Advanced Nozzle Flow and Spray Modeling...•Near nozzle spray features are better predicted by the...
Transcript of Advanced Nozzle Flow and Spray Modeling...•Near nozzle spray features are better predicted by the...
Copyright © 2014 Convergent Science Inc., All rights reserved.
Advanced Nozzle Flow and Spray Modeling
• Able to predict effects of needle wobble • Able to predict hole-to-hole variations
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• Start of injection simulations show gas injection before liquid • End of injection simulations show dribble and ingested gas in the sac
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• Improved near nozzle comparisons with x-ray data • Spray jet shock wave generation
End$of$Injec+on,
Liq.%Volume%Frac0on%
2200 µs
2250 µs
2300 µs
Dribble?%
3-4 weeks on 100 processors, ~20 million cells
Copyright © 2014 Convergent Science Inc., All rights reserved.
Advanced Nozzle Flow Modeling
eccentricity (positive x-axis)
1
2
3
4
5x
y
0 500 1000 1500 20000
50
100
150
200
250
Nee
dle
mov
emen
t (µm
)
Time (µs)
lifteccentricity (modulus)
▪ Effect of Needle Side Motion on Hole-to-Hole Mass Flow Variation
*Battistoni et al., SAE 2014Collaboration with Argonne and Cummins
Copyright © 2014 Convergent Science Inc., All rights reserved.
Advanced Spray Modeling
*Xue et al., SAE 2014
60 µm
30 µm
15 µm
X-ray measurements
Projected mass density
0.1 mm
2 mm
ECN Spray A
Collaboration with Argonne and Cummins
Copyright © 2014 Convergent Science Inc., All rights reserved.
Advanced Spray Modeling
*Quan et al. SAE 2014
0.81 kg/m3 2.55 kg/m3 11.7 kg/m3
▪ Eulerian-Eulerian coupled with VOF ▪ Compressible liquid and gas ▪ Dynamic structure LES ▪ AMR
Collaboration with Sandia and Argonne
Copyright © 2014 Convergent Science Inc., All rights reserved.
Advanced Turbulence ModelingRNG – 0.25 mm
The computational cost of grid-convergent LES (@ 0.0625 mm) is about 30-40 times compared to grid-convergent RANS (@ 0.25 mm)
Collaboration with Argonne and Cummins
Copyright © 2014 Convergent Science Inc., All rights reserved.
Advanced Turbulence Modeling
Radial Distance (mm)
-10 -5 0 5 10
Axi
al V
eloc
ity (m
/s)
0
25
50
75
100
125
150
MeasuredInstantaneous LES (20 Realizations)
Radial Distance (mm)
-10 -5 0 5 10
Axi
al V
eloc
ity (m
/s)
0
25
50
75
100
MeasuredEnsemble-Averaged LES 25 mm
25 mm 35 mm 45 mm
Radial Distance (mm)
-10 -5 0 5 10
Axi
al V
eloc
ity (m
/s)
0
25
50
75
100
MeasuredEnsemble-Averaged LES 35 mm
Radial Distance (mm)
-10 -5 0 5 10
Axi
al V
eloc
ity (m
/s)
0
25
50
75
100
MeasuredEnsemble-Averaged LES 45 mm
Sample Size
0 2 4 6 8 10 12 14 16 18 20
Per
cent
0
10
20
30
40
50
60
70
80
90
100
0.5 m/s1.0 m/s2.0 m/s5.0 m/s
Sample Size
0 2 4 6 8 10 12 14 16 18 20
Per
cent
0
10
20
30
40
50
60
70
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100
0.5 m/s1.0 m/s2.0 m/s5.0 m/s
Sample Size
0 2 4 6 8 10 12 14 16 18 20
Per
cent
0
10
20
30
40
50
60
70
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90
100
0.5 m/s1.0 m/s2.0 m/s5.0 m/s
*Senecal et al. ASME 2013
Radial Distance (mm)
-10 -5 0 5 10
Axi
al V
eloc
ity (m
/s)
0
25
50
75
100
125
150
MeasuredPredicted Average, 20 InjectionsPredicted Average, 8 Injections
8 cycles are needed to match the 20-cycle average to within a tolerance of 2 m/s
Collaboration with Argonne and Cummins
• Each simulation requires 60 hours on 64 cores • Peak cell count: ~20 million
Copyright © 2014 Convergent Science Inc., All rights reserved.
