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    Energy Procedia 23 (2012) 3 14

    1876-6102 2012 The Authors. Published by Elsevier Ltd. Selection and/or peer-review under responsibility of SINTEF Energi AS

    doi:10.1016/j.egypro.2012.06.057

    Trondheim CCS Conference - 6

    Comparison of current and advanced post-combustionCO2capture technologies for power plant applications

    Miguel A. Gonzalez-Salazar1a*, Robert J. Perryb, Ravi-Kumar Vipperlac,Alvaro Hernandez-Nogalesa, Lars O. Norda, Vittorio Michelassia,

    Roger Shislerb, Vitali Lissianskiba General Electric Global Research, 85748 Garching b. Munich, Germany

    b General Electric Global Research, 1 Research Circle, Niskayuna, NY 12309, UScGE Energy, 300 Garlington Road, Greenville, SC 29615, US

    Abstract

    Most energy scenarios suggest carbon capture and storage (CCS) from power generation might contributeto reduce the carbon emissions necessary to stabilize the long-term global average atmospherictemperature. GE is actively investigating and developing novel technologies for both capturing and

    compressing CO2from power plants with potential lower energy requirements and environmental impactthan state-of-the-art processes. One technology that is currently the focus of significant research effort is

    phase-changing absorbents for post-combustion capture applications. This investigation compared theperformance of phase-changing absorbents to state-of-the-art monoethanolamine (MEA) capture for threedifferent flue gas conditions with CO2 concentrations ranging from 4 mole% to 13 mole%. Resultsindicate that depending on the flue gas conditions, the specific equivalent work necessary for operating

    phase-changing absorbents is expected to be up to 40% lower than for MEA capture. However, as thelevel of maturity of phase-changing absorbents is certainly lower than MEA capture, higher uncertainty in

    performance is expected. Besides lower energy requirements, a reduction of up to 6% in specific watercooling load is expected from the phase-changing absorbents compared to MEA capture, in particular forcases with high CO2concentrations in the flue gas.

    2011 Published by Elsevier Ltd.Keywords: CCS; Carbon capture; Post-combustion; Phase-changing absorbents; CO2compression

    * Corresponding author. Tel.: +49 (0) 89 55283-549; fax: +49 (0) 89 55283-180.E-mail address: [email protected]

    Available online at www.sciencedirect.com

    2012 The Authors. Published by Elsevier Ltd. Selection and/or peer-review under responsibility of SINTEF Energi AS

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    4 Miguel A. Gonzalez-Salazar et al. / Energy Procedia 23 (2012) 3 14

    1.IntroductionMost energy scenarios suggest carbon capture and storage (CCS) from power generation might

    contribute to reduce the carbon emissions necessary to stabilize the long-term global average atmospherictemperature. While renewables would likely keep growing worldwide in the future, CCS from power

    plants would still be required to respond to an increasing energy demand while meeting emission targets.

    CCS technologies mainly address coal-fired power generation, partly because it offers the potential toreduce over 40% of the energy-related anthropogenic greenhouse gas emissions. In addition, applyingCCS to other power plants combusting carbon containing fuels might offer even further potential toreduce emissions.

    GE is actively investigating and developing novel technologies for both capturing and compressingCO2from power plants with potential lower energy requirements and environmental impact than state-of-the-art processes. One technology that is currently the focus of significant research effort is phase-changing absorbents for post-combustion applications.

    This investigation compared the performance of phase-changing absorbents to state-of-the-art

    monoethanolamine (MEA) capture for three different flue gas conditions with CO2 concentrationsranging from 4 mole% to 13 mole%. Evaluated applications included retrofit and greenfield power plants.While MEA is considered a mature and near commercial technology that might be employed in retrofitand greenfield applications, phase-changing absorbent is considered a next generation capture technologyand its performance was evaluated only for greenfield applications. With regard to CO2compression, anintegrally geared compression train with supercritical pumping was evaluated, as this solution proved to

    be the least energy intensive for a wide operational range. Aspen Plus and Thermoflex were used tosimulate the performance of both technologies for the different study cases. As the energy requirementsfor the two capture technologies varied qualitatively, the concept of specific equivalent work (MJ/kg-CO2) was used for comparing the performance of the capture technologies. Finally, the specific watercooling load (MJ/kg-CO2) was also estimated.

