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doi:10.1016/j.jcp.2005.12.002
www.itg.cam.ac.uk/people/grae/74.pdf12 Jun 2006: Values of these constants ka, b are presented in Fig. 4 as afunction of Tliquidus(Ci) Timp, in comparison with [1]. ... sλ a. ,b. Fig. 4. Dimensionless constants ka, b as a function of the temperature difference between the liquidus temperature at the -
Lee waves in a stratified flow Part 3. Semi-elliptical obstacle
www.itg.cam.ac.uk/people/heh/Paper8.pdf30 May 2006: 4.la, b ) G = KA = ( N H / U ) { ( B / H ) 2 - l}, h = e - l ( l - ) = ( ( B / H ) 2 - I}. ( -
The stability of a large gas bubble rising through liquid
www.itg.cam.ac.uk/people/heh/Paper81.pdf30 May 2006: ka = n, R ) = 50. -
flm145.dvi
www.itg.cam.ac.uk/people/heh/Paper197.pdf11 Oct 2006: t. Ka/. P c (0. ). P a/P. c (0. ). 2 4 6 8 10 120. 0.2. 0.4. 0.6. 0.8. 1.0 (a) (b).
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