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    Aspen Plus

    Aspen Plus Model of theCO2Capture Process byN-methyl 2-pyrrolidone

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    Copyright (c) 2008 by Aspen Technology, Inc. All rights reserved.

    Aspen Plus, the aspen leaf logo and Plantelligence and Enterprise Optimization are trademarks or registeredtrademarks of Aspen Technology, Inc., Burlington, MA.

    All other brand and product names are trademarks or registered trademarks of their respective companies.

    This document is intended as a guide to using AspenTech's software. This documentation contains AspenTechproprietary and confidential information and may not be disclosed, used, or copied without the prior consent ofAspenTech or as set forth in the applicable license agreement. Users are solely responsible for the proper use ofthe software and the application of the results obtained.

    Although AspenTech has tested the software and reviewed the documentation, the sole warranty for the softwaremay be found in the applicable license agreement between AspenTech and the user. ASPENTECH MAKES NOWARRANTY OR REPRESENTATION, EITHER EXPRESSED OR IMPLIED, WITH RESPECT TO THIS DOCUMENTATION,ITS QUALITY, PERFORMANCE, MERCHANTABILITY, OR FITNESS FOR A PARTICULAR PURPOSE.

    Aspen Technology, Inc.200 Wheeler RoadBurlington, MA 01803-5501USAPhone: (1) (781) 221-6400

    Toll Free: (1) (888) 996-7100URL: http://www.aspentech.com

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    Revision History 1

    Revision HistoryVersion Description

    V7.0 First version

    V7.1 Re-verified simulation results using Aspen Plus V7.1

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    2 Contents

    ContentsIntroduction............................................................................................................31 Components .........................................................................................................42 Process Description..............................................................................................53 Physical Properties...............................................................................................74 Simulation Approaches.......................................................................................165 Simulation Results .............................................................................................196 Conclusions........................................................................................................21References ............................................................................................................22

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    Introduction 3

    Introduction

    This document describes an Aspen Plus model of the CO2capture process by

    the physical solvent N-methyl 2-pyrrolidone(NMP) from a gas mixture of CO,CO2, H2, H2O, N2, Ar, CH4, NH3, and H2S from gasification of Illinois No. 6

    bituminous coal[1]. Due to lack of design data for NMP, the operation datafrom an engineering evaluation design case using DEPG as solvent by Energy

    Systems Division, Argonne National Laboratory (1994)[1]are used to specifythe feed conditions and unit operation block specifications in the process

    model. Since only the equilibrium stage results for the DEPG design case are

    available in the literature and the Aspen Plus DEPG model uses equilibriumstage simulation, the process model developed here is also based on the

    equilibrium stage distillation model instead of the more rigorous rate-based.

    In addition to the gases present in the design case, many other gascomponents such as COS, CH3SH and so on are also included in this model for

    potential needs by model users. Pure and/or binary parameters have beendetermined and included in the model for these compounds.

    NMP data for vapor pressure[2], liquid density[2], viscosity[3-5], thermal

    conductivity[6]

    and surface tension[4,7]

    are used to determine parameters inthermophysical property and transport property models used in this work. For

    all other components, thermophysical property models have been validated

    against DIPPR correlations[2], which are available in Aspen Plus, for

    component vapor pressure and liquid density. Vapor-liquid equilibrium data

    from Xu et al. (1992)[8]between propylene carbonate and selected

    components and solubility ratios[9,10]of gases in propylene carbonate and in

    NMP are used to estimate vapor-liquid data between NMP and gascomponents and then to adjust binary parameters in thermophysical property

    models. The designed packing information from the literature[1]is alsoincluded in the process model, which allows rigorous rate-based simulation to

    be performed.

    The model includes the following key features: PC-SAFT equation of state model for vapor pressure, liquid density, heat

    capacity, and phase equilibrium

    Transport property models Equilibrium distillation model for absorber with designed packing

    information from the literature[1]

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    4 1 Components

    1 Components

    The following components represent the chemical species present in the

    process.

