In-Cylinder Engine Calculations: New Features and Upcoming Capabilities
Richard Johns & Gerald Schmidt
Capabilities Richard Johns & Gerald Schmidt Contents Brief - - PowerPoint PPT Presentation
In-Cylinder Engine Calculations: New Features and Upcoming Capabilities Richard Johns & Gerald Schmidt Contents Brief Review of STAR-CD/es-ice v4.20 Combustion Models Spray Models LES New Physics Developments in v4.22
In-Cylinder Engine Calculations: New Features and Upcoming Capabilities
Richard Johns & Gerald Schmidt
NORA NOx model, CO, soot
submodels and extensive validation
Temperature = 398 K, Pressure = 0.5 MPa
2.1 ms 2.5 ms 2.9 ms
Liquid Phase Vapor Phase
GRUppoMOtori
Internal Combustion Engine Research Group
2 nd 3 rd 1 st 4 th 5 th 7 th 8 th 6 th 9 th 10 th 12 th 13 th 11 th 14 th 15 th 17 th 18 th 16 th 19 th 20 th
GRUppoMOtori
Internal Combustion Engine Research Group
Local flow field influence: 4th fastest 16th slowest
A B A B A B A B
GRUppoMOtori
Internal Combustion Engine Research Group
) ) var( ) var( ) , cov( ( ) , (
j j j i
Y X Y X abs Y X
0.2 0.4 0.6 0.8 1 ER_local VMAG_local TE_local
Correlation Coefficient (FSD_transition, Yj)
FSD_transition VS Yj (20 cycles)
CCV itself relevantly depends on the FSD_transition CCV. This parameter (thus the transition between the ignition model and the FSD equation) is mostly influenced by equivalence ratio and velocity fields close to the spark plug at the spark time occurrence.
GRUppoMOtori
Internal Combustion Engine Research Group
analyses in Star-CCM+ to calculate the local heat transfer
is applied to LES knocking combustion Mapped Wall Temperatures
Piston Crown Combustion Dome
GRUppoMOtori
Internal Combustion Engine Research Group
1.E+00 1.E+01 1.E+02 1.E+03 1.E+04 1.E+05 1.E+06 1.E+07 730 740 750 760 770 780 790 800 [W] Crank Angle
Heat Release Rate - Autoignition
Uniform Wall - Fast Cycle Uniform Wall - Medium Cycle Uniform Wall - Slow Cycle Mapped Wall - Fast Cycle Mapped Wall - Medium Cycle Mapped Wall - Slow Cycle
thermal field SAE Paper 2013-01-1088
fuel combustion
Picture source: http://www.westport.com/is/core-technologies/combustion
PVM-MF Dual-Fuel Combustion
– Bore 130 – Stroke 150 – Conrod 260 – Compression ratio 18
– Engine speed 1500 rev/min – AFR-NG 30.3, AFR-Diesel 273 – EGR 2.5% – Fuel injection
Cylinder pressure and temperature
200 400 600 800 1,000 1,200 1,400 1,600 1,800 0.0E+00 2.0E+06 4.0E+06 6.0E+06 8.0E+06 1.0E+07 1.2E+07 1.4E+07 1.6E+07 1.8E+07 2.0E+07 600 630 660 690 720 750 780
Temperature (K) Pressure (Pa) Crankangle (deg) Pressure Temperature
PVM-MF Dual-Fuel Combustion
Heat release rate
0.0E+00 2.0E+05 4.0E+05 6.0E+05 8.0E+05 1.0E+06 1.2E+06 1.4E+06 1.6E+06 1.8E+06 2.0E+06 700 710 720 730 740 750 760 770 780 790 800
Heat release rate (J/sec) Crankangle (deg)
Diesel Natural gas
PVM-MF Dual-Fuel Combustion
711.5oCA
Diesel PV NG T
712oCA 710oCA 708oCA
PVM-MF Dual-Fuel Combustion
717oCA
Diesel PV NG T
720oCA 715oCA 713oCA
PVM-MF Dual-Fuel Combustion
Fuel-1: Diesel Fuel-2: Natural gas
PVM-MF Dual-Fuel Combustion
Combustion progress variable Temperature
PVM-MF Dual-Fuel Combustion
– Thermal Nitric Oxide
Monat et al. 1979)
– NO mass fraction (used in example)
– NO mass fraction
– Soot
– Soot Mass (used in example)
– Soot Number Density – Soot Volume Fraction – Soot Surface Density – Soot Mean Diameter
– Carbon Monoxide CO (Hautman et al. 1981)
– CO mass fraction(used in example)
PVM-MF Dual-Fuel Combustion
Emissions
0.00E+00 1.00E-03 2.00E-03 3.00E-03 4.00E-03 5.00E-03 6.00E-03 7.00E-03 8.00E-03 9.00E-03 800 900 1,000 1,100 1,200 1,300 1,400 1,500 1,600 1,700 700 710 720 730 740 750 760 770 780 790 800
Emissions mass fraction Temperature (K) Crankangle (deg) Temperature Nox * 10 Soot CO
PVM-MF Dual-Fuel Combustion
Purpose of the Model:
