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Steady-State and Dynamic Modeling of a
Moving Bed Reactor for Solid-Sorbent CO2
Capture
Srinivasarao Modekurti, Debangsu Bhattacharyya
West Virginia University, Morgantown, WV
Stephen E. Zitney
National Energy Technology Laboratory, Morgantown, WV
David C. Miller
National Energy Technology Laboratory, Pittsburgh, WV
1
AIChE 2013 Annual Meeting
San Francisco, CA, USA, November 3-8, 2013
OUTLINE
Motivation
Dynamic Model Development
Results and Discussions
Conclusions
2
MOTIVATION
Under the auspices of US DOE’s Carbon Capture
Simulation Initiative (CCSI), we are developing
computational models of various post-combustion CO2
capture technologies
As part of this project, our current focus is on the
development of dynamic models and control systems for
solid-sorbent CO2 capture processes.
3
4
Optimized Process Developed using CCSI Toolset
GHX-001
CPR-001
ADS-001
RGN-001
BLR-001
Flue Gas from Plant
Clean Gas to Stack
CO2 to Sequestration SHX-01
SHX-02
CPR-002
LP/IP Steam from Power Plant
CPP-002
ELE-002
ELE-001
Flue Gas
Clean Gas
Rich Sorbent
LP Steam
HX Fluid
Legend
Rich CO2 Gas
Lean Sorbent
Parallel ADS Units
Parallel RGN Units
Parallel ADS Units
GHX-002
CPP-000
Cooling Water
Injected Steam
Cooling Water
Saturated Steam Return to Power Plant
Mild SteamDirectly Injected into Reactor
Compression Train
Co
nd
en
sed
W
ate
r
Co
nd
en
sed
W
ate
r
Solid Sorbent MEA27
(D10°C HX) MEA27
(D5°C HX) Q_Rxn (GJ/tonne CO2) 1.82 1.48 1.48
Q_Vap (GJ/tonne CO2) 0 0.61 0.74
Q_Sen (GJ/tonne CO2) 0.97 1.35 0.68
Total Q 2.79 3.44 2.90
ADS-001A ADS-001B
Diameter (m) 9.748
Bed Depth (m) 7.232 4.854
Total HX Area (m2) 1733.7 941.3
RGN-001
Diameter (m) 7.147
Height (m) 4.592
Total HX Area (m2) 1573.1
Solid Sorbent:
NETL 32D,
a mesoporous
amine-impregnated
silica substrate
MOVING BED DYNAMIC MODEL DEVELOPMENT
1-D two-phase pressure-driven non-isothermal dynamic
model of a moving bed reactor as part of a solid-
sorbent CO2 capture process
Model Assumptions Vertical shell & tube type reactor
Gas and solids flows are modeled by plug flow
model with axial dispersion.
Particles are uniformly dispersed through the
reactor with constant voidage
Particle attrition ignored
Temperature is uniform within the particles
Solid In
Solid Out
Gas In
Gas Out
Utility In
Utility Out
• Gaseous species : CO2, N2, H2O
• Solid phase components: bicarbonate,
carbamate, and physisorbed water.
5
MODEL DEVELOPMENT
• Radial variation neglected
• Perforated trays are used to distribute the solids
uniformly
• Stripping steam is used
• The solids enter the bed from a preheater at about 95oC
6
CONSERVATION EQUATIONS
Effective Axial Dispersion Coefficient*
Solid Phase
Gas Phase
7
*Ruthven, D. M. Principles of adsorption and adsorption processes; Wiley-Interscience, 1984
CONSERVATION EQUATIONS CONTD.
Energy Balance
Gas Phase
Solid Phase
Tube wall
8
Immersed Heat Exchanger Model
Heat Transfer Coefficient calculated by modified Packet Renewal theory1
0.140.225
22
,
0.44p p
i
xmf n i h
d g d
dv f a
0.14
22
,
, 0.33mf n i h
b i
p
v f af
d g
1Baskakov, et al., Heat Transfer to Objects Immersed in Fluidized Beds. Powder Technology, 1973. 8, pg. 273-282. 2Mickley and Fairbanks., Heat Transfer to Objects Immersed in Fluidized Beds. Powder Technology, 1973. 8, pg. 273-282.
