Ionic Wind Generation in the Vicinity of Dielectric Surface and in the Space Formed by Stacked Dielectric Materials Using Sliding Discharge

2016 ◽  
Vol 2016.25 (0) ◽  
pp. 2B3
Author(s):  
Ryusuke SAKAMOTO ◽  
Keiichiro YOSHIDA
Author(s):  
Jingguo Qu ◽  
Minjun Zeng ◽  
Dewei Zhang ◽  
Dakai Yang ◽  
Xiongwei Wu ◽  
...  

Abstract Ionic wind, an induced phenomenon during corona discharge, possessing the features of silent operation and no moving parts, has a wide range of applications. Ionic wind generation is accompanied by complex physical processes, involving gas ionization, ion recombination, flow, and various chemical reactions, as well as mutual couplings between some of them. Therefore, understanding the corona discharge process and ionic wind generation is crucial for researchers and engineers to better utilize this phenomenon in practical applications. In this review, the principles of corona discharge and its induced ionic wind are presented. Subsequently, ionic wind generators (IWGs) are discussed according to their applications, and the corresponding advances based on experimental studies and numerical simulations are also reviewed. Moreover, the challenges of transitioning the ionic wind technology from laboratory studies to practical applications are discussed. These challenges include the excessively high onset voltage of the corona, ozone emission, and influence of environmental conditions. Furthermore, the mechanisms of these barriers and several effective approaches for mitigating them are provided. Finally, some future research prospects and the conclusions are presented.


2015 ◽  
Vol 73 ◽  
pp. 125-130 ◽  
Author(s):  
Longnan Li ◽  
Seung Jun Lee ◽  
Wonjung Kim ◽  
Daejoong Kim

2019 ◽  
Vol 59 (8) ◽  
pp. 86-91
Author(s):  
Ludmila A. Brusnitsina ◽  
◽  
Elena I. Stepanovskih ◽  
Tatiana A. Aleхeeva ◽  
◽  
...  

In the processes of chemical and galvanic metallization of dielectric materials, in particular in the production of printed circuit boards, surface activation mainly uses compounds of precious metals and colloidal solutions characterized by limited stability during storage due to the coagulation process. To activate dielectric materials it is advisable to use true solutions based on monovalent copper compounds. For continuous metallization of the dielectric, it is necessary to obtain a sufficiently large number of catalytic active centers on the surface. This can be achieved in two ways: to create a high concentration of Cu(I) in the activation solution or to increase the thickness of the activating layer. The aim of this work is to modify the activating solution by introducing organic solvents and surfactants into its composition, contributing to an increase in the concentration of catalytically active centers on the dielectric surface. In order to better distribute the activating solution on the dielectric surface and in the holes, as well as to increase the sorption of copper(I) by the adhesive layer, the modifying effect of organic solvents on the activating composition was studied. As such solvents, dimethylformamide (DMFA) and dimethyl sulfoxide (DMSO) used in the preparation of the surface of the adhesive layer were studied. In the process of swelling, the solvent penetrates into the thickness of the adhesive layer. Due to this, the activator containing an organic solvent has the ability to be fixed on the surface not only due to the micro-roughness created in the etching process, but also able to penetrate deep into the swollen layer. It is established that the maximum thickness of the swollen layer for 10% solution is reached by the time of swelling 30-40 minutes, for 20% ‒ 20 minutes, for 50% ‒ more than 45 minutes. By the time of swelling, equal to 5 minutes, for 10, 20 and 50% solutions, the thickness of the swollen layer, respectively, is 1.00; 1.14; 1.55 microns. It is shown that the presence of organic solvents in the activator increases the adhesion of the metal coating by an average of 1.3 times. In order to better distribute the activator on the dielectric surface and in the holes, as well as to increase the adsorption of copper(I), it is advisable to introduce surfactants into the activator, which reduce the surface tension at the interface. Introduction to the composition of the surfactant activating solution affect the adhesion of the metal to the dielectric. It was found that the introduction of surfactant into the activating solution leads to an increase in the concentration of copper on the dielectric surface. Nonionic surfactant brand OP-10 in the activator provides a high concentration of catalytically active centers and get the highest adhesion of metal to the dielectric.


2021 ◽  
Vol 2059 (1) ◽  
pp. 012006
Author(s):  
S G Davydov ◽  
A N Dolgov ◽  
A A Kozlov ◽  
V A Maksimov ◽  
R Kh Yakubov

Abstract High-speed imaging and visible light stereomicroscopy were applied to do researches, which allowed us to find out differences in a dielectric surface discharge behavior in the triggered vacuum gap, when various dielectric materials (mica, muscovite and corundum-type ceramics) were used. Images of the discharge and the erosion in the electrode systems were analized to reveal that at the discharge on the ceramics surface a material of electrodes was mostly involved as a plasma-forming matter and on the mica it is the dielectric material.


1993 ◽  
Vol 323 ◽  
Author(s):  
M. J. Desilva ◽  
A. J. Pedraza ◽  
D. H. Lowndes ◽  
M. J. Godbole

AbstractWe have developed a new two-step process to generate a metallic pattern on dielectric materials. This method employs ultraviolet (uv) laser irradiation followed by electroless deposition. A few laser pulses are required to generate the pattern. After immersion in an electroless bath, the metal film is deposited only on the uv exposed area. Results of the application of this method to aluminum nitride and alumina are presented. The laser irradiation step is very fast, and the electroless deposition is simplified because it does not require any special seeding to promote activation, i.e. laser irradiation activates the dielectric surface for electroless deposition. In addition, the laser-induced activation of the insulator is maintained for a very long time allowing electroless deposition to be performed many months after irradiation. Patterns in the tens of microns can be produced on laser-exposed substrates. Pull tests have been performed to determine the bond strength. We have found that the bond strength can be further increased by annealing.


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