• 文献检索
  • 文档翻译
  • 深度研究
  • 学术资讯
  • Suppr Zotero 插件Zotero 插件
  • 邀请有礼
  • 套餐&价格
  • 历史记录
应用&插件
Suppr Zotero 插件Zotero 插件浏览器插件Mac 客户端Windows 客户端微信小程序
定价
高级版会员购买积分包购买API积分包
服务
文献检索文档翻译深度研究API 文档MCP 服务
关于我们
关于 Suppr公司介绍联系我们用户协议隐私条款
关注我们

Suppr 超能文献

核心技术专利:CN118964589B侵权必究
粤ICP备2023148730 号-1Suppr @ 2026

文献检索

告别复杂PubMed语法,用中文像聊天一样搜索,搜遍4000万医学文献。AI智能推荐,让科研检索更轻松。

立即免费搜索

文件翻译

保留排版,准确专业,支持PDF/Word/PPT等文件格式,支持 12+语言互译。

免费翻译文档

深度研究

AI帮你快速写综述,25分钟生成高质量综述,智能提取关键信息,辅助科研写作。

立即免费体验

表面粗糙度对微沟槽毛细上升的影响。

The effect of surface roughness on capillary rise in micro-grooves.

机构信息

Laboratory for Alternative Energy Conversion (LAEC), School of Mechatronic Systems Engineering, Simon Fraser University, Surrey, BC, V3T 0A3, Canada.

出版信息

Sci Rep. 2022 Sep 1;12(1):14867. doi: 10.1038/s41598-022-19111-w.

DOI:10.1038/s41598-022-19111-w
PMID:36050409
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9436964/
Abstract

The capillary action is a unique feature of micro-grooves with numerous applications. This spontaneous flow eliminates the need for an extra pumping device to deliver a liquid. Capillary action depends on physical properties and features of the solid surface, as well as on thermophysical properties of the liquid. In this study, our previously proposed unifying capillary rise model is extended to include the effect of surface roughness. A new characteristic length scale is proposed that includes salient geometrical parameters, such as micro-grooves height, width, and surface roughness. Furthermore, it is shown that by using the proposed characteristic length scale, it can be determined whether the capillary action would occur in a given micro-groove and liquid. Various metallic and polymeric surfaces with a wide range of surface roughness are fabricated from aluminum, stainless-steel, natural graphite sheet, and 3D-printed stainless-steel and a polymer. A profilometer and sessile drop method are used to measure surface roughness and the contact angles, respectively. The present unifying model is compared against our measured data, and it is shown that it can predict the capillary rise in rough micro-grooves with less than a 10% relative difference. It is observed that the capillary height can be increased for a wetting surface by introducing surface roughness and by using optimal micro-groove cross-sections that are triangular as opposed to rectangular. The proposed compact, unifying model can be used to predict the capillary rise for any given micro-groove cross-section, and as a design tool for numerous industrial and biomedical applications, such as heat pipes, power electronic cooling solutions, sorption systems, medicine delivery devices, and microfluidics that utilize capillary micro-grooves.

