liquid solutions.

    Our example is for citric acid partitioning between water and different

    organic solvents in the presence of TnOA, including the effect of saltson the TnOA partitioning for recovery and regeneration.

    The latest references summarizing this approach are by Maurer and

    co-workers.

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    At low aqueous-phase molalities of citric acid and fixed TnOA - the ratio of

    organic to aqueous phase concentrations of citric acid increases with

    increasing acid concentration.

    It then passes through a maximum and decreases at the highestconcentrations.

    This behavior is attributed to two competing effects.

    At low acid concentrations in the aqueous phase, the dissociation equilibrium

    for citric acid is shifted to its ionic species.

    As only neutral acid molecules can be extracted into the organic solvent, the

    partition coefficient increases when the amount of dissolved neutral citric acidincreases.

    The decrease of the partition coefficient observed at high acid concentrations

    results from complete complexation of the TnOA, so additional citric acid

    cannot be bound, and the acid remains in the aqueous phase.

    In such processes the aqueous phase may also contain strong electrolytes.

    While most strong electrolytes reduce the solubility of an organic compoundin an aqueous phase, i.e., salt-out the organic compound, the presence ofsalt actually reduces the partitioning of a carboxylic acid to the organic phase

    when a complexing agent, such as TnOA, is present.

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    Figure 11 Partition coefficient of citric acid (PCit(m) = mCit(org)/mCit(aq)) in theaqueous/organic two-phase system (citric acid + water + MIBK + TnOA + NaNO3) at

    298.15 K for equal volumes of the aqueous and the organic feed solutions at constant

    TnOA concentration (mTnOA(org),(0) = 1.24 molal) in the organic feed and several saltconcentrations in the aqueous feed solution:(63) (experiment) mNaNO3(aq),(0) = 0,= 0.01, = 0.05, = 0.1 molal; prediction.

    Figure 11 shows

    the influence of

    NaNO3 on thepartition

    coefficient of citric

    acid in the organic

    phase relative to

    aqueous phase

    for the system(citric acid + water

    + MIBK + TnOA +

    NaNO3)

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    For this complex system, the fugacities of the coexisting liquid phases are

    treated with the aqueous phase as an electrolyte solution as in eqs 6 and 8,

    while the organic phase has only neutral species as in eq 1.

    Pitzers excess Gibbs energy model is used in both phases.

    It has terms associated with electrostatics and ions in the aqueous phase,

    while a power-law equation is used for the organic phase.The organic-phase complexes of citric acid and TnOA are in chemical

    reaction equilibrium; most contain water, as verified by IR-spectroscopy.

    The stoichiometry of the complexes depends on the organic solvent and can

    be complicated.

    For example, two complexes (citric acid:TnOA:water = 2:3:2 and 1:1:1,

    respectively) were found for toluene, whereas four complexes (1:0:3, 1:2:3,1:1:3, and 2:1:6) were in methyl isobutyl ketone (MIBK).

    The equilibrium constants for the various reactions were expressed as in

    eqs 4, 5, 7, and 8. Figure 12 shows the resulting speciation for liquidliquid

    equilibria with toluene.

    Model Relations, Selection, and

    Information Sources

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    Figure 12. Speciation in liquidliquid

    phase equilibria for the system (citric

    acid + water + toluene + TnOA).

    Figure 12 shows the resulting

    speciation for liquidliquid

    equilibria with toluene.

    The equilibrium constants for

    the various reactions were

    expressed as in eqs 4, 5, 7,

    and 8. Figure 12 shows the

    resulting speciation for

    liquidliquid equilibria withtoluene.

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    Comparisons between predictions and experimental data

    are also shown in Figure 11; the agreement is within

    experimental uncertainty.

    When NaNO3 is added to equal volumes of aqueous andorganic feed solutions (NaNO3(aq),(0) = 0.05 mol kg1;

    TnOA(org),(0) = 1.24 mol kg1) giving Cit.tot(aq) = 0.02

    mol kg1 in the equilibrated aqueous solution, the

    partition coefficient of citric acid to the organic phase is

    about 0.4 compared to about 40 in the salt-free system.