    2.ApproachMost studies in literature comparing the performance of CO2capture technologies for power plants

    applications used two different methodologies. On one hand, some studies included very detailed modelsof the power plant and its interaction with the capture unit [1]-[3]. On the other hand, some other studiesdid not include any detail of the power plant and focused only on the capture unit [4]-[6]. In this study,

    priority was given to understand the performance of the capture and compression technologies for genericflue gas conditions, rather than the performance of specific power plants with CCS. Thus, the

    performance of both phase-changing absorbents and MEA was estimated at 90% capture for threedifferent flue gas conditions with CO2concentrations ranging from 4 mole% to 13 mole% (see Table 1).

    These selected flue gas conditions are representative for large scale power plants fuelled with fuelsranging from natural gas to coal.

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    Miguel A. Gonzalez-Salazar et al. / Energy Procedia 23 (2012) 3 14 5

    T

    p

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    (1

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    6 Miguel A. Gonzalez-Salazar et al. / Energy Procedia 23 (2012) 3 14

    p

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    .1.Process dThe genera

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    p1

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    Fig. 1 CO2Isl

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    e sprayed in

    formed are

    third action

    hich may b

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    ark of the Gener

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    odel was ca

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    operations (

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    collected in

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    ation (absorb

    stream at a

    a second op

    m a low pres

    ay be acco

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    oC under pr

    orbent. The h

    ng water. Th

    O2gas is re

    m of the sep

    bsorber unit

    pression cost

    ondense wat

    ith the CO2

    ents have in

    s in capture

    te the mass

    experimenta

    rb the CO2a

    e first is CO2

    er) wherein fi

    proximately

    ration which

    sure (~ 1 bar

    plished by t

    at exchangerthe absorbe

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    ot vapor fro

    e stream then

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    er found in

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    flows to a

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    ed back to

    action with

    upercritical

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    Miguel A. Gonzalez-Salazar et al. / Energy Procedia 23 (2012) 3 14 7

    3.2.Key system assumptionsThe energy needed by the CO2separator is provided by extraction of steam from the power plant. The

    steam will pass through the desorber reboiler, and must have a condensation temperature as high as thetemperature in the desorber. The system has four process variables that dominate the performance:absorber temperature, desorber temperature, desorber pressure, and rich/lean heat exchanger approachtemperature. The system model accounts for the major energy penalties for CO2 separation, and theyinclude the energy required:

    1. For vaporization of water.2. For desorbing the carbon dioxide (i.e. reaction energy).3. For sensible heating of the sorbent.The model also accounts for CO2compression energy and auxiliary loads. The sorbent rich loading is

    defined as the weight percentage of CO2in the rich sorbent leaving the absorber column. The sorbent leanloading is defined as the weight percentage of CO2in the lean sorbent leaving the desorber column. Thesorbent net loading is defined as the difference between the rich loading and the lean loading and is

    obtained from lab-scale experiments. The lab-scale isotherm data indicate that sorbent net loading of 8%is achievable with GAP-0. The key assumptions for the CO2separation unit utilizing the GAP-0 sorbentare listed in Table 2.

    Table 2.Parameters used in the baseline (GAP-0).Parameter Value

    Temperature of flue gas after direct contact cooler (oC) 32

    Absorber temperature (oC) 49

    Absorber pressure (bar) 1,03Desorber temperature (oC) 127

    Desorber pressure (bar) 13,8Rich-lean heat exchanger temperature approach (oC) 5,5

    The GAP-0 sorbent utilizes less energy than the MEA sorbent due to lower water in the sorbent mixtureand a low specific heat of the sorbent.

