Geometric mixing

Author:

Arrieta Jorge1ORCID,Cartwright Julyan H. E.23ORCID,Gouillart Emmanuelle4ORCID,Piro Nicolas5ORCID,Piro Oreste6ORCID,Tuval Idan16ORCID

Affiliation:

1. Institut Mediterrani d’Estudis Avançats, CSIC–Universitat de les Illes Balears, 07190 Esporles, Spain

2. Instituto Andaluz de Ciencias de la Tierra, CSIC–Universidad de Granada, 18100 Armilla, Granada, Spain

3. Instituto Carlos I de Física Teórica y Computacional, Universidad de Granada, 18071 Granada, Spain

4. Joint Unit CNRS Saint-Gobain, 93303 Aubervilliers, France

5. École Polytechnique Fédérale de Lausanne, 1015 Lausanne, Switzerland

6. Departament de Física, Universitat de les Illes Balears, 07071 Palma de Mallorca, Spain

Abstract

Mixing fluids often involves a periodic action, like stirring one’s tea. But reciprocating motions in fluids at low Reynolds number, in Stokes flows where inertia is negligible, lead to periodic cycles of mixing and unmixing, because the physics, molecular diffusion excepted, is time reversible. So how can fluid be mixed in such circumstances? The answer involves a geometric phase. Geometric phases are found everywhere in physics as anholonomies, where after a closed circuit in the parameters, some system variables do not return to their original values. We discuss the geometric phase in fluid mixing: geometric mixing. This article is part of the theme issue ‘Stokes at 200 (part 2)’.

Funder

Spanish Ministry of Economy and Competitiveness

Govern de les Illes Balears

Publisher

The Royal Society

Subject

General Physics and Astronomy,General Engineering,General Mathematics

Reference49 articles.

1. On the effect of the internal friction of fluids on the motion of pendulums;Stokes GG;Trans. Camb. Phil. Soc.,1851

2. Taylor GI. 1960 Low Reynolds number flow . Scotsdale AZ: Educational Services Incorporated. (16 mm film).

3. An Unmixing Demonstration

4. Quantal phase factors accompanying adiabatic changes

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