By Mike Verier
Osprey-Aerospace-ColourSeries- Cobra-Tank Killer ideally suited КНИГИ ;ВОЕННАЯ ИСТОРИЯ Автор:Mike Verier Название: Cobra-Tank Killer splendid Издательство: Osprey PublishingГод: 1989 Формат:pdf,rar+3%Размер: 36.2Mb Язык: английскийСтраниц:129*20
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A improvement of the winning Lockheed ‘medium twins’ of the overdue Thirties, the PV Ventura/Harpoon relations of patrol bombers observed common provider with either the U.S. Navy/Marine Corps and the TAF and Commonwealth from October 1942 onwards. The USAAF extensively utilized surplus Venturas initially ordered by way of the RAF, specified B-34 Lexingtons, within the bomber education and coastal patrol roles.
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Every one quantity during this sequence is devoted to precise plane types and describes its improvement, construction, operation and destiny, supported by way of many illustrations, commonly in color, and registration tables. Contents:AcknowledgementsIntroductionChapter I – Paper GiantsChapter II – The AirbusChapter III – concentration ChangeChapter IV – The release BattleChapter V – Long-haul VersionsChapter VI – The Race To FlyChapter VII – RolloutChapter VIII – Into ServiceChapter IX – input The sequence 30Chapter X – sequence 30 Into SeviceChapter XI – An Eventful YearChapter XII – combined FortunesChapter XIII – army VersionsChapter XIV – construction EndsAppendices:Appendix I – normal Dimensions & Engine version ComparisonsAppendix II – Write-offsAppendix III – construction record
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Extra info for Cobra: Tank Killer Supreme
This means that the fact of finding one molecule in a given state has no influence upon the probability of finding the second one in another given state, and is expressed by saying that the states of the molecules (in the case of thermal equilibrium of a monatomic ideal gas) are statistically uncorrelated. An elementary example of random events, which are also statistically uncorrelated, is given by the results of throwing a pair of dice; the fact that we obtain a certain number from one die does not influence the number which is shown by the other die, and the probability of getting a given combination (say, two from the first die and five from the 22 Basic Principles [Ch.
II and we have only to take j = i and sum from i = 1 to i = 3 in Eq. 7) to deduce i J~ 2! 9) Again the first term in the right-hand side will be macroscopically identified with the kinetic energy density, while the second term will be ascribed to the internal energy of the gas. 10) since the density of internal energy is obviously the product of the internal energy per unit mass times the mass density. , the sum of the three diagonal terms) of the stress tensor. In fact, Eqs. ) The spur divided by three gives the isotropic part of the stress tensor; it is therefore convenient to identify p = Pii/3 with the gas pressure, which is known to be isotropic, at least in the case of equilibrium (Pascal's principle; the identification is also correct for nonequilibrium situations in the case of a monatomic ideal gas, but is generally incorrect).
M. N. Kogan, Rarefied Gas Dynamics, Plenum Press, New York (1969). Reference 10 is also to be consulted for the Boltzmann equations describing gas mixtures and polyatomic gases. For recent developments in the justification of the Boltzmann equation see I 1. C. Cercignani, Transport Theory and Statistical Physics 2, 211 (1972); 12. 0. E. Lanford, III, in: Proceedings of the 1974 Battelle Rencontre on Dynamical Systems (J. ), Lecture Notes in Physics, Volume 35, Springer, Berlin (1975); 13. R. Illner and M.