The laminar and turbulent flame speed of methanol/ammonia/air, ethyl-acetate/ammonia/air, and dimethoxymethane/ammonia/air under atmospheric and elevated pressures

Experiments of the laminar and turbulent flame speed of typical E-fuels blended with ammonia: methanol/ammonia/(CH 3 OH/NH 3 )/air, ethyl-acetate/ammonia/(EA/NH 3 )/air, and dimethoxymethane/ammonia/(DMM/NH 3 )/air under atmospheric and elevated pressures (1 and 3 atm) are conducted in a fan-stirred constant volume combustion chamber , with initial temperature of 373 K. The results show that turbulent flame speed ( S T ) follow the same ranking order as laminar flame speed ( S L ) at fuel-lean side from high to low as: DMM, CH 3 OH, and EA; while with ammonia addition, CH 3 OH/NH 3 and EA/NH 3 have similar S L and S T values; and at fuel-rich side, DMM and EA show increasing S T and S T / S L values than at fuel-lean side Meanwhile, the measured Markstein length ( L b ) is decreasing towards the fuel-rich side and even becomes negative for EA. Ammonia addition enhances the turbulent flame wrinkling and deformation from the morphology analyses, and this leads to E-fuel/NH 3 blends always having higher normalized turbulent flame speed ( S T / S L ) than pure E-fuel. Next, we test several different turbulent flame speed correlations composed of ( u' / S L ) and ( l T / l F ), it is found that the power exponents of ( u' / S L ) and ( l T / l F ) do not necessarily have to be equal; they change as the turbulent regime varies in different zones. S T / S L / Ka = a ( Da / Le ) b performs best among all correlation types with 0.5 ≤ b ≤ 1 corresponding to the Damköhler's two limits. Comparing three types of Lewis number, it is found that volume based Le V has the best fitting goodness in the correlation of S T / S L / Ka = a ( Da / Le ) b . Taking into account the developing flame brush thickness, wrinkling ratio and integral length scale as a function of radius, the flame radius based Da R correlations are proposed: S T / S L / γ = a ( Da R / Le ) b where 0.5 ≤ b ≤ 1 which can unify present experimental data with Lewis number larger than unity and previous data with Lewis number less than unity.

Authors

Institutions

Publication Details

Journal
Combustion and Flame
Published
2025-04-18
DOI
https://doi.org/10.1016/j.combustflame.2025.114187
Citations
2
Primary Topic
Combustion and flame dynamics
Type
article
Field-Weighted Citation Impact
2.67

Funders

Controls
|||
ALL TIME
JAN
FEB
MAR
APR
MAY
JUN
JUL
AUG
SEP
OCT
article

The laminar and turbulent flame speed of methanol/ammonia/air, ethyl-acetate/ammonia/air, and dimethoxymethane/ammonia/air under atmospheric and elevated pressures

William L. Roberts, Ayman M. Elbaz, Zhihua Wang, Shixing Wang
2 citations
Combustion and Flame
Combustion and flame dynamics
2.67
article

The laminar and turbulent flame speed of methanol/ammonia/air, ethyl-acetate/ammonia/air, and dimethoxymethane/ammonia/air under atmospheric and elevated pressures

William L. Roberts, Ayman M. Elbaz, Zhihua Wang, Shixing Wang
article en
2 citations

Abstract

Experiments of the laminar and turbulent flame speed of typical E-fuels blended with ammonia: methanol/ammonia/(CH 3 OH/NH 3 )/air, ethyl-acetate/ammonia/(EA/NH 3 )/air, and dimethoxymethane/ammonia/(DMM/NH 3 )/air under atmospheric and elevated pressures (1 and 3 atm) are conducted in a fan-stirred constant volume combustion chamber , with initial temperature of 373 K. The results show that turbulent flame speed ( S T ) follow the same ranking order as laminar flame speed ( S L ) at fuel-lean side from high to low as: DMM, CH 3 OH, and EA; while with ammonia addition, CH 3 OH/NH 3 and EA/NH 3 have similar S L and S T values; and at fuel-rich side, DMM and EA show increasing S T and S T / S L values than at fuel-lean side Meanwhile, the measured Markstein length ( L b ) is decreasing towards the fuel-rich side and even becomes negative for EA. Ammonia addition enhances the turbulent flame wrinkling and deformation from the morphology analyses, and this leads to E-fuel/NH 3 blends always having higher normalized turbulent flame speed ( S T / S L ) than pure E-fuel. Next, we test several different turbulent flame speed correlations composed of ( u' / S L ) and ( l T / l F ), it is found that the power exponents of ( u' / S L ) and ( l T / l F ) do not necessarily have to be equal; they change as the turbulent regime varies in different zones. S T / S L / Ka = a ( Da / Le ) b performs best among all correlation types with 0.5 ≤ b ≤ 1 corresponding to the Damköhler's two limits. Comparing three types of Lewis number, it is found that volume based Le V has the best fitting goodness in the correlation of S T / S L / Ka = a ( Da / Le ) b . Taking into account the developing flame brush thickness, wrinkling ratio and integral length scale as a function of radius, the flame radius based Da R correlations are proposed: S T / S L / γ = a ( Da R / Le ) b where 0.5 ≤ b ≤ 1 which can unify present experimental data with Lewis number larger than unity and previous data with Lewis number less than unity.

Combustion and FlameVol. 277
Zhejiang Energy Group (China) (CN), King Abdullah University of Science and Technology (SA), Zhejiang University (CN)
King Abdullah University of Science and Technology, Key Technologies Research and Development Program, National Key Research and Development Program of China, Clean Combustion Research Center, King Abdullah University of Science and Technology
Openalex Percentile: Top 13%
Combustion and flame dynamics
2.67
AI Navigator

Ask Laika to Summarize, Analyze, and Connect papers live on the map.

Summarize Papers & Methodologies

Extract key findings, datasets, and comparative methods across publications.

Benchmark Rankings & Visual Analytics

Rank top research institutions, authors, funders, topics, and journals by Field-Weighted Citation Impact (FWCI) and paper volume with instant charts.

Connect Distant Disciplines

Bridge topological clusters on the map to find hidden collaborative intersections.