    When NaCl is the salt under the same conditions, the

    value is about 10.

    Results

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    A number of applications have been made by adding other reactive

    components to the scheme of Figure 12.

    The partitioning of inorganic acids (HCl, HNO3, and H2SO4) in TnOA-

    containing two-phase systems with toluene and MIBK and chloride

    partitioning in the system (citric acid + water + MIBK + TnOA + NaCl) have

    been studied.The addition of the salt of the carboxylic acid was predicted not to affect

    the partitioning of the acid, as there is no competition of different acids for

    the amine; this is found to be true for monocarboxylic acids like acetic acid,

    though not for acids with more than one carboxylic group.

    The model predicts all of the above behavior quantitatively, verifying the

    thermodynamic framework.

    Again, comprehensive use of, and comparisons with, many different data,

    along with careful speciation, allows quantitative description of many

    variations of these complex solutions. The results can be used for testing,

    for exploring options in process synthesis, and for process optimization.

    Extensions

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    Example 4 VLE for oleum

    Oleum, also known as fuming sulfuric acid, consists of SO3 dissolved in

    100% H2SO4.

    Thus, for example, 20 mol % oleum consists of 20% SO3 and 80% H2SO4by moles.

    The modeling objective is to provide VLE and heat of vaporization

    information for the system components in a case where corrosion andtoxicity make extensive measurements extremely challenging.

    There are known to be many different species complexes in the liquid

    phase of oleum in addition to the H2SO4 and SO3 components.

    However, the dominant complex is H2S2O7 which is formed from 1 mol each

    of H2SO4 and SO3 by the complexation reaction proposed by Nilges and

    Schrage(67) and by Mathias et al.:(68)

    No ions are considered to exist in the solution.

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    Model Relations, Selection, and

    Information Source

    The phase equilibrium is obtained with liquid fugacity expressions of the

    form of eq 1 and vapor fugacity expressions of the form of eqs 6 and 7.

    The activity coefficients were obtained from the NRTL excess Gibbs energy

    model since the non-ideality is strong.

    For this system where SO3 is the principal volatile component, the effect on

    VLE of parameters for the H2SO4H2S2O7 pair is very small and is thereforeignored.

    However, parameters for the SO3H2SO4 and SO3H2S2O7 pairs must be

    valid over a range of temperature both for VLE and for calorimetric

    properties.

    Since the pressure is elevated, there is vapor-phase non-ideality that was

    described by the RedlichKwong equation with standard parameters basedon critical properties.

    This is not expected to be rigorous, but the conditions are such that the

    limited composition dependence of the vapor non-ideality minimally affects

    the predicted behavior.

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    Figure 13 Comparisons of experimental data(71) and model calculations () for vapour

    pressures of oleum mixtures.

    Published in: John P. OConnell; Rafiqul Gani; Paul M. Mathias; Gerd Maurer; James D. Olson; Peter A. Crafts; Ind. Eng. Chem. Res. 2009, 48,4619-4637.

    DOI: 10.1021/ie801535aCopyright 2009 American Chemical Society

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    reaction equilibria of the system

    Defined by the equilibrium constant for reaction III plus the non-idealities of

    the three species in their liquid mixture:

    where the temperature dependence ofKoleum(T) is that of eq 5 plus polynomialsin T.

    Miles et al.(70) used two methods to measure the enthalpy of vaporization: (1)

    evaporation of SO3 from oleum under reduced pressure and (2) heat of solution

    (three sets of data) of addition of SO3 to oleum.

    The enthalpy of mixing used for matching the calorimetry data is obtained from

    the temperature dependence ofKoleum(T) and ofGE via the GibbsHelmholtz

    relation

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    Results

    Figure 14 shows experimental data(70) and model calculations for the

    enthalpy of vaporization of SO3 from oleum mixtures of various

    concentrations at 30 C.

    The enthalpy of vaporization here is the negative of the enthalpy change

    that occurs at 30 C when 1 kg of gaseous SO3 is dissolved in a largequantity of an oleum mixture of the given concentration.

