egr effect on auto ignition sandia labs
TRANSCRIPT
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The Effects of EGR and Its Constituents on theAutoignition of Single- and Two-Stage Fuels
John Dec, Magnus Sjberg, and Wontae HwangSandia National Laboratories
13th Diesel Engine-Efficiency and Emissions Research Conference August 13 16, 2007, Detroit, MI
Sponsors:U.S. DOE, Office of FreedomCAR & Vehicle Technologies
Program Manager: Gurpreet Singh
Saudi Aramco Oil CompanyProgram Manager: Ahmar Ghauri
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Introduction
z Advanced LTC diesel and HCCI engines can provide both highefficiencies and very low emissions of NO X and PM.
z Nearly all LTC and HCCI strategies use high levels of EGR/residuals.
1. Reduce peak combustion temperatures to control NO X.2. Delay the onset of ignition.
Controlling combustion phasing.For HCCI-like diesel, it allows more time for premixing before ignition.
3. For gasoline HCCI, hot residuals are used to promote autoignition, andcombined with cooled EGR, to control combustion phasing and NO X.
z Although EGR is widely used, its thermodynamic and chemical effectson autoignition are only understood in general terms.
z Objective: Provide a fundamental understanding of how EGR andits constituents affect the autoignition of single- andtwo-stage ignition fuels.
Conduct well-controlled experiments in an HCCI engine.
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HCCI Engine and Subsystems
Only premixedfueling is usedfor this study.
Cummins B
0.98 liter / cyl.CR = 14 piston
EGR Systemsz Real EGRz Simulated EGR &EGR constituents
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Baseline Points40
330 335 340 345 350 355 360 365 370Crank Angle [CA]
iso-OctaneGasolinePRF80PRF60, 29% CSP
CA50 =368CA
PRF60, 29% CSPPRF80Gasolineiso-Octane
Baseline Points
E G R
C/F = 37.8 ( = 0.40)CA50 = 368CA
Single-stageIgnitionTwo-stage
Ignition (LTHR)
No EGR 29% CSP
Gasoline
TDC
z Establish baseline operating pointsfor all four fuels. CA50 = 368CA (8 aTDC)
35
30
25
20
15z Study the retarding effects of EGR 10
and its constituents. 12001100
z Iso-octane and gasoline exhibitsingle-stage autoig. at these conds.
1000
900
800z PRF80 and PRF60 have two-stage 700
autoignition with LTHR. Similar to diesel fuel (CN = 21 & 30).
180z Baseline conditions have no EGR
except for PRF60 29% CSP.
Operating ConditionsP in = 100 kPa (naturally asp.)
1200 rpm.
C/F-mass ratio = 37.8,( = 0.40 without EGR.)
160
140
120
100
80
60
40
P r e s s u r e
[ b a r ]
M a s s - A v e r a g e d
T e m p . [ K
]
R e q u
i r e
d I n t a k e T e m p . [
C ]
50 60 70 80 90 100PRF Number, Anti-knock Index
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Composition of EGR (CSP)
z Consider complete combustion of iso-octane in "air".(Argon and atmospheric CO 2 lumped with N 2.)
z C 8H18 + 12.5 (O 2 + 3.773 N 2) 8 CO 2 + 9 H 2O + 47.16 N 2.
z For complete combustion with = 1, the gas composition (excl. fuel)changes from air: 21% O 2 & 79% N 2 (mole basis).
z to: 12.5% CO 2, 14.0% H 2O and 73.5% N 2 for wet exhaust (CSP).
z to: 14.5% CO 2 and 85.5% N 2 for dry exhaust (Dry CSP).
z These gas compositions will be referred to as:Complete Stoichiometric Products CSP & Dry CSP .
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Thermodynamic Effects of EGR (CSP)
z EGR influences the compressed-gas temperature. Heat-capacities of CSP & individual components are different from that of air.
z Start with motored operation. Examine effects of CSP & its
components on the mass-averaged temperature near TDC.z Displace air while
maintaining P in = 100 kPa.900
890
z Trends can be explained by 880changes in specific heat (C v).
