By Peter M. Grosz
Aviatik D.I. КНИГИ ;ВОЕННАЯ ИСТОРИЯ Aviatik D.I. (Windsock Datafile 45)ByPeter M. GroszPublisher: Albatros Productions Ltd1994 forty PagesISBN: 094841460XPDF20 MBThe Aviatik D.I, sometimes called Berg D.I or the Berg Fighter' (due to the truth that it was once designed via Oberingenieur Julius von Berg), was once the 1st indigenous fighter airplane of the Austro-Hungarian Air carrier (Luftfahrtruppen).Work at the prototype all started in August 1916, whereas the 1st flight of the Aviatik D.I prototype, marked 30.14, happened at sixteenth October 1916 at Aspern, regrettably killing the try pilot. importing BitroadDepositfiles eighty five 1 2 three four five
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Some such models are presented below. The elementary one-dimensional computing model of MW discharge The MW discharge is considered in one-dimensional cylindrical geometry. It means that a change of its parameters in a radial direction is many times greater than changes in an axial direction. If gas-dynamic processes are negligible for such a discharge, the following governing equations can be used: Energy conservation equation: Â Ã dT 1 d r D r dr dr 1 jEj2 2 Equation for electric field intensity: Â Ã dE 1 d C !
Div V/i C1,j C . 5ri ui C1,j 1/ i Ä C 2 hj vi ,j xj 1=2 Œ. div V/i ,j C . div V/i 1,j vi ri 1,j 1 « . div V/i ,j i . 123) it was supposed that i ,j . i ˙1=2,j ˙1=2 D The second calculation step. Intermediate values of the mass fluxes GQ u and GQ v , obtained at the first calculation step, are used here to find the pressure disturbances. 124) @Gv [email protected] D @[email protected] 125) with the operator r [email protected] fr [email protected], then: @. div G/ D @t div . grad p/. gradp/ D Q div G . 127) This equation gives birth to two groups of possible calculation models.
The problem is the radiation heating of the walls of the gas-dynamic channel in which the laser plasma is ignited and from which the plasma jet flows out. Solving this problem is important for two reasons. Firstly, it enables to determine the energy losses, integral over the spectrum, to the generator channel walls. Secondly, there is a risk of thermal damage to the channel walls by the thermal radiation at such high plasma temperatures. This is directly associated with the problem of generator design.
Aviatik D.I. by Peter M. Grosz