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    Comparison between experimental data(70) and model calculations for

    enthalpy of vaporization of SO3 from oleum mixtures of various

    concentrations at 30 C.

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    The sigmoidal shape of the enthalpy of vaporization curve is a clear

    fingerprint that strong chemical reactions are involved.

    At low SO3 concentrations, essentially all the added SO3 combines with

    H2SO4 to form H2S2O7.

    Hence, the total enthalpy of vaporization is approximately equal to theenthalpy of vaporization of pure SO3 ( 540 kJ kg

    1) plus the heat of reaction

    ( 210 kJ kg1).

    At about 50 mol % SO3 (45 wt % SO3), the amount of free H2SO4 has

    substantially decreased, so reaction does not occur and the enthalpy of

    vaporization rapidly decreases toward the enthalpy of vaporization of pure

    SO3.

    This is another example where success is obtained with an appropriate

    conceptual model and multiproperty fitting of quality data, though no

    molecular measurements were involved.

    In particular, calorimetric data proved quite valuable in validating a proposed

    chemistry model, given by the signature in the enthalpy of vaporization vsconcentration curve.

    This case shows how a speciation can be validated by careful use of both

    phase equilibrium and calorimetric data, giving a better chance of finding the

    most appropriate description.

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    Solvent Selection for

    Pharmaceutical Production

    Introduction

    Challenges to develop efficient environmentally friendly process for API

    only 1 in 10 new drug candidates survives through clinical trials to enter themarket

    not economical to collect large quantities of thermophysical data since thesystems frequently change

    predictive thermodynamic models to reduce the experimental search space

    Modern drugs are functionally complex(72) and often fall beyond thecapabilities of traditional predictive models like UNIFAC

    The reliable prediction of crystal structure and solid-state properties iscomputationally demanding, and still years away from mainstream application

    3 examples of service and advise role

    Typically, the industry deals with complex chemistry,(74) phase equilibriainvolving organic salts, and aqueous electrolytes. These factors make it clearthat pharmaceutical systems challenge the capability of modern property tools

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    Example 1 - Anisole Removal during

    Washing and Drying Operations

    In this problem, an environmentally friendly solvent is needed to wash and dry

    a crystalline pharmaceutical intermediate.

    The solvent must efficiently remove anisole residues from upstream

    chlorination and coupling reactions, where the product is precipitated as an

    organic HCl salt and separated by pressure filtration to yield a 40% w/wanisole wet cake.

    Due to anisoles low volatility, removing the residual anisole via inert gas drying

    is very slow and not commercially viable.

    Washing first with a more volatile solvent can increase the drying rate, and

    MTBE was used in early process development.

    However, at production scale, MTBE would possibly have required specificVOC abatement equipment, so a search for a better wash solvent was

    initiated.

    The final wash solvent was to be environmentally preferred, fully miscible with

    anisole, and promote vaporization of residual anisole.

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    Model Relations, Selection, and

    Information SourcesTo solve the above solvent selection problem, the solvent needs are

    translated into target properties.

    Table 1 lists an appropriate set of pure component and mixture property

    values.

    The boiling point and melting point indicate the liquid range.

    The key property to characterize the ease of anisole removal is the partialpressure, yip. As computed via eq 1, this quantity is increased by selecting awash solvent that gives anisole activity coefficients as large as possible.

    Since the anisole will be dilute after washing, the relevant activity coefficient

    for screening is its limiting value at infinite dilution, A,S.

    Thus, the solvent power, Sp, is used to rank prospective wash solvents for

    anisole volatilization

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    The miscibility criterion is explicit. In addition to Sp, the Hansen

    solubility parameters, h and p,(75, 76) were used to reduce the

    solvent search space since the feasible solvent candidates are to

    have low affinity for ionic solutes; i.e., small terms for hydrogen

    bonding and polarity.

    Finally, the functional groups were limited to those with goodenvironmental profiles.

    The ProCAMD solvent search software(77) was used to find

    solvent candidates matching the target properties listed in Table 1.

    The pure component target properties were first estimated from

    generated molecular structural information via the

    ConstantinouGani or MarerroGani(78) method.

