Abstract
We present a ‘‘Flory-type’’ mean-field theory to calculate the fractal dimension D of the radial viscous finger pattern formed by the less viscous fluid in a Hele-Shaw cell. We predict (a) the relation between the interfacial tension σ between the two fluids and the onset of the asymptotic behavior and (b) the variation of the effective fractal dimension with time in the transient regime for a fixed σ.
- Received 10 May 1994
DOI:https://doi.org/10.1103/PhysRevE.51.407
©1995 American Physical Society