Titlebook: Nonlinear PDE’s in Condensed Matter and Reactive Flows; Henri Berestycki,Yves Pomeau Book 2002 Springer Science+Business Media Dordrecht 2

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書目名稱Nonlinear PDE’s in Condensed Matter and Reactive Flows影響因子(影響力)




書目名稱Nonlinear PDE’s in Condensed Matter and Reactive Flows影響因子(影響力)學(xué)科排名




書目名稱Nonlinear PDE’s in Condensed Matter and Reactive Flows網(wǎng)絡(luò)公開度




書目名稱Nonlinear PDE’s in Condensed Matter and Reactive Flows網(wǎng)絡(luò)公開度學(xué)科排名




書目名稱Nonlinear PDE’s in Condensed Matter and Reactive Flows被引頻次




書目名稱Nonlinear PDE’s in Condensed Matter and Reactive Flows被引頻次學(xué)科排名




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書目名稱Nonlinear PDE’s in Condensed Matter and Reactive Flows年度引用學(xué)科排名




書目名稱Nonlinear PDE’s in Condensed Matter and Reactive Flows讀者反饋




書目名稱Nonlinear PDE’s in Condensed Matter and Reactive Flows讀者反饋學(xué)科排名

高度

https://doi.org/10.1007/978-94-010-0307-0condensed matter; dynamics; fluid dynamics; partial differential equation; superfluidity; turbulence; vort

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Ends of Laminar Flamelets: Their Structure, Behaviour and ImplicationsThis article attempts to offer a broader interpretation of the nature and role of laminar flamelets than is usually considered. In particular, when such flamelets have multiple solutions, as is commonly the case, it is possible to predict some interesting structures and important dynamical interactions between different possible types of flamelet.

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LAIR

The Ginzburg-Landau System for Superconducting Thin FilmsWhen a superconducting film of constant thickness, between the planes . = -. and . = . is submitted to an exterior magnetic field (0, 0, ..) parallel to the surface of the film, the state of the film can be described by the functions (.(.), .(.)) satisfyingthe Ginzburg-Landau system:

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Sinus-Rhythm

A Priori Estimates for Ginzburg-Landau Solutionse also how this semi-infinite model gives a good information on the behavior of a large film. We emphasize about the techniques of a priori estimates developed in [11], [12], [13], [6] and present also new estimates relating .(0) and .(0).

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