    Those structures (molecules) satisfying the target values were then

    examined for Sp and miscibility with the UNIFAC-LLE model.

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    Results

    A set of solvent candidates was identified among the 26837 molecular

    structures generated by excluding 13698 substances by the hparameter; 3533 by p; 2925 by Tmelt; 6484 by Tboil; 62 by Sp; and 7 by

    miscibility. That left 47 acceptable candidates as possible solvents;

    Table 2 shows representative properties of four candidates.

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    Of these, heptane was selected as the wash solvent for its Sp value,commercial availability, volatility, and environmental profile (fugitive

    releases to the atmosphere).

    Figures 15 and 16 show activity coefficients for anisole with the

    original MTBE wash solvent and the heptane replacement as

    predicted by the UNIFAC method.(79)

    The value of ln A,S in heptane is about a factor of 3 greater than that

    for MTBE.

    In pilot plant trials with heptane, the drying step was considered rapidat about 7 h, and residual anisole levels were significantly reduced.

    Perhaps most importantly, the VOC emissions were reduced from

    0.15 mol fraction for MTBE to 0.02 mol fraction for heptane.

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    Binary solution activity coefficients for MTBE

    and anisole predicted by UNIFAC.(79)

    Binary solution activity coefficients for

    heptane and anisole predicted by

    UNIFAC.(79)

    This example of solvent substitution demonstrates how group contribution

    methods may be applied in reverse and thus narrow the size of a search

    space and minimize time-consuming laboratory experiments.

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    Example 2 - Solvent Selection for an

    Enantiomeric PharmaceuticalThe synthesis of drugs often results in intermediates containing racemic

    mixtures of left- and right-handed enantiomers of chiral molecules. For esters,

    it is sometimes possible to use a catalytic lipase enzyme in an aqueous

    alcohol mixture to selectively dissociate the undesirable enantiomer into its

    acid via the reaction:

    After dissociation, the chirally resolved ester is easily separated from the acid

    and alcohol using pH-buffered liquidliquid extraction. A final crystallization

    yields the desired product. Finding the optimal conditions for the dissociation

    in a pH-buffered liquid extraction depends on estimating accurate values of

    the acid and ester dissociation equilibrium constants or pKa, while selection ofoptimal solvent(s) is needed for both partitioning and for crystallization.

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    Model Relations, Selection, and

    Information SourcesSeveral properties must be estimated for the process steps: the pKa valuesfor the ester and acid as well as LLE for extraction and SLE for

    crystallization of the product with the proposed solvents. A review of pKapredicting methods is presented in ref80. Note that there are two pKas forthe ester and three for the acid. Software from ACD Laboratories(81) was

    used to predict the pKas for these organic molecules with the values givenin Table 3. The OH groups on the reaction product alcohol and on the t-butanol are relatively stable and do not need to be considered.

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    Using straightforward calculations, the distributions of the species can be

    found as functions of pH. These are shown for the ester and acid in Figures

    17 and 18. Above pH 10, the ester is present in the uncharged state, while

    the acid is fully deprotonated with a charge of negative one. Under theseconditions, the partitioning gives maximum separation efficiency, since

    charged species prefer the aqueous phase, while the neutral ester prefers

    the organic phase. The pH is adjusted by adding a bicarbonate salt, since

    this acts as a sufficiently strong inorganic base for buffering during extraction

    but is not strong enough to hydrolyze the ester.

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    Species distributions for racemic ester

    dissociation as functions of pH.

    Species distributions for racemic acid formation

    as functions of pH.

    After a water wash to remove the bicarbonate and subsequent decanting, thepurified ester product is in a stream rich in t-butanol and saturated withapproximately 30% w/w water. However, direct crystallization of the product

    by cooling this solution gave a poor yield; the product solubility in aqueous t-butanol was too high. Thus, a solvent was sought where the product could be

    extracted for crystallization.

