An Improved Reaction Mechanism for Combustion of Core (C0...
Transcript of An Improved Reaction Mechanism for Combustion of Core (C0...
An Improved Reaction
Mechanism for Combustion of
Core (C0-C4) Fuels
Chitralkumar V. Naik*,
Karthik V. Puduppakkam, Ellen Meeks
July 13, 2011
The 7th International Conference on Chemical Kinetics
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Outline
● Why core hydrocarbons?
● Issues with existing reaction mechanisms
● Modeling approach
● Extensive model validation
● Concluding remarks
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Core hydrocarbons include all gaseous fuels
● Natural gas
– 425,000 wells in the US
– 105 trillion cubic feet worldwide
● Syngas, coal gas
– From gasification of coal, biomass
– In-situ coal gasification
● Biofuels
– Ethanol, butanol
● H2, C1-C4 hydrocarbons
– Selected oxygenates A coal-gas powered taxicab in England, 1920.
Natural gas well, 1907.
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Core hydrocarbons chemistry is core to
heavier liquid fuels
Hydrogen C1
C2
C3
C4
Liquid hydrocarbon combustion and emissions
Oxygenated species
NOx chemistry
Unsaturated species
PAH precursors
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Outline
● What are core hydrocarbons?
● Issues with existing reaction mechanisms
● Modeling approach
● Extensive model validation
● Concluding remarks
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Typical issues with many existing reaction
mechanisms
1. Applicability
– Not comprehensive enough
2. Accuracy
– Not accurate enough for broad range of conditions
3. Extensive validation
– Limited validation range and types of experiments
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Core chemistry in large mechanisms may
not be accurate or validated
Data from Jomaas et al.
2005 10
20
30
40
50
0.6 0.9 1.2 1.5
Fla
me
sp
ee
d (c
m/s
)
Equivalence ratio
Ethane/air, 298 K
1 atm
2 atm
5 atm
● Predictions for unsaturated components are worse
● LLNL n-heptane
mechanism
overpredicts
ethane flame
speeds
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Often mechanisms are validated for one or
two types of experiments
Flow reactor
Shock tube
Stirred reactor
Opposed-flow reactor
Laminar flames
RCM
● Together they cover the conditions in practical
applications (engines, turbines)
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Legacy fuel models are not suitable for
applications at high-P and low-T
Natural Gas Components Composition
Methane 70-90 %
Ethane, Propane, Butane 0-20 %
CO2 0-8 %
N2, H2S 0-5 %
Core hydrocarbons (C0-C4)
– GRI-mech limited to methane
Complex Negative Temperature Coefficient (NTC)
behavior <1000 K
– Autoignition of fuels critical for engines and turbines
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Existing core mechanisms may not be
comprehensive
● Dependencies between various small species
– e. g. ethylene chemistry also involves C4 species
– e.g.
● Missing components and inconsistencies
may affect predictive nature
– Be careful in merging various mechanisms
CH4 CH3 CH3O O2
H
CH3 CH3OCH3
CH3OH
Need comprehensive, accurate, and validated
core reaction mechanism
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Outline
● What are core hydrocarbons?
● Issues with existing reaction mechanisms
● Modeling approach
● Extensive model validation
● Concluding remarks
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Comprehensive
mechanism
The mechanism is generated in a systematic
way
Validation
Reactions
Rate Parameters
Thermo
Transport
Initial sub-mechanisms
from publications
- Add missing or necessary
reactions
- Enforce self-consistency
- Update k and thermo
- Optimize k within the
uncertainty
Accurate
mechanism
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RD2010 core mechanism is comprehensive
● Starting component sub-mechanisms from
various sources
– Merged to a consistent base
● Included low- and high-temperature pathways
● Updated rate constants based on recent
studies
– Pressure-dependent rate constants for important
reaction systems
● 18 fuel components
– 1161 species and 5622 elementary reactions
– Saturated, un-saturated, oxygenates
– NOx, soot precursors up to benzene
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The core mechanism is optimized for
accuracy
● Optimized rate constants for less than 5%
of the reactions
– Within the expected uncertainty
Reaction A n Ea Ref.
