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J. Fluid Mech. (2017), vol. 821, pp. 330–342. c© ...
www.itg.cam.ac.uk/people/heh/Paper259.pdf23 Dec 2021: s. h. ttps. ://do. i.org. /10. 1017. /jfm. 201. 7.24. 3. ... term. s. h. ttps. ://do. i.org. /10. 1017. /jfm. 201. 7.24. -
Symmetric coalescence of two hydraulic fracturesNiall J. O’Keeffea,1, …
www.itg.cam.ac.uk/people/heh/Paper266.pdf23 Dec 2021: In addition,power law fits provide α1 = 0.810.07, β1 = 0.310.02, α2 = 2.50.24,and β2 = 0.140.03. -
Experiments on the low-Reynolds-number settling of a sphere through a …
www.itg.cam.ac.uk/people/heh/Paper265.pdf23 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. -
J. Fluid Mech. (2019), vol. 874, pp. 285–298. c© ...
www.itg.cam.ac.uk/people/heh/Paper268.pdf23 Dec 2021: Thus,with 1ρ =ρ because the density of the overlying air can be neglected, β = 24.8 or0.295 cm1 s1 and (βV 1/3)1 was between 0.004 s ... A 24). Dow. nloa. ded. from. htt. ps://. ww. w.c. ambr. -
J. Fluid Mech. (2018), vol. 844, pp. 435–458. c© ...
www.itg.cam.ac.uk/people/heh/Paper263.pdf23 Dec 2021: 2.24). Using these dimensionless groups, we introduce the viscosity- and toughness-dominated scalings, denoting them with subscripts m and k, respectively. ... balance (2.24) to obtain the radial scaling,. Rk =. (Q2E′2t2. K′2. -
J. Fluid Mech. (2017), vol. 832, pp. 550–577. c© ...
www.itg.cam.ac.uk/people/heh/Paper261.pdf23 Dec 2021: 2πϕ r0. 0. h00. s0[h0(r), z]dzr dr =V, (2.24). where s0[h0(r), z] is the initial saturation distribution. ... By applying scaling analysis to (2.14) and (2.24) and rearranging, we find thefollowing relations between the dimensions of radius, height,
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