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23 Apr 2007: Received 15 November 2005; accepted 9 January 2007; published online 20 April 2007. ... Thewidely accepted reason for this scaling relationship is theconstant ratio of shear stress and normal stress.20.

25 Jan 2007: are similar to those derived in P a r t 1 (equations (3.19) and (3.20)), though they now involve the variable 8, and, as mentioned earlier, q5i is no ... Solidijcation of an alloy cooled from above. Part 2. 20. 15.

13 Nov 2007: Received 20 November 2006; accepted 11 July 2007; published online 2 October 2007. ... For Ls= 0.20 m / s and = 0.4 it is reduced to 0.08 s.

25 Jan 2007: 45. 20 30 40 0 10 20 30 40 0 10 I (min) t (min). ... Melting the roof of a chamber. Finally, (18) and (20) can be written J D.

8 May 2007: 6000. 0. 2. 4. 6. 8. 10. 0 20 40 60 80 100. ... 250. 300. 2 8 10t (min). 20 1.2 17.6 0.421 0.8 4.2 0.422 1.2 17.6 0.02. #

2 Apr 2007: The experiments werecarried out using cylinders and rectangular tanks 30 to 60 cm tall, and cover aspectratios between 0.5 and 20, where the aspect ratio is defined as the ratio ... 6. 4. 2. 0 5 10 15 20. Hei. ght (. cm). Horizontal distance (cm). XY. XY.

25 Jan 2007: 2= 307 J 337 J 20.0 "C. A 0.056 -. TABLE 1. ... 10. 5 -. 35 1. -. - h. E 0. 0 10 20 30 40 50.

16 Jan 2007: 0 10 20 30. c, (wt Yo) FIQURE 10. The non-dimensional growth rates A4, A, and A, (determined by Worster 1986) with. ... 20. 15 - v. 3 l 0 - fi 5 -. - -. X I I I I I. 0 10 20 30 40 50.

8 May 2007: h. t+. 8g sin β. 15νh2. h. z= 0. (2.20). The effect of confining boundaries on viscous gravity currents 499. ... 10. 20(a) (b). t/(v/ga). 103 104 105. t/(v/ga). z N /. (V/a. )1/2. 10. 100. z N /. (V4 s. in3 β.

25 Jan 2007: T, = -20 "C c, = 9.37%. 1. H 01 = -h,(AC)f = 2.40 x 10-4K, s-'. ... 0.04 - (b) -. 0.01. 0 5 10 15 20 25 0 5 10 15 20 25.