    Low water in the sorbent mixtureThe model accounts for absorption of water in the flue gas by the MEA sorbent and the vaporization of

    water in the desorber column. The baseline MEA sorbent concentrations are limited to 20-30% and theremaining is water due to viscosity and corrosion issues. The water in the sorbent necessitates significantamount of energy due to sensible heat as well as vaporization of the water.

    Low specific heat of the sorbentThe specific heat of GAP-0 is 2,3 kJ/kg-C while the specific heat of MEA is 3,73 kJ/kg-C. The lower

    specific heat for GAP-0 improves the energy efficiency of the process.

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    8 Miguel A. Gonzalez-Salazar et al. / Energy Procedia 23 (2012) 3 14

    3

    v

    T

    4

    a

    c

    a

    a

    e

    0

    s

    c

    .3.Design ofThe param

    alues are giv

    able 3. Design o

    Desor

    Net l

    Heat

    Rich l

    .MonoethaThe investi

    state-of-the

    haracterized

    bsorber colu

    bsorber inter

    specially sig

    ,28 mol CO2/

    tripped from

    ooled down

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    Fig.

    Experiment (

    ters that we

    n below (see

    f Experiment (D

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    ean heat exc

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    cooler was c

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    mol MEA). I

    the solution.

    nd sent bac

    e-based distil

    2. MEA capture

    DOE)

    e varied for

    Table 3 ).

    OE) for GAP-0.

    (bar)

    /kg)

    anger temper

    A) capture

    configuratioonstrated te

    gy requirem

    ntained in th

    osen to imp

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    the desorbe

    inally, purif

    to the abso

    lation). Fig.

    process

    the design o

    ature approac

    consists of achnology. T

    nts, thermal

    e flue gas rea

    rove the exo

    ntrations (hi

    , the reactio

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    shows the ca

    experiment

    M

    15

    7

    1

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    n absorber we selected

    degradation

    cts with the a

    thermic abso

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    is reversed a

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    pture process

    and the mea

    ean Stan

    ,85

    ,3

    68

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    above 125

    queous MEA

    ption reactio

    and high le

    nd the absorb

    ssion while t

    ed with Asp

    flow diagra

    and standar

    ard deviatio

    3,45

    2

    186

    5,5

    and a stripp0%wt MEA,

    and corrosi

    . The configu

    n. This impr

    n loadings (

    ed CO2is he

    e regenerate

    n Plus 7.1

    .

    deviation

    n

    r, which iswhich is

    ion. In the

    ration with

    ovement is

    igher than

    ted up and

    solvent is

    and Aspen

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    Miguel A. Gonzalez-Salazar et al. / Energy Procedia 23 (2012) 3 14 9

    s

    a

    d

    a

    a

    t

    f

    r

    i

    c

    r

    s

    a

    T

    F

    One simple

    udies that s

    pproach of F

    he flue gas b

    uty is higher

    lower outlet

    nd the abso

    utomatically

    e same quan

    om the stripp

    The strippe

    boiler temp

    creases, the

    ompression

    boiler, whic

    percritical c

    t 45C.Fig. 3

    able 4.Paramete

    ig. 3. CO2captur

    train is use

    ggest the u

    luor that prop

    lower is set u

    but the absor

    pressure is a

    ber. Table 4

    aried to ach

    tity of CO2t

    er outlet is th

    pressure is

    rature varies

    driving for

    ork. Howev

    h increases

    nditions (15

    shows the C

    rs used in the ba

    apture ratio

    tripper press

    tripper heig

    olumns dia

    emperature

    tripper cond

    acking type

    e process flow di

    to process a

    e of two ab

    oses the con

    stream of th

    er of flue ga

    tomatically

    shows the

    eve 90% cap

    at was captu

    e same as the

    et to 1.9 bar

    from 114C

    es to strip

    r, a higher s

    he energy p

    bar) by usi

    2compressi

    eline (MEA).