T e m
p e r a t u r e
@ 3
5 0 C A [ K ]
870
CO 2 has highest C v (mole bs.). 860 H2O high C v. 850
N2 Cv slightly less than air. 840 CSP between air and H 2O. 830
Dry CSP slightly lower C v820
than CSP.1112131415161718192021
Intake O2 Mole Fraction [%]
N2Dry CSPCSPH20CO2
Motored Data
Increasing Diluent
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900
Autoignition Retard for iso-Octane
z Investigate the effect of these gases on combustion phasing.
z The autoignition retard is highly dependent on the type of the diluent.
z The retarding effect of the various gases is ordered consistently withtheir "cooling capacity" - thermodynamic effect .
z However, N 2 addition increases the compression temperature, but thephasing is retarded, so there must be a weak chemical [O2] effect.
1112131415161718192021Intake O2 Mole Fraction [%]
N2Dry CSPCSPH20CO2
Motored Data
1 0 % B u r n e d
[ C A ]
373
372
371
370
369
368
367
1919.219.419.619.82020.220.420.620.821Intake O2 Mole Fraction [%]
CO2H2OCSPDry CSPN2
Tin = 175C
T e m p e r a t u r e
@
3 5 0 C A [ K ]
890
880
870
860
366
365820
830
840
850
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373
Temperature Traces for iso-Octane
1050
Air, BaselineN2CO2 CA10
370.5CA
CA10365.7CA
CO 2
N2
Air
z Retarding effect of lower [O 2]becomes more significant athigher levels of N 2 addition. Clearly, reduction of [O 2] has to
lead to misfire at some point.
z Temperature traces illustrate
1040
1030
1020
1010
1000
990980
970
960
1 0 % B u r n e d
[ C A ]
M a s s -
A v e r a g e d
T e m p . [
K ]
different mechanisms for retard. 950350 355 360 365 370 375
Crank Angle [CA]
16.51717.51818.51919.52020.521Intake O 2 Mole Fraction [%]
CO2H2OCSPDry CSPN2
iso-OctaneTin = 175C
373
372
371
370
369
368
372
1919.219.419.619.82020.220.420.620.821Intake O2 Mole Fraction [%]
CO2H2OCSPDry CSPN2
Tin = 175C
1 0 % B u r n e d
[ C A ]
371
370
369
367
366
365365
366
367
368
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900
Autoignition Retard for PRF80 (2-Stage Ignition)
z For PRF80, the retarding effects are not consistent with the "coolingcapacity" of the added gases (except for CO 2).
z N2 addition (reduced [O 2]) strongly retards combustion phasing.
1 0 % B u r n
e d [ C A ]
T e m p . R
i s e
3 3 5 -
3 5 2 C A
[ K ]
147
146
145
144
143
142
z
PRF80's high sensitivity to [O 2]occurs for two reasons: First, a reduced [O 2] reduces the
LTHR.
CO2H2ON2Dry CSPCSP
Tin = 72C
PRF80, N2
2nd Order Curve Fit
890
1112131415161718192021Intake O2 Mole Fraction [%]
N2Dry CSPCSPH20CO2
Motored Data
373
374
T e m p e r a t u r e @
3 5 0 C A [ K ]
880 372
371870
860 370
369
368
367
366
21 20.8 20.6 20.4 20.2 20 19.8 19.6 19.4 19.2 19
820
Intake O2 Mole Fraction [%]
830
840
850
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900
Autoignition Retard for PRF80 - [O 2]
z Second, a reduced [O 2] also affects hot ignition.1060104010201000
980960940920900880
T e m p e r a t u r e @
3 5 0 C A [ K ]
M a s s -
A v e r a g e d
T e m p . [
K ]
N2CO 2
[O2] = 20.7%
[O2] = 19.3%
Post-LTHRtemperatureis the same.
1 0 % B u r n
e d [ C A ]
T e m p . R
i s e
3 3 5 -
3 5 2 C A
[ K ]
147
146
145
144
143
142
CO2H2ON2Dry CSPCSP
Tin = 72C
PRF80, N2
2nd Order Curve Fit
350 355 360 365 370 375Crank Angle [CA]
890
1112131415161718192021Intake O2 Mole Fraction [%]
N2Dry CSPCSPH20CO2
Motored Data
373
374
880 372
371870
860 370
369
368
367
366
21 20.8 20.6 20.4 20.2 20 19.8 19.6 19.4 19.2 19
820
Intake O2 Mole Fraction [%]
830
840
850
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All Constituents for PRF80 - H 2O
z Thermodynamic "cooling" should add to [O 2] effect for all constituents.z Why is the retarding effect of H 2O equal to N 2?
z H2O enhances the intermediate chemistry, so thermal run-away occurs
at lower temperature. Almost perfectly counteracts the cooling effect of H 2O!z Also explains why CSP is less retarded than dry CSP.
z H2O does not enhance the intermediate chemistry for iso-Octane.
