A Comparison of Strategies for Direct Numerical Simulation of Turbulence Chemistry Interaction in Generic Planar Turbulent Premixed Flames
Abstract Three different methods to introduce turbulence in the computational domain of Direct Numerical Simulations (DNS) of statistically planar turbulent premixed flame configurations have been reviewed and their advantages and disadvantages in terms of run time, natural flame development, contro...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Klein, Markus [verfasserIn] |
|---|
| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2017 |
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| Schlagwörter: |
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| Anmerkung: |
© Springer Science+Business Media B.V. 2017 |
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| Übergeordnetes Werk: |
Enthalten in: Flow, turbulence and combustion - Springer Netherlands, 1998, 99(2017), 3-4 vom: 11. Aug., Seite 955-971 |
|---|---|
| Übergeordnetes Werk: |
volume:99 ; year:2017 ; number:3-4 ; day:11 ; month:08 ; pages:955-971 |
| Links: |
|---|
| DOI / URN: |
10.1007/s10494-017-9843-9 |
|---|
| Katalog-ID: |
OLC205957692X |
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| 520 | |a Abstract Three different methods to introduce turbulence in the computational domain of Direct Numerical Simulations (DNS) of statistically planar turbulent premixed flame configurations have been reviewed and their advantages and disadvantages in terms of run time, natural flame development, control of turbulence parameters and convergence of statistics extracted from the simulations have been discussed in detail. It has been found that there is no method, which is clearly superior to the other two alternative methods. An analysis has been performed to explain why Lundgren’s physical space linear forcing results in an integral length scale which is, independent of the Reynolds number, a constant fraction of the domain size. Furthermore, an evolution equation for the integral length scale has been derived, and a scaling analysis of its terms has been performed to explain the evolution of the integral length scale in the context of Lundgren’s physical space linear forcing. Finally, a modification to Lundgren’s forcing approach has been suggested which ensures that the integral length scale settles to a predetermined value so that DNS of statistically planar turbulent premixed flames with physical space forcing can be conducted for prescribed values of Damköhler and Karlovitz numbers. | ||
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| 700 | 1 | |a Ketterl, Sebastian |4 aut | |
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10.1007/s10494-017-9843-9 doi (DE-627)OLC205957692X (DE-He213)s10494-017-9843-9-p DE-627 ger DE-627 rakwb eng 500 600 VZ 50.34$jGasdynamik$jAerodynamik bkl 52.51$jFeuerungstechnik bkl Klein, Markus verfasserin aut A Comparison of Strategies for Direct Numerical Simulation of Turbulence Chemistry Interaction in Generic Planar Turbulent Premixed Flames 2017 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media B.V. 2017 Abstract Three different methods to introduce turbulence in the computational domain of Direct Numerical Simulations (DNS) of statistically planar turbulent premixed flame configurations have been reviewed and their advantages and disadvantages in terms of run time, natural flame development, control of turbulence parameters and convergence of statistics extracted from the simulations have been discussed in detail. It has been found that there is no method, which is clearly superior to the other two alternative methods. An analysis has been performed to explain why Lundgren’s physical space linear forcing results in an integral length scale which is, independent of the Reynolds number, a constant fraction of the domain size. Furthermore, an evolution equation for the integral length scale has been derived, and a scaling analysis of its terms has been performed to explain the evolution of the integral length scale in the context of Lundgren’s physical space linear forcing. Finally, a modification to Lundgren’s forcing approach has been suggested which ensures that the integral length scale settles to a predetermined value so that DNS of statistically planar turbulent premixed flames with physical space forcing can be conducted for prescribed values of Damköhler and Karlovitz numbers. Turbulent premixed combustion Statistically planar flame Turbulent forcing Turbulent inflow Chakraborty, Nilanjan aut Ketterl, Sebastian aut Enthalten in Flow, turbulence and combustion Springer Netherlands, 1998 99(2017), 3-4 vom: 11. Aug., Seite 955-971 (DE-627)254303641 (DE-600)1463163-5 (DE-576)074754068 1386-6184 nnns volume:99 year:2017 number:3-4 day:11 month:08 pages:955-971 https://doi.org/10.1007/s10494-017-9843-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OLC-CHE GBV_ILN_11 GBV_ILN_70 GBV_ILN_2014 GBV_ILN_4323 GBV_ILN_4700 50.34$jGasdynamik$jAerodynamik VZ 106419498 (DE-625)106419498 52.51$jFeuerungstechnik VZ 106419935 (DE-625)106419935 AR 99 2017 3-4 11 08 955-971 |
