Two transients for a radial nearly-horizontal flow

(Twenty-two subjects were tested. Two of these subjects, however, chose the first perceptually curved stimulus. This performance was significantly different from the

Russell used acquaintance to that effect: ÒI say that I am acquainted with an object when I have a direct cognitive relation to that object, that is when I am directly aware of

1/ Axisvmmetrical radial Hm\" without surface resistance, How' in a diverging channel and spatially varied flow in a uniform channel.. Ecoulement radiat et tl:âs!j'111étrique,

The second approach has been retained here in order to perform the coupling of a two-fluid model (which involves six governing partial differential equations in order to account

correct the observed horizontal directions for dislevelment of the horizontal axis. a) There are two possible reasons for the horizontal axis of a theodolite not being

In the present study, the interaction is between a viscous Tollmien-Schlichting wave and an inviscid internal gravity wave (see Figure 7). Hence, the coupling of the two stable

We introduce here a definition of weak solutions for (1.1)–(1.8) in two cases: slip boundary conditions at all boundaries, mixed slip/no-slip boundary conditions. The

For a “convergent” domain, the configuration observed in the previous case is reverted, and corresponds to a “finger coming from the inside”. This is shown on Figure 18.. of