MODEL-DERIVED CHEMICAL-LOOPING SYSTEM …...heat + mass transfer in gas Heat transfer between packed...
Transcript of MODEL-DERIVED CHEMICAL-LOOPING SYSTEM …...heat + mass transfer in gas Heat transfer between packed...
04/04/2014
IASE Seminar Series 1/37
Department of Chemical & Biomolecular Engineering University of Connecticut
http://pdsol.engr.uconn.edu
MODEL-DERIVED CHEMICAL-LOOPING SYSTEM DESIGNS
George M. Bollas
04/04/2014
IASE Seminar Series 2/37
Diploma in Chemical Engineering Aristotle University of Thessaloniki – Greece
Ph.D. in Chemical Engineering Aristotle University of Thessaloniki – Greece
Postdoc in Chemical Engineering Massachusetts Institute of Technology – USA
Assistant Professor University of Connecticut NSF CAREER Award 2011 ACS-PRF DNI Award 2013 >$2M in research grants in 2010-2013 9 graduate researchers 10 undergraduate researchers
About
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Research Group (PDSOL)
Catalysis for renewable fuels
Novel spouted-bed reactor for biomass thermochemical processes (pyrolysis, gasification, chemical-looping combustion)
Comprehensive catalyst characterization and catalyst activity dynamic simulation
FTIR real time analyzer
T
T
T
T
T T
T
Liquid & Gas Analysis
Char & Catalyst Collection
N2
N2
vent
vent
vent
Liquid Collection
Gas Collection
Gas Analysis
Coolant
Reactor
Filter
Flow Meter
AugerFeeder
½
¢µ
µ
z
Annulus:@Ca
@t= D@2Ca
@½2 ¡ uij@Ca
@½+ 2D
½@Ca
½
Spout:@Cs
@t+ @Cs
@z
¡us + 1
2dus
¢= 0
Process Design, Scale-up & Control
Dynamic simulation & optimization Optimal experimental design
Model-assisted scale-up based on dynamic sensitivity analysis
Chemical-looping combustion & reforming
Spouted-bed reactor for biomass pyrolysis
Catalyst characterization (ZSM-5 after pyrolysis)
Fixed-bed reactor developed and simulated in PDSOL. Application of Optimal Experimental Design on the laboratory reactor. Scale-up based on sensitivity analysis of the bench-scale reactor.
Dynamic simulation of a spouted bed
Enabling emerging energy technologies via integration of modeling with experimentation of processes lacking fundamental understanding
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IASE Seminar Series 4/37
Carbon capture needs to be deployed to effectively lower the global CO2 portfolio
Climate change urgency
Fig.1: University of Maine Environmental Change Model (UM-ECM) potential
biomes calculated for modern climate. From left to right: input cooled by 4°C; todays
input; input warmed by 2.5°C. Note the effect on the arctic sea ice. Data/images
obtained using Climate Reanalyzer™ (http://cci-reanalyzer.org), Climate Change
Institute, University of Maine, USA.
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Estimated total storage capacity of over 100 Gt in the continental US
US-wide CO2 storage capacity
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IASE Seminar Series 6/37
Back in 2008 Resource: America’s Energy Future Technology And Transformation, Committee On America’s Energy Future, National Academy Of Sciences, National Academy of Engineering, National Research Council of The National Academies, The National Academies Press
CO2 Capture Options
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Boot-Handford ME, Abanades JC, Anthony EJ, Blunt MJ, Brandani S, Mac Dowell N, et al. Carbon capture and storage update. Energy Environ Sci 2014.
Chemical-looping progress
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A method for inherent CO2 separation Oxygen carriers M : metal
MO : metal oxide
Reduction: endothermic CH4 + 4MO CO2 + 2H2O + 4M
Oxidation: exothermic M + ½ O2 MO
Circulating oxygen carrier: active metal oxides (Ni, Cu, Fe, Mn) supported over Al2O3, MgAl2O4, NiAl2O4, YSZ, TiO2, ZrO2. Reactivity testing: TGA, fixed-bed, interconnected fluidized-beds.
