Influence of equivalence ratio and hydrogen addition on thermoacoustic instabilities in premixed methane and propane flames in vertical tubes

This research examines the behavior of premixed flames within a vertical tube, considering both an open and a closed end configuration. The study utilizes a pilot flame as the ignition source. The methane (CH4) and propane (C3H8) flames were tested at equivalence ratios (ϕ) ranging from 0.9 to 1.2 a...

詳細記述

書誌詳細
出版年:Case Studies in Thermal Engineering
主要な著者: Abdullah M.A. Alsharif, Robert Woolley
フォーマット: 論文
言語:英語
出版事項: Elsevier 2025-05-01
主題:
オンライン・アクセス:http://www.sciencedirect.com/science/article/pii/S2214157X25002953
_version_ 1849469872707207168
author Abdullah M.A. Alsharif
Robert Woolley
author_facet Abdullah M.A. Alsharif
Robert Woolley
author_sort Abdullah M.A. Alsharif
collection DOAJ
container_title Case Studies in Thermal Engineering
description This research examines the behavior of premixed flames within a vertical tube, considering both an open and a closed end configuration. The study utilizes a pilot flame as the ignition source. The methane (CH4) and propane (C3H8) flames were tested at equivalence ratios (ϕ) ranging from 0.9 to 1.2 and constant hydrogen content at (RH = 0.1). High-speed cameras captured the flame propagation, revealing that several mechanisms, including pressure and velocity, influenced the flame shape and propagation rate. Increasing equivalence ratios initially raised laminar burning velocity, peaking at ϕ = 1.1, before decreasing. For C3H8, flames with lower burning velocity exhibited higher underlying flame speeds and maximum pressures alongside larger flame surface areas. It suggests that velocity coupling is the primary mechanism causing acoustic instability in flames that propagate downward. CH4 flames achieve maximum burning speed at a mixture ratio of ϕ = 1.1. Notably, the peak pressure and underlying speed remain constant. A comparative analysis of CH4 and C3H8 flames utilizing the RH method showed a distinctive correlation in behavior. Moreover, a comprehensive summary of CH4 and C3H8 flame behaviors is included, with (RH = 0–0.4) and (ϕ = 0.8–1.5).
format Article
id doaj-art-05967448b0524c049ef05264c07a7c3d
institution Directory of Open Access Journals
issn 2214-157X
language English
publishDate 2025-05-01
publisher Elsevier
record_format Article
spelling doaj-art-05967448b0524c049ef05264c07a7c3d2025-08-20T03:18:20ZengElsevierCase Studies in Thermal Engineering2214-157X2025-05-016910603510.1016/j.csite.2025.106035Influence of equivalence ratio and hydrogen addition on thermoacoustic instabilities in premixed methane and propane flames in vertical tubesAbdullah M.A. Alsharif0Robert Woolley1Department of Mechanical Engineering, College of Engineering at Yanbu, Taibah University, Yanbu Al-Bahr, 41911, Saudi Arabia; Corresponding author.Department of Mechanical Engineering, University of Sheffield, Sir Frederick Mappin Building, Mappin Street, Sheffield, S1 3JD, South Yorkshire, United KingdomThis research examines the behavior of premixed flames within a vertical tube, considering both an open and a closed end configuration. The study utilizes a pilot flame as the ignition source. The methane (CH4) and propane (C3H8) flames were tested at equivalence ratios (ϕ) ranging from 0.9 to 1.2 and constant hydrogen content at (RH = 0.1). High-speed cameras captured the flame propagation, revealing that several mechanisms, including pressure and velocity, influenced the flame shape and propagation rate. Increasing equivalence ratios initially raised laminar burning velocity, peaking at ϕ = 1.1, before decreasing. For C3H8, flames with lower burning velocity exhibited higher underlying flame speeds and maximum pressures alongside larger flame surface areas. It suggests that velocity coupling is the primary mechanism causing acoustic instability in flames that propagate downward. CH4 flames achieve maximum burning speed at a mixture ratio of ϕ = 1.1. Notably, the peak pressure and underlying speed remain constant. A comparative analysis of CH4 and C3H8 flames utilizing the RH method showed a distinctive correlation in behavior. Moreover, a comprehensive summary of CH4 and C3H8 flame behaviors is included, with (RH = 0–0.4) and (ϕ = 0.8–1.5).http://www.sciencedirect.com/science/article/pii/S2214157X25002953MethanePropaneHydrogen additionEquivalence ratioThermoacoustic
spellingShingle Abdullah M.A. Alsharif
Robert Woolley
Influence of equivalence ratio and hydrogen addition on thermoacoustic instabilities in premixed methane and propane flames in vertical tubes
Methane
Propane
Hydrogen addition
Equivalence ratio
Thermoacoustic
title Influence of equivalence ratio and hydrogen addition on thermoacoustic instabilities in premixed methane and propane flames in vertical tubes
title_full Influence of equivalence ratio and hydrogen addition on thermoacoustic instabilities in premixed methane and propane flames in vertical tubes
title_fullStr Influence of equivalence ratio and hydrogen addition on thermoacoustic instabilities in premixed methane and propane flames in vertical tubes
title_full_unstemmed Influence of equivalence ratio and hydrogen addition on thermoacoustic instabilities in premixed methane and propane flames in vertical tubes
title_short Influence of equivalence ratio and hydrogen addition on thermoacoustic instabilities in premixed methane and propane flames in vertical tubes
title_sort influence of equivalence ratio and hydrogen addition on thermoacoustic instabilities in premixed methane and propane flames in vertical tubes
topic Methane
Propane
Hydrogen addition
Equivalence ratio
Thermoacoustic
url http://www.sciencedirect.com/science/article/pii/S2214157X25002953
work_keys_str_mv AT abdullahmaalsharif influenceofequivalenceratioandhydrogenadditiononthermoacousticinstabilitiesinpremixedmethaneandpropaneflamesinverticaltubes
AT robertwoolley influenceofequivalenceratioandhydrogenadditiononthermoacousticinstabilitiesinpremixedmethaneandpropaneflamesinverticaltubes