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Bench-scale experiments and CFD simulations for Low Aqueous Solvent with different packings
Zhijie (Jay) Xu, Pacific Northwest National Lab (PNNL)Richard Zheng, Pacific Northwest National Lab (PNNL)
Christine Anderson-Cook, Los Alamos National Lab (LANL)
Challenges & Objectives
22
Challenges:Packing characterization at device scale: Effective mass transfer area ae
Gas-film mass transfer coefficient kg
Liquid-film mass transfer coefficient kl
Counter-current
flow
Flue Gas
Lean Solvent
PurifiedGas
Rich Solvent
to Stripper
film thickness~ O(0.1mm)
Layer height:~20cm
Corrugation height:O(10 mm)
Column:Φ ~10mH ~30m
Source4
Structured
Random
Objectives: Using CFD to
directly model mass transfer area at bench-scale
understand the local hydrodynamics /mass transfer with complex geometry
Using bench-scale column exp. to study the performance of
solvent/packing validate the CFD area model
Outline
Bench-scaled Packed Column (Overview) Experiments (EEMPA & MEA) CFD Simulations
• 1:1 full size column CFD modeling• Representative column CFD modeling
Experiment / CFD Comparison Plan for Sequential Design of Experiment (SDoE) Conclusion
3
Outline
Bench-scaled Packed Column Overview Experiments (EEMPA & MEA) CFD Simulations
• 1:1 full size column CFD modeling• Small size column CFD modeling
Experiment/CFD Comparison Plan for Sequential Design of Experiment (SDoE) Conclusion
4
Bench-scaled Packed Column Overview
Column Design
Gas
Solv
ent
Experiment Column
Solv
ent
Gas
1:1 Full Scale CFD Model
RepresentativeColumn Model
5.0 cm
1.0 cm
Packing Region
Sensitivity study and
SDoE(Sequential Design
of “Experiment”)
Bench-scale Column Design: Glass Jacket Column Diameter 3’’, Height 21’’Packing Type: Raschig rings
Diameter: 6 mm Height: 6 mm
8000-9000 rings Material: 316SS, Nylon 6 Porosity: 68% Specific area: 835 m2/m3
Solvents: MEA EEMPA
MEA EEMPAViscosity 𝜇𝜇
[cP] 1.4 7.1
Surface Tension 𝜎𝜎[N/m] 0.067 0.034
Outline
Bench-scaled Packed Column Overview Experiments (EEMPA & MEA) CFD Simulations
• 1:1 full size column CFD modeling• Representative column CFD modeling
Experiment/CFD Comparison Conclusion
6
Experiments of Bench-scale Packed Column
Packing Material 316 Stainless Steel Nylon 6
H = 6mmOD= 6mm
Wall=0.82 mm
Solvent/packing pairs: MEA and 316SS EEMPA and 316SS MEA and Nylon 6 EEMPA and Nylon 6
Measured Carbon Capture Efficiency (CE) CE increase with 𝑢𝑢𝐿𝐿/𝑢𝑢𝐺𝐺 Effective area back out from CE
0.005 0.01 0.015 0.020.15
0.2
0.25
0.3
0.35
0.4
0.45
Capt
u re
Effic
ienc
y[%
]
EEMPA+SS316EEMPA+Nylon 6MEA+SS316MEA+Nylon 6
Outline
Bench-scaled Packed Column Overview Experiments (EEMPA & MEA) CFD Simulations
• 1:1 full size column CFD modeling• Representative column CFD modeling
Experiment/CFD Comparison Conclusion
8
1:1 Full Size CFD Model
9
Gas
Liq
uid
Gas Outlet
SolventInlet
Green: Gas InletRed: Solvent Outlet
Top Boundary
Bottom Boundary
