The control of the solid phase decomposition of silver azide by noncontact electric field

1997 ◽  
Vol 101-103 (1-2) ◽  
pp. 161-164
Author(s):  
V Zakharov
2017 ◽  
Vol 736 ◽  
pp. 101-104
Author(s):  
A.P. Rodzevich ◽  
L.V. Kuzmina ◽  
E.G. Gazenauer ◽  
V.I. Krasheninin ◽  
D.Yu. Sozinov ◽  
...  

The experiments have emphasized that additionally introduced impurities of Fe and Pb ions are relevant to the initiation of slow and explosive decomposition of silver azide crystals by the external electric field and UV irradiation. External gas release was used for research purpose. Test-sensitivity is 10−12 mole. Time-to-explosion was measured by a stop watch. It’s been found out that the reaction of slow decomposition in silver azide under the action of electric field turns into explosion faster in samples with the additionally introduced impurities. The samples with additionally introduced Fe are the most explosive ones (time-to-explosion 3 minutes). The authors have assumed that external influence can generate non-equilibrium charge carriers (holes), which become localized on cationic vacancies and support formation of reactive sites. As soon as cut off concentration of these sites is reached, the solid-phase chain reaction turns into explosion. The growing concentration of impurity influences on the number of reactive sites, making their concentration critical. In view of the results obtained in experiments a procedure for monitoring the decomposition of crystals is suggested, which necessitates additional introduction of Fe and Pb ions.


2019 ◽  
Vol 6 (2) ◽  
pp. 111-114
Author(s):  
R. Kornev ◽  
P. Sennikov ◽  
V. Nazarov ◽  
A. Kut'in ◽  
A. Plekhovich

A contracted RF (40.68 MHz) arc discharge of atmospheric pressure, stabilized between two rod electrodes, was used to obtain trichlorosilane by the reaction of hydrogen reduction of silicon tetrachloride (SiCl<sub>4</sub>). In model mixtures of macro-composition in the ratio H<sub>2</sub>/SiCl<sub>4</sub>/CCl<sub>4</sub>=10/1/1, it was shown that C and SiC are the main solid-phase product which are deposited on the surface of electrodes in the form of dendrides. The temperature of the ends of the electrodes determined using emission thermometry is 1600 K. The thermodynamic analysis of H<sub>2</sub>+SiCl<sub>4</sub>+CCl<sub>4</sub> system confirms that the formation of C and SiC occurs in the temperature range of 1600 K. The deposition of solid-phase products occurs on the electrodes in the zone of high electric field strength.


Materials ◽  
2003 ◽  
Author(s):  
Marcelo J. Colac¸o ◽  
George S. Dulikravich ◽  
Thomas J. Martin

This paper presents a numerical procedure to reduce and possibly control the natural convection effects in a cavity filled with a molten material by applying an external electric field whose intensity and spatial distributions are obtained by the use of a hybrid optimizer. This conceptually new approach to manufacturing could be used in creation of layered and functionally graded materials and objects. In the case of steady electro-hydrodynamics (EHD), the flow-field of electrically charged particles in a solidifying melt is influenced by an externally applied electric field while the existence of any magnetic field is neglected. Solidification front shape, distribution of the charged particles in the accrued solid, and the amount of accrued solid phase in such processes can be influenced by an appropriate distribution and orientation of the electric field. The intensities of the electrodes along the boundaries of the cavity were described using B-splines. The inverse problem was then formulated to find the electric boundary conditions (the coefficients of the B-splines) in such a way that the gradients of temperature along the horizontal direction are minimized. For this task we used a hybrid optimization algorithm which incorporates several of the most popular optimization modules; the Davidon-Fletcher-Powell (DFP) gradient method, a genetic algorithm (GA), the Nelder-Mead (NM) simplex method, quasi-Newton algorithm of Pshenichny-Danilin (LM), differential evolution (DE), and sequential quadratic programming (SQP). The transient Navier-Stokes and Maxwell equations were discretized using the finite volume method in a generalized curvilinear non-orthogonal coordinate system. For the phase change problems, we used the enthalpy method.


1982 ◽  
Vol 13 (31) ◽  
Author(s):  
S. A. EL-FEKEY ◽  
M. N. A. EL-HAKIM ◽  
N. H. ROFAIL ◽  
M. A. KHILLA

2001 ◽  
Vol 664 ◽  
Author(s):  
Marek A. T. Izmajlowicz ◽  
Neil A. Morrison ◽  
Andrew J. Flewitt ◽  
William I. Milne