摘要

毛细作用是具有众多应用的微槽的独特特征。这种自发流动不需要额外的泵送装置来输送液体。毛细作用取决于固体表面的物理特性和特征,以及液体的热物理特性。在这项研究中,我们之前提出的统一毛细上升模型被扩展到包括表面粗糙度的影响。提出了一个新的特征长度尺度,该尺度包括突出的几何参数,如微槽的高度、宽度和表面粗糙度。此外,结果表明,通过使用所提出的特征长度尺度,可以确定在给定的微槽和液体中是否会发生毛细作用。使用轮廓仪和悬滴法分别测量表面粗糙度和接触角,从铝、不锈钢、天然石墨片以及 3D 打印不锈钢和聚合物制造了具有广泛表面粗糙度的各种金属和聚合物表面。将现有的统一模型与我们的测量数据进行比较,结果表明,它可以预测具有小于 10%相对差异的粗糙微槽中的毛细上升。观察到通过引入表面粗糙度并使用三角形而不是矩形的最佳微槽横截面,可以增加润湿表面的毛细高度。所提出的紧凑统一模型可用于预测任何给定微槽横截面的毛细上升,并且可作为许多工业和生物医学应用的设计工具,例如热管、电力电子冷却解决方案、吸附系统、药物输送装置和利用毛细微槽的微流控。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/099647685f28/41598_2022_19111_Fig16_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/830ac289f303/41598_2022_19111_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/b30d32d3893b/41598_2022_19111_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/fd65c44583cc/41598_2022_19111_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/a27658b0e31b/41598_2022_19111_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/31c1716c93e3/41598_2022_19111_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/d94ed3d68067/41598_2022_19111_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/0e797e24e629/41598_2022_19111_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/738f58832326/41598_2022_19111_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/29261990374f/41598_2022_19111_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/2d57a0e9bfe8/41598_2022_19111_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/40eec4eecd67/41598_2022_19111_Fig11_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/afa1df44db78/41598_2022_19111_Fig12_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/25e336b697a7/41598_2022_19111_Fig13_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/49f030dca55b/41598_2022_19111_Fig14_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/a7d8878c591b/41598_2022_19111_Fig15_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/099647685f28/41598_2022_19111_Fig16_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/830ac289f303/41598_2022_19111_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/b30d32d3893b/41598_2022_19111_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/fd65c44583cc/41598_2022_19111_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/a27658b0e31b/41598_2022_19111_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/31c1716c93e3/41598_2022_19111_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/d94ed3d68067/41598_2022_19111_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/0e797e24e629/41598_2022_19111_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/738f58832326/41598_2022_19111_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/29261990374f/41598_2022_19111_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/2d57a0e9bfe8/41598_2022_19111_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/40eec4eecd67/41598_2022_19111_Fig11_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/afa1df44db78/41598_2022_19111_Fig12_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/25e336b697a7/41598_2022_19111_Fig13_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/49f030dca55b/41598_2022_19111_Fig14_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/a7d8878c591b/41598_2022_19111_Fig15_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3fa/9436964/099647685f28/41598_2022_19111_Fig16_HTML.jpg

相似文献

1
The effect of surface roughness on capillary rise in micro-grooves.表面粗糙度对微沟槽毛细上升的影响。
Sci Rep. 2022 Sep 1;12(1):14867. doi: 10.1038/s41598-022-19111-w.
2
A general form of capillary rise equation in micro-grooves.微槽中毛细上升方程的一般形式。
Sci Rep. 2020 Nov 12;10(1):19709. doi: 10.1038/s41598-020-76682-2.
3
3D printed aluminum flat heat pipes with micro grooves for efficient thermal management of high power LEDs.用于高功率发光二极管高效热管理的带微槽的3D打印铝制扁平热管。
Sci Rep. 2021 Apr 15;11(1):8255. doi: 10.1038/s41598-021-87798-4.
4
Wetting morphologies at microstructured surfaces.微结构表面的润湿形态
Proc Natl Acad Sci U S A. 2005 Feb 8;102(6):1848-52. doi: 10.1073/pnas.0407721102. Epub 2005 Jan 27.
5
Revealing How Topography of Surface Microstructures Alters Capillary Spreading.揭示表面微观结构的地形如何改变毛细扩散。
Sci Rep. 2019 May 24;9(1):7787. doi: 10.1038/s41598-019-44243-x.
6
Wetting and Imbibition Characteristics of Biofilms Grown on Stainless Steel.不锈钢生物膜的润湿和吸液特性。
Langmuir. 2022 Aug 16;38(32):9810-9821. doi: 10.1021/acs.langmuir.2c00828. Epub 2022 Jul 5.
7
Surfactant solutions and porous substrates: spreading and imbibition.表面活性剂溶液与多孔基质:铺展与吸液
Adv Colloid Interface Sci. 2004 Nov 29;111(1-2):3-27. doi: 10.1016/j.cis.2004.07.007.
8
Molecular dynamics investigation of surface roughness scale effect on interfacial thermal conductance at solid-liquid interfaces.分子动力学研究固体-液体界面表面粗糙度对界面热导的尺度效应。
J Chem Phys. 2019 Mar 21;150(11):114705. doi: 10.1063/1.5081103.
9
Hierarchical surfaces: an in situ investigation into nano and micro scale wettability.分层表面:纳米和微观尺度润湿性的原位研究。
Faraday Discuss. 2010;146:223-32; discussion 283-98, 395-401. doi: 10.1039/b927136h.
10
Wetting morphologies and their transitions in grooved substrates.沟槽基底中的润湿形态及其转变。
J Phys Condens Matter. 2011 May 11;23(18):184108. doi: 10.1088/0953-8984/23/18/184108. Epub 2011 Apr 20.