changes in surface temperature. Important for:
and hence fuel evaporation rate which affects mixture distribution
the near-surface conducting layer – 1D heat flow assumption does not need an additional mesh
Fluid Cell Solid Layer 1 Solid Layer 2 FSI SSI
contact resistance
QF
F
1 2 3 4 5 6 7 8
B 5 10 15 20 25 30 35 40 0.0 1.0 2.0 3.0
Temperature Increase [K] Distance from surface [mm]
Temperature Increment vs Time
Time = 1 ms Time = 5 ms Time = 10 ms
bottom wall
450 K
conjugate heat transfer calculation
activated at bottom wall
property on wall temperature change
Tair= 350 K Pair= 1 bar Twall = 350 K Twall = 350 K Twall= 450 K (BASELINE) Conduction (CHT) Tbulk = 450 K (1DCHT)
Minimum temperature on bottom wall as a function of time: No major differences between the CHT & 1DCHT predictions, justifying the use of the 1D CHT model
444 445 446 447 448 449 450 5 10 15 Minimum Wall Temperature [K] Time [ms]
BASELINE CHT 1DCHT
BASELINE CHT 1DCHT
Predicted wall temperature at 15 ms after SOI
432 434 436 438 440 442 444 446 448 450 5 10 15 Minimum Wall Temperature [K] Time [ms]
2.50_80_1.0k 2.50_80_0.5k 2.50_80_0.1k
Therm ermal al prope
rties ies of the he soli lid d has a subst ubstan antial ial effect
erat atur ure, e, with h low-condu nductivit ivity mater erial ial experie perienc ncing ing the he larges rgest tem emper perat atur ure e drop
Wall l temperatu rature re distrib tributi tion at 15 ms afte ter r SOI: No major differences between the CHT & 1DCHT predictions
mesh
chamber center
model with 1.25mm BaTiO3 (barium titanate) layer
temperature of 500 K
model activated at bottom wall
conjugate heat transfer calculation
material property on wall temperature change
Tair= 800 K Pair= 5 bar Ω = 2000 rpm YC8H18 = 0.0623 Twall= 500 K (BASELINE) Conduction(CHT) Tbulk = 500 K (1DCHT) Twall = 500 K Twall = 500 K
BaTiO3 Aluminum
Density [kg/m3] 5840 2702 Thermal conductivity [W/mK] 2.6 237 Heat capacity [J/kgK] 434 903 Thickness [mm] 1.5 5.0
t = 2.5 ms t = 5.0 ms t = 15.0 ms
Maximum wall temperature increase as a function of time: No major differences between the CHT & 1DCHT predictions; verifying the validity of the 1D CHT model
500.0 502.0 504.0 506.0 508.0 510.0 512.0 514.0 5 10 15 20 25 30 35 40 45 50
Time [ms] 1DCHT_BaTiO3_1.25mm 1DCHT_Al_5.00mm
BASELINE CHT 1DCHT
Predicted wall temperature 25 ms after SOI
500.0 502.0 504.0 506.0 508.0 510.0 512.0 514.0 5 10 15 20 25 30 35 40 45 50
Time [ms]
Maximum Wall Temperature vs Time
BASELINE CHT_1.25mm 1DCHT_1.25mm
Thermal properties of the solid has a strong effect on wall temperature increase, must be properly accounted for in
predictions Wall temperature distribution 25 ms after SOI: No major differences between the CHT & 1DCHT predictions
efficiently
and accuracy of in-cylinder calculations
methodology new methods have been developed for use with IC Engine flows
available in 2014
Period: TDC > 30o ABDC (210o) Total of 6 meshes Max cells ~ 1.5M at BDC Period: TDC > 30o ABDC (210o) Scalar Flow & Mixing
Morphing/Remeshing/Mapping - Setup
Mesh generated at this time Mesh morphed in - time Mesh morphed in + time Solution mapped to next mesh
stages of the calculation
Constrained Polyhedra
Core Cartesian Mesh Prism Layers Polyhedral Mesh Local Coordinate Systems and Local Mesh Refinement Variable number
2-valve Gasoline with polyhedral mesh
The same concept can be used to embed a local coordinate system for eg a spray-adapted mesh in a gasoline engine Selected morphing used to control mesh motion
Gasoline Gasoline Spr Spray ay-Ada Adapted pted Mesh Mesh
Period: TDC > 30o ABDC (210o) Spray-adapted mesh between 80o BBDC > 50o BBDC Total of 7 meshes Max cells ~ 1.5M at BDC
Gasoline Spray-Adapted Mesh
Scalar Field from Intake Flow
Internal Combustion Engine capabilities in STAR-CCM+
STAR-CCM+