Chemical-looping combustion (CLC)
Reducer Oxidizer
CO2 H2O
Fuel
N2 O2
Air
MO
M
water
steam
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[1] Zhou Z, Han L, Bollas GM. Model-based analysis of bench-scale fixed-bed units for chemical-looping combustion. Chem Eng J 2013;233:331–48. [2] Han L, Zhou Z, Bollas GM. Heterogeneous Modeling of Chemical-Looping Combustion. Part 1: Reactor Model. Chem Eng Sci 2013;104:233 – 249. [3] Han L, Zhou Z, Bollas GM. Heterogeneous Modeling of Chemical-Looping Combustion. Part 2: Particle Model. Chem Eng Sci 2014;in press. [4] Zhou Z. Han L, Bollas GM. Overview of Chemical-Looping Reduction in Fixed Bed and Fluidized Bed Reactors Focused on Oxygen Carrier Utilization and Reactor Efficiency. Aerosol Air Qual Res 2014;14:559–71. [5] Zhou Z, Han L, Bollas GM. Kinetics of NiO reduction by H2 and Ni oxidation at conditions relevant to chemical-looping combustion and reforming. Int J Hydrogen Energy 2014;in press. [6] Han L, Zhou Z, Bollas GM. Chemical-looping combustion in a reverse-flow fixed-bed reactor. Appl Energy 2014;in review. [7] Zhou Z, Han L, Bollas GM. Model-assisted analysis of fluidized bed chemical-looping reactors. AIChE J 2014;in review. [8] Han L, Zhou Z, Bollas GM. Optimal Experimental Design for Fixed Bed Chemical-Looping Experiments. Comput Chem Eng 2014;in preparation.
Our work
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OED for process scaling of chemical-looping: Measurements of bench- and pilot- scale processes are used to develop state/space models. These models are subsequently used to identify time-varying experimental conditions that maximize the statistical significance of the measurements with respect to process scale, subject to constraints.
The “dream concept”
maximize information content of experiments integrate experimentation with reactor design obtain scale-independent process models estimate model parameters that increase the accuracy of process scale-up/scale-down reduce risk of technology scale-up/scale-down.
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Heterogeneous model Fluid phase
𝜀𝑏𝜕𝐶𝑖𝜕𝑡
+𝜕𝐹𝑖𝜕𝑉
=𝜕
𝜕𝑧𝜀𝑏𝐷𝑎𝑥,𝑖
𝜕𝐶𝑖𝜕𝑧
+ 𝑘𝑐,𝑖𝑎𝑣 𝐶𝑐,𝑖|𝑅𝑝 − 𝐶𝑖
𝜀𝑏𝐶𝑝𝑓𝐶𝑇𝜕𝑇
𝜕𝑡+ 𝐶𝑝𝑓𝐹𝑇
𝜕𝑇
𝜕𝑉 =
𝜕
𝜕𝑧𝜀𝑏𝜆𝑎𝑥
𝜕𝑇
𝜕𝑧
+ℎ𝑓𝑎𝑣 𝑇𝑐|𝑅𝑝 − 𝑇 +4𝑈
𝐷𝑅(𝑇𝑤 − 𝑇)
Solid phase
𝜀𝑐𝜕𝐶𝑐,𝑖𝜕𝑡
=1
𝑟𝒄2
𝜕
𝜕𝑟𝑐𝐷𝑒,𝑖 𝑟𝑐
2𝜕𝐶𝑐,𝑖𝜕𝑟𝑐
+ 𝜌𝑠 𝑅𝑖
1 − 𝜀𝑐 𝜌𝑠𝐶𝑝𝑠 + 𝜀𝑐𝐶𝑝𝑐𝐶𝑇,𝑐𝜕𝑇𝑐𝜕𝑡
=
𝜆𝑠𝑟𝑐2
𝜕
𝜕𝑟𝑟𝑐2𝜕𝑇𝑐𝜕𝑟𝑐
+ 𝜌𝑠 (−𝛥𝐻𝑖)(𝑅𝑖)
Pressure drop 𝑑𝑃
𝑑𝑧= −
