scholarly journals Thermodynamically Modeled Non-equilibrium Structure of Combustion Products and Decomposition of Hydrazine-based Liquid Propellants

2016 ◽  
Vol 16 (05) ◽  
Author(s):  
A Dorofeev ◽  
D Yagodnikov
Soft Matter ◽  
2021 ◽  
Author(s):  
Michael Bley ◽  
Joachim Dzubiella ◽  
Arturo Moncho Jorda

We employ reactive dynamical density functional theory (R-DDFT) and reactive Brownian dynamics (R-BD) simulations to study the non-equilibrium structure and phase behavior of an active dispersion of soft Gaussian colloids...


2007 ◽  
Vol 579 ◽  
pp. 173-226 ◽  
Author(s):  
B. ZALTZMAN ◽  
I. RUBINSTEIN

Electric conduction from an electrolyte solution into a charge selective solid, such as ion exchange membrane or electrode, becomes unstable when the electrolyte concentration near the interface approaches zero owing to diffusion limitation. The sequence of events leading to instability is as follows: upon the decrease of the interface concentration, the electric double layer at the interface transforms from its common quasi-equilibrium structure to a different, non-equilibrium one. The key feature of this new structure is an extended space charge added to the usual one of the quasi-equilibrium electric double layer. The non-equilibrium electro-osmotic slip related to this extended space charge renders the quiescent conductance unstable. A unified asymptotic picture of the electric double-layer undercurrent, encompassing all regimes from quasi-equilibrium to the extreme non-equilibrium one, is developed and employed for derivation of a universal electro-osmotic slip formula. This formula is used for a linear stability study of quiescent electric conduction, yielding the precise parameter range of instability, compared with that in the full electroconvective formulation. The physical mechanism of instability is traced both kinematically, in terms of non-equilibrium electro-osmotic slip, and dynamically, in terms of forces acting in the electric double layer.


Author(s):  
Daniel E. Martínez-Tong ◽  
Alejandro Sanz ◽  
Jaime Martín ◽  
Tiberio A. Ezquerra ◽  
Aurora Nogales

1971 ◽  
Vol 26 (7) ◽  
pp. 1147-1155 ◽  
Author(s):  
Cristiano Batalli-Cosmovici ◽  
Karl-Wolfgang Michel

AbstractThe emission spectrum from a two-phase nozzle jet, consisting of combustion products of Ba and CuO, revealed that non-equilibrium amounts of excited and ionized Ba atoms occur only during the nozzle starting transient. Traces of BaO-and Cu2-molecules could be identified in the cold outer parts of the jet. The particle temperature near the nozzle, derived from novel measurements of apparent color and brightness temperature, confirms LTE calculations if the vaporization of excess Ba is taken to be a fast process.


ChemPhysChem ◽  
2017 ◽  
Vol 18 (23) ◽  
pp. 3437-3442 ◽  
Author(s):  
Benedikt Buchmann ◽  
Fabian Manfred Hecht ◽  
Carla Pernpeintner ◽  
Theobald Lohmueller ◽  
Andreas R. Bausch

2015 ◽  
Vol 293 (9) ◽  
pp. 2555-2563 ◽  
Author(s):  
Lina Fukuhara ◽  
Kenichiro Kosugi ◽  
Yoshimasa Yamamoto ◽  
Hiroshi Jinnai ◽  
Hideo Nishioka ◽  
...  

1995 ◽  
Vol 73 (11) ◽  
pp. 1747-1756 ◽  
Author(s):  
Anthony J. Paine ◽  
Richard R. Shivers

The interior particle morphology of dispersion-polymerized polystyrene particles was investigated by freeze fracture TEM (FFTEM) in order to compare the morphology of particles formed under two extreme mechanistic conditions: (a) particle growth by scavenging of dead polymer chains formed in solution (which gives rise to large particles of 5–10 μm) and (b) particle growth by oligomeric radical capture and polymerization inside the particle (giving rise to small particles of 1 μm or less). Although not generally recognized in the literature, ascribing mechanistic significance to an observed morphology requires a demonstration that the morphology is of the non-equilibrium type, i.e., the morphology depends upon how the particle was formed. An equilibrium morphology, by definition, must be independent of the particle formation route, and therefore carries no mechanistic information. In this case, large PS particles of 6.5 μm were found to have a nodular morphology that was unchanged on heating well above Tg, indicating an equilibrium structure (the nodularity of amorphous polymers is briefly rationalized by comparison with literature results over the past 20 years). On the other hand, small PS particles of 1.3 μm had a pronounced radial structure that could be converted into the nodular morphology by the same heat treatment, or by dissolving and precipitating from a suitable solvent combination. This means that the small particles have a non-equilibrium morphology, from which we may attempt to draw mechanistic inferences consistent with the suspected growth mechanism. Keywords: dispersion-polymerized polystyrene, non-equilibrium polystyrene particle morphology, freeze fracture transmission electron microscopy.


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