引用本文的文献

1
Hybrid solar photovoltaic conversion and water desalination via quad-band fano-resonant optical coatings and superwicking cooling.通过四波段法诺共振光学涂层和超芯吸冷却实现混合太阳能光伏转换与海水淡化。
Light Sci Appl. 2025 Apr 17;14(1):165. doi: 10.1038/s41377-025-01796-z.
2
On the Dynamic Contact Angle of Capillary-Driven Microflows in Open Channels.关于明渠中毛细驱动微流的动态接触角
Langmuir. 2024 Apr 2;40(13):7215-7224. doi: 10.1021/acs.langmuir.4c00391. Epub 2024 Mar 21.
3
Nanoscale Porosity in Microellipsoids Cloaks Interparticle Capillary Attraction at Fluid Interfaces.

本文引用的文献

1
A numerical solution to the effects of surface roughness on water-coal contact angle.表面粗糙度对水-煤接触角影响的数值解。
Sci Rep. 2021 Jan 11;11(1):459. doi: 10.1038/s41598-020-80729-9.
2
A general form of capillary rise equation in micro-grooves.微槽中毛细上升方程的一般形式。
Sci Rep. 2020 Nov 12;10(1):19709. doi: 10.1038/s41598-020-76682-2.
3
Forces, pressures and energies associated with liquid rising in nonuniform capillary tubes.与液体在非均匀毛细管中上升相关的力、压力和能量。
微球中的纳米级孔隙在流体界面处掩盖了颗粒间的毛细吸引力。
ACS Nano. 2023 Jun 27;17(12):11892-11904. doi: 10.1021/acsnano.3c03301. Epub 2023 Jun 5.
J Colloid Interface Sci. 2015 Jul 15;450:135-140. doi: 10.1016/j.jcis.2015.03.007. Epub 2015 Mar 14.
4
Dynamics of capillary-driven liquid-liquid displacement in open microchannels.开放微通道中毛细驱动的液-液置换动力学
Phys Chem Chem Phys. 2014 Nov 28;16(44):24473-8. doi: 10.1039/c4cp03910f.
5
On the shape of a hydrostatic meniscus attached to a corrugated plate or wavy cylinder.关于附着在波纹板或波状圆柱上的液体静压弯月面的形状。
J Colloid Interface Sci. 2011 Apr 15;356(2):763-74. doi: 10.1016/j.jcis.2011.01.040. Epub 2011 Jan 21.
6
Capillarity at the nanoscale.纳米尺度的毛细现象。
Chem Soc Rev. 2010 Mar;39(3):1096-114. doi: 10.1039/b909101g. Epub 2010 Feb 2.
7
Hysteresis during contact angles measurement.接触角测量中的滞后现象。
J Colloid Interface Sci. 2010 Mar 15;343(2):574-83. doi: 10.1016/j.jcis.2009.11.055. Epub 2009 Dec 4.
8
An analytic solution of capillary rise restrained by gravity.重力抑制下毛细上升的解析解。
J Colloid Interface Sci. 2008 Apr 1;320(1):259-63. doi: 10.1016/j.jcis.2008.01.009. Epub 2008 Jan 13.
9
As-placed contact angles for sessile drops.静置液滴的放置时接触角。
J Colloid Interface Sci. 2008 Jan 1;317(1):241-6. doi: 10.1016/j.jcis.2007.09.029. Epub 2007 Sep 18.
10
On the derivation of Young's equation for sessile drops: nonequilibrium effects due to evaporation.关于固着液滴杨氏方程的推导:蒸发引起的非平衡效应。
J Phys Chem B. 2007 May 17;111(19):5277-83. doi: 10.1021/jp065348g. Epub 2007 Apr 25.