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J. Fluid Mech. (2021), vol. 911, A42, doi:10.1017/jfm.2020.1051…
www.itg.cam.ac.uk/people/heh/Paper282.pdf26 Mar 2023: 3.7. 3.6. 3.5. 3.410–6 10–4 10–2. 5.5. 5.0. 4.55 10 15 20. ... 40. 35. 30. 25. 20. 15. 10. 5. 010–4 10–2 100. -
Viscous free-surface flows past cylinders
www.itg.cam.ac.uk/people/heh/Paper274.pdf26 Mar 2023: HINTON, HOGG, AND HUPPERT. -20 -15 -10 -5 0 5 10 15 20. ... 5 10 15 20 25 30 35 40. 1.5. 2. 2.5. -
J. Fluid Mech. (2019), vol. 876, pp. 912–938. c© ...
www.itg.cam.ac.uk/people/heh/Paper270.pdf26 Mar 2023: 1Mm′(x2)=1. ĥ3+. dĥdξ. (4.20). http. s://. doi.o. rg/1. 0.10. 17/jf. m.2. ... 0. 10. 20. 0.5 1.0m. hm. 1.5 2.0. m = mc. -
Dense Suspension Flow in a Penny-Shaped Crack, Part I : Theory
www.itg.cam.ac.uk/people/heh/Paper278.pdf26 Mar 2023: Table 3Values of 𝐴𝑖, 𝐵𝑖 and 𝛤 obtained using (40) with effective viscosity absorbed into the scaling and(29)–(32) with 𝛱 {0.05, 0.20, 0.40, 0.55}. ... We use 𝑀 = 500 and 𝑁 = 4 throughout.𝛱 Absorbed 0.05 0.20 0.40 0.55. -
J. Fluid Mech. (2021), vol. 925, A26, doi:10.1017/jfm.2021.668…
www.itg.cam.ac.uk/people/heh/Paper280.pdf26 Mar 2023: ddτ. (1. ĥ4. )=. [1 κ 2ĥ2. ]1/2, (4.20). where. κ =(. a20 b20). /2a0b0. (4.21). Here, κ 0 is a measure of the initial eccentricity of the ellipse. ... 6.14a,b)925 A26-20. http. s://. doi.o. rg/1. 0.10. 17/jf. m.2. 021. 668. -
Predicting Safe Regions Within Lava Flows Over Topography
www.itg.cam.ac.uk/people/heh/Paper288.pdf26 Mar 2023: Overlain in blue are solutions to the characteristic. model Equation 4, with 20 characteristics emanating from a short line source at the vent. -
Experimental Insights on the Propagation of Fine‐Grained Geophysical…
www.itg.cam.ac.uk/people/heh/Paper279.pdf26 Mar 2023: The length of the immersed ramp varies as Ho/sin θ, where the slope angle is set to θ = 5, 10, 15, 20, and 30 and the water depth is varied
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