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    Experimental screening of product solubility suggested toluene would be a

    good crystallization solvent, but the yield from the actual process solution

    turned out to be poor. The reason is clear from the ternary LLE diagram of

    Figure 19, predicted with the original UNIFAC LLE parameters.(79) It

    shows tie lines and a binodal curve with t-butanol favoring the toluene-richorganic phase rather than the aqueous phase. Alternatives to water, while

    keeping toluene, were sought using the search criteria of Table 4, similar

    to the process above. In this case, the normal melting point and boiling

    point were estimated from group-contribution methods for pure

    component properties; for the liquid density, the Rackett equation(22) was

    used, while for the selectivity of the product for the organic phase and

    miscibility calculations, the UNIFAC-LLE model(79) with the associatedparameters was used.

    Result

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    Liquid phase compositions for aqueous t-butanol with toluene at T= 25 C, 1 atm from UNIFAC-LLE.(79)

    Published in: John P. OConnell; Rafiqul Gani; Paul M. Mathias; Gerd Maurer; James D. Olson; Peter A. Crafts; Ind. Eng. Chem. Res. 2009, 48,4619-4637.

    DOI: 10.1021/ie801535aCopyright 2009 American Chemical Society

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    The search led to three substances expected to be commercially available,

    with the properties shown in Table 5. With the best solvent, 1,3-propylene

    glycol, the LLE phase diagram appeared as in Figure 20. The tie linesbetween the toluene-rich and glycol-rich phases show the desired

    selectivity fort-butanol, but the two-liquid region extended too little towardthe t-butanol apex. It was concluded that toluene would not provide acommercially viable batch extraction process. Further solubility screening

    identified cyclohexane as a potential crystallization solvent, so it was

    examined as an extraction solvent, by modifying the polar solvent search

    criteria given in Table 4 to include selectivity with cyclohexane and an

    updated density limit of 0.8 g/mL.

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    Ternary LLE fort-butanol, 1,3-propylene glycol, and toluene at T= 25 C, 1 atm from UNIFAC-LLE.(79)

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    Again, the propylene glycols were identified as the top-ranking candidates.

    The phase diagram of Figure 21 for 1,3-propylene glycol with cyclohexane

    and t-butanol shows fully desirable characteristics. The two-liquid regionextends to a 50:50 volume ratio of cyclohexane to t-butanol, and the t-

    butanol partition coefficients are more appropriate for productivity. In fact, justtwo washes with propylene glycol reduces the t-butanol content to about 3%w/w with a residual level of propylene glycol in the organic phase of only

    0.5% w/w. This scheme gives good productivity in generic batch

    manufacturing equipment, which is common to the pharmaceuticals industry.

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    Ternary LLE fort-butanol, 1,3-propylene glycol, and cyclohexane at T= 25 C, 1 atm from UNIFAC-LLE.(79)

    Adequate success in this conceptual design project was obtained by flexibly

    searching for alternative solvents using phase equilibrium representations of

    multicomponent systems as computed from group contribution methods.

    Identifying the desired partitioning in the ternary system was particularly crucial.

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    Example 3 - Selection of Binary Solvent

    Mixtures for a Crystallization Process

    This example concerns a pharmaceutical intermediate produced by reaction

    in tetrahydrofuran (THF) with the desired product obtained by crystallization.

    The yield from THF alone was found to be poor, and water was introduced as

    an antisolvent to increase the yield. Laboratory test results showed

    inconsistencies, and it was suggested that the actual amount of water in the

    crystallization solvent was varying because of carryover from an upstream

    washing step. Predictions of the solubility in the aqueous THF solution were

    made to determine how water content could affect the product solubility.

    Details of this application can be found in ref82. This example highlights the

    use of techniques other than group contribution (GC) when the necessary

    parameters for a GC-based method are not available.