    Table 1. Components Used in the Model

    ID Type Name Formula

    NMP Conventional N-METHYL-2-PYRROLIDONE C5H9NO-D2

    CO2 Conventional CARBON-DIOXIDE CO2

    H2S Conventional HYDROGEN-SULFIDE H2S

    CO Conventional CARBON-MONOXIDE CO

    H2O Conventional WATER H2O

    CS2 Conventional CARBON-DISULFIDE CS2

    NH3 Conventional AMMONIA H3N

    N2 Conventional NITROGEN N2

    COS Conventional CARBONYL-SULFIDE COS

    O2 Conventional OXYGEN O2

    SO2 Conventional SULFUR-DIOXIDE O2SSO3 Conventional SULFUR-TRIOXIDE O3S

    CH3SH Conventional METHYL-MERCAPTAN CH4S

    C2H5SH Conventional ETHYL-MERCAPTAN C2H6S-1

    CH3SCH3 Conventional DIMETHYL-SULFIDE C2H6S-2

    HCN Conventional HYDROGEN-CYANIDE CHN

    H2 Conventional HYDROGEN H2

    BENZENE Conventional BENZENE C6H6

    CH4 Conventional METHANE CH4

    C2H6 Conventional ETHANE C2H6

    C2H4 Conventional ETHYLENE C2H4

    C3H8 Conventional PROPANE C3H8

    IC4H10 Conventional ISOBUTANE C4H10-2NC4H10 Conventional N-BUTANE C4H10-1

    C2H2 Conventional ACETYLENE C2H2

    C6H14 Conventional N-HEXANE C6H14-1

    C7H16 Conventional N-HEPTANE C7H16-1

    NO2 Conventional NITROGEN-DIOXIDE NO2

    NO Conventional NITRIC-OXIDE NO

    AR Conventional ARGON AR

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    2 Process Description 5

    2 Process Description

    In this NMP model, we use the operation data taken from a CO2capture

    design case by DEPG reported by Energy Systems Division, Argonne NationalLaboratory (ANL)[1]. The reported flowsheet includes an absorber for CO2

    absorption by DEPG at elevated pressure, flash tanks to release CO2andregenerate solvent at several different pressure levels, and compressors and

    turbines to change pressures of streams. However, the process modelpresented in this work focuses only on the absorber and the other unit

    operations are not included.

    The sour gas enters the bottom of the absorber, contacts with lean NMP

    solvent from the top counter-currently and leaves at the top as sweet gas,while the solvent flows out of the absorber at the bottom as the rich solvent

    with absorbed CO2and some other gas components.

    Two pressure levels for absorption were evaluated in the ANL report: 250psia

    and 1000psia. For each pressure case study, the gas feeds into the absorber

    is the same, but solvent flow rates and number of equilibrium stages used aredifferent. Typically, to achieve a certain CO2recovery, the high pressure case

    used less solvent and fewer stages. Table 2 represents some operation data.In this NMP model, we used the operation data of the low pressure case.

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    6 2 Process Description

    Table 2. Data of the Absorber

    Low Pressure Case High Pressure Case

    Absorber

    Number of Stages 12 10Diameter, ft 17 11

    Packing Height, ft 3 3

    Packing Type Pall ring Pall ring

    Packing Size, mm 50 50

    Sour Gas

    Flow rate, lbmol/hr 17614.58 17614.58

    CO2in Sour Gas, mole fraction 0.2461 0.2461

    Lean DEPG

    Flow rate, lbmol/hr 23000 6900

    Temperature, F 30 30Pressure, psia 250 1000

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    3 Physical Properties 7

    3 Physical Properties

    The PC-SAFT equation of state model is used to calculate vapor pressure,

    liquid density and phase equilibrium. The PC-SAFT pure componentparameters for gases have been regressed against vapor pressure and liquid

    density generated from DIPPR correlations[2]for each component or takenfrom the work by Gross and Sadowski (2001, 2002)[11,12]. The PC-SAFT pure

    parameters for NMP have also been regressed to fit vapor pressure and liquiddensity data from DIPPR correlations[2].

