Interdisciplinary Applied Mathematics

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r(t) oc (—V3t h


which shows a weak dependence on time. However, careful analysis shows that a thin precursor film of molecular dimensions is advancing at a rate proportional to л/t, i.e., it follows standard diffusion dynamics.


In nonsmooth surfaces the spreading of liquids follows different dynamics, since capillary wicking of small amounts of liquids into microgrooves occurs.


Capillary wicking is a well-known phenomenon that has been studied extensively, first in the pioneering work of (Washburn, 1921). Also, (Romero and Yost, 1996) performed a systematic analytical study of capillary flow into a V-shaped microgroove. A typical configuration is shown in Figure 8.5 with    the    flow out of    the    page; the groove    has height    h0,    the    height    of


the liquid is denoted by h(x,t), and the equilibrium contact angle is 90.


The pressure    drop    along    the    groove is    Ap    = p(x)    — p0    = yre(x),    where


k(x)    is    the    curvature and    p0    is    the    constant    pressure above    the    liquid.


This expression is valid if the capillary number Ca = Up/j ^ 1, which implies that surface tension forces dominate over viscous forces. For a long microgroove the curvature parallel to the flow direction is neglected, and thus


1    sin(a — 9) tan(a)


» * R(x)    h(x,t)


computed from the sketch of Figure 8.5. Following a quasi-one-dimensional flow analysis, Romero and Yost (1996) found that the flowrate is


dp


dx



Q


FIGURE 8.5. Sketch for liquid spreading in a V microgroove.


h4(x,t)


V    T{9, a)


P


which is an expression similar to that for Poiseuille flow. Also, Г(9, a) is a positive function that can be approximated numerically by

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