Presented at: Third Joint China/USA C hemical Engineering Conference (CUChE-3) Beijing, China, September 25 - 28, 2000 Modeling the Complex Chemical Reactions and Mass Transfer in a Phosphoric Acid Reactor † Paul M. Mathias†, Chau-Chyun Chen† and Marten Walters‡ ‡ Aspen Technology, Inc. KEMWorks Technology, Inc. Ten Canal Park 5925 Imperial Parkway, Suite 105 Cambridge, MA 02141-2201 Mulberry FL 33860-7621 U.S.A. U.S.A. Introduction The production of phosphoric acid by the “wet process” is a complex, large-scale industrial operation in which phosphate rock is beneficiated, reacted with sulfuric acid and filtered to remove the by-product, calcium sulfate. In this paper we demonstrate that valuable insight can be gained into this complex chemical process through a fundamental model implemented in the Aspen Plus® process simulator. Phosphoric acid is primarily produced by what is known in the industry as the wet process (Slack, 1968; Becker, 1989). In the wet process, phosphate rock, which includes calcium, phosphate and a number of impurities, is mined, beneficiated (concentrated) and then sometimes ground dry or wet through the use of ball mills or rod mills. The rock is fed into an attack tank or reactor and reacted (digested) with sulfuric acid (H2SO4). An extremely simple representation of the digestion is as follows: Ca 3(PO4)2 + 3H2SO4 + 6H2O > 2H3PO4 + 3CaSO4•2H2O (1) The reaction produces phosphoric acid (H3PO4) and calcium sulfate dihydrate or gypsum (CaSO4• 2H2O). The gypsum precipitates and is filtered, giving phosphoric acid as the product. In a variation of the wet process - the hemihydrate process - calcium sulfate hemihydrate (CaSO4• ½H2O) is produced as the precipitate. The present phosphoric-acid discussion focuses on the production of phosphoric acid by the dihydrate process. The dihydrate process contains sections Figure 1. Production of Phosphoric Acid by the Dihydrate Process such as attack and digestion reactors, flash Sul furi c HO Aci d coolers, filtration units, and phosphoric acid Evap. Water concentration. The present simulation Phosphate Rock focuses mainly on the sulfuric-acid-attack reactor, which is the heart of the process. We have used a rigorous description of the thermodynamic and rate-based chemistry occurring in the attack reactors to develop a Slurry steady-state model of the sections of the dihydrate process containing the attack and digestion reactors, the flash or vacuum Return Acid coolers and the filtration units. Figure 1 presents a simple representation of the Product Acid Gypsum process flow diagram. In general, the return acid is mixed with the sulfuric acid in order to dilute the sulfuric acid, as shown in Figure 1. But this is, of course, not necessary in the model. 2 Further details on the model and its application are available in Mathias and Mendez (1998) and Mathias (1999). Model Fundamentals – Thermodynamics, Kinetics and Mass Transfer Phosphate rock mineralogy can be highly variable depending primarily on the origin of the rock (sedimentary or igneous), formation and weathering. Most sedimentary deposits contain varieties of carbonate-fluorapatite collectively known as francolite, which contains calcium, phosphate, fluoride, carbonate and other species held together in a crystal lattice. When the rock is treated with a strong mineral acid, such as sulfuric acid, the phosphate constituent is solubilized as phosphoric acid. In the simulation we treat the phosphate compound in the rock as a mixture of fluorapatite (Ca 10(PO4)6F2) and trical or calcium phosphate (Ca3(PO4)2). In most cases we expect fluorapatite to be the dominant constituent, but we may also need small amounts of trical to quantitatively describe the measured rock composition. We treat the carbonate component as calcium carbonate and use calcium fluoride to describe any fluoride component in excess of that contained in the apatite. In order to obtain a realistic description of the phosphate rock, we include the following major impurities: SiO2, Al 2O3, Fe 2O3, MgO and Na 2O. It is necessary to include the ionic species that occur in the liquid phase of the attack tanks and much of the process (Linkson, 1998; Liu and Watanasiri, 1999). Rigorous description of the chemical equilibrium of the ionic and molecular species, and the nonideality of the resulting solution was often considered to be extremely difficult, but this has changed due to significant advances in the theoretical framework (Chen et al., 1982; Chen at al., 