Arrangement of Raschig Rings
Sectional plane view
Packed Column
Dimension:ID: 3’’
Height=21’’
Full Size CFD Model Setup Numerical Packing ProcessComposite
Particle Model
Experiment Packing
CFD Simulated Packing
Improved ring contact modeling
Stainless Steel Glass Ring
H = 6mm, OD= 6mm, Wall=0.82 mm 200 Small Ball (D=0.82 mm)
1:1 Full-size CFD ModelSimulation Conditions: Total 9434 Rings Total ring surface area: 1.99 m2 Liquid flow rate: 0.1-0.8 SLPM Gas flow rate: 25 SLPM Solvent viscosity: [1.4, 7.1] cP
10
x
Entrance Effect(with single
point injection)
Findings: Significant entrance effect for single
point injection, distributor required. 20% to 30% of column height before
reach fully distribution Stronger entrance effect for more
viscous solvent
0.00
0.05
0.10
0.15
0.20
0.25
0.30
0.00 0.10 0.20 0.30 0.40
Nor
mal
ized
Int
erfa
ce A
rea
a e/a
p
Distance from solvent inlet (m)
SLPM=0.115SLPM=0.215SLPM=0.415SLPM=0.760
Liquid fully distribution distance: ~0.15 m
Solvent: EEMPAViscosity: 𝜇𝜇 = 7.1 cP
Inlet
0.00
0.05
0.10
0.15
0.20
0.25
0.30
0.35
0.00 0.10 0.20 0.30 0.40Nor
mal
ized
Inte
rfac
e A
rea
a e/a
p
Distance from solvent inlet (m)
SLPM=0.1920SLPM=0.2793SLPM=0.3920SLPM=0.4595
Liquid fully distribution distance: ~0.10 m
Solvent: MEAViscosity: 𝜇𝜇 = 1.4 cP
Inlet
11
12
1:1 Full-size CFD ModelDistributor design in experiment
13
CFD Comparison w and w/o Distributor
3D Printed Distributor
12 drip holes for solvent injection
Distributor will be used for all experiments
0.00
0.05
0.10
0.15
0.20
0.25
0.30
0.00 0.05 0.10 0.15 0.20 0.25
Nor
mal
ized
Inte
rfac
e Ar
eaa e
/ap
Distance from solvent inlet (m)
Flow Rate: 0.76 SLPM
No Distributor
With Distributor
10 cm shorter in entrance length
Inlet
Outline
Bench-scaled Packed Column Overview Experiments (EEMPA & MEA) CFD Simulations
• 1:1 full size column CFD modeling• Representative column modeling
Experiment/CFD Comparison Conclusion
14
Representative Column Model
Representative Column Setup Column Size: H = 6 cm, OD= 7.62 cm Packing Height Z =[0 5] cm Raschig Ring Size 6 mm Specific Area ap = 857 m2/m3
15
Top Boundary Bottom Boundary
Gas Inlet/OutletLiquid Inlet/OutletRing Surface
2.9 million mesh with mesh size Run to 8s (3 hours Simulation)
for converged solution Good size for sensitivity study
Mesh Scene5.0 cm
1.0 cm
Packing Region
0 2 4 6 8 100
0.05
0.1
0.15
0.2
0.25
0.3
Nor
mal
ized
Inte
rfac
e ar
ea a
i/ap
27.7 mN/m, = 10o
27.7 mN/m, = 40o
27.7 mN/m, = 60o
27.7 mN/m, = 90o
Sensitivity Study For Solvent Parameters Fixed Parameter:𝜌𝜌𝐿𝐿 = 1077 kg/m3,𝑢𝑢𝐿𝐿 = 1.46 × 10−3m/s Varying one parameter at a time (~30 runs);
16
Contact angle 𝜃𝜃 [10o 90o] Surface tension 𝜎𝜎 [25 70] N/m Solvent viscosity 𝜇𝜇𝐿𝐿 [2 10] cP
Range covers MEA and EEMPA:
20 40 60 80 1000
0.05
0.1
0.15
0.2
0.25
0.3
Nor
mal
ized
Inte
rfac
e ar
ea a
i/ap
= 27.7 mN/m, L
=2.46 cP
= 27.7 mN/m, L
=5 cP
= 27.7 mN/m, L
=10 cP
0 20 40 60 800
0.05
0.1
0.15
0.2
