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Effect of blockage ratio on flow of a viscoelastic wormlike micellar solution past a cylinder in a microchannel

We present experiments on the flow of a viscoelastic wormlike micellar solution around cylinders (radius R) confined in straight microchannels (width W). Thirteen flow geometries are tested where the blockage ratio is varied over a wide range 0.055 ≤ B(R) = 2R/W ≤ 0.63. Experiments are performed at...

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Autores principales: Hopkins, Cameron C., Shen, Amy Q., Haward, Simon J.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: The Royal Society of Chemistry 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9709659/
https://www.ncbi.nlm.nih.gov/pubmed/36374283
http://dx.doi.org/10.1039/d2sm01162j
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author Hopkins, Cameron C.
Shen, Amy Q.
Haward, Simon J.
author_facet Hopkins, Cameron C.
Shen, Amy Q.
Haward, Simon J.
author_sort Hopkins, Cameron C.
collection PubMed
description We present experiments on the flow of a viscoelastic wormlike micellar solution around cylinders (radius R) confined in straight microchannels (width W). Thirteen flow geometries are tested where the blockage ratio is varied over a wide range 0.055 ≤ B(R) = 2R/W ≤ 0.63. Experiments are performed at negligible Reynolds number, and for Weissenberg numbers Wi = λU/R up to 1000, where U is the average flow speed and λ is the relaxation time of the fluid. Micro-particle image velocimetry is used to characterise the flow state at each B(R) and Wi. In all of the geometries, a first critical Weissenberg number marks a transition from symmetric flow to an asymmetric but time-steady flow state, while a second higher critical Weissenberg number marks the onset of time-dependent flows. However, we report a clear shift in behaviour over a narrow intermediate range of 0.33 ≲ B(R) ≲ 0.41. Channels with B(R) ≤ 0.33 fall in a ‘low’ B(R) regime, with instabilities that originate from the downstream stagnation point, while those with B(R) ≥ 0.44 fall in a ‘high’ BR regime, with instabilities developing at the upstream stagnation point. Behaviour within the newly-identified intermediate B(R) regime is complex due to the competing influence of the two stagnation points. We summarise all our results in a flow state diagram covering Wi–B(R) parameter space, clearly defining the different regimes of blockage ratio for the first time. Our results contribute to the understanding of the complexities of viscoelastic flow in this benchmark geometry.
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spelling pubmed-97096592022-12-20 Effect of blockage ratio on flow of a viscoelastic wormlike micellar solution past a cylinder in a microchannel Hopkins, Cameron C. Shen, Amy Q. Haward, Simon J. Soft Matter Chemistry We present experiments on the flow of a viscoelastic wormlike micellar solution around cylinders (radius R) confined in straight microchannels (width W). Thirteen flow geometries are tested where the blockage ratio is varied over a wide range 0.055 ≤ B(R) = 2R/W ≤ 0.63. Experiments are performed at negligible Reynolds number, and for Weissenberg numbers Wi = λU/R up to 1000, where U is the average flow speed and λ is the relaxation time of the fluid. Micro-particle image velocimetry is used to characterise the flow state at each B(R) and Wi. In all of the geometries, a first critical Weissenberg number marks a transition from symmetric flow to an asymmetric but time-steady flow state, while a second higher critical Weissenberg number marks the onset of time-dependent flows. However, we report a clear shift in behaviour over a narrow intermediate range of 0.33 ≲ B(R) ≲ 0.41. Channels with B(R) ≤ 0.33 fall in a ‘low’ B(R) regime, with instabilities that originate from the downstream stagnation point, while those with B(R) ≥ 0.44 fall in a ‘high’ BR regime, with instabilities developing at the upstream stagnation point. Behaviour within the newly-identified intermediate B(R) regime is complex due to the competing influence of the two stagnation points. We summarise all our results in a flow state diagram covering Wi–B(R) parameter space, clearly defining the different regimes of blockage ratio for the first time. Our results contribute to the understanding of the complexities of viscoelastic flow in this benchmark geometry. The Royal Society of Chemistry 2022-11-14 /pmc/articles/PMC9709659/ /pubmed/36374283 http://dx.doi.org/10.1039/d2sm01162j Text en This journal is © The Royal Society of Chemistry https://creativecommons.org/licenses/by/3.0/
spellingShingle Chemistry
Hopkins, Cameron C.
Shen, Amy Q.
Haward, Simon J.
Effect of blockage ratio on flow of a viscoelastic wormlike micellar solution past a cylinder in a microchannel
title Effect of blockage ratio on flow of a viscoelastic wormlike micellar solution past a cylinder in a microchannel
title_full Effect of blockage ratio on flow of a viscoelastic wormlike micellar solution past a cylinder in a microchannel
title_fullStr Effect of blockage ratio on flow of a viscoelastic wormlike micellar solution past a cylinder in a microchannel
title_full_unstemmed Effect of blockage ratio on flow of a viscoelastic wormlike micellar solution past a cylinder in a microchannel
title_short Effect of blockage ratio on flow of a viscoelastic wormlike micellar solution past a cylinder in a microchannel
title_sort effect of blockage ratio on flow of a viscoelastic wormlike micellar solution past a cylinder in a microchannel
topic Chemistry
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9709659/
https://www.ncbi.nlm.nih.gov/pubmed/36374283
http://dx.doi.org/10.1039/d2sm01162j
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