H+O2 = O+OH 3.55E+15 -0.406 1.66E+04 [12]
CO+OH = CO2+H 2.20E+05 1.89 -1.16E+03 [12], A*1.24
HCO+M = H+CO+M 4.75E+11 0.7 1.49E+04 [11]a
H+OH+M = H2O+M 4.50E+22 -2 0.00E+00 [19]a
C3H5-a+H(+M) = C3H6(+M) 2.00E+14 0 0.00E+00 [13]
Low pressure limit: 1.33E+60 -12 5.97E+03
Troe parameters: 0.02, 1.10E+03, 1.10E+03, 6.86E+03
CH3+CH3(+M) = C2H6(+M) 9.21E+16 -1.17 6.36E+02 [12]a
Low pressure limit: 1.14E+36 -5.246 1.71E+03
Troe parameters: 0.405, 1.12E+03, 69.6, 1.00E+10
CH3+HO2 = CH3O+OH 1.00E+12 0.269 -6.88E+02 [12]
CH4+H = CH3+H2 6.14E+05 2.5 9.59E+03 [12]
HO2+HO2 = H2O2+O2 4.20E+14 0 1.20E+04 [18]b
1.30E+11 0 -1.63E+03
CH4+HO2 = CH3+H2O2 1.13E+01 3.74 2.10E+04 [12]
Collision efficiencies: CH4 2.0, CO 1.9, CO2 3.8, C2H6 3.0, H2O 6.0, H2 2.0, Ar 0.7
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Example of the CO+OH = CO2+H rate
constants
● 118 records in the NIST
database
– 91 experimental data
– 20 theoretical calculations
– 7 review recommendations
– 1981-2007 data fit
k = 2e11 * exp(-300/RT)
● Recent data
– Agree within 25%
● Typical uncertainty ~
factor of 2
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Outline
● What are core hydrocarbons?
● Issues with existing reaction mechanisms
● Modeling approach
● Extensive model validation
● Concluding remarks
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Fundamental data are the best for reaction
mechanism validation
● Reduced impact of transport ➔
More focus on chemistry
Neat fuels
Laminar
flame speed
Shock
tube
Flow
reactor
Stirred
reactors
Burner
flames
Hydrogen √* √
Formaldehyde √
Methane √ √ √
Methanol √
Ethane √ √
DME √ √ √
Ethanol √
Propane √
n-Butane √ √
iso-Butane √
n-Butanol √ √ √
NOx √ √ 11
sa
tura
ted
fu
el
co
mp
on
en
ts
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Broad range of conditions covered
Experiment type T (K) P (atm)
Dilution of
oxidizer %*
Laminar flame
speeds 295 to 453 1 to 5 0.6 to 1.6 0 to 15
Shock-tubes 650 to 1800 1 to 340 Pyrolysis,
0.3 to 3 0 to >98
Flow reactors 500 to 948 1.5 to 12.5 0.005 to 1.19 97.6 to 98.8
Stirred reactors 700 to 1100 1-10 0.1 to 1 97.1 to 97.9
Burner-stabilized
flames 300 1 to 14.6 0.6 to 0.8
N2/O2 : 2.2/1 for
oxidizer
● Dilution with N2, Ar, or H2O with air or O2 as oxidizer.
● Saturated fuels
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Broad range of conditions covered for un-
saturated components and blends
● Un-saturated fuels
Experiment type T (K) P (atm)
Dilution of
oxidizer %
Laminar flame
speeds 298 1-5 0.6-2 0-16.5
Shock-tubes 1050-2250 0.85-9 0.5-2 0-97
Flow reactors 700-1350 1 0.05-1.4 97.9-99.7
Stirred reactors 700-1100 1-10 0.1-1.5 96-99.5
Experiment type T (K) P (atm)
Dilution of
oxidizer %
Laminar flame
speeds 298 1-2 0.5-4.5 0-16.5
Shock-tubes 1020-1750 1-256 0.5-3 92-99.9
Stirred reactors 950-1450 1-10 0.3-2 66.1-98.5
● Fuel blends
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Over 90+ comparison plots for validation
● A comparison plot contains one or more
data sets
● Overview of comparisons
– Grouped by experiment types
● Lines – predictions
● Symbols – published experimental data
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Laminar flame speeds: Fuel, T, P, and effects captured
5
25
45
65
85
0.4 0.6 0.8 1 1.2 1.4 1.6 1.8
Equivalence ratio
La
min
ar
fla
me
sp
ee
d (
cm
/s) Gulder et al., 300K
Egolfopoulos et al., 298K
Egolfopoulos et al., 363K
Egolfopoulos et al., 453K
Liao et al., 358K
Model, 298K
Model, 360K
Model, 453K
Ethanol
10
20
30
40
50
0.6 0.8 1 1.2 1.4 1.6Equivalence ratio
La
min
ar
fla
me
sp
ee
d (
cm
/s)
Jomaas et al., 1 atm
Vagelopoulos et al., 1 atm
Jomaas et al., 2 atm
Jomaas et al., 5 atm
Model, 1 atm
Model, 2 atm
Model, 5 atm
Propane
P
Ethylene
Fuel/air
P
Tin
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Laminar flame speeds:
Diluents and composition effects captured
● H2 with N2 or Ar
0
50
100
150
200
250
300
350
400
0 1 2 3 4 5Equivalence ratio
La
min
ar
fla
me
sp
ee
d (
cm
/s)
Aung et al.
Dowdy et al.
Tse et al.
Kwon et al.
Vagelopoulos et al.
Verhelst et al.
