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14 Jul 2009: E = π. 0. π/20. [L{Γ}ge(φ,θ; Γ). ]2sin θ dθ dφ. ... 20 L. C. Nitsche and E. J. Hinch. more vigorously than they are thrown back toward the centreline.

10 Jul 2009: a!, b!, c! Spatiotemporal diagrams obtained ford5 20 mm at asame density contrast At. ... Tube diameterd5 20 mm. The slope of the dashelines5 0.25 @see Eq.14!#.

13 Jul 2009: Downloaded13Jul2009to131.111.16.20.RedistributionsubjecttoAIPlicenseorcopyright;seehttp://pof.aip.org/pof/copyright.jsp. and depth of the vessel were uniform to within 0.05 cm. ... the Van der Waals force and the drag force was 20 000times the Van der

31 Jul 2009: J. 20, 128. MARUCCI, G. & ACIERNO, D. 1974 J. Polymer Sci. (

14 Jul 2009: Hinch. 40. 30. 01. 20. 10. 5 10 15 0 5 10 15. ... 1. o. 0.8. 0.6. D 0.4. 0.2. 0. SL 20. 10.

24 Aug 2009: 31). For r > 20 and < 0-05 respectively, the two sets of values a,gree well. ... With smaller particles, a relatively large number density could be allowed without violating any of our conditions (20), (21), or (22).

13 Jul 2009: 20. lz- 40 -3 3 :g 60. tl E a Q ) 80 78. ... Time, t”. Nicolai et al. Downloaded 13 Jul 2009 to 131.111.16.20.

10 Jul 2009: 20) except that the pressure gradient 1 p is negligible so that the momentumequation becomes. ... cn µ2(1p)/[p(3p)]s. 0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 20.

8 Jul 2009: z,t0) = 1 ε cos(2πz/20). Let us compare the flow obtained withsmall surface tension, Oh = 3.16 and De = 94.9 and with a. ... 20] J. Étienne, Simulation numérique d’écoulements gravitaires à fortesdifférences de densité, Application aux

8 Jul 2009: The forces acting between two col-liding grains are computed from the normal overlap, n, andthe equations of motion displacement and rotation are inte-grated using the Verlet method 20. ... Garcia-Rojo, H. Hermann, and S. McNamaraStuttgart, 2005, p. 853.