2 значения m avl.pdf
TRANSCRIPT
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AVL-BOOST COMBUSTION MODELS
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2 BOOST_CombustionModels_2011_Bras
Spatial Discretization
Single Zone (Zero-Dimensional)
Two Zone (Quasi-Dimensional)
Ignition Type (Mixture Preparation)
Spark Ignition
Compression Ignition
ROHR Type
ROHR Input
ROHR predicted by Combustion Model
Source
Standard BOOST
User Coding
ROHR (Rate Of Heat Release) CLASSIFICATION
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3 BOOST_CombustionModels_2011_Bras
SPATIAL DISCRETIZATION / SINGLE ZONE
Governing Equations
Energy Conservation
d
dmh
d
dQ
d
dQ
d
dVp
d
umd BBBB
wFc
c
ccc TRmV
p 1
Perfect Gas Equation
Thermodynamic State Vector
c
c
c
c
c
C
T
pS
FV
CP
FB
Cc
mf
mf
mf
C
n
Gc
mf
mf
mf
C.
1
1
Classic / General Species Transport GCcC /
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4 BOOST_CombustionModels_2011_Bras
SPATIAL DISCRETIZATION / TWO ZONE /1
Energy Conservation for burned and unburned Zone
uuubbbc TRmTRmV
p 1
Perfect Gas Equation
Thermodynamic State Vector
unburned
burnedc
S
SS
d
dmh
d
dmh
d
dQ
d
dQ
d
dVp
d
udm
bBB
bBBb
uWb
Fbc
bb
,
,
d
dmh
d
dmh
d
dQ
d
dVp
d
udm uBBuBB
bu
Wuuc
uu ,
,
bbbbc TRmup ,,,,
uuuuc TRmup ,,,,
uBBuBBbBBbBB dmhdmh ,,,,
dVpc
FdQ
WbdQ
WudQ budmh
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5 BOOST_CombustionModels_2011_Bras
Vibe Single Zone
ROHR Approach
Parameter Data Source
Fitting Result of Combustion Analysis Tool (BOOST-Burn)
Experience
1
1
myam
c
BTB eym
aQ
d
dQ
c
oy
... Combustion Progress
10
1
ma
BTB eQQ
Released Energy
ROHR INPUT FOR SPARK IGNITION ENGINES /1
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6 BOOST_CombustionModels_2011_Bras
ROHR INPUT FOR SPARK IGNITION ENGINES /2
Table Single Zone
Data Source
Result of Combustion Analysis Tool
(BOOST-Burn)
Adaptation
For physical reasons preprocessing
performed to guarantee monotonic
increase of Fuel Burned
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7 BOOST_CombustionModels_2011_Bras
ROHR INPUT FOR SPARK IGNITION ENGINES /3
Hires et al
Required Input
Vibe Combustion Parameters and Ignition
Delay for Reference Operating Point
Vibe Two Zone / Table Two Zone
Same ROHR Approach as for Single Zone
State Vector of Burned Zone allows to calculate:
NOx Production (Extended Zeldovich)
CO Production (Onorati)
State Vector of Unburned Zone allows to calculate:
Required Octane Number
at
t
T
B
nMFB
SOC
UBZ dtepA
ON
1
%851100
Model Approach for Variation of Ignition Delay and Combustion Duration dependent
on Engine Speed
3/23/1
,
s
s
f
f
n
n refref
ref
refcc
3/23/1
s
s
f
f
n
nidid
ref
refref
ref
s ... laminar flame speed
f ... piston to head distance at ignition timing
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8 BOOST_CombustionModels_2011_Bras
PREDICTED ROHR FOR SPARK IGNITION ENGINES /1 FRACTAL COMBUSTION MODEL
Motivation
All mentioned ROHR Types require input based on experimental data which show usually a strong dependency on the operating point (speed, load-
signal) of the engine.
For optimization issues (variable valve timing, engine control strategies, ...) a predictive combustion model which handles the influence of residual gas
content and charge motion is required.
This requirement can be fulfilled in a wide operation point range by the new introduced Fractal Combustion Model
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9 BOOST_CombustionModels_2011_Bras
PREDICTED ROHR FOR SPARK IGNITION ENGINES /2 FRACTAL COMBUSTION MODEL
Characteristics /1
The Fractal Combustion Model is based on a
physical model of the flame front
propagation:
Geometric Combustion Chamber Input Data leads to a Relation between Piston
Position, Geometric Free Flame Surface
and Burned Zone Volume
Increase of Burned Zone Volume is a function of Laminar Burning Speed and
Geometric Free Flame Surface.
A Simple multiplication => to small values
because
The flame front is a very thin and highly wrinkled surface (wrinkled-flamelet
combustion regime)
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10 BOOST_CombustionModels_2011_Bras
PREDICTED ROHR FOR SPARK IGNITION ENGINES /3 FRACTAL COMBUSTION MODEL
Characteristics /2
This wrinkling effect is driven by the in-cylinder turbulent flow and chiefly
responsible for the increased burning rate.