, , , , , ,
,
12
p a i s p s e i d i
d i
i
k ch
0.5 0.33
,
,
,
,
0.009 Prh i i i
l i p
h i
g i
Nu Ar
h dNu
k
, , , , ,1t i b i d i b i l ih f h f h
Between Solids and Heat Exchanger Tube2
Between Gas and Heat Exchanger Tube1 Overall Heat Transfer Coefficient
9
10.632 1.1Pr Re
gs p
p
g
h dNu
k
Pressure drop
Modified Ergun Equation is used by using the slip velocity between the interstitial
fluid velocity and particle velocity instead of the superficial velocity
10
HYDRODYNAMIC MODEL
Maximum Gas Velocity for Maintaining the Bed in the Moving Bed Regime*
External mass transfer resistance is considered by using Frössling correlation
Constraint
3
, ,
2
,
p g i s g i
i
g i
d gAr
11
* Chehbouni, et al., The Canadian Journal of Chemical Engineering 1995, 73, 41–50.
g cv U
REACTION KINETICS
𝐻2𝑂 𝑔 ↔ 𝐻2𝑂 𝑝ℎ𝑦𝑠
2𝑅2𝑁𝐻 + 𝐶𝑂2,(𝑔) ↔ 𝑅2𝑁𝐻2+ + 2𝑅2𝑁𝐶𝑂2
−
𝑅2𝑁𝐻 + 𝐶𝑂2,(𝑔) + 𝐻2𝑂 𝑝ℎ𝑦𝑠 ↔ 𝑅2𝑁𝐻2+ + 𝐻𝐶𝑂3
−
12
*Lee et al. A model for the Adsorption Kinetics of CO2 on Amine-Impregnated Mesoporous Sorbents in the Presence of Water, 28th
International Pittsburgh Coal Conference 2011, Pittsburgh, PA, USA.
12
REACTION KINETICS
*Lee et al. A model for the Adsorption Kinetics of CO2 on Amine-Impregnated Mesoporous Sorbents in the Presence of Water, 28th
International Pittsburgh Coal Conference 2011, Pittsburgh, PA, USA.
-52,100 -78.5
-36,300 -88.1
-64,700 -174.6
28,200 0.0559
58,200 2.6167
57,700 0.0989
1.17
13
H2O
Bic
Bic
Car
Car
m
H2O
Modeling of Balance of the Unit
Pressure flow-network developed along with the control valves
14
Variable Base Value Units
Reactor Diameter 9 m
Reactor Height 7 m
Average voidage 0.6
Steam inlet flow rate 1000 kmol/hr
HX steam flow rate 2983.09 kmol/hr
Diameter of HX tube 0.015 m
Solids inlet flow rate 550000 Kg/hr
Solids inlet temperature 52.32 oC
Initial loading of bicarbonate 0.263 mol/kg sorbent
Initial loading of carbamate 1.797 mol/kg sorbent
Initial loading of water 0.651 mol/kg sorbent
Regenerator Parameters and Operating Conditions
15
SOLUTION METHODOLOGY
All the equations are written and solved in
Aspen Custom Modeler
The dynamic model is solved using the
Method of Lines
16
Moving Bed Regenerator: Results
0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.90.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
Z/L
Mo
le F
racti
on
CO2
H2O
Gas OutletGas Inlet
0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.90.4
0.6
0.8
1
1.2
1.4
1.6
1.8
Z/L
Mo
lar
Lo
adin
g (
mo
l/kg
so
lids)
Bic
Car
H2O
Solids InletSolids Outlet
0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9110
112
114
116
118
120
122
124
126
128
130
Z/L
So
lids
Tem
per
atu
re (C
)
Solids Outlet Solids Inlet 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9900
1000
1100
1200
1300
1400
1500
1600
1700
1800
1900
Z/L
Gas
Flo
w R
ate
(km
ol/h
r)
Gas Inlet Gas Outlet
17
Transient Response of Key Regenerator Variables Due to 10% Step
Increase in Sorbent Flowrate (open- loop)
W
Time Seconds
Str
ipper_
TC
.PV
C
B1.S
olid
OU
T.w
("H
2O
") m
ol/kg s
olid
B1.S
olid
OU
T.w
("C
ar"
) m
ol/kg s
olid
B1.S
olid
OU
T.w
("B
ic")
mol/kg s
olid
0.0 100.0 200.0 300.0 400.0 500.0
115.0
120.0
125.0
130.0
135.0
140.0
0.7
50.7
75
0.8
0.8
25
0.8
50.8
75
0.9
0.9
25
0.8
0.8
25
0.8
50.8
75
0.9
0.9
25
0.9
50.9
75
0.2
80.2
90.3
0.3
10.3
20.3
30.3
4
18
Sorbent flowrate increased by 10%, only outlet temperature controlled W
Time Seconds
Str
ipper_
TC
.PV
C
B1.S
olid
OU
T.w