374
373
372
371
370
369
368
367
366
1 0 % B u r n e d
[ C A ]
880
900
920
940
960
980
1000
350 355 360 365 370 375Crank Angle [CA]
M a s s -
A v e r a g e d
T e m p . [
K ]
iso-Octane, CO2iso-Octane, H2OPRF80, N2PRF80, H2O
PRF80CA10 371CA
iso-OctaneCA10 370.4CA
1919.219.419.619.82020.220.420.620.821Intake O2 Mole Fraction [%]
CO2H2ON2Dry CSPCSP
Tin = 72C
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Comparing [O 2] Sensitivities
z Have now identified three mechanisms by which EGR affects phasing.1. C v effect (thermodynamic retarding).
2. O 2-concentration effect (chemical retarding).
3. H2O effect (chemical enhancing).
z Compare side by side for all fuels.
z N2 addition gives most reductionin [O 2] for least change in C v.
373
372z The two-stage ignition fuels
PRF80 and PRF60 are371
much more sensitive. 370369
z Lower [O 2] both reducesLTHR and counteracts 368
the hot ignition. 367366
z Gasoline is initially very
insensitive to [O 2].
1 0 %
B u r n e
d [ C A ]
15.51616.51717.51818.51919.52020.521Intake O 2 Mole Fraction [%]
PRF60PRF80iso-OctaneGasolineGas., 3rd order
N2
addition
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Comparing Thermal Sensitivities
1. C v effect (thermodynamic retarding).
2. O 2-concentration effect (chemical retarding).
3. H 2O effect (chemical enhancing).
z CO 2 addition gives mostthermodynamic cooling, with 373least change in [O 2].
20.220.320.420.520.620.720.820.921Intake O 2 Mole Fraction [%]
Gasolineiso-OctanePRF80
PRF60
CO 2 addition372
371
1 0 % B u r n e d
[ C A ]
z The single-stage ignition fuels,iso-octane and gasoline, aremuch more sensitive to thecooling effect of CO 2.
370
369
368
367z The reason for this explained in:Proceedings of the Combustion 366Institute , Vol. 31, pp. 28952902,2007.
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Comparing CSP Effects
1. C v effect (thermodynamic retarding).
2. O 2-concentration effect (chemical retarding).
3. H 2O effect (chemical enhancing).
z The overall effect of CSP results from the combination of these threemechanisms.
374z CSP gives similar amounts of 373
retard for all four fuels. 372z But underlying mechanisms 371
1 0 %
B u r n
P o
i n t [ C A ]
are different. 370369
z Trace species in real EGR 368add to these effects. 367366
19.219.419.619.82020.220.420.620.821Intake O 2 Mole Fraction [%]
iso-OctanePRF60, Shifted 6.1%PRF80Gasoline
CSP addition
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Real EGR Effects
z Real EGR contains trace species 373372that also affect the autoignition. 371 Unburned fuel, partially oxidized 370369
fuel, formaldehyde, CO, and other 368
species. 367366z For iso-Octane and Gasoline, 365
372real EGR retards less than CSP. 371370
z For PRF80, real EGR has a 369retards slightly more than CSP. 368
367
366z The net effect of these species is 365
to advance the ignition for iso- 372371
octane and gasoline... 370369
z ...but to retard it for PRF80. 368367
366
1 0 % B u r n
P o
i n t [ C A ]
CSP
Real EGR
PRF80Tin = 72C
CSP
Real EGR
GasolineT in = 149C
CSP
Real EGR
iso-OctaneT in = 175C
21 20.8 20.6 20.4 20.2 20 19.8 19.6 19.4 19.2 19
Intake O 2 Mole Fraction [%]
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Summary / Conclusionsz EGR is very effective for suppressing autoignition reactivity.
Can be used beneficially for controlling combustion phasing across loadand speed ranges.