1 − 𝜀𝑏𝜀𝑏
3
𝜌𝑢02
𝐷𝑝
150
𝑅𝑒𝑝+ 1.75
Fixed-bed model description
Fu
rna
ce
wa
ll
Tube wall
Oxygen carrier
particles
Axial convective
heat + mass
transfer in gas
Heat transfer between
packed bed and wall
Axial dispersion of
heat and mass
External diffusion
across film
Reactions on
pore surface
Pore diffusion
Bulk
fluid
Solid
phase
Heat conduction
Heat conduction
through packed-bed
Han, L.; Zhou, Z.; Bollas, G. M. Heterogeneous Modeling of Chemical-Looping Combustion. Part 1: Reactor Model. Chemical Engineering
Science 2013
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Application to experimental data of CLC by Iliuta et al. (2010), Ryden et al. (2008) and CLR data by Jin (2002)
Fixed-bed model application
Han, L.; Zhou, Z.; Bollas, G. M. Heterogeneous Modeling of Chemical-Looping
Combustion. Part 1: Reactor Model. Chemical Engineering Science 2013
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Reduction reactions with NiO
Oxygen carrier
reduction
reactions
CH4 oxidation CH4 + 2NiO ↔ 2Ni + CO2 + 2H2 ΔH°= 165 kJ/mol
H2 oxidation H2 + NiO ↔ Ni + H2O ΔH°= -2.2 kJ/mol
CO oxidation CO + NiO ↔ Ni + CO2 ΔH°= -43.3 kJ/mol
Partial CH4 oxidation CH4 + NiO ↔ Ni + 2H2+CO ΔH°= 203 kJ/mol
Reactions
catalyzed by Ni
Steam reforming CH4 + H2O ↔ 3H2 + CO ΔH°= 205 kJ/mol
Water gas shift CO + H2O ↔ H2 + CO2 ΔH°= -41.1 kJ/mol
Dry reforming CH4 + CO2 ↔ 2CO + 2H2 ΔH°= 247 kJ/mol
Methane
decomposition
CH4 ↔ 2H2 + C ΔH°= 88 kJ/mol
Carbon gasification by
steam
C + H2O ↔ CO + H2 ΔH°= 131 kJ/mol
Carbon gasification by
CO2
C + CO2 ↔ 2CO ΔH°= 173 kJ/mol
Zhou, Z.; Han, L.; Bollas, G. M. Model-based Analysis of Bench-Scale Fixed-Bed Units for Chemical-Looping Combustion. Chemical
Engineering Journal 2013
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Mass balance
Intraparticle velocity (forced convection)
Boundary Conditions
Mass Balance around the crucible
Boundary Conditions
TGA Model
, 2 2
, eff, ,2 2
1 1
c i
c c c i c i c i s
c c c c
j
c
c
Cr C r D C
t r r r r rv R
1
,
1
j
j
c
i
c
c i
R
r
v
C
eff, ,
, c, ,( )cc p c p
c p
p
i c i
c c i i c i ir r r rr rc
r r
D Cv C k C C
r
0
,
0
0c
c
r
r
c i
c
c
Cv
r
, c, ,( )
c pv r r
i ib b ax i i c i ia
C CD k C C
t z z
,
,
0
0( )TGA
iz
m iib ax i i
zz
CDC
D C
0i
z h
C
z
Han, L.; Zhou, Z.; Bollas, G. M. Heterogeneous Modeling of Chemical-Looping
Combustion. Part 2: Particle Model. Chemical Engineering Science 2013