    Par

    ure (bar)

    t (m)

    eter conditio

    f flue gas an

    nser tempera

    agram

    ll the exhaus

    orber trains

    truction of b

    flash cooler.

    s inlet tempe

    designed to

    fixed parame

    ure in the ab

    ed in the abs

    absorber sol

    o avoid possi

    and 120C,

    the CO2 are

    ripper worki

    enalty. After

    g a 6-stage i

    n process flo

    meter

    solvent at a

    ture (C)

    t gases from

    and one stri

    gger absorbe

    . Compared t

    ature is redu

    vercome the

    ters used in

    sorber. The s

    rption colu

    ent inlet.

    ble MEA de

    epending on

    enhanced,

    ng pressure

    the capture

    tegrally gea

    w diagram.

    sorber inlet

    the power pl

    per [7], [8]

    r diameters t

    the downstr

    ed, enhancin

    pressure dro

    the simulati

    ripping proc

    n. Therefore,

    radation (125

    the loading.

    reducing the

    eeds better q

    process, the

    ed compress

    V

    80%

    4

    4

    FLEXI

    ant. In spite

    this study

    reduce capit

    am position,

    the absorpti

    s in the flue

    n. The solv

    ss is designe

    the solvent l

    C). At this p

    As the stripp

    reboiler dut

    uality steam

    CO2 is co

    r train with i

    alue

    0%

    1,9

    10

    looding

    0C

    0C

    AC 1Y

    f previous

    ollows the

    al cost [9].

    the blower

    on process.

    gas cooler

    ent rate is

    d to desorb

    an loading

    ressure the

    er pressure

    y and the

    to feed the

    pressed to

    tercooling

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    10 Miguel A. Gonzalez-Salazar et al. / Energy Procedia 23 (2012) 3 14

    4.1.Design of Experiment (DOE)In order to evaluate the behavior of the capture plant under different flue gas conditions, three

    variables were selected: lean loading, absorber height and heat exchanger temperature approach. The leanloading and the heat exchanger temperature approach affect the energy requirements in the stripper, in

    particular the sensible and the latent heat. The absorber height affects significantly the absorption capacityand water cooling load in the absorber and just slightly the energy requirement in the stripper. Table 5shows the selected parameters for the design of experiments.For the sake of brevity not all steps of theSix Sigma methodology are shown.

    Lean loadingThe lean loading is defined as the molar ratio of CO2to MEA in the absorber inlet solvent stream. A

    low lean loading means a high capacity of the solvent to absorb CO2, but also a lower CO2 partialpressure at the bottom of the stripper which means a higher amount of energy to desorb CO2. Althoughother studies consider lean loading levels higher than 0,3 mol CO2/mol MEA [4], [10], the market preferslower loading levels to reduce the absorber capital cost. Based on previous experience and data found inthe literature [7], [8], the selected most likely values for the lean loading are 0,25, 0,27 and 0,29 for Case

    1, 2 and 3 respectively, see Table 5. It is important to note that while these are most likely values,optimizing the lean loading for each case was not in the scope of this work.

    Absorber heightThe absorber height was varied for the three flue gas conditions. As the CO2concentration of the flue

    gas increases, higher solvent rate is needed to achieve 90% capture rate. While the diameter of thecolumns is automatically designed to achieve 80% flooding, it is still necessary to adapt the height to theincreasing solvent rate for the different flue gas conditions. Based on previous experience and data foundin the literature [7], [8], the most likely absorber heights are 15, 20 and 25 m for Case 1, 2 and 3respectively.

    Heat exchanger temperature approachThe cold side temperature approach of the heat exchanger considerably affects the sensible heatrequirements in the reboiler duty. Recent papers [10] show the possibility of using 5C instead of 10C toimprove the performance of the plant. This reduction leads to a strong increase in the capital cost. Thesuitability of using a smaller or higher temperature approach will be determined by the business plan. Inthis investigation the selected most likely value for the heat exchanger temperature approach is 9C andthat agrees with another study [11].