0.25
0.3
Nor
mal
ized
Inte
rfac
e ar
ea a
i/ap
= 2.46 cP, = 10o
= 2.46 cP, = 40o
= 2.46 cP, = 60o
= 2.46 cP, = 90o
Representative Column Model
0 2 4 6 8 100
0.05
0.1
0.15
0.2
0.25
0.3
Nor
mal
ized
Inte
rfac
e ar
ea a
i/ap
27.7 mN/m, = 10o
27.7 mN/m, = 40o
27.7 mN/m, = 60o
27.7 mN/m, = 90o
Sensitivity Study For Solvent Parameters Fixed Parameter:𝜌𝜌𝐿𝐿 = 1077 kg/m3,𝑢𝑢𝐿𝐿 = 1.46 × 10−3m/s Varying one parameter at a time (~30 runs);
17
Contact angle 𝜃𝜃 [10o 90o] Surface tension 𝜎𝜎 [25 70] N/m Solvent viscosity 𝜇𝜇𝐿𝐿 [2 10] cP
Range covers MEA and EEMPA:
20 40 60 80 1000
0.05
0.1
0.15
0.2
0.25
0.3
Nor
mal
ized
Inte
rfac
e ar
ea a
i/ap
= 27.7 mN/m, L
=2.46 cP
= 27.7 mN/m, L
=5 cP
= 27.7 mN/m, L
=10 cP
0 20 40 60 800
0.05
0.1
0.15
0.2
0.25
0.3
Nor
mal
ized
Inte
rfac
e ar
ea a
i/ap
= 2.46 cP, = 10o
= 2.46 cP, = 40o
= 2.46 cP, = 60o
= 2.46 cP, = 90o
Contact angel 𝜽𝜽 has the most significant impact on interface area prediction
Contact angle >> Surface Tension > Viscosity
Representative Column Model
18
SDoE for CFD Initial 50 runs to explore 5-dim
parameter (𝑢𝑢𝐿𝐿,𝑢𝑢𝐺𝐺 , 𝜇𝜇𝐿𝐿,𝜎𝜎,𝜃𝜃) space Selected to cover bench experiment
conditionsCFD Parameters RangeViscosity 𝜇𝜇𝐿𝐿 [cP] [5 15]Surface Tension 𝜎𝜎 [N/m] [0.01 0.04]Contact Angle 𝜃𝜃 [°] [5 80]Solvent Flow Rate 𝑢𝑢𝐿𝐿 [L/min] [0.1 0.9]Gas Flow Rate 𝑢𝑢𝐺𝐺 [SLPM] [10 100]
Effect Summary Sensitivity Score
Sensitivity Rank
Contact Angle 27.341 1
Solvent Flow Rate 13.375 2
Surface Tension 9.434 3Solvent Flow Rate*Solvent Flow Rate 6.484
Others …
Statistical Analysis of 50 CFD Runs
Representative Column Model
Outline
Bench-scaled Packed Column Overview Experiments (EEMPA & MEA) CFD Simulations
• 1:1 full size column CFD modeling• Small size column CFD modeling
Experiment/CFD Comparison Conclusion
19
Experiment / CFD Comparison
Physical Properties of Solvent Solvent type: MEA, EEMPA Three key parameters:
Viscosity 𝜇𝜇𝐿𝐿 Surface tension 𝜎𝜎 Contact angle 𝜃𝜃 (much larger uncertainty)
Three data sources: Measured at PNNL Aspen predicted Existing correlation
Identify the range of these parameters in packed column Quantify the uncertainty in CFD interface area prediction
20
Experiment/CFD Results Comparison
21
0 0.1 0.2
Aspen Predicted
0
0.1
0.2
0.3
CFD
Pre
dict
ed
EEMPA+SS316
0 0.1 0.2
Aspen Predicted
0
0.1
0.2
0.3C
FD P
redi
cted
EEMPA+Nylon 6
0 0.1 0.2
Aspen Predicted
0
0.1
0.2
0.3
CFD
Pre
dict
ed
MEA+SS316
0 0.1 0.2
Aspen Predicted
0
0.1
0.2
0.3
CFD
Pre
dict
ed
MEA+Nylon 6Normalized Interface Area 𝒂𝒂𝒊𝒊/𝒂𝒂𝒑𝒑 Comparison
Experiment Pair Contact Angle [o] (Best Guess)
Surface Tension[N/m] (From
Aspen & Paper)
Liquid Viscosity[cP] (From
Aspen & Paper)EEMPA+SS316 [30, 46] [0.026, 0.038] [6.2, 7.6]
EEMPA+Nylon6 [15, 23] [0.026, 0.038] [6.2, 7.6]
MEA+SS316 [19.8, 52.6] [0.054, 0.07] [1.38, 2.54]
MEA+Nylon6 [19.8, 52.6] [0.054, 0.07] [1.38, 2.54]
Contact angle in column:(difficult to precisely determine) Roughness Geometry Loading Temperature, etc.
