@Article{SeverinoDoniFach:2021:TrOnSt,
author = "Severino, Matheus de P{\'a}dua and Donini, Mariovane Sabino and
Fachini Filho, Fernando",
affiliation = "{Instituto Nacional de Pesquisas Espaciais (INPE)} and {Instituto
Nacional de Pesquisas Espaciais (INPE)} and {Instituto Nacional de
Pesquisas Espaciais (INPE)}",
title = "Dynamics of diffusion flames in a very low strain rate flow field:
from transient one-dimensional to stationary two-dimensional
regime",
journal = "Combustion Theory and Modeling",
year = "2021",
volume = "25",
number = "5",
pages = "861--888",
month = "July",
keywords = "diffusion flamediffusion flame dynamicsdouble Tsuji flameflame
with continuous geometric variation1D transient flame to 2D
stationary flame.",
abstract = "The present work describes the transition of transient
one-dimensional diffusion flame into a steady two-dimensional
regime in a new flow field configuration. To that end, a
cylindrical burner from which fuel is ejected radially and
uniformly is positioned in the middle of two impinging flows. The
chosen conditions are such that the strain rate is very low. The
majority of the flame is located in a region of the flow field
where spatial coordinates are scaled with the reciprocal of the
square root of the strain rate, and the velocities are scaled with
the square root of the strain rate. To simplify the model, a
potential flow is assumed, with its results compared with those
from a more detailed incompressible Navier-Stokes flow solution.
The evolution of the flame is similar in both cases, which shows
that the idealised potential flow describes well the flow field in
such a geometry. Mixture fraction and excess enthalpy variables
are employed to describe the infinitely fast chemical reaction,
and therefore, fuel mass fraction, oxidiser mass fraction, and
temperature fields. Results show that the initial flame
displacement is controlled by the radial transport of fuel near
the burner, where the impinging flows have a negligible influence.
After that region, the flame is strongly influenced by the
impinging flows where its acceleration is observed. Moreover, the
proposed asymptotic solutions highlight the main transport
mechanisms of reactants to the flame under different conditions
and show the dependence of the flame on the chemical and flow
field parameters. The stationary solution presents a diffusion
flame with continuous geometric variation, from the counterflow to
the coflow regime.",
doi = "10.1080/13647830.2021.1957155",
url = "http://dx.doi.org/10.1080/13647830.2021.1957155",
issn = "1364-7830",
language = "en",
targetfile = "severino_dynamics.pdf",
urlaccessdate = "11 jun. 2024"
}