    Table 5.Design of Experiment (DOE) for MEAMean Standard

    deviationCase 1 Case 2 Case 3

    Absorber height (m) 15 20 25 1Lean loading (mol CO2 / mol MEA) 0,25 0,27 0,29 0,005

    Heat exchanger approach (C) 9 9 9 0,8

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    Miguel A. Gonzalez-Salazar et al. / Energy Procedia 23 (2012) 3 14 11

    5.Equivalent workAs the energy requirements for the phase-changing absorbent and MEA varied qualitatively, the

    concept of specific equivalent work was used for comparing the performance of the capture technologies.The specific equivalent work has been used in the literature to compare the overall energy requirements(heating, electricity) of different process configurations, capture technologies or solvents [4], [6], [12].Rochelle et al. define the specific equivalent work as the sum of the electric power consumed in the

    process (CO2compressor, pumps, flue gas blower, others) and the work that otherwise could be generatedwith the steam condensing in the reboiler, assuming a 75% Carnot efficiency (see Equation 2).

    Weq=

    (2)

    While the specific equivalent work as defined above might be useful to compare capture technologieswithout the need for specifying details of the power plant, it does not fully describe the overall energy

    penalty. In particular the first term of the equation, defined as the work that could be generated with thesteam condensing in the reboiler (THeating), assumes that the steam extracted from the power plant issaturated and that the heating process is isothermal. However, extraction steam at the specific pressurerequired in the reboiler (~3 bar) rarely occurs in most of todays steam power plants and when it occurs isin superheated condition. This means that the actual extraction temperature is much higher than thesaturation temperature required in the reboiler (max. 125C for MEA to avoid solvent degradation) andtherefore the extracted steam should be desuperheated. This desuperheating effect is though not describedin Equation 2.

    An alternative to account for the desuperheating effect in the specific equivalent work is suggestedhere (see Fig. 4). The approach of converting the heating requirements of the capture plant into specific

    equivalent work is accomplished in two steps. In the first step, the needed steam flow is calculated inThermoflex based on the heat requirements of the desorption process (Q) and the conditions of theextraction steam. It is assumed that the reboiler has a pinch temperature of 10C and therefore therequired steam temperature should be 10C higher than the reboiler temperature. As such, the conditionsof the steam required for the desorption process with MEA are 2,7 bar/130C, 2,6 bar/128,8C and 2,5

    bar/127,6C for cases 1, 2 and 3 respectively. For the phase-changing absorbent the conditions of therequired steam are 2,47 bar/127C. Regarding retrofit and greenfield applications, it is assumed that theextraction steam conditions in both cases are different. For retrofit applications extraction steamconditions are assumed to be those of state-of-the-art supercritical steam power plants, i.e. 5 bar / 291C(Case 11 from DOE/NETL report [1]). For greenfield applications it is assumed that future steam power

    plants will be designed to have steam extraction close to the conditions required for the desorptionprocess, i.e. 3,1 bar/135C. Note that as the pressure and temperature of the available steam are higherthan required, a throttle valve and a desuperheater are used to ensure the right conditions. Throttling anddesuperheating the extraction steam have been commonly used in the CCS literature [1]-[3].

    Once the amount of extraction steam is estimated, the second step is calculating the equivalent powerthat could be otherwise generated. For this purpose a simplified process layout including a low-pressuresteam turbine, a condenser and water pumps was built in Thermoflex. A condenser pressure of 0,069

    bar (1 psia) and a dry step efficiency of 90% for the steam turbine are assumed. Although the described

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    12 Miguel A. Gonzalez-Salazar et al. / Energy Procedia 23 (2012) 3 14

    t

    a

    p

    a

    6

    a

    s

    d

    4

    s

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    o-steps app

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    Fig.