Grid Convergence
Time (ms)
0.0 0.2 0.4 0.6 0.8 1.0
Liqu
id P
enet
ratio
n (m
m)
0
10
20
30
40
50
60
70
80
Measureddx = 2.0 mmdx = 1.0 mmdx = 0.5 mmdx = 0.25 mmdx = 0.125 mmdx = 0.0625 mmdx = 0.03125 mm
•Great care has been taken to ensure grid convergence in the CONVERGE spray models, such that the results can be analyzed with confidence
•Cell sizes down to 30 microns have been analyzed (AMR)
•Allows for accuracy/run-time tradeoff*Senecal et al. ASME 2012
Grid-convergent AMR cell size of 0.25 mm for RANS
Up to 4 - 5 cells inside the nozzle diameter at finest resolution
O2 Concentration (%)
8 10 12 14 16 18 20 22
Flam
e Li
ft-of
f Len
gth
(mm
)
0
5
10
15
20
25
30
35
40
Measureddx = 1.0 mmdx = 0.5 mmdx = 0.25 mmdx = 0.125 mm
Collaboration with Argonne
Copyright © 2014 Convergent Science Inc., All rights reserved.
Extending Grid Convergence to Engines
*Senecal et al. JEGTP 2014Collaboration with Sandia and Caterpillar
Cell size, dx (mm)
0.0 0.2 0.4 0.6 0.8 1.0
Flam
e Li
ft-O
ff Le
ngth
(mm
)
0
5
10
15
20
25
30
35
40
45
50
MeasuredPredicted, No Cell LimitPredicted, 300k Cell Limit
Copyright © 2014 Convergent Science Inc., All rights reserved.
Extending Grid Convergence to Engines
*Senecal et al. JEGTP 2014Collaboration with Sandia and Caterpillar
Measured CL of OH*
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Extending Grid Convergence to Engines
SOC (deg. ATDC)
-2 0 2 4 6
NO
x (p
pm)
0
50
100
150
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MeasuredCONVERGE - Full Geometry
Crank Angle (deg. ATDC)
-40 -20 0 20 40 60
Pre
ssur
e (M
Pa)
0
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MeasuredCONVERGE - Full Geometry
-2SOC
Crank Angle (deg. ATDC)
-40 -20 0 20 40 60
Pre
ssur
e (M
Pa)
0
2
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MeasuredCONVERGE - Full Geometry
2SOC
Crank Angle (deg. ATDC)
-40 -20 0 20 40 60
Pre
ssur
e (M
Pa)
0
2
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MeasuredCONVERGE - Full Geometry
6SOC
OH* Chemiluminescence vs. OH iso-surface, 7.5 degrees after SOC
The grid-convergent methodology results in excellent agreement with global combustion behavior as well as flame lift-off length and flame location
2 million cells utilized
*Senecal et al. JEGTP 2014Collaboration with Sandia and Caterpillar
Copyright © 2014 Convergent Science Inc., All rights reserved.
Collaborations with LLNL654 Species, 2827 Reactions Total Time (days)
SAGE 150
SAGE-MZ, Direct 60
SAGE-MZ, Iterative 8
SAGE-MZ-DMR, Iterative 2
GPU ???
Mechanisms with up to 1,000 species can now be simulated with CFD
Year
Tota
l Run
time
(Day
s)
0
50
100
150
200Diesel, 654 Species, 2827 Reactions
2010 2011 2012 2013
101 102 103 104
102
103
104
2-methyl-alkanes
before 2000 2000-2005 2005-2010 after 2010
biodiesel
(USC) JetSURFC8(ENSIC-CNRS) C8
C4 (LLNL)
(Konnov) CH4
C4 (LLNL)C2 (San Diego)
CH4 (Leeds)
MDC16
C14C12
C10
(USC) C4(USC) C2
PRF
C7
C7, C8 skeletal (Lu&Law)
DME (Curran)(Qin) C3GRI3.0
Nu
mbe
r of r
eact
ions
, I
Number of species, K
GRI1.2
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Key Findings and Recommendations RANS Spray Simulations
LES Spray Simulations
Eulerian Spray Simulations
Nozzle Flow Simulations
•0.25 mm cell sizes provide reasonably grid converged results for non-evaporating, vaporizing, and combusting sprays
•0.125 mm or finer resolutions necessary (recommended to use 0.0625 mm) •Multi-realization averaging is necessary to mimic experimental data (at least 8 realizations need to be averaged)
•Near nozzle spray features are better predicted by the EE model •EE simulations require at least 15 micron resolution near the nozzle
•10-15 micron resolution is sufficient to capture bulk flow features •5 micron or finer may be needed to capture opening and closing transients •Needle wobble has a large influence on plume-to-plume variations
Copyright © 2014 Convergent Science Inc., All rights reserved.
▪ Massively parallel simulations, CPUs and GPUs ▪ Improved chemical mechanisms and emissions models - predictive soot ▪ LES with grid-converged mesh resolution ▪ Eulerian spray modeling linked to nozzle flow ▪ Multiple cycles routinely ▪ Multiple cylinders routinely ▪ CHT routinely !
High Performance Computing is a significant enabler to helping us achieve these goals.
Future Directions - Engine CFD in 5 Years in CONVERGE