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21 Mar 2016: Received 24 June 2015; revised manuscript received 1 January 2016; published 24 February 2016). ... 24)] while the effective permeability decreases like H1(cf. (22)). The porosity also approaches an asymptotic profilewith φ0 0 as H.

27 Apr 2006: 2.18), which can be (2.23) and (2.24) more closely.used in (2.22) to show that Segregation is more sensitive to the value of. ... 4.24)mass reduce to and we use this condition together with (4.21)—.

23 Dec 2021: seal” configurations observed for inertial impacts of spheres ontoair-water [24] and fluid-fluid [26] interfaces. ... Phys. 3, 180. (2007).[23] D. Lee and H. Kim, Impact of a superhydrophobic sphere onto water, Langmuir 24, 142 (2008).[24] J.

29 Apr 2010: we can make the approximation G(y) π y. Equation (2.24) then becomesπ. ... By dimensionalization of equation (3.24), we findthat the system is stable when.

30 May 2006: 2.21). (2.22). (2.23). (2.24). where EN is the value of [ at r = rN(t). ... Substituting (2.23) and (2.24) into (2.21) and (2.22), we find that $ ( z ) , where z = c/&, satisfies.

9 Mar 2004: 6.3 6.3 24.3 5.89 1.00 3.86 9.6 6.1 3.8 0.7417 6.3 6.3 24.3 10.71 1.00 ... 86 9.6 8.2 5.2 0.8118 6.3 6.3 24.3 20.37 1.00 3.86 9.6 11.3 7.1 0.8919 13.2

26 Sep 2011: 24). F o r a solution to be possible the right-hand side o f (24) must be positive, that is (with Yr negative).

27 Aug 2010: However, variations in fountain height in episode 4, asplotted in figure 1.24 of Wolfe et al. ... the night of 24–25 July 1983,when the flow front divided into two parallel lobes.

26 Mar 2023: The governing Eq. (7) in the rescaledcoordinates is. h3. x̂=. [. x̂. (h3. h. x̂. ). ŷ. (h3. h. ŷ. )]. (24). ... 5.0 24 15 7.14 1.2 0.853.5 48 13.2 4.50 1.72 0.615.0 24 7.9 3.76 1.28 0.773.5

18 Nov 2009: y1=2ð1 þ yÞ1=2ln. y1=2 þffiffiffiffiffiffiffiffiffiffiffiffi1 þ y. p s þ c1; (24). ... Am.Math. Soc. 46 (1940) 615–683. [24] T.B. Benjamin, Gravity currents and related phenomena, J.