    The modifi

    Weq=

    Where WEqddition to th

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    dicate that fo

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    for the speci

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    d as follows:

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    within one st

    eriment (DO

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    cessary to op

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    ing the specific e

    ic equivalent

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    and specific

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    onditions stu

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    work is show

    d in the twwater coolin

    water coolin

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    ted to be low

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    cations, the

    er than that

    (3)

    (4)

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    Miguel A. Gonzalez-Salazar et al. / Energy Procedia 23 (2012) 3 14 13

    o

    f

    a

    a

    o

    a

    c

    c

    a

    d

    c

    s

    4

    cs

    s

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    Reduced e

    f three main

    or non-absor

    bsorption an

    nd 3) lower

    ccurs at a

    bsorbents is

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    EA retrofit,

    ases the spe

    pplications,

    esorption pro

    With regar

    oncentration

    pecific water

    mole% CO

    ooling load tpecific water

    EA capture

    tandard devia

    hanging abso

    Fig. 5. (a) Comp

    .ConclusionGE is activ

    O2 from po

    tate-of-the-ar

    tate-of-the-ar

    etrofit applica

    ergy require

    actors: 1) les

    ing co-solve

    desorption a

    O2compress

    ressure high

    expected to

    in flue gas t

    at 13 mole%

    cific equival

    s it is assu

    cess in green

    to the speci

    for both pha

    cooling load

    concentrati

    han MEA recooling load,

    and therefor

    tion of the sp

    rbent was ab

    arison of specifi

    s

    ely investiga

    er plants w

    processes. T

    monoethan

    tions.

    ents are exp

    heat is requi

    ts that shoul

    oids the ther

    ion power is

    er than ME

    e more pron

    e specific e

    CO2the redu

    ent work fo

    ed that the

    ield cases tha

    fic water co

    se-changing

    is 8% lower

    ns phase-ch

    pectively. Inthe level of

    higher unce

    ecific equival

    ut 0,05 MJ/k

    equivalent wor

    ting and dev

    th potential

    his investiga

    lamine (ME

    ected for pha

    red in the des

    be heated (

    mal separatio

    equired as th

    (~16 bar).

    ounced at hi

    uivalent wor

    ction could b

    r MEA in

    conditions

    n in retrofit c

    ling load, th

    absorbents a

    or MEA than

    nging absor

    spite of offaturity of th

    rtainty in pe

    ent work in

    -CO2.

    ; (b) Compariso

    loping novel

    ower energy

    ion compare

    ) capture f

    se-changing

    orption proce

    ater in the c

    n and distillat

    e desorption

    This impro

    gher CO2 co

    k of phase-c

    e as high as 4

    reenfield ap

    f extraction

    ases.

    lowest obse

    d MEA cap

    for phase-ch

    ent presente

    ring potentiae phase-chan

    formance is

    EA was abo

    of specific wat

    technologies

    requirements

    the perform

    r different f

    bsorbent co

    ss as a pure a

    ase of MEA),

    ion processes

    rocess in the

    ed perform

    centrations.

    anging abso

    2%. It is imp

    plications is

    steam are

    rvable value

    ture. At this

    nging absor

    d 5% and 6

    l lower speciing absorbe

    expected. Fo

    t 0,010 MJ/

    r cooling load.

    for both ca

    and environ

    ance of phas

    ue gas cond

    pared to M

    sorbent avoi

    2) phase cha

    needed in M

    phase-changi

    nce of phas

    hile at 4

    bent is 25%

    rtant to note

    lower than

    ore appropri

    occurs at 8

    CO2 concen

    ent. Howeve

    lower spe

    ic equivalent is certainly

    instance the

    g-CO2, while

    turing and c

    ental impa

    -changing ab

    tions in gre

    A because

    ds the need

    nge during

    EA capture

    ng concept

    e-changing

    ole% CO2

    lower than

    that for all

    in retrofit

    ate for the

    ole% CO2

    ration, the

    , at 13 and

    cific water

    work andlower than

    calculated

    for phase-

    mpressing

    t less than

    sorbents to

    nfield and

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    14 Miguel A. Gonzalez-Salazar et al. / Energy Procedia 23 (2012) 3 14

    Results indicate that depending on the flue gas conditions, the specific equivalent work necessary foroperating phase-changing absorbents is expected to be up to 40% lower than for MEA capture. Besideslower energy requirements, a potential reduction of up to 6% in specific water cooling load might beexpected for phase-changing absorbent over MEA, for the cases of 4 and 13 mole% CO2 concentrations.However, as the level of maturity of the alternative capture technology is certainly lower than MEAcapture, higher uncertainty in performance is expected.

