• 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

液滴撞击加热壁面过程中的热毛细中心薄片凹陷

Thermocapillary central lamella recess during droplet impacts onto a heated wall.

作者信息

Palmetshofer Patrick, Geppert Anne K, Steigerwald Jonas, Arcos Marz Tim, Weigand Bernhard

机构信息

Institute of Aerospace Thermodynamics, University of Stuttgart, 70569, Stuttgart, Germany.

出版信息

Sci Rep. 2024 Jan 11;14(1):1102. doi: 10.1038/s41598-024-51382-3.

DOI:10.1038/s41598-024-51382-3
PMID:38212423
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC10784541/
Abstract

We experimentally observe a new phenomenon, the formation of a toroidal region of lower film thickness in the center of the lamella formed during high Weber number water droplet impacts onto smooth heated walls. This region forms around the air bubble, which is entrapped during the initial impact phase at the impact center. Our study encompasses a variation of the droplet size, impact velocity, surface wettability and temperature. We show how this phenomenon can be explained considering a two-step process involving thermocapillary convection in two separate regions: The temperature gradient along the surface of the entrapped air bubble caused by heat conduction induces flow that pumps warmer liquid to the lamella-ambient interface due to the Marangoni effect. The non-uniform temperature distribution along it then causes fluid acceleration in the radial direction, depleting the fluid volume around the bubble in a self-amplifying manner. We use direct numerical simulations of a stagnant liquid film with an enclosed bubble at the wall to confirm this theory.

摘要

我们通过实验观察到一种新现象,即在高韦伯数水滴冲击光滑加热壁面过程中形成的薄片中心出现了一个薄膜厚度较低的环形区域。该区域围绕着气泡形成,气泡在初始冲击阶段于冲击中心处被截留。我们的研究涵盖了液滴尺寸、冲击速度、表面润湿性和温度的变化。我们展示了如何通过一个两步过程来解释这一现象,该过程涉及两个独立区域的热毛细对流:由热传导引起的截留气泡表面的温度梯度会引发流动,由于马兰戈尼效应,这种流动会将较热的液体泵送到薄片与周围环境的界面。沿其不均匀的温度分布随后会导致流体在径向方向上加速,以自增强的方式耗尽气泡周围的流体体积。我们使用壁面处带有封闭气泡的静止液膜的直接数值模拟来证实这一理论。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6248/10784541/4e701b6dac32/41598_2024_51382_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6248/10784541/b52930f36de4/41598_2024_51382_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6248/10784541/5c63f4493246/41598_2024_51382_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6248/10784541/e9bac9ab586d/41598_2024_51382_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6248/10784541/106d32a06f13/41598_2024_51382_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6248/10784541/837515f423ef/41598_2024_51382_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6248/10784541/96a7ae53b91d/41598_2024_51382_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6248/10784541/4e701b6dac32/41598_2024_51382_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6248/10784541/b52930f36de4/41598_2024_51382_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6248/10784541/5c63f4493246/41598_2024_51382_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6248/10784541/e9bac9ab586d/41598_2024_51382_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6248/10784541/106d32a06f13/41598_2024_51382_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6248/10784541/837515f423ef/41598_2024_51382_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6248/10784541/96a7ae53b91d/41598_2024_51382_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6248/10784541/4e701b6dac32/41598_2024_51382_Fig7_HTML.jpg