    No vapor-liquid equilibrium data for the gases in NMP were found to regress

    the PC-SAFT binary parameters. However, Xu et al. (1992)[8]reported Henrysconstants for CO2, H2S and SO2with propylene carbonate and according to

    reference [9], CO2solubility in propylene carbonate and in NMP are very

    similar in both the volume-solvent basis and the mole-solvent basis. So CO2

    Henrys constant with propylene carbonate were used as a starting point to

    regress binary parameters between CO2and NMP. Then CO2solubility in NMPat 25C and 1atm was calculated using the binary parameters. Comparison of

    the calculated CO2solubility and the literature data[9]supplies direction to

    adjust the Henrys constant data. Several iterations were made to get suitable

    Henrys constant data for CO2with NMP, which can give suitable binaryparameters between CO2and NMP, allowing accurate estimation of CO2

    solubility in NMP at 25C and 1atm. A diagram of the process is shown in

    Figure 1.

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    8 3 Physical Properties

    Estimate CO2Henrysconstantwith NMP

    Regress kijbetween CO2and NMP

    Estimate CO2solubility inNMP at 25C and 1atm

    MatchCO2solubility Data

    [9]in NMP?

    CO2 Henrys constant data[8]

    with PC

    Output CO2Henrysconstant and kijin NMP

    Yes

    No

    Figure 1. Diagram of estimation process of PC-SAFT binary parameter for CO2and NMP.

    Once Henrys constant for CO2with NMP were figured out, solubility ratios[10]

    of the other gases to CO2were used to determine their Henrys constants with

    NMP, with the assumption that solubility ratios are equivalent to Henrys

    constant ratios. Then these estimated Henrys constant served to regressbinary parameters between these gas components and NMP.

    DIPPR model parameters for NMP are regressed to fit data for viscosity[3-5],thermal conductivity[6]and surface tension[4,7].

    Figures 2-16 show property predictions together with literature data.

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    3 Physical Properties 9

    NMP vapor pressure

    1.00E-06

    1.00E-04

    1.00E-02

    1.00E+00

    1.00E+02

    0 200 400 600 800

    Temperature, K

    VaporPresure,ba

    rData

    PC-SAF

    Figure 2. NMP vapor pressure. PC-SAFT is used to fit data from DIPPRcorrelation[2]for NMP.

    NMP liquid density

    600

    800

    1000

    1200

    100 200 300 400 500 600

    Temperature, K

    Liquiddensity,kg/m3

    Data

    PC-SAF

    Figure 3. NMP liquid density. PC-SAFT is used to fit data from DIPPRcorrelation[2]for NMP.

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    10 3 Physical Properties

    CO2 vapor pressure

    0

    10

    20

    30

    40

    50

    60

    70

    200 220 240 260 280 300 320

    Temperature, K

    Vaporpressure,ba

    r Data

    PC-SAFT

    Figure 4. CO2vapor pressure. PC-SAFT is used to fit data generated fromDIPPR correlation[2]for CO2.

    CO2 liquid density

    500

    600

    700

    800

    900

    1000

    1100

    1200

    1300

    200 220 240 260 280 300 320

    Temperature, K

    Liquiddensity,kg/m3

    Data

    PC-SAFT

    Figure 5. CO2liquid density. PC-SAFT is used to fit data generated fromDIPPR correlation[2]for CO2.

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    3 Physical Properties 11

    H2S vapor pressure

    0

    10

    20

    30

    40

    50

    60

    70

    80

    180 230 280 330 380

    Temperature, K

    Vaporpressure,ba

    rData

    PC-SAFT

    Figure 6. H2S vapor pressure. PC-SAFT is used to fit data generated fromDIPPR correlation[2]for H2S.

