4 research outputs found
Experimental and Modeling Investigation of the Low-Temperature Oxidation of Dimethyl Ether
The
oxidation of dimethyl ether (DME) was studied using a jet-stirred
reactor over a wide range of conditions: temperatures from 500 to
1100 K; equivalence ratios of 0.25, 1, and 2; residence time of 2
s; pressure of 106.7 kPa (close to the atmospheric pressure); and
an inlet fuel mole fraction of 0.02 (with high dilution in helium).
Reaction products were quantified using two analysis methods: gas
chromatography and continuous wave cavity ring-down spectroscopy (cw-CRDS).
cw-CRDS enabled the quantification of formaldehyde, which is one of
the major products from DME oxidation, as well as that of hydrogen
peroxide, which is an important branching agent in low-temperature
oxidation chemistry. Experimental data were compared with data computed
using models from the literature with important deviations being observed
for the reactivity at low-temperature. A new detailed kinetic model
for the oxidation of DME was developed in this study. Kinetic parameters
used in this model were taken from literature or calculated in the
present work using quantum calculations. This new model enables a
better prediction of the reactivity in the low-temperature region.
Under the present JSR conditions, error bars on predictions were given.
Simulations were also successfully compared with experimental flow
reactor, jet-stirred reactor, shock tube, rapid compression machine,
and flame data from literature. The kinetic analysis of the model
enabled the highlighting of some specificities of the oxidation chemistry
of DME: (1) the early reactivity which is observed at very low-temperature
(e.g., compared to propane) is explained by the absence of inhibiting
reaction of the radical directly obtained from the fuel (by H atom
abstraction) with oxygen yielding an olefin + HO<sub>2</sub>·;
(2) the low-temperature reactivity is driven by the relative importance
of the second addition to O<sub>2</sub> (promoting the reactivity
through branching chain) and the competitive decomposition reactions
with an inhibiting effect
Hydroperoxide Measurements During Low-Temperature Gas-Phase Oxidation of <i>n-</i>Heptane and <i>n-</i>Decane
A wide range of hydroperoxides
(C<sub>1</sub>–C<sub>3</sub> alkyl hydroperoxides, C<sub>3</sub>–C<sub>7</sub> alkenyl
hydroperoxides, C<sub>7</sub> ketohydroperoxides, and hydrogen peroxide
(H<sub>2</sub>O<sub>2</sub>)), as well as ketene and diones, have
been quantified during the gas-phase oxidation of <i>n-</i>heptane. Some of these species, as well as C<sub>10</sub> alkenyl
hydroperoxides and ketohydroperoxides, were also measured during the
oxidation of <i>n-</i>decane. These experiments were performed
using an atmospheric-pressure jet-stirred reactor at temperatures
from 500 to 1100 K and one of three analytical methods, time-of-flight
mass spectrometry combined with tunable synchrotron photoionization
with a molecular beam sampling: time-of-flight mass spectrometry combined
with laser photoionization with a capillary tube sampling, continuous
wave cavity ring-down spectroscopy with sonic probe sampling. The
experimental temperature at which the maximum mole fraction is observed
increases significantly for alkyl hydroperoxides, alkenyl hydroperoxides,
and then more so again for hydrogen peroxide, compared to ketohydroperoxides.
The influence of the equivalence ratio from 0.25 to 4 on the formation
of these peroxides has been studied during <i>n-</i>heptane
oxidation. The up-to-date detailed kinetic oxidation models for <i>n-</i>heptane and for <i>n-</i>decane found in the
literature have been used to discuss the possible pathways by which
these peroxides, ketene, and diones are formed. In general, the model
predicts well the reactivity of the two fuels, as well as the formation
of major intermediates
Products from the Oxidation of Linear Isomers of Hexene
The experimental study of the oxidation
of the three linear isomers
of hexene was performed in a quartz isothermal jet-stirred reactor
(JSR) at temperatures ranging from 500 to 1100 K including the negative
temperature coefficient (NTC) zone, at quasi-atmospheric pressure
(1.07 bar), at a residence time of 2 s and with dilute stoichiometric
mixtures. The fuel and reaction product mole fractions were measured
using online gas chromatography. In the case of 1-hexene, the JSR
has also been coupled through a molecular-beam sampling system to
a reflectron time-of-flight mass spectrometer combined with tunable
synchrotron vacuum ultraviolet photoionization. A difference of reactivity
between the three fuels, which varies with the temperature range has
been observed and is discussed according to the changes in the possible
reaction pathways when the double bond is displaced. An enhanced importance
of the reactions via the Waddington mechanism and of those of allylic
radicals with HO<sub>2</sub> radicals can be noted for 2- and 3-hexenes
compared to 1-hexene
Elliptical micropillars for efficient generation and detection of coherent acoustic phonons
Coherent acoustic phonon generation and detection assisted by optical resonances are at the core of efficient optophononic transduction processes. However, when dealing with a single optical resonance, the optimum generation and detection conditions take place at different laser wavelengths, i.e. different detunings from the cavity mode. In this work, we theoretically propose and experimentally demonstrate the use of elliptical micropillars to reach these conditions simultaneously at a single wavelength. Elliptical micropillar optophononic resonators present two optical modes with orthogonal polarizations at different wavelengths. By employing a cross-polarized scheme pump-probe experiment, we exploit the mode splitting and couple the pump beam to one mode while the probe is detuned from the other one. In this way, at a particular micropillar ellipticity, both phonon generation and detection processes are enhanced. We report an enhancement of a factor of ~3.1 when comparing the signals from elliptical and circular micropillars. Our findings constitute a step forward in tailoring the light-matter interaction for more efficient ultrahigh-frequency optophononic devices