    Acknowledgements

    The information, data, or work presented herein was funded in part by the Advanced ResearchProjects Agency - Energy (ARPA-E), U.S. Department of Energy under the following contract: Award

    Number DE-AR0000084 in collaboration with University of Pittsburgh.

    Disclaimer: "The information, data, or work presented herein was funded in part by an agency of theUnited States Government. Neither the United States Government nor any agency thereof, nor any oftheir employees, makes any warranty, express or implied, or assumes any information, apparatus, product,or process disclosed, or represents that its use would not infringe on privately owned rights. Reference

    herein any specific commercial product, process, or service by trade name, trademark, manufacturer, orotherwise does not necessarily constitute or imply its endorsement, recommendation, or favoring by theUnited States Government or any agency thereof. The views and opinions of authors expressed herein donot necessarily state or reflect those of the United States Government of any agency thereof."

    References

    [1] DOE/NETL. Cost and performance baseline for fossil energy plants, Volume 1: bituminous coal and natural gas to electricity.Revision 2; 2010.

    [2] Galindo Cifre P, Brechtel K, Hoch S, Garcia H, Asprion N, Hasse H, Scheffknecht G. Integration of a chemical process modelin a power plant modeling tool for the simulation of an amine based CO 2scrubber.Fuel 2009; 88:2481-2488.

    [3] Korkmaz , Oeljeklaus G, Grner K. Analysis of retrofitting coal-fired power plants with carbon dioxide capture. EnergyProcedia2009; 1: 1289-1295

    [4] Plaza J M, Van Wagener D, Rochelle G T. Modeling CO2capture with aqueous monoethanolamine. International Journal ofGreenhouse Gas Control 2010; 4: 161-166

    [5] Kothandaraman A, Nord L, Bolland O, Herzog HJ, McRae GJ. Comparison of solvents for post-combustion capture of CO2bychemical absorption.Energy Procedia 2009; 1: 1373-1380

    [6] Oyenekan B A, Rochelle G T. Stripper models for CO2capture by aqueous solvents. Greenhouse Gas Control Technologies2005; 7: 1861-1864

    [7] Berstad D, Arasto A, Jordal K, Haugen G. Parametric study and benchmarking of NGCC, coal and biomass power cyclesintegrated with MEA-based post-combustion CO2 capture.Energy Procedia2011; 4: 1737-1744

    [8] Lawal A, Wang M, Stephenson P, Obi O. Demonstrating full-scale post-combustion CO2 capture for coal-fired power plantsthrough dynamic modelling and simulation.Fuel2010. Article in Press.

    [9] Reddy S, Johnson D, Gilmartin J. Fluors Econamine FG PlusSM technology for CO2 capture at coal-fired power plants. Airand Waste Management Association - 7th Power Plant Air Pollutant Control 'Mega' Symposium 20081, pp. 63-79

    [10] Van Wagener D H, Rochelle G T. Stripper configurations for CO2 capture by aqueous monoethanolamine and piperazine. Energy Procedia2011; 4: 1323-1330

    [11] Schach M O, Schneider R, Schramm H, Repke J U. Exergoeconomic Analysis of Post-Combustion CO2 Capture Processes.Computer Aided Chemical Engineering2010; 28: 997-1002

    [12] Rochelle G T, et Al. CO2capture by absorption with potassium carbonate.DOE Report, DE-FC26-02NT41440; 2007