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Analysis of available literature on reduction of supported and unsupported NiO by H2
Models of varying degree of fidelity (number of parameters) F-test Akaike Information Criterion
Non-catalytic gas-solid reactions
Zhou, Z.; Han, L.; Bollas, G. M. Kinetics of NiO reduction by H2 and Ni oxidation at conditions relevant to chemical-looping
combustion and reforming. Int. Journal of Hydrogen Energy, 2014
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Fixed-bed apparatus NiO/Al2O3 oxygen carrier preparation
Dry impregnation with loading of 20 wt% Ni Particle size: 50-150 μm Surface area: 90 m2/g
Current experimental setup
Experimental conditions
Reduction temperature
800°C
Reduction time 1 min
Reducing gas flow 20 CH4 + 80 Ar ml/min
Solid loading 2 g
Purge time 3 min
Oxidizing gas 100 air ml/min
Oxidation time 3 min
Tube ID 0.99 cm
Tube length 30 cm
Ar
Air
CH4
Filter
Mass
selective
detectorVent
Reactor
Oxygen
Carrier
F
MFC3
F
MFC2
F
MFC1
T1
T2
Vent
Pressure
Regulator
Furnace
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Model, system of DAE’s 𝐟 𝐱 𝑡 , 𝐱 𝑡 , 𝐮 𝑡 ,𝐰 , 𝛉, 𝑡 = 0 𝐲 𝑡 = 𝐡(𝐱 𝑡 )
Sensitivity matrix
𝑸 =
𝜕𝑦 1
𝜕𝜃𝑖⋯
𝜕𝑦 1
𝜕𝜃𝑝
⋮ ⋱ ⋮𝜕𝑦 𝑛
𝜕𝜃𝑖⋯
𝜕𝑦 𝑛
𝜕𝜃𝑝
Dynamic Sensitivity Analysis
Local methods Differentiation of model equations
d
dt
𝜕𝐲
𝜕𝛉=𝜕𝐟
𝜕𝐲 ∙𝜕𝐲
𝜕θ+𝜕𝐟
𝜕𝛉
𝐟 : continuous function
𝐱 𝑡 ∶ differential state variables
𝐮 𝑡 ∶ time-varying controls
𝐰 ∶ time-constant controls
𝛉 ∶ parameter vector
𝐡 𝐱 𝑡 : measured state variables
𝐲 t ∶ measured responses
Results for CLC fixed-bed reactor:
00.2
0.40.6
0.81
05
10
15
20
25
300
20
40
60
Length (normalized)Time [sec]
No
rma
lize
d s
en
sitiv
ity
00.2
0.40.6
0.81
05
10
15
20
25
300
0.2
0.4
0.6
0.8
Length (normalized)TIme [sec]
No
rma
lize
d s
en
sitiv
ity
00.2
0.40.6
0.81
05
10
15
20
25
300
0.5
1
1.5
Length (normalized)Time [sec]
No
rma
lize
d s
en
sitiv
ity
k1 k2
k3 k4
00.2
0.40.6
0.81
0
5
1015
20
25
300
0.2
0.4
0.6
0.8
Length (normalized)Time [sec]
Norm
alized s
ensitiv
ity
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Structural local identifiability test (SLI) (1) Correlation of sensitivity matrix is different from ±1 (2) Fisher information matrix is non-singular
Structural global identifiability test (SGI) Verifies if parameter sets do not provide the same model responses
Identifiability Analysis
SLI test Design
experiment SGI test det (𝐻𝜃
∗) = 0
?