    H2S liquid density

    300

    400

    500

    600

    700

    800

    900

    1000

    1100

    180 230 280 330 380

    Temperature, K

    Liquiddensity,kg/m3

    Data

    PC-SAFT

    Figure 7. H2S liquid density. PC-SAFT is used to fit data generated fromDIPPR correlation[2]for H2S.

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    12 3 Physical Properties

    CO vapor pressure

    0

    5

    10

    15

    20

    25

    30

    35

    40

    70 90 110 130

    Temperature, K

    Vaporpressure,ba

    r

    Data

    PC-SAFT

    Figure 8. CO vapor pressure. PC-SAFT is used to fit data generated fromDIPPR correlation[2]for CO.

    CO liquid density

    400

    450

    500

    550

    600

    650

    700

    750

    800

    850

    70 90 110 130

    Temperature, K

    Liquiddensity,kg/m3

    Data

    PC-SAFT

    Figure 9. CO liquid density. PC-SAFT is used to fit data generated from DIPPRcorrelation[2]for CO.

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    3 Physical Properties 13

    NH3 vapor pressure

    0

    10

    20

    30

    40

    50

    60

    70

    80

    90

    200 250 300 350 400

    Temperature, K

    Vaporpressure,ba

    r

    Data

    PC-SAFT

    Figure 10. NH3vapor pressure. PC-SAFT is used to fit data generated fromDIPPR correlation[2]for NH3.

    NH3 liquid density

    400

    450

    500

    550

    600

    650

    700

    750

    200 250 300 350 400

    Temperature, K

    Liquiddensity,kg/m3

    Data

    PC-SAFT

    Figure 11. NH3liquid density. PC-SAFT is used to fit data generated fromDIPPR correlation[2]for NH3.

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    14 3 Physical Properties

    VLE for CO2-NMP

    0

    0.005

    0.01

    0.015

    290 300 310 320 330 340 350

    Temperature, K

    Pressure,MPa

    Data

    PC-SAFT

    Figure 12. Vapor-liquid equilibria of CO2-NMP. Comparison of estimated datato calculation results of PC-SAFT with adjustable binary parameter.

    VLE for H2S-NMP

    0

    0.005

    290 300 310 320 330 340 350

    Temperature, K

    Pressure,M

    Pa Data

    PC-SAFT

    Figure 13. Vapor-liquid equilibria of H2S-NMP. Comparison of estimated datato calculation results of PC-SAFT with adjustable binary parameter.

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    3 Physical Properties 15

    Surface tension of NMP

    0

    0.01

    0.02

    0.03

    0.04

    0.05

    0.06

    200 300 400 500 600 700

    Temperature (K)

    Surfacetension(N/m)

    DIPPR

    Data

    Figure 14. NMP liquid surface tension. DIPPR correlation model[4] is used tofit data[4,7].

    Viscosity of NMP

    0

    0.0005

    0.001

    0.0015

    0.002

    0.0025

    0.003

    0.0035

    0.004

    0.0045

    0.005

    200 300 400 500 600

    Temperature (K)

    Viscosity(Pa.s)

    DIPPR

    Data

    Figure 15. NMP liquid viscosity. DIPPR correlation model[4] is used to fitdata[3-5].

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    16 3 Physical Properties

    Thermal conductivity of NMP

    0.09

    0.1

    0.11

    0.12

    0.13

    0.14

    0.15

    200 300 400 500

    Temperature (K)

    Thermalconductivity(W

    /m.K)

    DIPPRData

    Figure 16. NMP liquid thermal conductivity. DIPPR correlation model[4] isused to fit data[6].

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    4 Simulation Approaches 17

    4 Simulation Approaches

    As stated in the previous sections, this NMP model uses operation data of a

    DEPG design case from [1], the low pressure case. Feed conditions, absorberconfigurations and operation conditions of the DEPG low pressure case were

    used in this model as a base case and then solvent flow rate is adjusted toreach the same CO2capture amount as DEPG does.

