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Energy balances for axisymmetric gravity currents in homogeneous and…
www.itg.cam.ac.uk/people/heh/Paper213.pdf10 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. -
flm661.dvi
www.itg.cam.ac.uk/people/aa/JFM2.pdf9 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. -
flm661.dvi
www.itg.cam.ac.uk/people/heh/Paper178.pdf9 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. -
The fluid mechanics of solidification
www.itg.cam.ac.uk/people/heh/Paper92.pdf16 Jan 2007: Composition, wt % Na,SO,. FIGURE 15. The predicted results a n d experimental d a t a for cooling a n aqueous solution of Ka,SO, from above for t h -
flm412.dvi
www.itg.cam.ac.uk/people/heh/Paper174.pdf9 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. -
The Crystallization of Lava Lakes
www.itg.cam.ac.uk/people/grae/21.pdf29 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 -•
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