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Title: A numerical study of the diffusive-thermal instability of opposed nonpremixed tubular flames

Abstract

The diffusive-thermal (D-T) instability of opposed nonpremixed tubular flames near extinction is investigated here using two-dimensional (2-D) direct numerical simulations together with the linear stability analysis. Two different initial conditions (IC), i.e. the perturbed IC and the C-shaped IC are adopted to elucidate the effects of small and large amplitude disturbances on the formation of flame cells, similar to conditions found in linear stability analysis and experiments, respectively. The characteristics of the D-T instability of tubular flames are identified by a critical Damköhler number, DaC, at which the D-T instability first occurs and the corresponding number of flame cells for three different tubular flames with different flame radii. It is found that DaC predicted through linear stability analysis shows good agreement with that obtained from the 2-D simulations performed with two different ICs. The flame cell number, Ncell, from the 2-D simulations with the perturbed IC is also found to be equal to an integer close to the maximum wavenumber, kmax, obtained from the linear stability analysis. However, Ncell from the 2-D simulations with the C-shaped IC is smaller than kmax and Ncell found from the simulations with the perturbed IC. This is primarily because the strong reaction at themore » edges of the horseshoe-shaped cellular flame developed from the C-shaped IC is more likely to produce larger flame cells and reduce Ncell. It is also found that for cases with the C-shaped IC, once the cellular instability occurs, the number of flame cells remains constant until global extinction occurs by incomplete reaction manifested by small Da. It is also verified through the displacement speed, Sd, analysis that the two edges of the horseshoe-shaped cellular flame are stationary and therefore do not merge due to the diffusion–reaction balance at the edges. Moreover, large negative Sd is observed at the local extinction points while small positive or negative Sd features in the movement of flame cells as they adjust their location and size towards steady state.« less

Authors:
 [1];  [2];  [3]; ORCiD logo [4]
  1. Ulsan National Inst. of Science and Technology (UNIST) (Korea, Republic of). Dept. of Mechanical Engineering
  2. Seoul National Univ. of Science and Technology (Korea, Republic of). Dept. of Mechanical and Automotive Engineering
  3. Sandia National Lab. (SNL-CA), Livermore, CA (United States). Combustion Research Facility
  4. Ulsan National Inst. of Science and Technology (UNIST) (Korea, Republic of). Dept. of Mechanical Engineering. School of Mechanical and Nuclear Engineering
Publication Date:
Research Org.:
Sandia National Lab. (SNL-CA), Livermore, CA (United States); Ulsan National Inst. of Science and Technology (UNIST) (Korea, Republic of)
Sponsoring Org.:
USDOE Office of Science (SC), Basic Energy Sciences (BES); National Research Foundation of Korea (NRF); Ministry of Science, ICT and Future Planning (MSIP) of Korea
OSTI Identifier:
1497641
Alternate Identifier(s):
OSTI ID: 1254880
Report Number(s):
SAND2015-10478J
Journal ID: ISSN 0010-2180; 672293
Grant/Contract Number:  
AC04-94AL85000; 2015M1A3A3A02027319; 2015R1A2A2A01007378
Resource Type:
Accepted Manuscript
Journal Name:
Combustion and Flame
Additional Journal Information:
Journal Volume: 162; Journal Issue: 12; Journal ID: ISSN 0010-2180
Publisher:
Elsevier
Country of Publication:
United States
Language:
English
Subject:
42 ENGINEERING; diffusive-thermal instability; nonpremixed tubular flame; hydrogen; linear stability analysis; displacement speed

Citation Formats

Bak, Hyun Su, Lee, Su Ryong, Chen, Jacqueline H., and Yoo, Chun Sang. A numerical study of the diffusive-thermal instability of opposed nonpremixed tubular flames. United States: N. p., 2015. Web. doi:10.1016/j.combustflame.2015.09.019.
Bak, Hyun Su, Lee, Su Ryong, Chen, Jacqueline H., & Yoo, Chun Sang. A numerical study of the diffusive-thermal instability of opposed nonpremixed tubular flames. United States. https://doi.org/10.1016/j.combustflame.2015.09.019
Bak, Hyun Su, Lee, Su Ryong, Chen, Jacqueline H., and Yoo, Chun Sang. Thu . "A numerical study of the diffusive-thermal instability of opposed nonpremixed tubular flames". United States. https://doi.org/10.1016/j.combustflame.2015.09.019. https://www.osti.gov/servlets/purl/1497641.
@article{osti_1497641,
title = {A numerical study of the diffusive-thermal instability of opposed nonpremixed tubular flames},
author = {Bak, Hyun Su and Lee, Su Ryong and Chen, Jacqueline H. and Yoo, Chun Sang},
abstractNote = {The diffusive-thermal (D-T) instability of opposed nonpremixed tubular flames near extinction is investigated here using two-dimensional (2-D) direct numerical simulations together with the linear stability analysis. Two different initial conditions (IC), i.e. the perturbed IC and the C-shaped IC are adopted to elucidate the effects of small and large amplitude disturbances on the formation of flame cells, similar to conditions found in linear stability analysis and experiments, respectively. The characteristics of the D-T instability of tubular flames are identified by a critical Damköhler number, DaC, at which the D-T instability first occurs and the corresponding number of flame cells for three different tubular flames with different flame radii. It is found that DaC predicted through linear stability analysis shows good agreement with that obtained from the 2-D simulations performed with two different ICs. The flame cell number, Ncell, from the 2-D simulations with the perturbed IC is also found to be equal to an integer close to the maximum wavenumber, kmax, obtained from the linear stability analysis. However, Ncell from the 2-D simulations with the C-shaped IC is smaller than kmax and Ncell found from the simulations with the perturbed IC. This is primarily because the strong reaction at the edges of the horseshoe-shaped cellular flame developed from the C-shaped IC is more likely to produce larger flame cells and reduce Ncell. It is also found that for cases with the C-shaped IC, once the cellular instability occurs, the number of flame cells remains constant until global extinction occurs by incomplete reaction manifested by small Da. It is also verified through the displacement speed, Sd, analysis that the two edges of the horseshoe-shaped cellular flame are stationary and therefore do not merge due to the diffusion–reaction balance at the edges. Moreover, large negative Sd is observed at the local extinction points while small positive or negative Sd features in the movement of flame cells as they adjust their location and size towards steady state.},
doi = {10.1016/j.combustflame.2015.09.019},
journal = {Combustion and Flame},
number = 12,
volume = 162,
place = {United States},
year = {Thu Oct 22 00:00:00 EDT 2015},
month = {Thu Oct 22 00:00:00 EDT 2015}
}

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Works referencing / citing this record:

Numerical investigation of non-premixed and premixed rotational tubular flame: a study of flame structure and instability
journal, December 2019

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