    The absorber is modeled with the Equilibrium calculation type instead of the

    more rigorous rate-based calculation type because the design cases from [1]were based on equilibrium stage calculations. This allows us to make

    meaningful comparison between our model and the DEPG model, which alsouses the Equilibrium calculation type because only equilibrium results are

    available for comparison in [1]. However, we included packing design

    information from the literature in the model so that the rate-based calculationtype can be used. In addition, as shown above, transport properties, which

    are crucial for rate-based calculations, have also been validated. Therefore,

    this model is ready for rate-based calculations, in which correlations and scalefactors of interfacial area, mass transfer coefficient, heat transfer coefficient,

    liquid holdup and so on can be selected and adjusted. You can also select thefilm resistance types and flow models to be used.

    Simulation Flowsheet The absorber has been modeled with the following

    simulation flowsheet in Aspen Plus, shown below.

    LEANIN

    GASIN

    GASOUT

    RICHOUT

    ABSORBER

    Figure 17. NMP Process Flowsheet in Aspen Plus

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    18 4 Simulation Approaches

    Unit Operations Major unit operations in this model have beenrepresented by Aspen Plus Blocks as outlined in Table 3.

    Table 3. Aspen Plus Unit Operation Blocks Used in theNMP Model

    Unit Operation Aspen Plus Block Comments / Specifications

    ABSORBER RadFrac The absorber for the low pressure case with the followingsettings:

    1. Calculation type: Equilibrium stage

    2. Number of stages: 12

    3. Top Pressure: 250psia

    4. Column diameter: 17ft

    5. Packing Type: Pall ring

    6. Packing Size: 50mm(2in)

    7. Packing Height per stage: 3ft

    Streams The gas feeds of the NMP model is GASIN, containing CO, CO2, H2,H2O, N2, Ar, CH4, NH3, and H2S.

    The solvent liquid feeds is LEANIN, containing NMP and a small amount of CO2

    and H2O.

    Feed conditions are summarized in Table 4.

    Table 4. Feed specification

    Stream ID GASIN LEANIN

    Substream: MIXED

    Temperature: F 68.13 30

    Pressure:psia 248 250Mole-flow: lbmol/hr

    NMP 0 23000

    CO 77.37 0.0

    CO2 4335.99 395.00

    H2 5611.86 0.0

    H2O 61.91 2.25

    N2 7306.65 0.0

    AR 88.6 0.0

    CH4 128.77 0.0

    NH3 2.99 0.0

    H2S 0.4 0.0

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    5 Simulation Results 19

    5 Simulation Results

    The simulation was performed using Aspen Plus V7.1 with the absorber

    calculation type set to Equilibrium. Key simulation results are presented inFigure 18 and 19, together with the simulation results of the DEPG model

    using the low pressure case operation data.

    As shown by Figures 18 and 19, with the same flow rate (23000lbmol/hr) andtemperature (30F) for the fed solvent to the absorber, DEPG (Squares in

    Figures 18 and 19) has a much higher remove capacity than NMP (Solid linesin Figures 18 and 19). To achieve a similar CO2removal to what DEPG does,

    NMP flow rate should be increased to about 50700lbmol/hr (Dashed Lines inFigures 18 and 19), which is about 2.2 times of DEPG flowrate.

