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Elastic Relaxation of Fluid-Driven Cracks and the Resulting Backflow…
www.itg.cam.ac.uk/people/heh/Paper257.pdf18 May 2017: radius R 20 mm, half thickness W 0.04 mm, and atypical time scale halfway through an experiment t 100 s,the effective Reynolds number in the crack is Reeff ρurW2μ1R1 -
J. Fluid Mech. (2016), vol. 802, pp. 750–759. c© ...
www.itg.cam.ac.uk/people/heh/Paper256.pdf18 May 2017: M =πa2C1/γ p1/γ u=πa2C1/γ(. kµ. )p1/γ. dpdz. (2.19a,b). Thus. p/pD [1H(z)/H(L)]γ/(1γ) (2.20)= (1z/L)γ/(1γ) ... 19:. 20:. 21:. 22:. ikona:. 751:. 752:. 753:. 754:. 755:. 756:. -
rspa.royalsocietypublishing.org ResearchCite this article: Cooray H,…
www.itg.cam.ac.uk/people/heh/Paper255.pdf18 May 2017: The figure shows that the analytical expression is an accurate solution for (5.20). ... We now consider the limitψ1 = ψ2 = ψ, where (5.20) is written as. -
J. Fluid Mech. (2017), vol. 820, pp. 400–423. c© ...
www.itg.cam.ac.uk/people/heh/Paper258.pdf18 May 2017: Imberger. 0 0.1 0.2 0.3 0.4 0.5. 0.05. 0.10. 0.15. 0.20. ... 0.25. 0.300 20 40 60 80 100 120. Reduced gravity with time offset. -
J. Fluid Mech. (2016), vol. 791, pp. 329–357. c© ...
www.itg.cam.ac.uk/people/heh/Paper254.pdf18 May 2017: n 0.25. 0.25. 0.25. 1. 1. 4. 4. 20. 20. (a) (b). ... To prove this, we first use thechain rule to change the integration variable in (2.20) from c to ξ to give ξN.
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