powder aerosol
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Author(s):  
Tobias Nazarenus ◽  
Kira Schlesier ◽  
Simon Biberger ◽  
Jörg Exner ◽  
Jaroslaw Kita ◽  
...  

Coatings ◽  
2021 ◽  
Vol 11 (7) ◽  
pp. 844
Author(s):  
Mario Linz ◽  
Jörg Exner ◽  
Jaroslaw Kita ◽  
Florian Bühner ◽  
Martin Seipenbusch ◽  
...  

This work shows that the powder aerosol deposition (PAD) method allows the formation of films in powder quantities of less than 60 mg, rather than the large amounts that are typically required for conventional powder aerosol deposition systems. This was achieved by changing the operation mode to a discontinuous one, resulting in operation times of several seconds. Semiconducting strontium titanate ferrate SrTi0.65Fe0.35O3−δ (STF35) was used as the powder to prove the equal behavior in terms of adhesion, film quality and electric conductivity compared to conventional powder-aerosol-deposited films.


2021 ◽  
Vol MA2021-01 (56) ◽  
pp. 1521-1521
Author(s):  
Ralf Moos ◽  
Murat Bektas ◽  
Gunter Hagen ◽  
Jaroslaw Kita ◽  
Daniela Schoenauer-Kamin ◽  
...  

Materials ◽  
2021 ◽  
Vol 14 (10) ◽  
pp. 2502
Author(s):  
Philipp Glosse ◽  
Stefan Denneler ◽  
Oliver Stier ◽  
Ralf Moos

The powder aerosol deposition method (PAD) is a vacuum-based spray coating technology. It allows for production of highly dense coatings at room temperature, especially of brittle-breaking materials. This yields new options for coating substrate materials that even melt at low temperatures. The film formation mechanism is called room temperature impact consolidation (RTIC). The occurrence of this mechanism is strongly linked to the gas jet used in the process. The velocity and direction of the particles in the gas jet forming between the nozzle orifice and the substrate are the main factors influencing the quality of the coating. This dependency aimed to be elaborated with a measurement setup and coating experiments and is shown in this work. We investigated the gas jet formation using a shadow optical imaging system. Regions of different gas density are visualized by this technique. Several parameter sets, in particular gas flow rates and chamber pressures, were investigated. In addition, coatings were produced on glass substrates with the same parameters. As a coating material, the superconducting ceramic-like magnesium diboride (MgB2) was chosen. A correlation between shadow images and thickness profiles of the coatings shows how the gas jet formation affects the uniformity of thickness. Shadow optical images provide valuable information on the flight direction of the particles and allow validation of simulation results.


2020 ◽  
Vol 591 ◽  
pp. 120027
Author(s):  
Amr Hassan ◽  
Dale Farkas ◽  
Worth Longest ◽  
Michael Hindle

Author(s):  
Nico Leupold ◽  
Stefan Denneler ◽  
Gotthard Rieger ◽  
Ralf Moos

Abstract The powder aerosol deposition (PAD) method is a well-known process to fabricate dense layers at room temperature directly from the powder. It is particularly suitable for the deposition of ceramic materials. Compared to these, the use of metal powders (here iron), which are significantly more ductile and have a higher density than typical ceramic powders, has not yet been investigated in detail for PAD. In the first step of this work, the iron powder is characterized by scanning electron microscopy and x-ray diffraction. In order to improve the deposition behavior, the influence of heat treatment on the crystallite and the particle size of the iron powder is investigated. It is shown that the crystallite size of iron powders is reduced down to a nanocrystalline size during deposition. The magnetic properties of the iron powder as well as the layers are investigated by means of coercive field development. Although the initial coercivity raises after deposition, potential applications for flux guiding in microelectronic sensors and devices are feasible. In the second step, thin metal layers (iron) and ceramics (aluminum oxide) are deposited alternatingly to produce iron–alumina multilayer structures.


2020 ◽  
Vol 7 (22) ◽  
pp. 2001114
Author(s):  
Tobias Nazarenus ◽  
Jaroslaw Kita ◽  
Ralf Moos ◽  
Jörg Exner

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