Y
N
Change model structure
𝑃𝑎𝑠𝑠? End Y
N
*
1 1
ytsNN
T
θ ij i j
i j
H Q Q
* *
, *max ε
TI
θ θ θ θ
θ θ W θ θ
y
τ
y
Tdt ε,,,, 00
0
00 **θuyθuyWθuyθuy
Subject to:
𝛉, 𝛉∗: parameter sets 𝐲 ∶ model trajectory 𝒖𝟎 ∶ initial controls 𝐖 ∶ weights 𝜀𝜃 , 𝜀𝑦 ∶ small numbers
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Arrhenius Expression: SLI results:
1 experiment High correlation Unidentifiable
2 experiments Identifiable
SGI results: Φ𝐼 = 4E-10 < εθ = 1E-6 ε𝑦 = 1E-3
Identifiability Analysis: Arrhenius Expression
Optimal experiments
T [℃] 600 800
QCH4 [sccm] 30 30
Solids [g] 1.2 2.2
Ea1 Ea2 Ea3 Ea4 k1 k2 k3 k4
Ea1 1.000
Ea2 -0.394 1.000
Ea3 -0.247 -0.022 1.000
Ea4 -0.140 -0.143 -0.589 1.000
k1 -0.817 0.287 0.644 -0.271 1.000
k2 -0.396 1.000 -0.025 -0.140 0.289 1.000
k3 -0.290 -0.017 0.999 -0.575 0.666 -0.019 1.000
k4 -0.052 0.316 -0.165 -0.573 0.045 0.317 -0.158 1.000
Ea1 Ea2 Ea3 Ea4 k1 k2 k3 k4
Ea1 1.000
Ea2 -0.108 1.000
Ea3 -0.917 0.199 1.000
Ea4 -0.726 0.164 0.810 1.000
k1 -0.385 0.035 0.213 -0.002 1.000
k2 -0.134 -0.044 0.317 0.339 -0.048 1.000
k3 -0.758 0.193 0.886 0.818 -0.214 0.333 1.000
k4 0.027 0.166 0.047 -0.050 -0.291 -0.053 0.145 1.000
Correlation matrix of Arrhenius parameters
Correlation matrix of Arrhenius parameters
Han L, Zhou Z, Bollas GM. Optimal Experimental Design for Fixed Bed
Chemical-Looping Experiments. Comput Chem Eng 2014
k = kref exp −E
R
1
T−
1
Tref
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Build first principles process model
T
Design optimal experiment
Conduct experiment at
specified conditions
Estimate parameters &
confidence intervals
Interval #1 Interval #2
Model-guided experiment
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Motivation: maximize information content for parameter estimation
𝝋𝑜𝑝𝑡 =argmin𝛗
det 𝑯𝛉−1 𝛉,𝛗
subject to: 𝐟 𝐱 𝑡 , 𝐱 𝑡 , 𝐮 𝑡 ,𝐰 , 𝛉, 𝑡 = 0
φ𝑖𝐿 ≤ φ𝑖
≤ φ𝑖𝑈
Model + experimental results
Optimal experimental design (OED)
Kinetics Nominal exp. Optimal exp.
k1 0.3880 0.1654
k2 1.4416 0.8379
k3 0.6005 0.1461
k4 3.2706 0.3118
Norm 95% confidence interval
0 5 10 15 20 25 300
0.02
0.04
0.06
0.08
0.1
0.12
0.14
0.16
0.18
0.2
Time [sec]
Mol
e fr
actio
n of
gas
spe
cies
Comparison of optimal (-) and baseline (--) experiments
CO2
CO
CH4
data4
data5
data6
data7
data8
data9
data10
data11
Design criterion: D-OPTIMALITY
Improves parameter estimation
for all uncertain kinetic
parameters
Experiments
Standard Optimal
T [℃] 700 700
QCH4 [sccm] 10 20
Solids [g] 2 2
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Kunii & Levenspiel 3-phase model
ub
uo
us
ue
Bubble phase
us
Wake
Emulsion phase
Dense phase
Freeboarduf us,f
Fluidized bed model
Zhou, Z.; Han, L.; Bollas, G. M. Modeling
Chemical-Looping Combustion in
Bubbling Fluidized Bed Reactors. AIChE
J. 2014
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Fluidized Bed chemical-looping – prediction and analysis
Model is predictive (kinetic mechanism and constants of the fixed bed models used)
Freeboard contributes significantly to CH4 conversion and completion of oxidation
Consistent with all relevant experimental observations from various laboratories
Fluidized bed operation
- Zhou, Z.; Han, L.; Bollas, G. M. Modeling Chemical-Looping Combustion in Bubbling Fluidized Bed Reactors. AIChE J. 2014
- Zhou, Z.; Han, L.; Bollas, G. M. Overview of chemical-looping reduction in fixed-bed and fluidized-bed reactors focused on oxygen carrier utilization
and reactor efficiency. Aerosol & Air Quality Research. 2014
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Comprehensive comparison of two reactor designs (fixed and fluidized bed) of the same oxygen carrier loading The fixed bed reactor is inferior in all aspects including
CO2 selectivity Carbon formation Bed isothermality
Fixed/Fluidized beds comparison
Zhou Z, Han L, Bollas GM, Overview of Chemical-Looping Reduction in Fixed Bed and
Fluidized Bed Reactors Focused on Oxygen Carrier Utilization and Reactor Efficiency.