Iso-Octane Gasoline PRF80 PRF60
Effect: Single-stage Two-stage with LTHR
Retarding C v effect (thermodynamic) Strong Weak
[O 2 ] effect (chemical) Weak Strong
Enhancing H 2 O effect (chemical) None to weak Strong
Trace Species Moderate enhancing Moderate retarding
z The net result of the different thermal, O 2, and H 2O sensitivities is afairly similar effect of CSP for all fuels.
z Trace species (unburned and partially oxidized fuel, and CO) influence
the effect of real EGR. Details in: SAE 2007-01-0207
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900
Autoignition Retard for PRF80 - [O 2]
z Lower [O 2] also affects hot ignition, in addition to reducing the LTHR.
M a s s - A v e r a g e
d T e m p . [
K ]
N2
CO 2
[O 2] = 20.7%
[O 2] = 19.3%
1040
1000
960
920
880
840
800
1 0 % B u r n e d
[ C A ]
T e m p . R
i s e
3 3 5 -
3 5 2 C A
[ K ]
147
146
145
144
143
142
CO2H2ON2Dry CSPCSP
Tin = 72C
PRF80, N22nd Order Curve Fit
760335 340 345 350 355 360 365 370 375
Crank Angle [CA]
890
1112131415161718192021Intake O2 Mole Fraction [%]
N2Dry CSPCSPH20CO2
Motored Data
373
374
T e m p e r a t u r e
@ 3
5 0 C A [ K ]
880 372
371870
860 370
369
368
367
366
21 20.8 20.6 20.4 20.2 20 19.8 19.6 19.4 19.2 19
820
Intake O2 Mole Fraction [%]
830
840
850
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Autoignition Retard for Gasoline
z N2 addition shows that the chemical [O 2] effect is very weak.
z Retarding effect of H 2O is weaker than expected based on its high C v.
z CSP (with water) has a slightly weaker retarding effect than dry CSP.
z Temperature traces confirm that H 2O has an enhancing effect onautoignition for gasoline.
z Effect is stronger than for iso-octane, but much weaker than for PRF80.
350 355 360 365 370 375Crank Angle [CA]
CO2
H2O
GasolineCA10 370.3CA
3731020
CO2H2O
Dry CSPCSPN2
GasolineT in = 149C
M a s s -
A v e r a g e d
T e m p . [
K ]
372
371
370
1000
1 0 % B u r n e d
[ C A ]
980
369960
368
367
366
365
21 20.8 20.6 20.4 20.2 20 19.8 19.6 19.4 19.2 19Intake O 2 Mole Fraction [%]
900
920
940
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Real EGR Effects (2)z Intake concentrations increase with
EGR level and retard. 373372z These effects of Real EGR are also 371
370important for explaining the effects of 369retained residuals. 368
367z Discussed in Proceedings of the 366Combustion Institute , Vol. 31, pp. 365
CSP
Real EGR
PRF80Tin = 72C
CSP
Real EGR
GasolineT in = 149C
CSP
Real EGR
iso-OctaneT in = 175C
28952902, 2007.
1 0 % B u r n P o
i n t [ C A ] 372
371
370
369368
367
366
PRF80iso-OctaneGasoline
Intake CO
iso-OctanePRF80Gasoline
Intake HC
300
250
200
150
100 I n t a k e C O - [ p p m
]
50 3650 372
1200
1000
I n t a k e H C -
[ p p m
] 371
370
369
368
400 367
200 36621 20.8 20.6 20.4 20.2 20 19.8 19.6 19.4 19.2 19
21 20.8 20.6 20.4 20.2 20 19.8 19.6 19.4 19.2 19 Intake O 2 Mole Fraction [%]Intake O 2 Mole Fraction [%]
0
600
800
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Compare with NIST Database
z All air displacement except N 2 reduce the compression temperature.z Can be explained by changes of the specific heat capacity.z CO 2 has highest specific heat capacity on a mole basis.z H2O has high specific heat capacity.z N2 has slightly lower specific heat capacity compared to air.z CSP falls between Air and H 2O.z Dry CSP has slightly lower C v compared to CSP.
T e m p e r a t u r e
@ 3
5 0 C A [ K ]
15
20
25
30
35
40
45
50
H e a
t C a p a c i t y -
C v
[ J / K * m o
l ]
CO2H2OCSPDry CSP
Air N2
NIST ChemistryWebBook
900
890
880
870
860850
840
Motored Data
N2Dry CSPCSPH20CO2
830
820
300 400 500 600 700 800 900 1000 1100 1200 21 20 19 18 17 16 15 14 13 12 11Temperature [K] Intake O2 Mole Fraction [%]