“…This model can be approximately realized for flows where 0 < dA/dx ,~ 1 for x > xk. In fact it can be shown that this model is precisely what is achieved in the differently scaled droplet growth zones of the asymptotic theories of Blythe and Shih (1976) and Clarke and Delale (1986). In this case the function A, denoted herein by A3(g', x), and the critical amount of heat q*, denoted herein by * ' q3 (g, x), are given by R(g', x) is strictly increasing, thereby q*(g', x) and q* (g', x) j = 2, 3, 4 are strictly increasing whereas q*(g', x) is a constant.…”