Compact or fractal patterns in diffusion limited growth

While these individual resonant layers are properly defined solutions of the MHD equations, their physical relevance is not obvious a priori since their narrow width might

Abstract.2014 We present the morphological pressure-temperature phase diagram for viscous fingering patterns observed in the isotropic, nematic and smectic A phases of the

As C~~~ m Log (A, ), where A, is the relative amplitude of the noise present in the system [2], the self-similar distribution function and the associated physical

Besides the standard Saffmann-Taylor instability, we observe - with increasing finger velocities - the existence of two new regimes: (a) a stick-slip regime for which the finger

4 we show, for different values of the Froude number and for Pr * ⫽ 1, the evolution of the critical Rayleigh number as a function of the frequency in the case where the fluid layer

The analysis of fluidelastic instability in tube bundles of the results is often limited to the determination of a stiffness coefficient and a damping coefficient, to model

This study confirms that M2H4 (rat odontoblast) and ALC (mouse mature ameloblast) after culture conditions optimization are good mi- neralization dental cell lines models

Le point de vue adopt´e, comme dans [W] chapitre X, est de param´etrer les classes de conjugaison, ou de conjugaison stable, des ´el´ements semi-simples r´eguliers d’un tel groupe