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10.1007/s10494-017-9843-9 doi (DE-627)OLC205957692X (DE-He213)s10494-017-9843-9-p DE-627 ger DE-627 rakwb eng 500 600 VZ 50.34$jGasdynamik$jAerodynamik bkl 52.51$jFeuerungstechnik bkl Klein, Markus verfasserin aut A Comparison of Strategies for Direct Numerical Simulation of Turbulence Chemistry Interaction in Generic Planar Turbulent Premixed Flames 2017 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media B.V. 2017 Abstract Three different methods to introduce turbulence in the computational domain of Direct Numerical Simulations (DNS) of statistically planar turbulent premixed flame configurations have been reviewed and their advantages and disadvantages in terms of run time, natural flame development, control of turbulence parameters and convergence of statistics extracted from the simulations have been discussed in detail. It has been found that there is no method, which is clearly superior to the other two alternative methods. An analysis has been performed to explain why Lundgren’s physical space linear forcing results in an integral length scale which is, independent of the Reynolds number, a constant fraction of the domain size. Furthermore, an evolution equation for the integral length scale has been derived, and a scaling analysis of its terms has been performed to explain the evolution of the integral length scale in the context of Lundgren’s physical space linear forcing. Finally, a modification to Lundgren’s forcing approach has been suggested which ensures that the integral length scale settles to a predetermined value so that DNS of statistically planar turbulent premixed flames with physical space forcing can be conducted for prescribed values of Damköhler and Karlovitz numbers. Turbulent premixed combustion Statistically planar flame Turbulent forcing Turbulent inflow Chakraborty, Nilanjan aut Ketterl, Sebastian aut Enthalten in Flow, turbulence and combustion Springer Netherlands, 1998 99(2017), 3-4 vom: 11. Aug., Seite 955-971 (DE-627)254303641 (DE-600)1463163-5 (DE-576)074754068 1386-6184 nnns volume:99 year:2017 number:3-4 day:11 month:08 pages:955-971 https://doi.org/10.1007/s10494-017-9843-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OLC-CHE GBV_ILN_11 GBV_ILN_70 GBV_ILN_2014 GBV_ILN_4323 GBV_ILN_4700 50.34$jGasdynamik$jAerodynamik VZ 106419498 (DE-625)106419498 52.51$jFeuerungstechnik VZ 106419935 (DE-625)106419935 AR 99 2017 3-4 11 08 955-971 |
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10.1007/s10494-017-9843-9 doi (DE-627)OLC205957692X (DE-He213)s10494-017-9843-9-p DE-627 ger DE-627 rakwb eng 500 600 VZ 50.34$jGasdynamik$jAerodynamik bkl 52.51$jFeuerungstechnik bkl Klein, Markus verfasserin aut A Comparison of Strategies for Direct Numerical Simulation of Turbulence Chemistry Interaction in Generic Planar Turbulent Premixed Flames 2017 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media B.V. 2017 Abstract Three different methods to introduce turbulence in the computational domain of Direct Numerical Simulations (DNS) of statistically planar turbulent premixed flame configurations have been reviewed and their advantages and disadvantages in terms of run time, natural flame development, control of turbulence parameters and convergence of statistics extracted from the simulations have been discussed in detail. It has been found that there is no method, which is clearly superior to the other two alternative methods. An analysis has been performed to explain why Lundgren’s physical space linear forcing results in an integral length scale which is, independent of the Reynolds number, a constant fraction of the domain size. Furthermore, an evolution equation for the integral length scale has been derived, and a scaling analysis of its terms has been performed to explain the evolution of the integral length scale