Model
Kwon et al., 79/21 Ar/O2
Model, 79/21 Ar/O2
● Syngas with 50/50
to 95/5 CO/H2
H2
Ar
N2
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Autoignition delay times: Effects of fuel, T, P, and captured
1.E-06
1.E-05
1.E-04
1.E-03
1.E-02
0.5 0.7 0.9 1.11000/T (1/K)
Ign
itio
n d
ela
y t
ime
(s
) Herzler et al., 1 atm
Herzler et al., 4 atm
Herzler et al., 16 atm
Model, 1 atm
Model, 4 atm
Model, 16 atm
H2
Propyne
90/10
Methane/propane
P
P
Fuel-rich
O2/Ar
O2/Ar
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Autoignition delay times:
Effects of loading and diluents captured
1.E-06
1.E-05
1.E-04
1.E-03
1.E-02
0.5 0.6 0.7 0.8 0.9
1000/T (1/K)
Ign
itio
n t
ime
(s
)
Model, 0.6% fuel
Model, 3.5% fuel
Black et al., 3.5% fuel
Black et al., 0.6% fuel
n-Butanol
Ethylene
loading
O2/Ar
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Species profiles: Shock-tube
Accurate predictions at very high pressures
● Pyrolysis at 340 bar
0.0E+00
5.0E-05
1.0E-04
1.5E-04
2.0E-04
2.5E-04
3.0E-04
1000 1100 1200 1300 1400 1500Inlet temperature (K)
Mo
le f
racti
on
Sivaramakrishnan et al., ethane
Sivaramakrishnan et al., ethylene
Sivaramakrishnan et al., acetylene
Model, ethane
Model, ethylene
Model, acetylene
250 ppm ethane in Ar
Uncertainty in
: 1.25 - 1.6 ms
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Species profiles: Flow-reactor Effect of on propyne oxidation captured
● Products acetylene
and allene predicted
well
– Important PAH
precursors
0.0E+00
5.0E-04
1.0E-03
1.5E-03
2.0E-03
2.5E-03
3.0E-03
0.00 0.05 0.10
Time (sec)
Pro
py
ne
mo
le f
rac
tio
n Davis et al., phi of 0.7
Davis et al., phi of 1
Davis et al., phi of 1.4
Model, phi of 0.7
Model, phi of 1
Model, phi of 1.4
0.0E+00
5.0E-04
1.0E-03
1.5E-03
2.0E-03
2.5E-03
3.0E-03
0.00 0.05 0.10
Time (sec)
Mo
le f
rac
tio
n
Davis et al., propyne
Davis et al., allene
Davis et al., acetylene
Model, acetylene
Model, allene
Model, propyne
● 1170 K, 1 atm,
0.03% fuel Fuel-rich
= 1
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Species profiles: Stirred-reactor
Products evolution in methanol captured
● Methanol oxidation at 10 atm in a stirred-reactor
0.0E+00
2.0E-03
4.0E-03
6.0E-03
8.0E-03
1.0E-02
700 800 900 1000 1100Inlet temperature (K)
Mo
le f
rac
tio
n
Dyma et al., CH3OH
Model, CO
Dyma et al., CO
Model, CO
Dyma et al., CO2
Model, CO2
Dyma et al., CH2O
Model, CH2O
0.6, 1 s 8000 ppm fuel, 800 ppm H2O
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NOx emissions from premixed flames: Pressure and effects captured
● High-pressure premixed flames
– Radiation heat losses included in CHEMKIN-PRO
Methane with
N2/O2 in 2.2/1 ratio
Tflame: 1750-1900 K
Fuel-rich
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Outline
● What are core hydrocarbons?
● The problem and our modeling approach
● Extensive model validation
● Concluding remarks
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Accurate predictions need comprehensive
core mechanism
● Sensitivity analysis for autoignition delay time
-0.15 -0.1 -0.05 0 0.05 0.1
CH3+O2 = CH2O+OH
CH3O2+CH3 = 2CH3O
CH3+HO2 = CH3O+OH
CH4+HO2 = CH3+H2O2
CH3+HO2 = CH4+O2
HCO+HO2 = CH2O+O2
H+O2(+M) = HO2(+M)
CH4+H = CH3+H2
2HO2 = H2O2+O2
2CH3(+M) = C2H6(+M)
Temperature sensitivity coefficient
Methane/air, 3
140 atm, 1400 K
Methane Ethane Formaldehyde
Ethanol Ethylene Acetaldehyde
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Comprehensiveness of the core mechanism
even more important for blends
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Chemistry of unsaturated fuels is more
involved than their saturated counterparts
● Allene oxidation in a stirred-reactor
– 1000 K, 10 atm, 1.5 s, and phi of 1.5
● Reactions of C1 and C2 most sensitive
● Reactions of C4 and C5 also important
– C5H6+H <= C2H2+C3H5-a
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Summary
● Successful development of a detailed core
(H2, C1-C4) reaction mechanism
– Comprehensive: 18 neat fuels and their 8+ blends
Includes oxygenated fuels
NOx, and PAH precursors
● Successful validation using broad range of
conditions and experiments
– Over 90+ comparison plots using 30 years of the data
from the publications
* Results on saturated components to appear in
J. Eng. Gas Turbines Power
ICCK 2011 34
Thank You