1984; Zemaitis et al., 1986; Chen, 1986) and the technological capability of process simulators such as Aspen Plus (for further information, see Aspen Plus Getting Started Manual: “Modeling Processe s with Electrolytes”). The Chen Electrolyte NRTL (ElecNRTL) model (Chen et al., 1982; Chen at al., 1984; Chen, 1986) has been used in this work. Details of the electrolyte-based thermodynamic model are presented elsewhere (Mathias and Mendez, 1998; Mathias, 1999). Here we only present some examples that demonstrate the concept. H2SO4 + H2O <> H3O+ + HSO4HSO4- + H2O <> H3O+ + SO42Ca 2+ + SO42- + 2H2O <> CaSO4•2H2O (2) (3) (4) Eqns. (2) and (3) present the dissociation of sulfuric acid and Eqn. (4) shows the precipitation of gypsum. Many of the parameters in the thermodynamic model can be estimated or derived from published values of chemical thermodynamic properties, for example Wagman et al. (1982). The Aspen Plus databanks provide many of the model parameters. Finally, the default values of the model parameters often provide adequate accuracy. However, key model parameters must be obtained by fitting experimental data. The Aspen Plus Data Regression System (DRS) has been used to obtain the optimum values of the model parameters needed to accurately describe the important process conditions. Figure 2 Vapor Pr essure of Phosphoric Acid Solutions 800 700 600 Vapor Pressure (mmHg) Figure 2 presents a comparison between model and data (Brown and Carlton, 1952) for the vapor pressure of pure phosphoric acid solutions. These data are important because accurate representation of the vapor pressure is important for an accurate simulation of the flash coolers. The good agreement between model and data also indicates that the model provides an accurate description of the nonideality of phosphoric acid-water mixtures, the two major components in the product acid. 500 100°C 400 90°C 300 80°C 200 An excellent source for solubility data relevant to the phosphoric-acid process is the compilation by Linke (1958). The solubility of gypsum in solutions of phosphoric acid and sulfuric is extremely 70°C 100 60°C 50°C 0 0 10 20 30 Wt% P 2O5 40 50 60 The present thermodynamic model provides a comprehensive description of the thermodynamic properties of this system. Further details are provided in Mathias and Mendez (1998). Fi gure 3 Solubi li ty of Calcium Sul fate in P hosphori c Acid Sol uti ons Comparison of ASPE N PLUS Model to Data of Taperova (1940) and Taperova and Shul gina (1945) 1.6 1.4 Wt% CaSO 4 in Saturated Solution important to the process. Figure 3 presents a comparison between model and data for the solubility of gypsum in phosphoric acid solutions. The model provides an accurate correlation over a wide range of conditions. 80 °C 1.2 6 0°C 1.0 4 0°C 0.8 2 5°C 0.6 0.4 0.2 The key reaction kinetics and mass transfer phenomena in the reactor are rock dissolution and Wt% P O in Solution its tendency to coat, precipitation of gypsum (both normal and nucleated) and co-precipitation of phosphate compounds in the gypsum (Slack, 1968; Becker, 1989). The plant losses are the undissolved or coated rock (known as citrate-insoluble or CI loss) and the phosphate co-precipitation (known as the citrate-soluble or CS loss). These rate phenomena have been captured with the following assumptions: 0.0 0 10 20 30 2 40 50 60 5 1. Rock dissolution, assumed to be proportional to the concentration of undissolved rock and inversely proportional to the sulfate concentration. 2. Rock coating, assumed to be proportional to the concentration of undissolved rock, the gypsum precipitation rate and the sulfate concentration. 3. Normal gypsum precipitation, assumed to be proportional to the calcium and sulfate concentrations and the distance from equilibrium. 4. Nucleated gypsum precipitation, assumed to be negligible up to the supersaturated limit, and extremely fast once this limit is reached. 