Rheology of Colloidal Gas Aphrons (Microfoams)
- Author(s): Larmignat, Sophie
- Vanderpool, Damien
- Lai, Heung
- Pilon, Laurent
- et al.
Published Web Locationhttp://www.sciencedirect.com/science?_ob=ArticleURL&_udi=B6TFR-4S2F5JV-5&_user=4423&_coverDate=06%2F05%2F2008&_alid=767783819&_rdoc=1&_fmt=high&_orig=search&_cdi=5233&_sort=d&_docanchor=&view=c&_ct=1&_acct=C000059605&_version=1&_urlVersion=0&_userid=4423&md5=d0ca43d4a769c48017218d5876a12c2d
This paper reports on the effect of surfactant concentration and pipe shape and size on the rheological properties of colloidal gas aphrons (CGA) or microfoams. CGA consist of closely packed spherical gas bubbles with diameter ranging from 10 to 100 microns surrounded by a surfactant shell. It is produced by stirring an aqueous surfactant solution at high speed in a baffled beaker. Pipe flow experiments were performed in cylindrical pipes with diameter ranging from 1.0 to 3.0 mm under adiabatic laminar flow conditions. The porosity, bubble size distribution, surface tension, and pH were systematically measured. First, it is established that there was no slip velocity at the wall and CGA did not change morphology and porosity between the inlet and outlet of the pipes less than 2 mm in diameter. Compressibility effects were accounted for through the volume equalization approach. Then, pipe shape and diameter have no effect on the CGA rheology. Finally, CGA can be considered as a shear thinning fluid. The dimensionless volume equalized shear stress \tau* is proportional to $(Ca*)^m$ where Ca* is the Capillary number and m = 0.65+/-0.06. The results are in good agreement with theoretical models suggesting \tau*=C(x)Ca*^(2/3) where C(x) is determined experimentally and increases with surfactant mass fraction x. The Fanning friction factor f for CGA under laminar flows follows the standard relationship f=16/Re where Reynolds number is determined using the measured CGA effective viscosity.
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