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Part 2: Vapor–Liquid Equilibrium Calculations and more Slides Computer Aided Design (CAD) in PDF only on Docsity! Dr. Javad Ahmadpour Babol Noshirvani University of Technology Computer aided design (CAD) with Aspen Plus Part 2: Vapor–Liquid Equilibrium Calculations Using an Equation of State Liquid-Liquid Equilibria in Aspen Plus® V9
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Methanol(1) + Water (2) - Use the Peng-Robinson (PR) equation of state to model the VLE behavior of a binary mixture containing methanol and water at 313.03 K in Aspen Plus: a. Property analysis method (Pxy diagram) b. Simulation method: find dew point of equimolar mixture c. Estimate the binary parameter for the PR equation of state by performing a regression on data retrieved from the Aspen databases. Generate a Pxy diagram. • Open Aspen Plus® and add the components methanol (1) – water (2) • Select PENG-ROB as the method to model the system
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• b. Simulation method. Create a Flash2 and enter the input information: temperature and vapor fraction. Make sure the mole fraction box under Setup>Report Options> Stream is checked • b. Simulation method. Enter input information about the feed stream and run simulation • c. Create new regression and set up input as shown below. Click run and check results
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Aspen Plus Flowsheet Features creating a simulation of the mixture of a feed stream of 100 kg/h of the 50-50 wt.% acetone–water mix with a solvent stream of 100 kg/h of MIBK. • The overall goal of this problem is to separate the feed stream into two streams that have greater than 95% purity of water and acetone, respectively. BINARY INTERACTIONS liquid phase: “NRTL, gas phase: ideal gas mixture. BINARY INTERACTIONS If the applied pressure is relatively high (e.g., above 10 bar), then the source of data can be changed from “APV88 VLE-IG” to a non-ideal gas mixture, such as “APV88 VLE-RK” (i.e., Redlich–Kwong equation of state). BINARY INTERACTIONS Both plots do exhibit the same pattern, except that they slightly differ in predicting the onset of azeotropic condition at higher values of acetone mole fraction In this example, pressure below 10 bar; no need to go to the non-ideal gas mixture.
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DATA INPUT Entering the first feed stream properties in terms of P, T, and compositional flow rate. DATA INPUT Entering the first feed stream properties in terms of P, T, and compositional flow rate.
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Main Flowsheet Setup - Report Options » ” Control Panel » | +
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COMPUTATION GRDER FOR THE FLOWSHEET:
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->Calculations begin ...
Block: MIXER-1 Model: MIKER
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Units H2O+ACET = MIBK = TREMX =
Molar Liquid Fraction 1 1 1
Molar Solid Fraction 0 0 0
Mass Vapor Fraction 0 0 0
Mass Liquid Fraction 1 1 1
Mass Salid Fraction 0 0 0
Molar Enthalpy keal/mel 66.501 -78.1367 -69,0076
Mass Enthalpy keal/eg -2418.18 -780.114 1599.15
Molar Entropy cal/mal-K 48.269 -146.609 -69303
Mass Entropy caligm-K -1,75521 -1.46374 -1.60599
Molar Density mol/cc 00318814 000795159 o.o1988s3
Mass Density kg/eum 876.753 796.437 258.02
Enthalpy Flow Gcal/nr 0241818 -0.0780114 0319829
Average MW 27.5005 100.161 43,1528
> 4 Mole Flows kmol/br 3.6363 0.998396 4.6347
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NIST/TDE EXPERIMENTAL DATA for acetone–water binary interaction parameters, some experimental data sets failed the consistency tests and others passed. Hence, one set of isobaric VLE data with an overall data quality equal to unity was selected for regression purposes. The data source is from [Huang, R., Gu, Y. and Hou, Y. (1984) VLE of acetone-water- isobutyraldehyde system. Chemical Engineering (China), 4, 26–29].
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The mixer material and energy balance using “UNIQUAC” as the property method with NIST/TDE experimental data. THE CLEAN PARAMETERS STEP Regression by Property Constant EStimation (“R-PCES”) method Simulation Results Convergence Reset the simulator back to the initial state (or point) via using the “Reset” button The reset feature is useful when modifying an existing simulation in terms of input data, operating condition(s), and/or any constraint imposed on a given block. The solver, may converge for all blocks except for a few (i.e., one or two) blocks, then the user’s duty is to keep changing specifications for that particular non-converging block until a converging and reasonable solution is reached. Some factors that usually lead to convergence difficulties are a poor choice for the property method (i.e., thermodynamics) and the creation of recycle streams.