Combustion Model for Engine Concept Development · Combustion model for engine concept simulation ....

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Arne Andersson; Bincheng Jiang Volvo Global Trucks Technology Karin Fröjd; Simon Bjerkborn; Lars Seidel Michał Pasternak; Andrea Matrisciano; Fabian Mauss Lund Combustion Engineering LOGE AB DEER 2012 Conference Combustion model for engine concept simulation

Transcript of Combustion Model for Engine Concept Development · Combustion model for engine concept simulation ....

Page 1: Combustion Model for Engine Concept Development · Combustion model for engine concept simulation . Global Trucks Technology Arne Andersson, DEER 2012 Combustion model needed for

Arne Andersson; Bincheng Jiang Volvo Global Trucks Technology

Karin Fröjd; Simon Bjerkborn; Lars Seidel Michał Pasternak; Andrea Matrisciano; Fabian Mauss

Lund Combustion Engineering – LOGE AB

DEER 2012 Conference

Combustion model for engine concept simulation

Page 2: Combustion Model for Engine Concept Development · Combustion model for engine concept simulation . Global Trucks Technology Arne Andersson, DEER 2012 Combustion model needed for

Global Trucks Technology Arne Andersson, DEER 2012

Combustion model needed for advanced combustion in engine concept development Systems approach is needed Integration with GT-Power

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PPC is challenging to model A wide span of combustion modes in a load sweep

IMEP 8 bar Like HCCI

IMEP 12 bar PPC

IMEP 26 bar Diffusion combustion

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The Stochastic Reactor Model (SRM)

The particle properties (Temperature/enthalpy, species concentration) are statistically described by a Probability Density Function (PDF). The development of the PDF is calculated through particle interaction (mixing) and detailed chemistry.

In the zero-dimensional Stochastic Reactor Model, the in-cylinder gas mass is discretized into a set of particles without any spatial resolution. Each individual particle is treated as a well-stirred reactor.

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The Stochastic Reactor Model (SRM)

Mixing is modeled as a stochastic process: Particles are randomly selected to interact with each other. Both temperature and chemical composition is exchanged. The frequency of mixing events is determined by the turbulent mixing time τ

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The SRM model makes use of detailed chemistry.

Three different mechanisms were evaluated:

• 33-species Tsurushima mechanism

• 200-species NICE mechanism

• 477-species Toluene Reference Fuel (TRF) mechanism

The 33-species mechanism was found to yield unrealistic ignition timing, whereas the differences between the 200-species mechanism and the 477-species mechanism were negligible.

The 200-species NICE mechanism has been used for all simulations in this presentation.

Chemistry

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• Vaporized fuel is introduced as new particles in the SRM.

• These particles are mixed with the background gas (air and EGR) according to the turbulent mixing time.

Fuel injection

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Example: Vaporized cold fuel mixing with background gas and igniting

T

Ф

T

Ф

lg(Xi)

lg(Xi)

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Example: Vaporized cold fuel mixing with background gas and igniting

T

Ф

T

Ф

lg(Xi)

lg(Xi)

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PPC modeling with the SRM

Problem: While the SRM model presumes statistical homogeneity in the combustion chamber, this assumption is not true for the PPC. At the point of ignition, much fuel is still concentrated in a rich zone

Solution: Divide the background gas in the SRM into two distinct zones. Let the injected fuel be introduced into one of the zones. Mix predominantly within each zone to capture the effects of stratification.

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PPC modeling with the SRM

With the two-zone approach, each property of the gas is described by two superimposed PDF:s. The total mass of background gas to be allocated into the fuel-rich zone is a user parameter, as is the scale factor for the amount of mixing between the zones.

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Two-zone PDF development

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Two-zone PDF development

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Two-zone PDF development

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Two-zone PDF development

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CFD calculations support the notion that a portion of the fuel is found in a localized rich zone for a significant amount of time after EOI. Zone volumes for the different operating points were approximated based on the Z distribution.

Fuel density distribution from CFD calculations

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The mixing time is taken from CFD calculations for each respective operating point. In order to model the mixing within the rich zone, tau profiles conditioned on mixture fraction 0.06 to 0.08 were used.

Turbulent mixing time from CFD calculations

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Case 1 – IMEP 12 bar A good agreement was found using the CFD provided mixing time.

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Case 2 – IMEP 8 bar All relevant parameters except the turbulence profile and zone volume was kept constant between the cases.

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Case 3 – IMEP 26 bar All relevant parameters except the turbulence profile and zone volume was kept constant between the cases.

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3D combustion CFD generate statistical input data for the 0D combustion model • With the right statistical parameters we can create a 0D

combustion model capable of PPC simulation • A 2-zone stocastic approach is required to match CFD data • The Stocastic approach enables the use of big enough

kinetic mechanisms • The stocastic approach enables the combustion model

integration in GT-Power

Sum up and conclusions

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Acknowledgements

This material is based upon work supported by – Department of Energy National Energy Technology Lab under

Award Number DE-EE0004232

– Department of Energy National Energy Technology Lab under Award Number DE-FC26-07NT43222

This report was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor any agency thereof, nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States Government or any agency thereof. The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States Government or any agency thereof.