Aerosol Air Qual Res 2014;14:559–71
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Chemical-Looping Most efficient method for CO2 capture Very high research effort Tremendous research expenditure Combustion or reforming are feasible Mature process
Summary of background
Our work Modeled all fixed bed reactors with CH4 and NiO Predicted all fluidized beds with CH4 & NiO Compared fixed and fluidized bed CLC and CLR Setup a bench-scale fixed bed reactor
Process Options Fluidized beds Fixed beds Rotary beds Rotating beds Moving beds
Reactor options for Chemical-looping Combustion (CLC): (a) circulating fluidized-bed; (b) rotating reactor; and (c) alternating flow over a fixed-bed.
O2
N2
Air
CO2
H2O
Fuel
MeO
Me
Reducer Reactor Oxidizer Reactor
O2
N2
AirCO2
H2O
Rotating Reactor
MeO
Me
O2
N2
Air
CO2
H2O
Fuel
Alternating Flow
Fuel MeO
Me
Me
MeO
(a) (b) (c)
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Typical fixed-bed experiment
Experimental settings
Reduction temperature
800°C
Reduction time 1 min
Reducing gas flow
10 CH4 in 100 ml/min
Solid loading 2 g
Oxygen carrier conversion
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Design of the novel reactor setup
Reverse-Flow Fixed-bed CLC Reactor
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A novel fixed-bed chemical-looping reactor configuration was invented, in which the fuel flow direction is periodically switched during each cycle. The new design significantly improves the performance of fixed-bed chemical-looping reactors, making them competitive to their fluidized-bed equivalents, while overcoming their operating bottlenecks. The novel system enables:
(1) improved oxygen carrier utilization, (2) higher CO2 capture efficiency (by up to 50%), (3) mitigation of hot and cold zones, (4) elimination of gas-solids separation steps, (5) resistance to carbon deposition.
Advantages relevant to the oxygen carrier used (as compared to current process configurations) relate to the elimination of:
(6) need for oxygen carrier fluidizability, (7) attrition, (8) toxic solid fines effluents, (9) need for oxygen carrier addition.
Patent Claims (Bollas, Han 2014)
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Model Description
1D heterogeneous model
Dusty-gas model (concentrated transport)
Time varying boundary conditions for the
fluid phase
Full heterogeneous design equations
Reverse-Flow Fixed-bed Reactor Model
, 2
2
( 1
)c c i
c s ii
c c
Cr R
t r rJ
,i
1 ij i
1Nc i
k i i ke ejc K
C Jy J y J
r D D
, , ,
2
2
1
1( )
cc s p s c p c T c
cc s s i i
c c
TC C C
tT
r H Rr r r
Solid
ph
ase
Flu
id p
ha
se , , ,
)( ( )
c P
b i i i
b ax i c i v rc iri
C uC CD k a C C
t z z z
, ,( ) (C )
c P
b p f T T p f
b ax f v c r r
uC C T C T Th a T
t z z zT
2
0
3
1 1501.75b
b p p
udP
dz d Re
outz LP P
0
0
0 c
c
ci r
c r
TJ
r
, ,
Pc cpi c i c i ir rr r
J k C C
c p
c p
cs f c r r
c r r
Th T T
r
U t t u
1, 1 , 1 2
1, 1 2 ,
s s
s s
t n t n tt
t n t nt
,in
,
,in
1,
20
1,
2
i ii
b ax i
i i
C zt
C
u CC
Dz t
u C z L
,
,
, 01
2
1,
2
in T p f
b ax
in T p f
tu T T C C
T
z tu T T C C
z
z L
Han L, Zhou Z, Bollas GM. Chemical-looping combustion in a reverse-
flow fixed-bed reactor. Applied Energy 2014
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CH4 conversion and CO2 selectivity
Reactor in this study is suboptimal for fair comparison with existing fixed bed reactors
Performance metrics I
Table: CO2 capture efficiency for varying oxygen carrier conversion
← Bench-scale reactor
Industrial-scale reactor →
Han L, Zhou Z, Bollas GM. Chemical-looping combustion in a reverse-
flow fixed-bed reactor. Applied Energy 2014
Bollas GM, Han L. Reverse-Flow Reactor for Chemical-Looping
Combustion and Reforming of Gaseous Fuels; US Provisional Patent -
University of Connecticut, 2014.