ABSTRACTFor application to active matrix liquid crystal displays (AMLCDs), a low temperature (< 600 °C) process for the production of polycrystalline silicon is required to permit the use of inexpensive glass substrates. This would allow the integration of drive electronics onto the display panel. Current low temperature processes include excimer laser annealing, which requires expensive equipment, and solid phase crystallization, which requires high temperatures. It is known that by adding small amounts of metals such as nickel to the amorphous silicon the solid phase crystallization temperature can be significantly reduced. The rate of this solid phase metal induced crystallization is increased in the presence of an electric field. Previous work on field aided crystallization has reported crystal growth that either proceeds towards the positive terminal or is independent of the direction of the electric field. In this work, extensive investigation has consistently revealed directional crystallization, from the positive to the negative terminal, of amorphous silicon thin films during heat treatment in the presence of an electric field. This is the first time that this phenomenon has been reported. Models have been proposed for metal induced crystallization with and without an applied electric field in which a reaction between Ni and Si to produce NiSi is the rate-limiting step. The crystallization rate is increased in the presence of an electric field through the drift of positive Ni ions.


1999 ◽  
Vol 77 (11) ◽  
pp. 1899-1910 ◽  
Author(s):  
Glenn A Facey ◽  
Tina P Fong ◽  
Dmitry Gusev ◽  
Peter M Macdonald ◽  
Robert H Morris ◽  
...  

Variable temperature 2H NMR is used to measure the T1min values of the η2-D2 and D ligands in trans-[M(η2-D2)(D)(dppe)2]+, M = Ru (1) and Os (2) in solution. The rapid spinning motion of the η2-D2 ligand results in a much longer T1min than that of the terminal deuteride. The quadrupole coupling constant (CQ) for the terminal deuteride is calculated to be 79 kHz for 1 and 81 kHz for 2 while motion-reduced coupling constant (CQeff) for the D in the η2-D2 ligands in 1 and 2 are in the range 19-22 and 27-31 kHz, respectively. The actual CQ for these ligands with short D-D distances (<1 Å) should be at least 2CQeff and probably greater than that of the terminal deuteride but less than that of D2(g), 227 kHz. A fast spinning (>>61 MHz) and tilting of the primary electric field gradient component of between 90° and 60° or between 50° and 40° with respect to the axis of D2 rotation is an explanation for the small CQeff. Therefore neither D-D nor M-D bonding dominates the electric field gradient direction in these M(η2-D2) bonds. The complex [RuD2(C5Me5)(dppm)]+ 3, which exists in solution as a 3.3:1 mixture of Ru(D···D) (3a) and Ru(D)2 (3b) tautomers, has T1min(D) values that provide CQeff values of 66 kHz for 3a and 71 kHz for 3b. The elongated D···D ligand in 3a with d(D···D) ~ 1.10 Å may be "static" compared to the 61.4 MHz 2H spectrometer frequency and therefore have "compressed dihydride" character and display similar Ru-D bonds as in 3b. However, it is more likely that the static CQ for the D of 3a is much larger than that of a terminal Ru-D but averaged to 66 kHz by a 180° flip of the D2 as observed in 7. The complexes trans-[M(D···D)(Cl)(dppe)2]PF6, M = Ru (4), Os (5), and Ru(η2-D2)(dppb)(µ-Cl)3RuCl(dppb) (6) also have motion-reduced CQ values. Some 2H NMR quadrupole echo wide-line spectra of 1, 4, and Os(D···D)(Cl)2(CO)(PiPr3)2 (7) (contaminated with 20% Os(H···D)) were recorded in the solid phase from 293 to 123 K. These also indicate that the CQeff of the D in the D2 ligands are motion-reduced. Simulation of the spectra of 7 are suggestive of a twofold reorientation of a D2 ligand with a static CQ value in the range of 120-167 kHz, a tilt angle of the electric field gradient of about 50°, and an asymmetry parameter near to zero. Significantly, the MAS 2H spectrum of 7 has a broad doublet, possibly due to a non-averaged D-D dipolar/quadrupolar interference phenomenon; this is first time this has been observed. Variable temperature T1 data for solid 7 are also reported, which allow the evaluation of the activation barrier to the twofold flipping motion of the D2; the only other way of quantifying such an energy barrier is by use of an inelastic neutron scattering method.Key words: dihydrogen, deuterium, NMR, ruthenium, osmium, complexes, dynamics, hydride, bonding.


2011 ◽  
Vol 23 (9) ◽  
pp. 1055-1059 ◽  
Author(s):  
Martin Stenicka ◽  
Vladimir Pavlinek ◽  
Petr Saha ◽  
Natalia V Blinova ◽  
Jaroslav Stejskal ◽  
...  

The compatibility of solid phase–liquid medium appears to be an important factor for controlling the electrorheological (ER) efficiency of ER fluids. Controlled protonation of polyaniline particles with perfluorooctanesulfonic, tartaric, or sulphamic acid provides particles in a broad range of hydrophobicity as a suitable model to study this phenomenon. The relation between organization of such particles in silicone oil suspensions in on/off electric field at rest and during flow at various volume concentrations was demonstrated.


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