in the context of Lundgren’s physical space linear forcing. Finally, a modification to Lundgren’s forcing approach has been suggested which ensures that the integral length scale settles to a predetermined value so that DNS of statistically planar turbulent premixed flames with physical space forcing can be conducted for prescribed values of Damköhler and Karlovitz numbers. Turbulent premixed combustion Statistically planar flame Turbulent forcing Turbulent inflow Chakraborty, Nilanjan aut Ketterl, Sebastian aut Enthalten in Flow, turbulence and combustion Springer Netherlands, 1998 99(2017), 3-4 vom: 11. Aug., Seite 955-971 (DE-627)254303641 (DE-600)1463163-5 (DE-576)074754068 1386-6184 nnns volume:99 year:2017 number:3-4 day:11 month:08 pages:955-971 https://doi.org/10.1007/s10494-017-9843-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OLC-CHE GBV_ILN_11 GBV_ILN_70 GBV_ILN_2014 GBV_ILN_4323 GBV_ILN_4700 50.34$jGasdynamik$jAerodynamik VZ 106419498 (DE-625)106419498 52.51$jFeuerungstechnik VZ 106419935 (DE-625)106419935 AR 99 2017 3-4 11 08 955-971 |
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10.1007/s10494-017-9843-9 doi (DE-627)OLC205957692X (DE-He213)s10494-017-9843-9-p DE-627 ger DE-627 rakwb eng 500 600 VZ 50.34$jGasdynamik$jAerodynamik bkl 52.51$jFeuerungstechnik bkl Klein, Markus verfasserin aut A Comparison of Strategies for Direct Numerical Simulation of Turbulence Chemistry Interaction in Generic Planar Turbulent Premixed Flames 2017 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media B.V. 2017 Abstract Three different methods to introduce turbulence in the computational domain of Direct Numerical Simulations (DNS) of statistically planar turbulent premixed flame configurations have been reviewed and their advantages and disadvantages in terms of run time, natural flame development, control of turbulence parameters and convergence of statistics extracted from the simulations have been discussed in detail. It has been found that there is no method, which is clearly superior to the other two alternative methods. An analysis has been performed to explain why Lundgren’s physical space linear forcing results in an integral length scale which is, independent of the Reynolds number, a constant fraction of the domain size. Furthermore, an evolution equation for the integral length scale has been derived, and a scaling analysis of its terms has been performed to explain the evolution of the integral length scale in the context of Lundgren’s physical space linear forcing. Finally, a modification to Lundgren’s forcing approach has been suggested which ensures that the integral length scale settles to a predetermined value so that DNS of statistically planar turbulent premixed flames with physical space forcing can be conducted for prescribed values of Damköhler and Karlovitz numbers. Turbulent premixed combustion Statistically planar flame Turbulent forcing Turbulent inflow Chakraborty, Nilanjan aut Ketterl, Sebastian aut Enthalten in Flow, turbulence and combustion Springer Netherlands, 1998 99(2017), 3-4 vom: 11. Aug., Seite 955-971 (DE-627)254303641 (DE-600)1463163-5 (DE-576)074754068 1386-6184 nnns volume:99 year:2017 number:3-4 day:11 month:08 pages:955-971 https://doi.org/10.1007/s10494-017-9843-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OLC-CHE GBV_ILN_11 GBV_ILN_70 GBV_ILN_2014 GBV_ILN_4323 GBV_ILN_4700 50.34$jGasdynamik$jAerodynamik VZ 106419498 (DE-625)106419498 52.51$jFeuerungstechnik VZ 106419935 (DE-625)106419935 AR 99 2017 3-4 11 08 955-971 |
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ddc 500 bkl 50.34$jGasdynamik$jAerodynamik bkl 52.51$jFeuerungstechnik misc Turbulent premixed combustion misc Statistically planar flame misc Turbulent forcing misc Turbulent inflow |
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A Comparison of Strategies for Direct Numerical Simulation of Turbulence Chemistry Interaction in Generic Planar Turbulent Premixed Flames |
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A Comparison of Strategies for Direct Numerical Simulation of Turbulence Chemistry Interaction in Generic Planar Turbulent Premixed Flames |
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a comparison of strategies for direct numerical simulation of turbulence chemistry interaction in generic planar turbulent premixed flames |
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A Comparison of Strategies for Direct Numerical Simulation of Turbulence Chemistry Interaction in Generic Planar Turbulent Premixed Flames |
