Titlebook: IUTAM Symposium on Free Surface Flows; Proceedings of the I A. C. King,Y. D. Shikhmurzaev Conference proceedings 2001 Springer Science+Busi

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書目名稱IUTAM Symposium on Free Surface Flows網(wǎng)絡(luò)公開度學(xué)科排名




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書目名稱IUTAM Symposium on Free Surface Flows年度引用學(xué)科排名




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書目名稱IUTAM Symposium on Free Surface Flows讀者反饋學(xué)科排名

沙漠

Thin-Film Flows And High-Order Degenerate Parabolic Equations,ing both PDE and ODE (partial and ordinary differential equation) methods. Here we summarise aspects of this mathematical literature, and of the related physics literature, in terms of the spreading of Newtonian fluids, particularly in the completely-wetting case.

Root494

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HOWL

Fluid Mechanics of Single Cavitation Bubble Luminescence, flatrigid boundary are presented. Particular attention is paid to the parameter regime investigated experimentally by Lau terborn and others using laser induced bubbles and high-speed photography, in which light emission has been observed during the collapse of the bubble. Calculations are provid e

碌碌之人

Orchiectomy

The Recoil of A Broken Liquid Bridge,read is observed to have the shape of a slender cone close to the bifurcation point. In this paper, we study the evolution of an ideal fluid which is initially conical. The only force acting on the fluid is due to surface tension. We derive a simplified one-dimensional model and find an asymptotic s

delta-waves

A Numerical Model of Gas-Liquid-Solid Contact Line,lation of two-phase flows. The extension concerns the ability of such a method to take into account the motion of a contact line. The selected numerical model enables one to simulate moving contact line by bypassing the mathematical singularity with the use of a staggered grid. It does not pretend t

creatine-kinase

,A Bubble Rising in Viscous Fluid: Lagrange’s Equations for Motion at A High Reynolds Number,revious analytical calculations of that shape at high Reynolds numbers have ignored viscosity. This paper shows that if one includes viscosity by incorporating Rayleigh’s dissipation integral in Lagrange’s equations, then the speed of rise is that given by Moore, and the shape is that found for . fl

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