Experiment/CFD Results Comparison
22
0 0.1 0.2
Aspen Predicted
0
0.1
0.2
0.3
CFD
Pre
dict
ed
EEMPA+SS316
0 0.1 0.2
Aspen Predicted
0
0.1
0.2
0.3C
FD P
redi
cted
EEMPA+Nylon 6
0 0.1 0.2
Aspen Predicted
0
0.1
0.2
0.3
CFD
Pre
dict
ed
MEA+SS316
0 0.1 0.2
Aspen Predicted
0
0.1
0.2
0.3
CFD
Pre
dict
ed
MEA+Nylon 6Normalized Interface Area 𝒂𝒂𝒊𝒊/𝒂𝒂𝒑𝒑 Comparison
Experiment Pair Contact Angle [o] (Best Guess)
Surface Tension[N/m] (From
Aspen & Paper)
Liquid Viscosity[cP] (From
Aspen & Paper)EEMPA+SS316 [30, 46] [0.026, 0.038] [6.2, 7.6]
EEMPA+Nylon6 [15, 23] [0.026, 0.038] [6.2, 7.6]
MEA+SS316 [19.8, 52.6] [0.054, 0.07] [1.38, 2.54]
MEA+Nylon6 [19.8, 52.6] [0.054, 0.07] [1.38, 2.54]
Contact angle in column:(difficult to precisely determine) Roughness Geometry Loading Temperature, etc.
Contact angel 𝜽𝜽 contribute the most uncertainty to the interface area prediction
Contact angle >> Surface Tension > Viscosity
Next Step: Plan for SDoE
23
CFD Parameters Space Filling
Experiment Parameters Space Filling
SDoEDesign
Aspen PlusBench Cart Experiment
CFD Simulation
SDoEOptimization
Interface Area(ai)
Capture Efficiency (CE)
Compare
MeasuredInput
Improve CFD Modeling
CFD Parameters RangeViscosity 𝜇𝜇𝐿𝐿 [cP] [5 15]Surface Tension 𝜎𝜎 [N/m] [0.01 0.04]
Contact Angle 𝜃𝜃 [°] [5 80]Solvent Flow Rate [L/min]
Same as Exp
Gas Flow Rate [SLPM] Same as Exp
Experiment Parameters
Range
Solvent Flow Rate [L/min]
[0.1 0.9]
Gas Flow Rate [SLPM]
[10 100]
Loading/Reboiler Temperature
<135°C
Absorber Temperature [°C]
[30 60]
Measured Results
Nominal Input
Effective Area (ae)
Regression
Aspen calculated viscosity/surface tensionwill put constraints while
exploring CFD parameter space
Conclusion
24
Validation Against Bench-cart Column Experiment Solvents: MEA, EEMPA Packing: SS316, Nylon 6 Leverage Aspen prediction of properties
CFD Approach Optimized Direct calculation of interface area Full-size column for entrance effect:
Viscous solvent has stronger effect Liquid distributor will reduce 2/3 of the effect
Computationally efficient representative column modelSensitivity Study
Contact angle 𝜃𝜃 has the largest impact to the CFD interface area prediction. We need better understanding of its role and influential factors.
Acknowledgements
25
PNNL: Dushyant Barpaga, Charlie Freeman, David Heldebrant, Jie Bao, Rajesh
Singh, Chao Wang, Yucheng Fu
LANL: Christine Anderson-Cook, Sham Bhat, John Baca, Christopher Russell
NETL: Michael Matuszewski, Benjamin Omell, Joshua Morgan, Grigorios Panagakos
UT Austin: Gary Rochelle
Disclaimer: This work is made available as an account of work sponsored by an agency of the United States Government. Neither the UnitedStates Government nor any agency thereof, nor any of their employees, makes any warranty, express or implied, or assumes any legal liability orresponsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its usewould 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 StatesGovernment or any agency thereof. The views and opinions of authors expressed herein do not necessarily state or reflect those of the UnitedStates Government or any agency thereof.
For more informationhttps://www.acceleratecarboncapture.org/
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