5. Co-precipitation losses, assumed to be proportional to the total gypsum precipitation rate and ratio of the phosphate and sulfate concentrations. All these effects have been incorporated into a user subroutine for the stirred-tank reactor (RCSTR) in Aspen Plus. Aspen Plus Implementation and Results The key building blocks for the Aspen Plus ® simulation model are the thermodynamic model Figure 4. Aspen Plus Simulation of the D ihydrate Process S ulfuric Acid Phosphate Rock and the RCSTR model. Each tank of the reactor 0.0 1 0.01 0.01 is an RCSTR block and the other pieces of Water 0.98 equipment in the plant are represented by 0.01 blocks such as HEATER, FLASH2 (2-phase 0.01 Rx 1 Rx 2 flash), SEP2 (two-outlet component splitter) etc. 0 .01 Gases P roduct Acid The filtration system is treated as a series of H 2O Evap. 0.98 Rx 9 Rx 3 SEP2 blocks. A schematic representation of a Filter 0.98 particular Aspen Plus flowsheet is presented in Gypsum Figure 4. It is assumed that most of the rock is Ret urn Rx 8 Rx 4 Acid fed to Rx2, and that most of the sulfuric acid and return acid are fed to Rx3. The sulfuric acid and return acid are assumed to be piped Rx 6/7 Rx 5 independently, but, as noted earlier, in current Slurry practice recycle acid and sulfuric acid are generally mixed prior to addition to the reactor. Other plant configurations can easily be modeled. The Aspen Plus model has many uses, including gaining insight into the process, trouble-shooting plant problems and anticipating the effect of design changes. Here we only briefly describe three studies of the effect of plant operation on CI and CS losses. A. Plant throughput B. Sulfate level C. Sulfuric acid split between Reactors 2 and 3 (see Figure 4) In all the studies presented below, the acid strength was held constant at 26% P 2O5. A. Plant throughput. The model predicts that the effect of increased production with the same equipment is to increase CI losse s, while keeping the CS losses approximately constant. This effect results because the reactors have less residence time to dissolve the rock, and the result is in agreement with plant experience. Figur e 5. Lo sses as a F un ctio n of SO4 Weight % CS and CI Losses B. Sulfate level. Figure 5 shows the effect of 6 increasing the sulfuric acid flow to the plant, which will result in an increase in the residual 5 CSL+CI L sulfate level of the product acid. The CS losses 4 go through a weak maximum at a sulfate level of about 2.5%. This is a complicated effect CSL 3 resulting from the direct beneficial effects of increasing the sulfate level (lower CS losse s) 2 and the negative secondary effect where CIL 1 increased sulfate level shifts more of the gypsum precipitation to Compartment #2 where 0 the sulfate levels are lower (higher CS loss). 1. 5 2. 0 2. 5 3.0 This kind of insight into the interaction of effects Weight % SO4 in Product Acid can only be gained through a complete plant model like the present one. It should be noted that the present model suggests operating at the lowest possible sulfate levels in order to minimize the total phosphate loss. However, it is well known that the gypsum crystals that form at low sulfate levels are difficult to filter. In future versions of the model we plan to include the description of the particle-size distribution of the gypsum crystals. The above examples indicate the value that can be gained from a fundamentally based process model incorporated into a process simulator. F ig ure 6. Effect of Su lfu ric Acid Sp lit o n Los ses 6 CSL+CIL 5 WQeight % CS and CI Losses C. Sulfuric acid split. Figure 6 predicts the effect of feeding the sulfuric acid to the rock compartment (Rx 2 in Figure 4) rather than Compartment #3. The CS losse s come down because sulfate level in the rock compartment rises, but unfortunately the CI losse s rise faster because the higher sulfate level significantly increases the rate of rock coating. 3.5 CSL 4 3 2 CIL 1 0 0 5 10 15 % of Sul furi c Acid Fed to Com partment 2 Conclusions Phosphoric acid reactors have been considered to be too complex to be modeled on a fundamental basis. This work demonstrates that these kinds of chemical processe s can indeed be modeled and that the benefits in terms of process understanding and rational process improvement are considerable. 20 References Becker, P., “Phosphates and Phosphoric Acid. Raw Materials, Technology, and Economics of the Wet Process,” Marcel Dekker, Inc., Second Edition (1989). Brown, E. H.; Carlton, D. W., “Vapor Pressure of Phosphoric Acid,” Ind. Eng. Chem., 44, 615, (1952) Chen, C.-C., “Representation of Solid-Liquid Equilibrium of Aqueous Electrolyte Systems with the Electrolyte NRTL Model,” Fluid Phase Equilibria, 27, 457, (1986) Chen, C.-C.; Britt, H.I.; Boston, J.F., “Process Simulation of Electrolyte Systems,” Proceedings of 1984 Summer Computer Simulation Conference, Boston, pages 552-557, 1984. Chen, C.-C.; Britt, H.I.; Boston, J.F.; Evans, L.B., “Local Composition Model for Excess Gibbs Energy of Electrolyte Systems. 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