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在卡西-巴克斯特状态下通过表面几何形状调节润湿性

Tuning Wetting Properties Through Surface Geometry in the Cassie-Baxter State.

作者信息

Scheff Talya, Acha Florence, Diaz Armas Nathalia, Mead Joey L, Zhang Jinde

机构信息

Department of Plastics Engineering, University of Massachusetts Lowell, Lowell, MA 01854, USA.

出版信息

Biomimetics (Basel). 2025 Jan 2;10(1):20. doi: 10.3390/biomimetics10010020.

DOI:10.3390/biomimetics10010020
PMID:39851736
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11762741/
Abstract

Superhydrophobic coatings are beneficial for applications like self-cleaning, anti-corrosion, and drag reduction. In this study, we investigated the impact of surface geometry on the static, dynamic, and sliding contact angles in the Cassie-Baxter state. We used fluoro-silane-treated silicon micro-post patterns fabricated via lithography as model surfaces. By varying the solid fraction (ϕ), edge-to-edge spacing (L), and the shape and arrangement of the micro-posts, we examined how these geometric factors influence wetting behavior. Our results show that the solid fraction is the key factor affecting both dynamic and sliding angles, while changes in shape and arrangement had minimal impact. The Cassie-Baxter model accurately predicted receding angles but struggled to predict advancing angles. These insights can guide the development of coatings with enhanced superhydrophobic properties, tailored to achieve higher contact angles and customized for different environmental conditions.

摘要

超疏水涂层有利于自清洁、防腐和减阻等应用。在本研究中,我们研究了表面几何形状对Cassie-Baxter状态下的静态、动态和滑动接触角的影响。我们使用通过光刻制造的氟硅烷处理的硅微柱图案作为模型表面。通过改变固体分数(ϕ)、边到边间距(L)以及微柱的形状和排列,我们研究了这些几何因素如何影响润湿行为。我们的结果表明,固体分数是影响动态角和滑动角的关键因素,而形状和排列的变化影响最小。Cassie-Baxter模型准确地预测了后退角,但难以预测前进角。这些见解可以指导具有增强超疏水性能的涂层的开发,以实现更高的接触角并针对不同的环境条件进行定制。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/2fcb8c520fb2/biomimetics-10-00020-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/ae1b1d591a15/biomimetics-10-00020-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/e3f4c3f70037/biomimetics-10-00020-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/8fa7d75a0b77/biomimetics-10-00020-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/100e0cbbefc7/biomimetics-10-00020-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/2d5371a5091e/biomimetics-10-00020-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/b5065ddbab5d/biomimetics-10-00020-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/bfc68d1c5052/biomimetics-10-00020-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/0682d0116d3a/biomimetics-10-00020-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/e23ca765411c/biomimetics-10-00020-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/efb294a9262c/biomimetics-10-00020-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/1ccc0a75c1a4/biomimetics-10-00020-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/e40e5f953ada/biomimetics-10-00020-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/2fcb8c520fb2/biomimetics-10-00020-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/ae1b1d591a15/biomimetics-10-00020-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/e3f4c3f70037/biomimetics-10-00020-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/8fa7d75a0b77/biomimetics-10-00020-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/100e0cbbefc7/biomimetics-10-00020-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/2d5371a5091e/biomimetics-10-00020-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/b5065ddbab5d/biomimetics-10-00020-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/bfc68d1c5052/biomimetics-10-00020-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/0682d0116d3a/biomimetics-10-00020-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/e23ca765411c/biomimetics-10-00020-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/efb294a9262c/biomimetics-10-00020-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/1ccc0a75c1a4/biomimetics-10-00020-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/e40e5f953ada/biomimetics-10-00020-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5329/11762741/2fcb8c520fb2/biomimetics-10-00020-g013.jpg

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High-resolution liquid patterns via three-dimensional droplet shape control.通过三维液滴形状控制实现高分辨率液相图案。
Nat Commun. 2014 Sep 25;5:4975. doi: 10.1038/ncomms5975.
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Reliable measurement of the receding contact angle.可靠的后退接触角测量。
Langmuir. 2013 Mar 26;29(12):3858-63. doi: 10.1021/la400009m. Epub 2013 Mar 11.
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An effect of silicon micro-nano-patterning arrays on superhydrophobic surface.硅微纳图案阵列对超疏水表面的影响。
J Nanosci Nanotechnol. 2011 Oct;11(10):8967-73. doi: 10.1166/jnn.2011.3505.
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A modified Cassie-Baxter relationship to explain contact angle hysteresis and anisotropy on non-wetting textured surfaces.一种修正的Cassie-Baxter关系,用于解释非润湿性纹理表面上的接触角滞后和各向异性。
J Colloid Interface Sci. 2009 Nov 1;339(1):208-16. doi: 10.1016/j.jcis.2009.07.027. Epub 2009 Jul 17.
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Petal effect: a superhydrophobic state with high adhesive force.花瓣效应:一种具有高附着力的超疏水状态。
Langmuir. 2008 Apr 15;24(8):4114-9. doi: 10.1021/la703821h. Epub 2008 Mar 1.
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Comment on How Wenzel and Cassie Were Wrong by Gao and McCarthy.高和麦卡锡对温泽尔和卡西错误之处的评论。
Langmuir. 2007 Dec 18;23(26):13242; discussion 13243. doi: 10.1021/la7022117. Epub 2007 Nov 15.
8
On the range of applicability of the Wenzel and Cassie equations.关于文泽尔方程和卡西方程的适用范围。
Langmuir. 2007 Sep 11;23(19):9919-20. doi: 10.1021/la701324m. Epub 2007 Aug 1.
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Cassie and Wenzel: were they really so wrong?卡西和温泽尔:他们真的错得那么离谱吗?
Langmuir. 2007 Jul 17;23(15):8200-5. doi: 10.1021/la7011167. Epub 2007 Jun 20.
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How Wenzel and cassie were wrong.温泽尔和卡西是如何出错的。
Langmuir. 2007 Mar 27;23(7):3762-5. doi: 10.1021/la062634a. Epub 2007 Feb 22.