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Performance metrics II
Oxygen carrier conversion Bed Temperature Profile
Carbon Formation Solid Carbon selectivity and Max Bed T drop
Han L, Zhou Z, Bollas GM. Chemical-looping combustion in a reverse-
flow fixed-bed reactor. Applied Energy 2014
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Scaled-up Performance metrics I
Scale-up procedure Commercially realistic industrial-scale fixed-bed reactor Small particle size (300 µm) to minimize diffusion effects Significant pressure drop in the system =>
Constraint: bed height should not exceed 1 m
Scaling factors: L/D ratio and Froude number
Reactor still suboptimal Performance enhancement improved
Han L, Zhou Z, Bollas GM. Chemical-looping combustion in a reverse-
flow fixed-bed reactor. Appl Energy 2014
Bollas GM, Han L. Reverse-Flow Reactor for Chemical-Looping
Combustion and Reforming of Gaseous Fuels; US Provisional Patent -
University of Connecticut, 2014.
Bench-scale reactor Industrial-scale reactor L [m] 0.22 1.0
D [m] 0.055 0.25
Q (L/min) 16.68 (100% CH4) 3000 (100% CH4) Fr 0.34 0.39
L/D 4 4
Rep 0.80 6.9
ΔP [bar] 0.3 4
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Scaled-up Performance metrics II
Han L, Zhou Z, Bollas GM. Chemical-looping combustion in a reverse-
flow fixed-bed reactor. Applied Energy 2014
Oxygen carrier conversion Bed Temperature Profile
Carbon Formation Solid Carbon selectivity and Max Bed T drop
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What we should have done (Model-Based Development) Statistical Analysis of Existing Data and Kinetics Models (F-test, AICc) Fixed-bed model utilizing statistically significant kinetics Optimal Experimental Design for derivation/validation of unknown kinetics Fluidized-bed model prediction and validation Fixed-bed / Fluidized-bed comparison Reverse-flow fixed-bed reactor invention
What we accomplished so far: A novel reactor concept was invented that addresses the roadblocks to commercialization of existing chemical-looping processes
Our Aim to put chemical-looping research and technology on a fundamentally new learning curve; one that relaxes the requirement for fluidized-bed reactor systems and is capable of making chemical-looping a disruptive new technology
Conclusions
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Zhiquan Zhou 4th year PhD Student, CBE UConn Fluidized bed modeling, dynamic parameter estimation, statistical analysis
Lu Han 3rd year PhD Student, CBE UConn gPROMS, sensitivity analysis, optimal experimental design
Acknowledgments
NSF CAREER Award No. 1054718 Process and Reaction Engineering Program, CBET
UCONN Prototype Fund Office of the Vice President for Research
Ari Fischer Oscar Nordness Catherine Cheu
Kyle Such Clarke Palmer
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Thank you!
Department of Chemical & Biomolecular Engineering University of Connecticut
http://pdsol.engr.uconn.edu
George M. Bollas