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Abstract Three different methods to introduce turbulence in the computational domain of Direct Numerical Simulations (DNS) of statistically planar turbulent premixed flame configurations have been reviewed and their advantages and disadvantages in terms of run time, natural flame development, control of turbulence parameters and convergence of statistics extracted from the simulations have been discussed in detail. It has been found that there is no method, which is clearly superior to the other two alternative methods. An analysis has been performed to explain why Lundgren’s physical space linear forcing results in an integral length scale which is, independent of the Reynolds number, a constant fraction of the domain size. Furthermore, an evolution equation for the integral length scale has been derived, and a scaling analysis of its terms has been performed to explain the evolution of the integral length scale in the context of Lundgren’s physical space linear forcing. Finally, a modification to Lundgren’s forcing approach has been suggested which ensures that the integral length scale settles to a predetermined value so that DNS of statistically planar turbulent premixed flames with physical space forcing can be conducted for prescribed values of Damköhler and Karlovitz numbers. © Springer Science+Business Media B.V. 2017 |
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Abstract Three different methods to introduce turbulence in the computational domain of Direct Numerical Simulations (DNS) of statistically planar turbulent premixed flame configurations have been reviewed and their advantages and disadvantages in terms of run time, natural flame development, control of turbulence parameters and convergence of statistics extracted from the simulations have been discussed in detail. It has been found that there is no method, which is clearly superior to the other two alternative methods. An analysis has been performed to explain why Lundgren’s physical space linear forcing results in an integral length scale which is, independent of the Reynolds number, a constant fraction of the domain size. Furthermore, an evolution equation for the integral length scale has been derived, and a scaling analysis of its terms has been performed to explain the evolution of the integral length scale in the context of Lundgren’s physical space linear forcing. Finally, a modification to Lundgren’s forcing approach has been suggested which ensures that the integral length scale settles to a predetermined value so that DNS of statistically planar turbulent premixed flames with physical space forcing can be conducted for prescribed values of Damköhler and Karlovitz numbers. © Springer Science+Business Media B.V. 2017 |
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Abstract Three different methods to introduce turbulence in the computational domain of Direct Numerical Simulations (DNS) of statistically planar turbulent premixed flame configurations have been reviewed and their advantages and disadvantages in terms of run time, natural flame development, control of turbulence parameters and convergence of statistics extracted from the simulations have been discussed in detail. It has been found that there is no method, which is clearly superior to the other two alternative methods. An analysis has been performed to explain why Lundgren’s physical space linear forcing results in an integral length scale which is, independent of the Reynolds number, a constant fraction of the domain size. Furthermore, an evolution equation for the integral length scale has been derived, and a scaling analysis of its terms has been performed to explain the evolution of the integral length scale in the context of Lundgren’s physical space linear forcing. Finally, a modification to Lundgren’s forcing approach has been suggested which ensures that the integral length scale settles to a predetermined value so that DNS of statistically planar turbulent premixed flames with physical space forcing can be conducted for prescribed values of Damköhler and Karlovitz numbers. © Springer Science+Business Media B.V. 2017 |
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A Comparison of Strategies for Direct Numerical Simulation of Turbulence Chemistry Interaction in Generic Planar Turbulent Premixed Flames |
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