Interplay between elastic instabilities and shear-banding: three categories of Taylor–Couette flows and beyond
In the past twenty years, shear-banding flows have been probed by various techniques, such as rheometry, velocimetry and flow birefringence. In micellar solutions, many of the data collected exhibit unexplained spatiotemporal fluctuations. Recently, it has been suggested that those fluctuations orig...
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Royal Society of Chemistry, The
2013
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Online Access: | http://hdl.handle.net/1721.1/80865 https://orcid.org/0000-0001-8323-2779 |
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author | Fardin, Marc-Antoine Grenard, V. Divoux, T. Manneville, S. Lerouge, S. Ober, Thomas Joseph McKinley, Gareth H. |
author2 | Massachusetts Institute of Technology. Department of Mechanical Engineering |
author_facet | Massachusetts Institute of Technology. Department of Mechanical Engineering Fardin, Marc-Antoine Grenard, V. Divoux, T. Manneville, S. Lerouge, S. Ober, Thomas Joseph McKinley, Gareth H. |
author_sort | Fardin, Marc-Antoine |
collection | MIT |
description | In the past twenty years, shear-banding flows have been probed by various techniques, such as rheometry, velocimetry and flow birefringence. In micellar solutions, many of the data collected exhibit unexplained spatiotemporal fluctuations. Recently, it has been suggested that those fluctuations originate from a purely elastic instability of the shear-banding flow. In cylindrical Couette geometry, the instability is reminiscent of the Taylor-like instability observed in viscoelastic polymer solutions. The criterion for purely elastic Taylor–Couette instability adapted to shear-banding flows suggested three categories of shear-banding depending on their stability. In the present study, we report on a large set of experimental data which demonstrates the existence of the three categories of shear-banding flows in various surfactant solutions. Consistent with theoretical predictions, increases in the surfactant concentration or in the curvature of the geometry destabilize the flow, whereas an increase in temperature stabilizes the flow. However, experiments also exhibit some interesting behaviors going beyond the purely elastic instability criterion. |
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format | Article |
id | mit-1721.1/80865 |
institution | Massachusetts Institute of Technology |
language | en_US |
last_indexed | 2024-09-23T08:34:31Z |
publishDate | 2013 |
publisher | Royal Society of Chemistry, The |
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spelling | mit-1721.1/808652022-09-23T13:00:50Z Interplay between elastic instabilities and shear-banding: three categories of Taylor–Couette flows and beyond Fardin, Marc-Antoine Grenard, V. Divoux, T. Manneville, S. Lerouge, S. Ober, Thomas Joseph McKinley, Gareth H. Massachusetts Institute of Technology. Department of Mechanical Engineering Ober, Thomas Joseph McKinley, Gareth H. Fardin, Marc-Antoine In the past twenty years, shear-banding flows have been probed by various techniques, such as rheometry, velocimetry and flow birefringence. In micellar solutions, many of the data collected exhibit unexplained spatiotemporal fluctuations. Recently, it has been suggested that those fluctuations originate from a purely elastic instability of the shear-banding flow. In cylindrical Couette geometry, the instability is reminiscent of the Taylor-like instability observed in viscoelastic polymer solutions. The criterion for purely elastic Taylor–Couette instability adapted to shear-banding flows suggested three categories of shear-banding depending on their stability. In the present study, we report on a large set of experimental data which demonstrates the existence of the three categories of shear-banding flows in various surfactant solutions. Consistent with theoretical predictions, increases in the surfactant concentration or in the curvature of the geometry destabilize the flow, whereas an increase in temperature stabilizes the flow. However, experiments also exhibit some interesting behaviors going beyond the purely elastic instability criterion. National Science Foundation (U.S.). Graduate Research Fellowship Program 2013-09-23T15:58:30Z 2013-09-23T15:58:30Z 2012-08 2012-06 Article http://purl.org/eprint/type/JournalArticle 1744-683X 1744-6848 http://hdl.handle.net/1721.1/80865 Fardin, M. A., T. J. Ober, V. Grenard, T. Divoux, S. Manneville, G. H. McKinley, and S. Lerouge. “Interplay between elastic instabilities and shear-banding: three categories of Taylor–Couette flows and beyond.” Soft Matter 8, no. 39 (2012): 10072. https://orcid.org/0000-0001-8323-2779 en_US http://dx.doi.org/10.1039/c2sm26313k Soft Matter Creative Commons Attribution-Noncommercial-Share Alike 3.0 http://creativecommons.org/licenses/by-nc-sa/3.0/ application/pdf Royal Society of Chemistry, The MIT web domain |
spellingShingle | Fardin, Marc-Antoine Grenard, V. Divoux, T. Manneville, S. Lerouge, S. Ober, Thomas Joseph McKinley, Gareth H. Interplay between elastic instabilities and shear-banding: three categories of Taylor–Couette flows and beyond |
title | Interplay between elastic instabilities and shear-banding: three categories of Taylor–Couette flows and beyond |
title_full | Interplay between elastic instabilities and shear-banding: three categories of Taylor–Couette flows and beyond |
title_fullStr | Interplay between elastic instabilities and shear-banding: three categories of Taylor–Couette flows and beyond |
title_full_unstemmed | Interplay between elastic instabilities and shear-banding: three categories of Taylor–Couette flows and beyond |
title_short | Interplay between elastic instabilities and shear-banding: three categories of Taylor–Couette flows and beyond |
title_sort | interplay between elastic instabilities and shear banding three categories of taylor couette flows and beyond |
url | http://hdl.handle.net/1721.1/80865 https://orcid.org/0000-0001-8323-2779 |
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