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    Model Relations, Selection, and

    Information SourcesThe structure of many heterocyclic pharmaceutical molecules cannot be

    treated with GC-based models like UNIFAC, due to missing functional

    groups or interaction parameters. The NRTL-SAC model(83) is an

    alternative approach which uses characteristic surface segments to describe

    intermolecular interactions from surface charge density. The NRTL binary

    interaction parameters between the segments are fixed, and there are

    adjustable characteristic segment values for each molecular species. The

    NRTL-SAC database contains segment profiles for 130 solvents derived

    from available literature VLE and LLE data. For a particular solvent, the 4

    solute segment parameters are regressed from solubilities in at least 4, and

    up to 10, pure solvents spanning the expected surface segment values. This

    will allow prediction of solid solubility of a solute, in pure or binary solvents of

    the components in the database, with sufficient accuracy for solvent-ranking

    and trends in ternary systems. For the present system, an NRTL-SAC model

    was established from existing solubility data in 25 pure solvents over the

    temperature range of 1080 C.

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    Results

    The solubility of the pharmaceutical intermediate in mixtures of THF and

    water with the regression and prediction results shown in Figure 22, along

    with solute solubilities in the mixed THFwater solvent shown in detail inFigure 23. While the calculated values were sometimes far from

    experiment, they were adequate for the purposes of the problem. Figure 23

    shows that water was acting unexpectedly. At low concentrations, it is a

    cosolvent, increasing the solubility. At higher amounts, the water depresses

    solubility. The strong variation with the water fraction suggested why the

    laboratory tests on the process stream were not consistent: fluctuatingcarryover combined with extreme sensitivity to composition.

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    Regression results of NRTL-SAC

    model(83) parameters for 25 puresolvents.

    Experimental and predicted solubilities of product

    in THFwater mixtures.

    From these results, a different and more robust crystallization process was

    developed. The key was the estimation of solubilities and careful scrutiny of the

    sensitivity of properties to variations in conditions.

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    5. Emerging Methods for Property

    Estimation

    The examples given above demonstrate current approaches and capabilities

    for property modeling when data sources are available or the opportunity for

    new measurements exists. We now give two examples using advanced

    techniques to overcome the limitations of current approaches such as group-

    contribution methods. They use contemporary computational techniques

    either directly or indirectly to predict phase equilibria. The first describes how

    unavailable group-contribution parameters can be obtained with a new

    method based only on chemical structure, with application to VLE. The

    concept is appealing, and it suggests an avenue for future developments. The

    other is for a separations process and compares different modeling

    techniques, including molecular methods. The results have implications forefforts to improve predictive modeling capabilities.

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    Estimation of Group-Contribution

    ParametersRecently, Gani et al.(84) have suggested how already availableexperimental data might be used to predict group-contribution model

    parameters that are missing in a host tabulation, such as the

    MarreroGani(78) group-contribution method for pure component

    properties. The basis is an atom-connectivity index, developed under the

    principle of additivity of contributions of different descriptors for a specific

    property that gives contributions to molecular properties by atoms and theirconnectivities. With atoms, many fewer parameters are needed to

    represent groups of atoms. Further, index parameter values for

    connectivity indices can be found from the same available experimental

    data as for regressing group-contribution parameters. Combining known

    group contributions (GC) with estimated group contributions from atom-

    connectivity indexes (CI) results in an approach called GCplus. The methodcan be applied to any host group contribution model. Extension to a wide

    range of property models for pure component properties and to average

    properties of polymer repeat units has been made

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    Gonzalez et al.(86) have applied the GCplus approach to predict missing

    group-interaction parameters when the host method is the UNIFAC model for

    activity coefficients (GC). The available experimental data used for UNIFAC

    group contributions were employed in regressing the interaction parametersfor the atom-connectivity indices (CI). Then, the CI values were used to

    estimate missing group-interaction parameters.

    Examples applying GCplus to pure component properties are given in refs

    8486. Here, we illustrate GCplus for mixture properties. In each case, the

    chemicals and the phases of interest are given along with the host model and

    the group(s) with missing values. Then predicted UNIFAC group parametersare given, along with comparison of predicted and measured phase behavior

    results.

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    VLE for 1,2-DichloroethaneDMSO

    If the original UNIFAC-VLE model(87) is the base method, the missing

    group interaction parameters are for the pair CCl and DMSO. Using the CI

    method, estimates of the missing group interaction parameters are listed

    in Table 6. Figure 24 shows TxyVLE comparisons from using theseparameters along with the GC parameters in the UNIFAC table with

    measured VLE.(88) These data were not used for the CI-model parameterestimation, but the agreement is excellent

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    TxyVLE diagram at 0.953 bar for 1,2-dichloroethane with DMSO from the UNFAC-CI method with parameters not used for the

    CI model regression compared to measured values: (experiment)(88).

