5216 R. Taylor, R. Krishna / Chemical Engineering Science 55 (2000) 5183}5229Prevost (1998) brie#y addressed some numerical problemsthat can be encountered in the simulation of <strong>reactive</strong>absorption using NEQ models. We have already notedthe success (using e!ective di!usivities and enhancementfactor approaches to mass transfer with reaction) of NEQmodels of amine-based gas treating processes (Careyet al., 1991; Altiqi et al., 1994).6. Reactive <strong>distillation</strong> designDesign and simulation of RD operations are verydi!erent types of calculation, calling for verydi!erent approaches. Most conceptual design models arebased on the EQ stage model described above. However,as discussed below, some recent developments haveopened up the possibility of using NEQ models for RDdesign, and a limited number of papers suggest that NEQmodels already have a place in industrial RD designpractice.6.1. Conceptual designBarbosa and Doherty (1988c) developed the "xedpointmethod for the design of single-feed RD columns.The method is based on the following assumptions: the column is adiabatic; the molar heat of vaporisation is constant; the heat of mixing is negligible; sensible heat e!ects can be ignored; the heat of reaction is negligible compared to theenthalpy of the vapor; the feed is a saturated liquid; phase equilibrium is achieved on each stage; the column operates with a partial condenser.These assumptions ensure that the vapor and liquid #owsinside the column are constant, thereby permitting theenergy balances to be solved essentially independent ofthe remaining stage equations.The "xed-point method uses material balance equationswritten around a stage in each section of the column(above and below the feed stage) and thecorresponding end of the column. With reference to Fig.18(a), for example, we have, for the rectifying sectionX " rH #1 > ! 1 > (32) rH rH and for the stripping section the material balance readsX "sH sH#1 > ! 1sH#1 X . (33) Note that these equations have been written in terms ofthe transformed composition variables de"ned by Eq. (3).The transformed re#ux and stripping ratios are de"nedas follows:rH "¸ (ν !ν x )D(ν !ν y ) , sH "
R. Taylor, R. Krishna / Chemical Engineering Science 55 (2000) 5183}5229 5217Fig. 30. Column pro"les in RD design (Doherty method).The attainable region approach to reactor networkfeasibility is based on geometric properties and has beenstudied in depth mainly by Glasser, Hildebrandt, andtheir co-workers (see, for example, Glasser & Hildebrandt,1997; Feinberg & Hildebrandt, 1997; Feinberg,1999). McGregor, Glasser & Hildebrandt (1997) andNisoli, Malone and Doherty (1997) apply the attainableregion approach in order to develop a systematic approachto identifying the feasible compositions that canbe obtained in RD processes. Once again, the Damkohlernumber emerges as the important parameter.Hauan and co-workers (see Hauan, 1998; Hauan& Lien, 1996, 1998; Hauan, Westerberg & Lien, 2000b)have developed what they call a phenomena-basedmethod for the analysis and design of <strong>reactive</strong> separationprocesses. Within this framework the change in the compositionof any particular phase is given by the vectorequationdx"mix#sep#rx (35)dtwhere x is the composition of the phase in question, andmix, sep, and rx are vectors that represent the compositionchanges due to mixing, separation, and reaction,respectively. For these vectors Hauan et al. (2000b) writemix"M(x F !x), (36)rx"R(ν!xν), (37)sep"[S](x!y), (38)where M is a scalar equal to the relative amounts ofmaterial being mixed, x is the current composition andx F is the feed composition, and R is a scalar that dependson such things as catalyst activity, hold-up, and temperature.[S] is matrix of component speci"c mass transferrates. If the phases are assumed to be in equilibrium then[S] reduces to a simple scalar. The direction of thesecombined vectors indicates the feasibility of a particularprocess; their length is a measure of the process e$ciency.Hauan and Lien (1998) illustrated their methodologywith an analysis of the MTBE process.More interestingly, this formulation admits the possibility,so far unexplored, of using a properly formulatedmodel of mass transfer in multicomponent systems asdiscussed above.A "xed point exists when the mix, sep, and rx vectorsnullify each other.0"mix#sep#rx. (39)When the reaction and separation vectors have zeromagnitude then the "xed point is an equilibrium point.A kinetic "xed point (azeotrope) arises when all threevectors have non-zero magnitudes, but still nullify eachother. The location of these kinetic "xed points hasa direct in#uence on the product compositions that canbe realised in an RD column (see, also, Mahajani, 1999a).Hauan et al. (2000b) have provided a comprehensiveanalysis of the kinds of "xed point that can arise fromcancellation of di!erent combinations of these vectors.They also introduce the reaction di!erence point as the
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