Paper Number
NF23
Session
Non-Newtonian Fluid Mechanics & Flow Instabilities
Title
Viscous fingering instabilities in carbon black gels
Presentation Date and Time
October 17, 2018 (Wednesday) 3:45
Track / Room
Track 7 / Plaza II
Authors
- Marsit, Badis (MIT, Mechanical Engineering)
- Kaloga, Yacouba (MIT, Mechanical Engineering)
- Bischofberger, Irmgard (MIT, Mechanical Engineering)
- Divoux, Thibaut (CNRS Bordeaux, CNRS-MIT, MSE2)
Author and Affiliation Lines
Badis Marsit1, Yacouba Kaloga1, Irmgard Bischofberger1, and Thibaut Divoux2
1Mechanical Engineering, MIT, Cambridge, MA 02139-4307; 2MSE2, CNRS Bordeaux, CNRS-MIT, Cambridge, MA
Speaker / Presenter
Divoux, Thibaut
Text of Abstract
Pattern formation in fluids occurs in numerous physical processes in which mechanical mixing, chemical reactions, evaporation and/or surface effects play a key role. When the pattern develops in a non-Newtonian fluid, the non-linear rheology interferes with the patterning process, which often generates a richer dynamics than that commonly observed for a Newtonian fluid. Here we focus on the viscous fingering instability in a time-dependent yield stress fluid. We study experimentally the flow of a carbon black gel sandwiched in a parallel plate geometry, for which the upper plate is being lifted up at constant velocity. We show the existence of a critical initial gap spacing and a critical lift velocity, above which the flow becomes unstable, leading to the growth of viscous finger originating from the Saffman-Taylor instability at the fluid-air interface. The resulting pattern in the gel consists in a tree-like branched structure, and covers only a fraction of the plate surface. Varying the gel concentration, we demonstrate that the extent of the pattern is governed by the yield strain of the carbon black gel, while for a fixed gel concentration, the span of the pattern increases for increasing lift velocity and decreasing initial gap width. Moreover, we observe three different regimes in the selection of the wavelength: a yield stress dominated regime, a viscous dominated regime and a surface tension dominated regime. Finally, we show that the shear history of the gel has a strong influence on the pattern morphology and allows us to generate a broad variety of patterns, from heavily ramified structures composed of thin branches when the gel is rejuvenated by a preshear of high intensity followed by an abrupt flow cessation, to coarse patterns characterized by a large core and a few thicker branches when the gel is rejuvenated by a preshear of high intensity followed by a slow cessation of shear.