    Published in: John P. OConnell; Rafiqul Gani; Paul M. Mathias; Gerd Maurer; James D. Olson; Peter A. Crafts; Ind. Eng. Chem. Res. 2009, 48,4619-4637.

    DOI: 10.1021/ie801535aCopyright 2009 American Chemical Society

    SLE f A i h

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    SLE for Acetaminophen

    (Paracetamol) with 1-Butanol

    If a later revision of the original UNIFAC-VLE model(86) is the host for this

    system, only the ACNH2CH2CO interactions are missing. However, for

    illustration, we also present results when all the group interactionparameters are obtained via CI. Table 7 lists GCplus group interaction

    parameters for the system where those for ACNH2/CH2CO (in bold) are

    estimated with CI. Table 8 lists the parameters when all are estimated from

    CI. The values are different. Figure 25 shows the comparisons of the results

    for both cases with data.(89) Over the limited range of paracetamol

    compositions, both sets of parameters describe the data well. Thus, whileparameter values may differ, the data can be adequately predicted with both

    methods.

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    Figure 25. Solubility of paracetamol in 1-butanol as a function of

    temperature estimated with CI-generated values: only for

    ACNH2/CH2CO groups (original UNIFAC(87) parameters for other

    groups), - - - all parameters estimated from CI; (experiment)(89

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    VLE for Methylethylketonen-Heptane

    This system involves only the CH2 and CH2CO groups, but there is a

    significant temperature variation to be dealt with. The later UNIFAC model(90)

    has parameter values, so a comparison can be made among data, GC

    prediction, and CI prediction. The CI-computed parameter matrix with

    temperature dependence is given in Table 9

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    VLE for the methylethylketonen-heptane system at 318.15 K: calculated with UNIFAC(90) group-contribution parameters, - -

    - calculated with CI-estimated group-contribution parameters; (experiment)(90) y, x.

    Published in: John P. OConnell; Rafiqul Gani; Paul M. Mathias; Gerd Maurer; James D. Olson; Peter A. Crafts; Ind. Eng. Chem. Res. 2009, 48,4619-4637.

    DOI: 10.1021/ie801535aCopyright 2009 American Chemical Society

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    Figure 26 shows the calculated Pxydiagram with the UNIFAC Dortmund parameters and the CI-computed parameters, along with data from ref91. The agreement for the CI method is not as good

    as with the GC method over the whole data range, but the pressure and composition of the azeotrope

    are given reasonably accurately.

    VLE for the methylethylketonen-heptane system at 318.15 K: calculated with UNIFAC(90) group-contribution parameters, - -

    - calculated with CI-estimated group-contribution parameters; (experiment)(90) y, x.

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    These examples illustrate the possibilities of using models based on limited

    information, such as connectivity indices, as well as a level of compromiseencountered when they are used in place of more elaborate methods such

    as UNIFAC. In general, CI may be a reliable expedient to determine

    unavailable, and perhaps less sensitive, parameters for use with incomplete

    group contribution methods. It is not proposed as a replacement for

    experiments, but rather to focus on a few experiments through which the

    extension can be verified.

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    5.2 Molecular Calculations

    While methods such as CI are easily used to obtain group-contribution

    parameters, their accuracy and generality may be limited. An alternative

    which does not, in principle, require data for model parameter

    regression is quantum chemistry calculations for inter- and

    intramolecular force fields followed by molecular simulation or statistical

    thermodynamic methods to obtain properties

    S l t f E t ti Di till ti f

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    Solvents for Extractive Distillation of

    1,3-Butadiene

    Mathias et al.(92) describe an investigation using quantum mechanics and

    molecular simulation to improve process simulation for the classical problem

    of 1,3-butadiene recovery from steam cracker C4 hydrocarbons by

    determining the relative effectiveness ofn,n-dimethylformamide (DMF) and

    acetonitrile (ACN) as extractive-distillation solvents. The principal propertiesobtained were the activity coefficients of the hydrocarbon components in the

    presence of the extractive solvent for use in eq 1. Comparisons were made

    among a quantum mechanical and statistical mechanical method, COSMO-

    RS,(-36, 37) a molecular dynamics simulation approach, SPEADMD,(93)

    group contributions from UNIFAC,(94) and thermodynamic intuition. Mathias

    et al.(92) describe the methods and results in some detail; only a briefsummary is given here to indicate the findings.

