By Edwin Henry Barton
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015 and Pe = 1. Each curve is normalized by the maximum vertical distance between the tip and the wall that is reached for all ßo values at that time. 15) in the vertical direction of the figure. Each curve represents a different time and from the bottarn to the top the times are 5, 10, 15 and 20. Again there is a distinct increase in the optimal ßo value with time. 5 degrees, and at the final time 20 it has increased to 30 degrees . 4 ..... 8 \ \ ' 'llo, / / ;I / ·-- * llt \ '' / \ '\ I / \ \ / / \ \ ~ ;I llt llt \ /.
F. 1970 'The Origin of Freckles in Unidirectionally Solidified Castings', Met. , vol 1, p 2193-2205. Caroli, B. Caroli, C. Misbah, C. and Roulet, B. Journal de Phy_sique C, vol46(3), p. 401, (1985). J. F. 'Convective and interfacial instabilities during unidirectional solidification of a binary alloy', J. Crystal Growth, vol 49, pp 13-28, (1980). R. B. F. F. Sekerka, J. Crystal Growth, vol69, p. 15, (1984). P. , J. , vol 297, p. 293-305, (1995). A. S. , Proc. S. National Congress of Applied Mechanics, J.
An introduction to the mechanics of fluids by Edwin Henry Barton