("H
2O
") m
ol/kg s
olid
B1.S
olid
OU
T.w
("C
ar"
) m
ol/kg s
olid
B1.S
olid
OU
T.w
("B
ic")
mol/kg s
olid
0.0 250.0 500.0 750.0 1000.0 1250.0 1500.0 1750.0 2000.0
120.0
125.0
130.0
135.0
140.0
0.7
50.7
75
0.8
0.8
25
0.8
50.8
75
0.9
0.9
25
0.8
0.8
25
0.8
50.8
75
0.9
0.9
25
0.9
50.9
75
0.2
80.2
90.3
0.3
10.3
20.3
30.3
4Transient Response of Key Regenerator Variables Due to 10% Step
Increase in Sorbent Flowrate (Only Outlet Temperature Controlled)
19
W
Time Seconds
Str
ipper_
TC
.PV
C
B1.S
olid
OU
T.w
("H
2O
") m
ol/kg s
olid
B1.S
olid
OU
T.w
("C
ar"
) m
ol/kg s
olid
B1.S
olid
OU
T.w
("B
ic")
mol/kg s
olid
0.0 250.0 500.0 750.0 1000.0 1250.0 1500.0 1750.0
127.9
128.0
128.1
128.2
128.3
128.4
0.8
30.8
35
0.8
40.8
45
0.8
50.8
55
0.8
6
0.8
90.8
95
0.9
0.9
05
0.3
05
0.3
10.3
15
0.3
20.3
25
Transient Response of Key Regenerator Variables Due to 10% Step
Increase in Sorbent Flowrate (Both Outlet Temperature and Steam to
Sorbent Ratio Controlled)
20
Comparison of Initial Steady State Conditions to the Steady
State Conditions After 10% Step Increase in Sorbent Flowrate
21
Bicarbamate (mol/kg solid)
Carbamate (mol/kg solid)
Physiosorbed Water
(mol/kg solid)
Initial 0.311 0.891 0.837
Only Outlet Temperature
Control
0.322 0.923 0.836
Both Outlet Temperature
and Ratio Controlled
0.313 0.895 0.842
W
Time Seconds
Str
ipper_
TC
.PV
C
B1.S
olid
OU
T.w
("H
2O
") m
ol/kg s
olid
B1.S
olid
OU
T.w
("C
ar"
) m
ol/kg s
olid
B1.S
olid
OU
T.w
("B
ic")
mol/kg s
olid
0.0 250.0 500.0 750.0 1000.0 1250.0 1500.0 1750.0
120.0
125.0
130.0
135.0
140.0
0.7
50.7
75
0.8
0.8
25
0.8
50.8
75
0.9
0.9
25
0.8
0.8
25
0.8
50.8
75
0.9
0.9
25
0.9
50.9
75
0.2
80.2
90.3
0.3
10.3
20.3
30.3
4Transient Response of Key Regenerator Variables Due to 20% Step
Increase in Carbamate Loading (Both Outlet Temperature and Ratio Controlled)
22
CONCLUSIONS 1. A one-dimensional, non-isothermal, pressure-driven dynamic
model of a moving bed reactor mainly to be used as the
regenerator has been developed in ACM.
2. The model has been developed in analogy to fixed bed and
fluidized bed reactors.
3. When both the outlet temperature and the ratio of the
stripping steam flowrate to the solids flowrate are controlled,
the reactor is found to reject disturbances satisfactorily.
23
Acknowledgements: • As part of the National Energy Technology Laboratory’s
Regional University Alliance (NETL-RUA), a collaborative
initiative of the NETL, this technical effort was performed under
the RES contract DEFE0004000.
Disclaimer: This presentation was prepared as an account of work sponsored by an
agency of the United States Government. Neither the United States
Government nor any agency thereof, nor any of their employees, makes
any warranty, express or implied, or assumes any legal liability or
responsibility for the accuracy, completeness, or usefulness of any
information, apparatus, product, or process disclosed, or represents that
its use would not infringe privately owned rights. Reference herein to any
specific commercial product, process, or service by trade name,
trademark, manufacturer, or otherwise does not necessarily constitute or
imply its endorsement, recommendation, or favoring by the United States
Government or any agency thereof. The views and opinions of authors
expressed herein do not necessarily state or reflect those of the United
States Government or any agency thereof.
24
Thank you
25