相似文献

1
Thermocapillary central lamella recess during droplet impacts onto a heated wall.液滴撞击加热壁面过程中的热毛细中心薄片凹陷
Sci Rep. 2024 Jan 11;14(1):1102. doi: 10.1038/s41598-024-51382-3.
2
Numerical investigation of bubble-induced Marangoni convection.气泡诱导的马兰戈尼对流的数值研究。
Ann N Y Acad Sci. 2009 Apr;1161:304-20. doi: 10.1111/j.1749-6632.2008.04332.x.
3
Circulating Marangoni flows within droplets in smectic films.近晶膜中液滴内的循环马兰戈尼流。
Phys Rev E. 2022 Nov;106(5-2):055105. doi: 10.1103/PhysRevE.106.055105.
4
Thermocapillary convection around gas bubbles: an important natural effect for the enhancement of heat transfer in liquids under microgravity.气泡周围的热毛细对流:微重力条件下增强液体传热的一种重要自然效应。
Ann N Y Acad Sci. 2002 Oct;974:220-45. doi: 10.1111/j.1749-6632.2002.tb05910.x.
5
Influence of Marangoni Effect on Heat and Mass Transfer during Evaporation of Sessile Microdroplets.马兰戈尼效应对静态微滴蒸发过程中传热传质的影响。
Micromachines (Basel). 2022 Nov 13;13(11):1968. doi: 10.3390/mi13111968.
6
Thermocapillary convection during subcooled boiling in reduced gravity environments.微重力环境下过冷沸腾过程中的热毛细对流。
Ann N Y Acad Sci. 2009 Apr;1161:173-81. doi: 10.1111/j.1749-6632.2008.04327.x.
7
Numerical Investigation of the Flow Dynamics and Evaporative Cooling of Water Droplets Impinging onto Heated Surfaces: An Effective Approach To Identify Spray Cooling Mechanisms.数值研究水滴撞击受热表面的流动动力学和蒸发冷却:一种识别喷雾冷却机制的有效方法。
Langmuir. 2016 Sep 13;32(36):9135-55. doi: 10.1021/acs.langmuir.6b02205. Epub 2016 Aug 30.
8
Measurement of the lamella thickness during droplet impact onto differently wettable smooth surfaces using an extension of the LASER Pattern Shift Method with naturally occurring patterns.
Rev Sci Instrum. 2021 Oct 1;92(10):105111. doi: 10.1063/5.0060407.
9
Dynamics of a wetting layer and Marangoni convection in microgravity.
Phys Rev E Stat Nonlin Soft Matter Phys. 2011 Aug;84(2 Pt 1):021202. doi: 10.1103/PhysRevE.84.021202. Epub 2011 Aug 22.
10
Thermocapillary Flow and Aggregation of Bubbles on a Solid Wall.热毛细流动与固体壁面上气泡的聚集
J Colloid Interface Sci. 2000 Dec 1;232(1):111-120. doi: 10.1006/jcis.2000.7210.

本文引用的文献

1
Measurement of the lamella thickness during droplet impact onto differently wettable smooth surfaces using an extension of the LASER Pattern Shift Method with naturally occurring patterns.
Rev Sci Instrum. 2021 Oct 1;92(10):105111. doi: 10.1063/5.0060407.
2
Bubble entrapment during the recoil of an impacting droplet.撞击液滴回弹过程中的气泡截留。
Microsyst Nanoeng. 2020 Jun 29;6:36. doi: 10.1038/s41378-020-0158-y. eCollection 2020.
3
Air entrapment and bubble formation during droplet impact onto a single cubic pillar.液滴撞击单个立方柱体过程中的气体截留与气泡形成。
Sci Rep. 2021 Sep 9;11(1):18018. doi: 10.1038/s41598-021-97376-3.
4
Dynamics of high-speed micro-drop impact: numerical simulations and experiments at frame-to-frame times below 100 ns.高速微滴撞击动力学:低于100纳秒逐帧时间的数值模拟与实验
Soft Matter. 2015 Mar 7;11(9):1708-22. doi: 10.1039/c4sm02474e.
5
How does an air film evolve into a bubble during drop impact?在液滴撞击过程中,气膜是如何演变成气泡的?
Phys Rev Lett. 2012 Nov 16;109(20):204501. doi: 10.1103/PhysRevLett.109.204501. Epub 2012 Nov 13.
6
Skating on a film of air: drops impacting on a surface.在气膜上滑行:液滴撞击表面。
Phys Rev Lett. 2012 Feb 17;108(7):074503. doi: 10.1103/PhysRevLett.108.074503. Epub 2012 Feb 15.
7
Numerical investigation of bubble-induced Marangoni convection.气泡诱导的马兰戈尼对流的数值研究。
Ann N Y Acad Sci. 2009 Apr;1161:304-20. doi: 10.1111/j.1749-6632.2008.04332.x.
8
Singular jets and bubbles in drop impact.液滴撞击中的奇异射流和气泡。
Phys Rev Lett. 2006 Mar 31;96(12):124501. doi: 10.1103/PhysRevLett.96.124501. Epub 2006 Mar 27.