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Self-determined shapes and velocities of giant near-zero drag gas cavities
Minimizing the retarding force on a solid moving in liquid is the canonical problem in the quest for energy saving by friction and drag reduction. For an ideal object that cannot sustain any shear stress on its surface, theory predicts that drag force will fall to zero as its speed becomes large. Ho...
Autores principales: | , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Association for the Advancement of Science
2017
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5590785/ https://www.ncbi.nlm.nih.gov/pubmed/28913434 http://dx.doi.org/10.1126/sciadv.1701558 |
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author | Vakarelski, Ivan U. Klaseboer, Evert Jetly, Aditya Mansoor, Mohammad M. Aguirre-Pablo, Andres A. Chan, Derek Y. C. Thoroddsen, Sigurdur T. |
author_facet | Vakarelski, Ivan U. Klaseboer, Evert Jetly, Aditya Mansoor, Mohammad M. Aguirre-Pablo, Andres A. Chan, Derek Y. C. Thoroddsen, Sigurdur T. |
author_sort | Vakarelski, Ivan U. |
collection | PubMed |
description | Minimizing the retarding force on a solid moving in liquid is the canonical problem in the quest for energy saving by friction and drag reduction. For an ideal object that cannot sustain any shear stress on its surface, theory predicts that drag force will fall to zero as its speed becomes large. However, experimental verification of this prediction has been challenging. We report the construction of a class of self-determined streamlined structures with this free-slip surface, made up of a teardrop-shaped giant gas cavity that completely encloses a metal sphere. This stable gas cavity is formed around the sphere as it plunges at a sufficiently high speed into the liquid in a deep tank, provided that the sphere is either heated initially to above the Leidenfrost temperature of the liquid or rendered superhydrophobic in water at room temperature. These sphere-in-cavity structures have residual drag coefficients that are typically less than [Formula: see text] those of solid objects of the same dimensions, which indicates that they experienced very small drag forces. The self-determined shapes of the gas cavities are shown to be consistent with the Bernoulli equation of potential flow applied on the cavity surface. The cavity fall velocity is not arbitrary but is uniquely predicted by the sphere density and cavity volume, so larger cavities have higher characteristic velocities. |
format | Online Article Text |
id | pubmed-5590785 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2017 |
publisher | American Association for the Advancement of Science |
record_format | MEDLINE/PubMed |
spelling | pubmed-55907852017-09-14 Self-determined shapes and velocities of giant near-zero drag gas cavities Vakarelski, Ivan U. Klaseboer, Evert Jetly, Aditya Mansoor, Mohammad M. Aguirre-Pablo, Andres A. Chan, Derek Y. C. Thoroddsen, Sigurdur T. Sci Adv Research Articles Minimizing the retarding force on a solid moving in liquid is the canonical problem in the quest for energy saving by friction and drag reduction. For an ideal object that cannot sustain any shear stress on its surface, theory predicts that drag force will fall to zero as its speed becomes large. However, experimental verification of this prediction has been challenging. We report the construction of a class of self-determined streamlined structures with this free-slip surface, made up of a teardrop-shaped giant gas cavity that completely encloses a metal sphere. This stable gas cavity is formed around the sphere as it plunges at a sufficiently high speed into the liquid in a deep tank, provided that the sphere is either heated initially to above the Leidenfrost temperature of the liquid or rendered superhydrophobic in water at room temperature. These sphere-in-cavity structures have residual drag coefficients that are typically less than [Formula: see text] those of solid objects of the same dimensions, which indicates that they experienced very small drag forces. The self-determined shapes of the gas cavities are shown to be consistent with the Bernoulli equation of potential flow applied on the cavity surface. The cavity fall velocity is not arbitrary but is uniquely predicted by the sphere density and cavity volume, so larger cavities have higher characteristic velocities. American Association for the Advancement of Science 2017-09-08 /pmc/articles/PMC5590785/ /pubmed/28913434 http://dx.doi.org/10.1126/sciadv.1701558 Text en Copyright © 2017 The Authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original U.S. Government Works. Distributed under a Creative Commons Attribution NonCommercial License 4.0 (CC BY-NC). http://creativecommons.org/licenses/by-nc/4.0/ This is an open-access article distributed under the terms of the Creative Commons Attribution-NonCommercial license (http://creativecommons.org/licenses/by-nc/4.0/) , which permits use, distribution, and reproduction in any medium, so long as the resultant use is not for commercial advantage and provided the original work is properly cited. |
spellingShingle | Research Articles Vakarelski, Ivan U. Klaseboer, Evert Jetly, Aditya Mansoor, Mohammad M. Aguirre-Pablo, Andres A. Chan, Derek Y. C. Thoroddsen, Sigurdur T. Self-determined shapes and velocities of giant near-zero drag gas cavities |
title | Self-determined shapes and velocities of giant near-zero drag gas cavities |
title_full | Self-determined shapes and velocities of giant near-zero drag gas cavities |
title_fullStr | Self-determined shapes and velocities of giant near-zero drag gas cavities |
title_full_unstemmed | Self-determined shapes and velocities of giant near-zero drag gas cavities |
title_short | Self-determined shapes and velocities of giant near-zero drag gas cavities |
title_sort | self-determined shapes and velocities of giant near-zero drag gas cavities |
topic | Research Articles |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5590785/ https://www.ncbi.nlm.nih.gov/pubmed/28913434 http://dx.doi.org/10.1126/sciadv.1701558 |
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