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26 Mar 2023: 554, 299–322. (doi:10.1017/S002211200600930X)2. Baxter SJ, Power H, Cliffe KA, Hibberd S.

30 May 2006: 4.la, b ) G = KA = ( N H / U ) { ( B / H ) 2 - l}, h = e - l ( l - ) = ( ( B / H ) 2 - I}. (

13 Nov 2007: Many models adopt a hydrostatic as-sumption such that ka 1, consistent with experimental re-sults of Pouliquen and Forterre.10. ... There are two key parameters, the Earth pressure coeffi-cient ka, which Larrieu et al.

30 May 2006: ka = n, R ) = 50.

11 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).

18 May 2017: 2012 Wetting of flexible fibre arrays. Nature 482,510–513. (doi:10.1038/nature10779). 9. Wu X-F, Bedarkar A, Vaynberg KA.

19 Jul 2010: cal g- 1 o C- 1 apr 0.380 cal g- 1 o C- 1 ka 0.008 cal cm -1 s -1 øC-1 k•5 0.008 cal cm -•

10 Mar 2009: J. Fluid Mech. (2008), vol. 616, pp. 303–326. c 2008 Cambridge University Pressdoi:10.1017/S002211200800400X Printed in the United Kingdom. 303. Energy balances for axisymmetric gravitycurrents in homogeneous and linearly. stratified ambients.

9 Mar 2004: J. Fluid Mech. (2003), vol. 497, pp. 167–199. c 2003 Cambridge University PressDOI: 10.1017/S002211200300661X Printed in the United Kingdom. 167. Solidification and compositional convectionof a ternary alloy. By ANDREW F. THOMPSON†, HERBERT E.

9 Mar 2004: J. Fluid Mech. (2003), vol. 483, pp. 165–197. c 2003 Cambridge University PressDOI: 10.1017/S0022112003004129 Printed in the United Kingdom. 165. A model for diffusion-controlled solidification ofternary alloys in mushy layers†. By D. M.