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Direct numerical simulations of premixed and stratified flame propagation in turbulent channel flow

Direct numerical simulations of premixed and stratified flame propagation in turbulent channel flow
Direct numerical simulations of premixed and stratified flame propagation in turbulent channel flow
Direct numerical simulations are performed to investigate the transient upstream flame propagation (flashback) through homogeneous and fuel-stratified hydrogen-air mixtures transported in fully-developed turbulent channel flows. Results indicate that, for both cases, the flame maintains steady propagation against the bulk flow direction and the global flame shape and the local flame characteristics are both affected by the occurrence of fuel stratification. Globally, the mean flame shape undergoes an abrupt change when the approaching reactants transition from an homogeneous to a stratified mixing configuration. A V-shaped flame surface, whose leading-edge is located in the near-wall region, characterizes the non-stratified, homogeneous mixture case while a U-shaped flame surface, whose leading-edge propagates upstream at the channel centreline, distinguishes the case with fuel stratification (fuel-lean in the near-wall region and fuel-rich away from the wall). The characteristic thickness, wrinkling and displacement speed of the turbulent flame brush are subject to considerable changes across the channel due to the dependence of the turbulence and mixture properties on the distance from the channel walls. More specifically, the flame transitions from a moderately wrinkled, thin-flamelet combustion regime in the homogeneous mixture case to a strongly wrinkled flame brush more representative of a thickened-flame combustion regime in the near-wall region of the fuel-stratified case. The combustion regime may be related to Karlovitz number and it is shown that a nominal channel-flow Karlovitz number, Kachin, based on the wallnormal variation of canonical turbulence (tη = (ν/ε) 1/2) and chemistry (tl = δl/Sl) time scales in fully-developed channel flow, compares well with an effective Karlovitz number, Kachfl, extracted from the present DNS datasets using conditionally sampled values of tη and tl in the immediate vicinity of the flame (0.1 < C < 0.3).
2469-990X
Gruber, Andrea
e2c365ab-5e1b-4af1-a2f8-05063688f850
Richardson, Edward
a8357516-e871-40d8-8a53-de7847aa2d08
Aditya, Konduri
91c79e9c-3395-4220-a16f-b743ca4ff5da
Chen, Jacqueline
67d089d6-0639-4175-b3cd-3697f4acec30
Gruber, Andrea
e2c365ab-5e1b-4af1-a2f8-05063688f850
Richardson, Edward
a8357516-e871-40d8-8a53-de7847aa2d08
Aditya, Konduri
91c79e9c-3395-4220-a16f-b743ca4ff5da
Chen, Jacqueline
67d089d6-0639-4175-b3cd-3697f4acec30

Gruber, Andrea, Richardson, Edward, Aditya, Konduri and Chen, Jacqueline (2018) Direct numerical simulations of premixed and stratified flame propagation in turbulent channel flow. Physical Review Fluids, 3 (11), [110507]. (doi:10.1103/PhysRevFluids.3.110507).

Record type: Article

Abstract

Direct numerical simulations are performed to investigate the transient upstream flame propagation (flashback) through homogeneous and fuel-stratified hydrogen-air mixtures transported in fully-developed turbulent channel flows. Results indicate that, for both cases, the flame maintains steady propagation against the bulk flow direction and the global flame shape and the local flame characteristics are both affected by the occurrence of fuel stratification. Globally, the mean flame shape undergoes an abrupt change when the approaching reactants transition from an homogeneous to a stratified mixing configuration. A V-shaped flame surface, whose leading-edge is located in the near-wall region, characterizes the non-stratified, homogeneous mixture case while a U-shaped flame surface, whose leading-edge propagates upstream at the channel centreline, distinguishes the case with fuel stratification (fuel-lean in the near-wall region and fuel-rich away from the wall). The characteristic thickness, wrinkling and displacement speed of the turbulent flame brush are subject to considerable changes across the channel due to the dependence of the turbulence and mixture properties on the distance from the channel walls. More specifically, the flame transitions from a moderately wrinkled, thin-flamelet combustion regime in the homogeneous mixture case to a strongly wrinkled flame brush more representative of a thickened-flame combustion regime in the near-wall region of the fuel-stratified case. The combustion regime may be related to Karlovitz number and it is shown that a nominal channel-flow Karlovitz number, Kachin, based on the wallnormal variation of canonical turbulence (tη = (ν/ε) 1/2) and chemistry (tl = δl/Sl) time scales in fully-developed channel flow, compares well with an effective Karlovitz number, Kachfl, extracted from the present DNS datasets using conditionally sampled values of tη and tl in the immediate vicinity of the flame (0.1 < C < 0.3).

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Direct numerical simulations of premixed - Accepted Manuscript
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Accepted/In Press date: 12 October 2018
e-pub ahead of print date: 21 November 2018

Identifiers

Local EPrints ID: 425446
URI: http://eprints.soton.ac.uk/id/eprint/425446
ISSN: 2469-990X
PURE UUID: bb65f51f-d3f9-449e-853e-89051a8334fb
ORCID for Edward Richardson: ORCID iD orcid.org/0000-0002-7631-0377

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Date deposited: 19 Oct 2018 16:30
Last modified: 16 Mar 2024 04:05

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Contributors

Author: Andrea Gruber
Author: Konduri Aditya
Author: Jacqueline Chen

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