5 research outputs found
Theoretical Investigation of the Reactivity of Sodium Dicyanamide with Nitric Acid
There
is a need to replace current hydrazine fuels with safer propellants,
and dicyanamide (DCA<sup>–</sup>)-based systems have emerged
as promising alternatives because they autoignite when mixed with
some oxidizers. Previous studies of the hypergolic reaction mechanism
have focused on the reaction between DCA<sup>–</sup> and the
oxidizer HNO<sub>3</sub>; here, we compare the calculated pathway
of DCA<sup>–</sup> + HNO<sub>3</sub> with the reaction coordinate
of the ion pair sodium dicyanamide with nitric acid, NaÂ[DCA] + HNO<sub>3</sub>. Enthalpies and free energies are calculated in the gas phase
and in solution using a quantum mechanical continuum solvation model,
SMD-GIL. The barriers to the NaÂ[DCA] + HNO<sub>3</sub> reaction are
dramatically lowered relative to those of the reaction with the bare
anion, and an exothermic exit channel to produce NaNO<sub>3</sub> and
the reactive intermediate HDCA appears. These results suggest that
NaÂ[DCA] may accelerate the ignition reaction
Shock Tube Investigation of CH<sub>3</sub> + CH<sub>3</sub>OCH<sub>3</sub>
The title reaction has been investigated in a diaphragmless
shock
tube by laser schlieren densitometry over the temperature range 1163–1629
K and pressures of 60, 120, and 240 Torr. Methyl radicals were produced
by dissociation of 2,3-butanedione in the presence of an excess of
dimethyl ether. Rate coefficients for CH<sub>3</sub> + CH<sub>3</sub>OCH<sub>3</sub> were obtained from simulations of the experimental
data yielding the following expression which is valid over the range
1100–1700 K: <i>k</i> = (10.19 ± 3.0)<i>T</i><sup>3.78</sup> exp<sup>(−4878/T)</sup> cm<sup>3</sup> mol<sup>–1</sup>s<sup>–1</sup>. The experimental
results are in good agreement with estimates by Curran and co-workers
[Fischer, S. L.; Dryer, F. L.; Curran, H. J. <i>Int. J. Chem.
Kinet.</i> <b>2000</b>, <i>32</i> (12), 713–740.
Curran, H. J.; Fischer, S. L.; Dryer, F. L. <i>Int. J. Chem.
Kinet.</i> <b>2000</b>, <i>32</i> (12), 741–759]
but about a factor of 2.6 lower than those of Zhao et al. [Zhao, Z.;
Chaos, M.; Kazakov, A.; Dryer, F. L. <i>Int. J. Chem. Kinet.</i> <b>2008</b>, <i>40</i> (1), 1–18]
Shock Tube Investigation of CH<sub>3</sub> + CH<sub>3</sub>OCH<sub>3</sub>
The title reaction has been investigated in a diaphragmless
shock
tube by laser schlieren densitometry over the temperature range 1163–1629
K and pressures of 60, 120, and 240 Torr. Methyl radicals were produced
by dissociation of 2,3-butanedione in the presence of an excess of
dimethyl ether. Rate coefficients for CH<sub>3</sub> + CH<sub>3</sub>OCH<sub>3</sub> were obtained from simulations of the experimental
data yielding the following expression which is valid over the range
1100–1700 K: <i>k</i> = (10.19 ± 3.0)<i>T</i><sup>3.78</sup> exp<sup>(−4878/T)</sup> cm<sup>3</sup> mol<sup>–1</sup>s<sup>–1</sup>. The experimental
results are in good agreement with estimates by Curran and co-workers
[Fischer, S. L.; Dryer, F. L.; Curran, H. J. <i>Int. J. Chem.
Kinet.</i> <b>2000</b>, <i>32</i> (12), 713–740.
Curran, H. J.; Fischer, S. L.; Dryer, F. L. <i>Int. J. Chem.
Kinet.</i> <b>2000</b>, <i>32</i> (12), 741–759]
but about a factor of 2.6 lower than those of Zhao et al. [Zhao, Z.;
Chaos, M.; Kazakov, A.; Dryer, F. L. <i>Int. J. Chem. Kinet.</i> <b>2008</b>, <i>40</i> (1), 1–18]
Shock Tube Investigation of CH<sub>3</sub> + CH<sub>3</sub>OCH<sub>3</sub>
The title reaction has been investigated in a diaphragmless
shock
tube by laser schlieren densitometry over the temperature range 1163–1629
K and pressures of 60, 120, and 240 Torr. Methyl radicals were produced
by dissociation of 2,3-butanedione in the presence of an excess of
dimethyl ether. Rate coefficients for CH<sub>3</sub> + CH<sub>3</sub>OCH<sub>3</sub> were obtained from simulations of the experimental
data yielding the following expression which is valid over the range
1100–1700 K: <i>k</i> = (10.19 ± 3.0)<i>T</i><sup>3.78</sup> exp<sup>(−4878/T)</sup> cm<sup>3</sup> mol<sup>–1</sup>s<sup>–1</sup>. The experimental
results are in good agreement with estimates by Curran and co-workers
[Fischer, S. L.; Dryer, F. L.; Curran, H. J. <i>Int. J. Chem.
Kinet.</i> <b>2000</b>, <i>32</i> (12), 713–740.
Curran, H. J.; Fischer, S. L.; Dryer, F. L. <i>Int. J. Chem.
Kinet.</i> <b>2000</b>, <i>32</i> (12), 741–759]
but about a factor of 2.6 lower than those of Zhao et al. [Zhao, Z.;
Chaos, M.; Kazakov, A.; Dryer, F. L. <i>Int. J. Chem. Kinet.</i> <b>2008</b>, <i>40</i> (1), 1–18]
Theoretical and Experimental Insights into the Dissociation of 2‑Hydroxyethylhydrazinium Nitrate Clusters Formed via Electrospray
Ionic
liquids are used for myriad applications, including as catalysts,
solvents, and propellants. Specifically, 2-hydroxyethylhydrazinium
nitrate (HEHN) has been developed as a chemical propellant for space
applications. The gas-phase behavior of HEHN ions and clusters is
important in understanding its potential as an electrospray thruster
propellant. Here, the unimolecular dissociation pathways of two clusters
are experimentally observed, and theoretical modeling of hydrogen
bonding and dissociation pathways is used to help rationalize those
observations. The cation/deprotonated cation cluster [HEH<sub>2</sub> – H]<sup>+</sup>, which is observed from electrospray ionization,
is calculated to be considerably more stable than the complementary
cation/protonated anion adduct, [HEH + HNO<sub>3</sub>]<sup>+</sup>, which is not observed experimentally. Upon collisional activation,
a larger cluster [(HEHN)<sub>2</sub>HEH]<sup>+</sup> undergoes dissociation
via loss of nitric acid at lower collision energies, as predicted
theoretically. At higher collision energies, additional primary and
secondary loss pathways open, including deprotonated cation loss,
ion-pair loss, and double-nitric-acid loss. Taken together, these
experimental and theoretical results contribute to a foundational
understanding of the dissociation of protic ionic liquid clusters
in the gas phase