2016
DOI: 10.1016/j.cam.2015.11.016
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Nonlinear simulations of elastic fingering in a Hele-Shaw cell

Abstract: This work is motivated by the recent experiments of two reacting fluids in a Hele-Shaw cell [Phys. Rev. E 76 (1) (2007) 016202] and associated linear stability analysis of a curvature weakening model [SIAM J. Appl. Math 72 (3) (2012) 842-856]. Unlike the classical Hele-Shaw problem posed for moving interfaces with surface tension, the curvature weakening model is concerned with a newly-produced gel-like phase that stiffens the interface, thus the interface is modeled as an elastic membrane with curvature depen… Show more

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Cited by 26 publications
(38 citation statements)
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References 32 publications
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“…This might be due to the formation of more interfacial material at higher C, resulting in an increased thickness which would impede finger tip-splitting. An increased elasticity of the material with C could also lead to the suppression of tip-splitting, as shown numerically for fingers in a model where the interface is represented as a membrane with both elasticity and surface tension [36].…”
mentioning
confidence: 87%
“…This might be due to the formation of more interfacial material at higher C, resulting in an increased thickness which would impede finger tip-splitting. An increased elasticity of the material with C could also lead to the suppression of tip-splitting, as shown numerically for fingers in a model where the interface is represented as a membrane with both elasticity and surface tension [36].…”
mentioning
confidence: 87%
“…Mat.) Although this spreading process appears superficially similar to viscous fingering in a Hele-Shaw geometry [22,23], there are numerous distinguishing characteristics. First, the measured fractal dimension (D = 1.30 ± 0.05) is smaller than the value observed in viscous fingering (D = 1.7).…”
mentioning
confidence: 93%
“…To overcome these difficulties, we develop a spectrally accurate boundary integral method in which a new time and space rescaling is implemented. The rescaling idea [29,49,50] is to map the original time and space (x, t) into new coordinates (\= x, \= t) such that the interface can evolve at an arbitrary speed in the new rescaled frame. In particular, for the shrinking interface problem, we choose (1) the space scaling function R( \= t) so that the shrinking interface is always mapped back to its initial size, i.e., the interface does not shrink in the rescaled frame; (2) the time scaling function \rho ( \= t) to slow down the motion of the interface, especially at later times when the interface becomes very small and shrinks extremely rapidly.…”
Section: B1207mentioning
confidence: 99%
“…The time scaling function \rho (t) = \= \rho ( \= t) maps the original time t to the new time \= t and \rho (t) has to be positive and continuous. The evolution of the interface in the scaled frame can be accelerated [50,49] or decelerated by choosing a different \rho (t). A straightforward calculation shows the normal velocity in the new frame…”
Section: Rescaling Idea Introduce a New Framementioning
confidence: 99%