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1 - 13 of 13 search results for KA :PC53 24 |u:www.itg.cam.ac.uk where 0 match all words and 13 match some words.
  1. Results that match 2 of 3 words

  2. 29 Apr 2010: Thermal conductivities of air and thecondensed phase are given by ka and ks, respectively. ... By dimensionalization of equation (3.24), we findthat the system is stable when.
  3. doi:10.1016/j.jcp.2005.12.002

    www.itg.cam.ac.uk/people/grae/74.pdf
    12 Jun 2006: g. [23,24]). The major difficulties then consist in the formulation of accurate internalboundary conditions and in following the evolution of the interfaces through time. ... Values of these constants ka, b are presented in Fig. 4 as afunction of
  4. Static and flowing regions in granular collapses down…

    www.itg.cam.ac.uk/people/heh/Paper208.pdf
    13 Nov 2007: Method. Glass beads 24 Rotating drume. 0.25–0.35 24 Smooth inclined planef. ... There are two key parameters, the Earth pressure coeffi-cient ka, which Larrieu et al.
  5. 30 May 2006: 4.la, b ) G = KA = ( N H / U ) { ( B / H ) 2 - l}, h = e - l ( l - ) = ( ( B / H ) 2 - I}. ( ... a$'(@, SY), DPI = { P } [ 1 , 1 , S&I, (4.23) where yil) = P-1Bi/Ms$2) (4.24 a).
  6. 18 May 2017: x = h(y) = 16 y3 c1y c2, (4.24)where c1 and c2 are constants. ... 2012 Wetting of flexible fibre arrays. Nature 482,510–513. (doi:10.1038/nature10779). 9. Wu X-F, Bedarkar A, Vaynberg KA.
  7. flm145.dvi

    www.itg.cam.ac.uk/people/heh/Paper197.pdf
    11 Oct 2006: After some algebra and use of(2.24), we obtain. ρD. Dt. [1. ... 374 M. Ungarish and H. E. Huppert. t0 4 8 12 16 20 24.
  8. The stability of a large gas bubble rising through liquid

    www.itg.cam.ac.uk/people/heh/Paper81.pdf
    30 May 2006: Stability of a large gas bubble rising through liquid 417. 24. ... 1. oo 1.712 1.26 1.42 1.10 1.24. 13.61 1.200 0.79 1.06 1.
  9. The Crystallization of Lava Lakes

    www.itg.cam.ac.uk/people/grae/21.pdf
    29 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. The Crystallization of Lava Lakes

    www.itg.cam.ac.uk/people/heh/Paper118.pdf
    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 -•
  11. The fluid mechanics of solidification

    www.itg.cam.ac.uk/people/heh/Paper92.pdf
    16 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
  12. 10 Mar 2009: Conservation of volume. v = 0. (2.24)2. Momentum balance. ρDv. Dt= p (ρ ρb)g ẑ μ2v, (2.25). ... After some algebra and use of(2.24), we obtain. ρD. Dt. [1.
  13. flm661.dvi

    www.itg.cam.ac.uk/people/aa/JFM2.pdf
    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.
  14. flm661.dvi

    www.itg.cam.ac.uk/people/heh/Paper178.pdf
    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.

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