GPF modeling supported by size-resolved filtration efficiency … · 2019-11-26 · 09/11/2019...

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1 09/11/2019 MODEGAT 2019 GPF modeling supported by size-resolved filtration efficiency measurements Michail Mitsouridis , Grigorios Koltsakis, Zissis Samaras Aristotle University Thessaloniki Jeremy Gidney, John Goodwin Johnson Matthey Christian Martin AVL List GmbH

Transcript of GPF modeling supported by size-resolved filtration efficiency … · 2019-11-26 · 09/11/2019...

Page 1: GPF modeling supported by size-resolved filtration efficiency … · 2019-11-26 · 09/11/2019 MODEGAT 2019 1 GPF modeling supported by size-resolved filtration efficiency measurements

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GPF modeling supported bysize-resolved filtration efficiency measurements

Michail Mitsouridis, Grigorios Koltsakis, Zissis SamarasAristotle University ThessalonikiJeremy Gidney, John GoodwinJohnson MattheyChristian MartinAVL List GmbH

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• Target: Particle free gasoline engines with cost-effective GPFsHow can we use GPF modeling to support system optimization?

• Background: GPF modeling shares many common features and challenges as the long established DPF modeling.However, there are some important differences:– Lower PM/PN emissions -> operation in depth filtration

– Lack of O2 and NO2 for thermal regeneration

– Higher exhaust gas temperatures -> thermal shock risks

– How to combine TWC functions?

– ...

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Background & motivation

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Spherical collector filtration model

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dgrain =3

2

1−εpore

εporedpore

Agglomerate structure = f(fpart, Rppart, ρppart, Rmc)

• fpart: Particle fractal dimension [-] → agglomerate geometry standardization

• Rppart: Primary particle radius [m]

• ρppart: Primary particle density [kg/m3]

• Rmc: Aggregate cluster mobility radius [m] → the diameter of a spherical particle with the same mobility (ease to have constant motion) as the agglomerate in question

porous wall unit cell

deposit layer

washcoat

grainEwall = 1 − e−ηg

3

2

1−εpore,0

εpore,0

Δw

dgrain,0 , Δw: node thickness

ηg = ηg,0 + 1 − ηg,0 erf3nload

2Wcap , Wcap=

εpore,0 − εpore

εpore,0

ηg,0 = ηD + ηR

ηD = nclean,D ∙ 3.5εpore,0

Ku

1

3PenPe , Pe =

uw∙dgrain,0

Dpart

ηR = nclean,R ∙ 1.5εpore,0

Ku

R2

1+R m, m =3−2∙εpore,0

3∙εpore,0, R =

2Rc

dgrain,0

dpore

dgrain

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Filtration model calibration

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The size-resolved filtration efficiency is well captured by the model for particles > 30 nm.

Uncoated GPF Coated GPF: 50 g/l

nclean,D = 0.35

nclean,R = 5

Particulate Filter Test System• 250 kg/h, 240°C

• GPF cell structure: 12mils, 300cpsi

• Calibration of:

– nclean,D: Diffusion mechanism correction factor

– nclean,R: Interception mechanism correction factor

nclean,D = 0.25

nclean,R = 4.5

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Model application & validation with thinner wall filters

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Uncoated GPFs Coated GPFs: 50 g/l

nclean,D = 0.35

nclean,R = 5nclean,D = 0.25

nclean,R = 4.5

The filtration model is predictive for filters of different wall thickness.

This coating does not have a major impact on filtration efficiency (FE).

Model parameters: based on the calibration with the 12/300 GPF

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Effect of soot loading

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nload = 4.5 nload = 8

The model captures reasonably well the filtration efficiency increase due to progressive soot accumulation.

12mils, 300cpsi

Uncoated GPF Coated GPF: 50 g/l

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Total PN filtration efficiency vs soot loading

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Increasingwall thickness

Increasingwall thickness

The filtration model predicts the rate of FE increase as function of collected soot amount.

Uncoated GPFs Coated GPFs: 50 g/l

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Filtration efficiency prediction in real exhaust

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CC: 50 g/l UF: 100 g/l

Engine sweep tests0-700kg/h

T=300-800°C

2.0 l TGDIengine test bed UF: 100 g/l

CC: 50 g/l

The filtration model performs well in the whole engine map.

Engine sweep tests with two exhaust line configurations.

Initial soot loading: 0 g/l

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Towards predictive filtration modeling

The available database was used to derive correlation functions for the filtration model

tuning parameters

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Pressure drop modelingSoot-free filters

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2.2 l Diesel engine(Daimler OM646)

UncoatedEffect of wall thickness

CoatedEffect of washcoat loading on wall permeability

dP

dw=

ሻμ ∙ v(w

kw

kw = kw,0 ⋅ 1 + C4p0pμ

T

Mg

kw,0: Clean wall permeabilityC4: Slip correction factor

Same kw,0 Increasing kw,0

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Pressure drop modelingSoot loaded filters

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The effect of soot in the wall on deltaP is strongly affected by the microstructure after coating.