The relation between geometric free and effective (highly wrinkled) flame area can
be described by a fractal structure.
Fractal is a mathematical method describing irregular geometry with self
similarity (length of British coast?).
Mandelbrot Set
Burned Gas
Unburned Gas
SL
SL
SL u
L
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11 BOOST_CombustionModels_2011_Bras
PREDICTED ROHR FOR SPARK IGNITION ENGINES /9 FRACTAL COMBUSTION MODEL
Extension to stratified charge
Input possibility for 1D distribution of
fuel vapor and combustion product
concentration (stratified charge) in
the direction of flame propagation
1D distribution can be imported from
AVL FIRE in-cylinder simulation
(standard output )
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12 BOOST_CombustionModels_2011_Bras
PREDICTED ROHR FOR SPARK IGNITION ENGINES /10 FRACTAL COMBUSTION MODEL
Project Experience
The fractal combustion model has the potential to predict the influence of the
valve timing variation on the rate of heat
release.
Out of 7 parameters for the combustion model only the 2 turbulence parameters
are function of engine speed and valve
timing.
The tuning of the turbulence parameter is based on 3D CFD results.
BSFC [g/kWh]
Res. Gas [%]
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13 BOOST_CombustionModels_2011_Bras
PREDICTED ROHR FOR SPARK IGNITION ENGINES /11 OPEN CHAMBER GAS ENGINE COMBUSTION MODEL
Main features:
2 Zone (unburned/burned) flame propagation model
Arrhenius / Magnussen approach combination for ignition delay simulation
In-cylinder turbulence level (used for the relation between laminar and turbulent
flame speed) is sourced by swirl and
squish flow
Combined with BOOST Classic Gas Properties Preparation Tool which allows
to generate properties for arbitrary fuel
blends (e.g. lean gas as mixture of CH4,
CO2, ), as alternative to general species transport
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14 BOOST_CombustionModels_2011_Bras
ROHR INPUT FOR COMPRESSION IGNTION ENGINES /1
Vibe Single Zone
ROHR Approach
Parameter Data Source
Fitting Result of Combustion Analysis Tool (BOOST-Burn)
Experience
1
1
myam
c
BTB eym
aQ
d
dQ
c
oy
... Combustion Progress
Evaporation Assumption
ROE (Rate of Evaporation) is direct linked to ROHR
d
dQ
Hd
dm B
u
FV 1
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15 BOOST_CombustionModels_2011_Bras
ROHR INPUT FOR COMPRESSION IGNTION ENGINES /2
Double Vibe (Single Zone)
ROHR Approach
Superposition of 2 Vibe
Functions to meet Premixed
Combustion Peak and/or more
Complex Injection Strategies
Parameter Data Source
Fitting Result of Combustion Analysis Tool (BOOST-Burn)
Experience
21 Vibe
B
Vibe
BB
d
dQ
d
dQ
d
dQ
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16 BOOST_CombustionModels_2011_Bras
ROHR INPUT FOR COMPRESSION IGNTION ENGINES /3
Woschni/Anisits
Vibe Two Zone / Table Two
Zone
Same ROHR Approach as for Single Zone
State Vector of Burned Zone allows to calculate:
NOx Production (Extended Zeldovich)
CO Production (Onorati)
Soot Production (Bolochous)
Table Single Zone
Identical to spark ignition engines +
Evaporation Assumption
Required Input
Vibe Combustion Parameters and Ignition Delay for Reference Operating Point
Model Approach for Variation of Combustion Duration and Vibe Parameter m dependent on
Engine Speed and Ignition Delay
5.06.0
,
ref
ref
refccn
n
AF
AF
3.0
,
,
6.0
refIVC
refIVC
refIVC
IVCref
refn
n
T
T
p
p
id
idmm
Ignition delay according to relations found by Andree and Pachernegg (exceeding
Temperature*Time Integral threshold)
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17 BOOST_CombustionModels_2011_Bras
PREDICTED ROHR FOR COMPRESSION IGNTION ENGINES /1 AVLMCC COMBUSTION MODEL
AVLMCC Combustion Model
Model Approach
Mixture controlled combustion (MCC) part of
heat release is controlled by fuel
quantity available and the spray
induced turbulent kinetic energy
density.
Premixed combustion
is modeled by a vibe function which
parameters are determined from the ROI
(Rate of Injection) considering Ignition
delay.