    According to Table 1 in reference [9], at 25C, CO2solubility is

    0.485ft3/gallon DEPG and 0.477ft3/gallon propylene carbonate. At 25C,specific gravity is 1030kg/m3for DEPG, whose molecular weight is 280, and

    1027kg/m3for propylene carbonate, whose molecular weight is 99. If

    transformed to a mole-solvent base, CO2solubility in DEPG is about 2.9 timesof the solubility in propylene carbonate at 25C

    1

    2

    3

    4

    5

    6

    7

    8

    9

    10

    11

    12

    0 5 10 15 20 25 30 35 40 45 50 55 60 65

    T e m p e r a t u r e F

    Sta

    umb

    DEPG 23000 30F

    NMP 23000 30F

    NMP 50700 30F

    Figure 18. Absorber Temperature Profile

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    20 5 Simulation Results

    1

    2

    3

    4

    5

    6

    7

    8

    9

    10

    11

    12

    0 0.05 0.1 0.15 0.2 0.25 0.3

    CO Mole Fraction

    Saumb

    DEPG 23000 30F

    NMP 23000 30F

    NMP 50700 30F

    Figure 19. Absorber Vapor Phase CO2Composition Profile

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    6 Conclusions 21

    6 Conclusions

    The NMP model provides an equilibrium stage simulation of the process and

    validated property models which allow rigorous rate-based simulation. Keyfeatures of this model include the PC-SAFT equation of state model for vapor

    pressure, liquid density and phase equilibrium, rigorous transport propertymodeling, equilibrium stage simulation with RadFrac and packing information

    from the literature[1].

    The model is meant to be used as a guide for modeling the CO2captureprocess with NMP. Users may use it as a starting point for more sophisticated

    models for process development, debottlenecking, plant and equipmentdesign, among others.

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    References

    [1] R.D. Doctor, J.C. Molburg, P.R. Thimmapuram, G.F. Berry, C.D. Livengood,

    Gasification Combined Cycle: Carbon Dioxide Recovery, Transport, andDisposal, Energy System Divison, Argonne National Laboratory (1994)

    [2] DIPPR801 database, BYU-Thermophysical Properties Laboratory (2007)

    [3] V.A. Granzhan, O.G. Kirillova, "Physico-Chemical Analysis of the Systemn-Methyl-alpha-Pyrrolidone-Methanol," J. Appl. Chem. USSR, 43, 1898 (1970).

    [4] M-Pyrol Handbook, GAF Corporation, New York (1972)

    [5] J.A. Riddick, W.B. Bunger, "Organic Solvents: Physical Properties and

    Methods of Purification, 3rd ed., " Wiley Interscience, New York (1970)

    [6] A. Missenard, "Conductivite Thermique des Solides, Liquides, Gaz et de

    Leurs Melanges, " Editions Eyrolles, Paris, 5 (1965); Also see Missenard, A.,Comptes Rendus, 260, 5521 (1965)

    [7] S. Sugden, "The Variation of Surface Tension with Temperature and Some

    Related Functions," J. Chem. Soc. (London, Transactions), 125, 32 (1924)

    [8] Y. Xu, R.P. Schutte, L.G. Helper, Solubilities of Carbon Dioxide, HydrogenSulfide and Sulfur Dioxide in Physical Solvents, Can. J. Chem. Eng., 70, 569-

    573 (1992)

    [9] G. Ranke, V.H. Mohr, The Rectisol Wash: New Developments in Acid GasRemoval from Synthesis Gas, from Acid and Sour Gas Treating Processes,

    Stephen A. Newman, ed., Gulf Publishing Company, Houston, 80-111(1985)

    [10] R. Epps, Processing of Landfill Gas for Commercial Applications: the

    SELEXOL Solvent Process, Union Carbide Chemicals & Plastics TechnologyCorporation, June, 1992. (Prepared for Presentation at ECO WORLD 92, June

    15, 1992, Washington D. C.)

    [11] J. Gross, G. Sadowski, Perturbed-Chain SAFT: An Equation of State

    Based on a Perturbation Theory for Chain Molecules, Ind. Eng. Chem. Res.,40, 1244-1260 (2001)

    [12] J. Gross, G. Sadowski, Application of the Perturbed-Chain SAFTEquation of State to Associating Systems, Ind. Eng. Chem. Res., 41, 5510-

    5515 (2002)