The empirical model may have a compromised accuracy in the transition region.

dP

dw=

ሻμ ∙ v(w

kw, kw =

1

1kw,0

+ C1 ⋅ ρP + C2 ⋅ ρP2⋅ 1 + C4

p0pμ

T

Mg

dP

dw=

ሻμ ∙ v(w

kp, kp=

ρp,0 ∗ k0

ρp1 + C4

p0pμ

T

Mg

kw: Soot loaded wall permeabilityρp,l: Reference wall soot loading

ρp,0: Soot reference density

k0: Soot permeability

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Towards predictive pressure drop modeling

Correlations of wall permeability for clean and loaded wall state were derived

for a range of 0 to 500 g/l wall.

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Reference wall soot loading: 2.5 g/lwall

Is it possible to avoid filter permeability recalibration for each new filter configuration, i.e. various washcoat loadings (grams per liter of filter), cell- and wall micro-structures?

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Model application in RDE cycle conditions

(100g/l w/c loading)

UF: 100 g/l

CC: 50 g/l

(50g/l w/c loading)

1.8l TGDI enginechassis dynamometer

RDE protocol

• During the RDE test, soot oxidation may take place during fuel cut-off events and high temperatures.

• The UF: 100 g/l has a lower regeneration potential compared to the CC: 50 g/l filter.

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Combined model validationLoss of filtration efficiency due to wall cleaning

CC: 50 g/l washcoat

PN slip: 14%

0.18

RDE high temperature cycle with preloaded GPF (=0.4 g/l)

PN slip (normalized over total emitted engine out PN) appears after soot

loading goes below ~0.2 g/l

Due to high temperature and frequent fuel cutoffs, soot is

oxidized (simulation result only)

The GPF combined model (filtration, transport, reaction phenomena) manages to predict the observed PN slip

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withfuel cut-off events

withoutfuel cut-off events

To validate that the PN slip is associated with wall cleaning, the test was repeated de-activating fuel cut-off events.

Deactivation of fuel-cut off mode drastically reduces the PN slip.The model predictions are in line with the measured observations.

Verification of modelDeactivation of fuel cutoff

CC: 50 g/l washcoat

PN slip: 2%

PN slip: 14%

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Model application exampleUnderfloor vs close-coupled positioning

CC: 50 g/l washcoat UF: 100 g/l washcoat

0.18

Same RDE cycle run with UF and higher w/c loading filter. Initial soot loadings: CC filter: 0.4 g/l, UF filter: 0.1 g/l

PN slip: 14%

UF filter exposed to lower temperature -> less soot is oxidizedThe remaining soot in the UF filter is sufficient to maintain very low PN slip

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Pressure drop prediction accuracy in RDE cycle

Good prediction accuracy under complex operating conditions

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CC: 50 g/l washcoat UF: 100 g/l washcoat

Data zoom in high flow rate operating mode

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Ash transport testing & modeling

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Ash & soot loading250°C187 kg/h

Layer ashdetachment

Redeposition aslayer ash

Deposition asplug ash

SootAsh

Testing Modeling in axisuite(previously parameterized)

Oven regeneration• 650°C in air• 187kg/h• 3 hours

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Ash loaded model validation

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UF: 50 g/l

Engine sweep tests with filters loaded at various ash levels

The model may be used for lifecycle analysis for various filter designs and driving profiles

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Ash model validation in RDE transient cycles

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23g/l ash

42g/l ash

0g/l ash

UF: 50 g/l

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• In view of the increasing gasoline after-treatment requirements and complexity, a practical/balanced modeling approach was developed.

• Based on a small database of calibrated models, correlation functions were developed to support permeability and filtration modeling for various washcoat loadings, cell- and wall micro-structures.

• Due to the low engine-out emissions, it is important to maintain sufficient soot amount in the filter to reduce the risk of PN slip. Regenerations during fuel cutoff are of key importance.

• Inclusion of ash transport modeling allows a life cycle analysis and assessment of GPF designs and application-specific model-based optimization.

• Current-future work: – Improve filtration efficiency predictions for very small particles

– Advanced filtration models accounting for pore size distribution

– Model application in non-uniformly coated substrates: zoning & layering

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Summary & conclusions

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The results were obtained within the project UPGRADE. This project has received funding from the European Union’s Horizon 2020 research and innovation programme under grant agreement No 724036.

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Acknowledgements

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We gratefully acknowledge:- the financial support of EU - the great work of our colleagues at LAT/AUTh, AVL and JM involved in the measurements. - The valuable support of NGK Europe GmbH providing many of the test samples used in

this work

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Thank you very much!

09/11/2019 23SIA Powertrain, Rouen 2014

MODEGAT 2019

Michail Mitsouridis

[email protected]