Combustion process stages
Injection Turbulence Evaporation Ignition Delay Combustion
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18 BOOST_CombustionModels_2011_Bras
PREDICTED ROHR FOR COMPRESSION IGNTION ENGINES /4 AVL MCC COMBUSTION MODEL
PL1
SB1 SB2
MP1
MP2
MP3
MP4 MP5 MP6 MP7 MP8 MP9
MP10 MP11 MP12 MP13MP14 MP15
MP16
MP17 MP18
MP19
MP20
CO1
TC1
J1
J2
J3J4
1
2
3
4 5 6 7 8 9
10 11 12 13 14 15
16 17
18 19
20
21
CO2
CAT122
R1
CO3
23
24
25
J5
2627
J6
J7
28
R2
29
30
C1 C2 C3 C4 C5 C6
MP21
MP22
MP23
MP24
R3
31
CL1
32MP25
R4
33
p_11, T_11
p_21, T_21
p_2_1, T_2_1
p_IM, T_IM
p_41, T_41, NOx_S1, ...
Intake Throttle
EGR Valve
p_EGR, T_EGR
T_EGRHEOp_31_1, T_31_1 p_31_2,
T_31_2
TAZ6TAZ2 TAZ3
Wastegate
Air Cleaner
Charge Air Cooler
Exhaust Gas Treatment Devices
Intake Manifold
-20 -10 0 10 20 30 40 50 60 70 80 90 100 110 120
Crankangle [deg]
RO
HR
[J/d
eg]
0
20
40
60
80
100
120
140
160
180
200
Basis1_Ah_0038.50%.1800
Basis1_Ah_0038_MCC.50%.1800
1-zonig Analyse der 1-zonigen Sim.
1-zonig Analyse der 2-zonigen Sim.
Engine Speed rpm 1800.0
Compression Ratio - 18.500Energy Balance - 1.0149
Burn_bst_MCC_Ah38_B50.cly
BMEP [bar] 8.8542
BMEP [bar] 9.0688
MFB10 [deg] 7.4354MFB10 [deg] 6.7318
MFB50 [deg] 16.648
MFB50 [deg] 16.089
MFB90 [deg] 31.985
MFB90 [deg] 27.916
Calibration Parameters
Cmod combustion constant Cdiss dissipations constant Cturb turbulent constant CNO NOx formation constant Cign ignition delay constant
Project Experience
Parameters are engine specific but for than valid for a wide range
of operating points
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19 BOOST_CombustionModels_2011_Bras
PREDICTED ROHR FOR COMPRESSION IGNTION ENGINES /5 HCCI COMBUSTION MODEL
Single Zone HCCI
Simulation based on General Species Transport
CHEMKIN compatible
no CHEMKIN needed
arbitrary no. of species (CO, CO2, H2, O, H, ...)
arbitrary no. of chemical reactions (two sets for unburned
and burned Zone Chemistry) C7H16 + O2 = C7H15-1 + HO2 2.500E+13 0.0 48810.0
C7H16 + O2 = C7H15-2 + HO2 2.800E+14 0.0 47180.0
C7H16 + H = C7H15-1 + H2 5.600E+07 2.0 7667.0
C7H16 + H = C7H15-2 + H2 4.380E+07 2.0 4750.0
C7H16 + OH = C7H15-1 + H2O 8.600E+09 1.10 1815.0
nSpcGas
i
ii
F
d
dwu
d
dQ
1
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20 BOOST_CombustionModels_2011_Bras
PREDICTED ROHR FOR COMPRESSION IGNTION ENGINES /6 HCCI COMBUSTION MODEL
6 Zone HCCI Combustion
6 zones
General species transport
Non uniform species distribution in zones
2 Heat Transfer
Zone to zone (engery potential driven)
Boundary zone to wall
Isooctane mechanism (~291 species 875 reactions in CHEMKIN Format)
Kozarac et al.: SAE 2010-01-1083
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21 BOOST_CombustionModels_2011_Bras
BOOST CLASSIC / GENERAL SPECIES TRANSPORT
Utilites
Calculated
ROHR
Pre-defined
ROHR
Classic General
Vibe (1zone, 2zone, Hires,...)
Table (1zone, 2zone)
Diesel: MCC
Gasoline: Fractal
HCCI -
User Coded Combustion Models
Set Conditions at SHP
General Species Transport
Flexibility
CHEMKIN Chemistry can be used comfortably in BOOST (HCCI)
Coupling of Combustion-, Emission- and Aftertreatment models
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22 BOOST_CombustionModels_2011_Bras
BOOST-FIRE COMBUSTION & EMISSION SIMULATION
BOOST ESE-Diesel Link
3D Combustion through ESE Diesel BOOST
Coupling
BOOST Automatically Initialize and Starts
ESE Diesel Calculations for The Combustion
Phase
Modes of Coupling:
HPC-mode: Combustion
Calculated for One BOOST
Cylinder and ROHR Copied
to the Others
MHPC-mode: Combustion
Calculated for Each BOOST
Cylinder Individually
Engine Simulation Environment - Diesel