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    The COSMO-RS method reliably predicted the trends of infinite-dilution

    activity coefficients with accuracy comparable to UNIFAC, but only with

    systematic empirical corrections. This limited the true predictive capability

    of the method. The SPEADMD molecular simulation used a force field fromthe principle of transferability,(95, 96) which assumes that forces inferred

    from experimental data for one set of mixtures can be applied to other

    compounds and mixtures. The computed results provided unique qualitative

    structural and orientational insights at the molecular scale about the

    solvation interactions between the polar solvents and the olefinic moieties

    in the hydrocarbon compounds. The differences in accessibility for DMF

    and ACN and the sizes and shapes that affect intermolecular contacts were

    reliably characterized. However, to achieve accuracy for activity

    coefficients, the molecular simulations required refinement of the interaction

    potentials by regression to data, similar to finding UNIFAC parameters.

    E t i f M l l

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    Extensions of Molecular

    CalculationsThe experience of Mathias et al.(92) suggests some of the limitations

    and future prospects of molecular simulation, as do the International

    Fluid Property Simulation Challenges (IFPSC).(97) The present

    important question about the potential for molecular simulation as a

    routine tool to provide quantitative property data for process and

    product design is, Are we there yet?. In our opinion, the answer is a

    qualified no. While progress is being made, the results are often like

    the butadiene example: good, perhaps adequate for the advice role

    without high accuracy, but not sufficient for the service role.

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    A common shortcoming of molecular simulation methods is the lack of easily

    available and suitable force fields(98) to solve the wide variety of problems

    under consideration.(99) In particular, what should be done when noexperimental data exist for empirically fitting a force field? As an example,

    consider the molecule whose chemical formula is C10H19N and structure is

    the following

    There are no experimental data and not even a CAS number has been

    assigned. If this molecule is of interest in a product design for a particular

    application or is an impurity that must be effectively removed in a processdesign, molecular simulation could not be used for property estimation unless

    ab inito quantum methods alone could produce a force field. Figure 27

    suggests a strategy to obtain force field parameters of molecules of industrial

    interest

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    Schematic for developing molecular simulation force fields for cases with different amounts of available data.

    Published in: John P. OConnell; Rafiqul Gani; Paul M. Mathias; Gerd Maurer; James D. Olson; Peter A. Crafts; Ind. Eng. Chem. Res. 2009, 48,4619-4637.

    DOI: 10.1021/ie801535aCopyright 2009 American Chemical Society

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    Other limitations in simulations occur at lower temperatures and for larger

    molecules (high density) and for transport properties. For quantum

    calculations, the system size may be limiting, the fundamental basis setsmight not be accurate enough, and the way to improve results may not be

    clear. Also, while only a few molecular-simulation researchers and reviewers

    now list computing machinery and computing resources as a major limitation

    in the extension of MC and MD to new fluid property applications,

    computational capabilities beyond those currently available are needed for

    computational chemistry to directly treat many practical systems.Finally, a key issue for practical application molecular simulation is the lack of

    availability of tools for nonexpert users. There is no standard toolbox for

    molecular simulation as pointed out by Wei.(100, 101) Our experience is that

    even experts can have problems, giving one pause about very widespread

    application of computation. For example, in at least two entries during IFPSC

    contests, expert researchers incorrectly transcribed molecular parametersthat then produced nonrepresentative and erroneous results. In such cases,

    what would nonexperts find? We mention two efforts to produce standard

    molecular simulation tools which are the TOWHEE project(102) and the

    LAMMPS project;(103) others should appear in the future