F. Virot, G. Tymen, D. Hébert, J.-L. Rullier, E. Lescoute
{"title":"Experimental investigation of the interaction between a water droplet and a shock wave above Mach 4","authors":"F. Virot, G. Tymen, D. Hébert, J.-L. Rullier, E. Lescoute","doi":"10.1007/s00193-023-01139-0","DOIUrl":null,"url":null,"abstract":"<div><p>Experimental results on the interactions between a single water droplet and a shock wave propagating at Mach number above 4 are presented in this paper. A detonation-driven shock-tube test facility is used to work within a Mach range at <span>\\({M}=4.3\\)</span> (high-supersonic regime) and <span>\\({M}=10.6\\)</span> (hypersonic regime), for which the maximum studied dimensionless times <i>T</i> are up to 9.4 and 5.5, respectively. For both Mach ranges, the initial droplet diameters typically vary between 430 and 860 <span>\\(\\upmu \\hbox {m}\\)</span> and the associated Weber numbers vary from <span>\\(5 \\times 10^{4}\\)</span> to <span>\\(11 \\times 10^{4}\\)</span>. Ultra-high-speed cameras are used to record the evolution of the water droplet when the shock wave impacts it. Until <span>\\({T} \\approx 2.5\\)</span>, the qualitative and quantitative analyses of our frames show that the initial diameter as well as the Mach number studied have an apparent weak influence on the droplet dimensionless displacement. Beyond this time, the results for <span>\\({M}=10.6\\)</span> are more dispersed than the data for <span>\\({M}=4.3\\)</span> revealing a possible effect of the droplet size. One of the main results of this paper is that the droplet disappearance occurs at <span>\\({T}=[4.5\\)</span>–5.5] for <span>\\({M}=10.6\\)</span>, while some mist is still present at <span>\\({T}>9\\)</span> for <span>\\({M}=4.3\\)</span>. We note also that the droplet is always supersonic for <span>\\({M}=10.6\\)</span> whereas it becomes subsonic at <span>\\({T}\\approx 3.5\\)</span> for <span>\\({M}=4.3\\)</span>.</p></div>","PeriodicalId":775,"journal":{"name":"Shock Waves","volume":null,"pages":null},"PeriodicalIF":1.7000,"publicationDate":"2023-08-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Shock Waves","FirstCategoryId":"5","ListUrlMain":"https://link.springer.com/article/10.1007/s00193-023-01139-0","RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"MECHANICS","Score":null,"Total":0}
引用次数: 0
Abstract
Experimental results on the interactions between a single water droplet and a shock wave propagating at Mach number above 4 are presented in this paper. A detonation-driven shock-tube test facility is used to work within a Mach range at \({M}=4.3\) (high-supersonic regime) and \({M}=10.6\) (hypersonic regime), for which the maximum studied dimensionless times T are up to 9.4 and 5.5, respectively. For both Mach ranges, the initial droplet diameters typically vary between 430 and 860 \(\upmu \hbox {m}\) and the associated Weber numbers vary from \(5 \times 10^{4}\) to \(11 \times 10^{4}\). Ultra-high-speed cameras are used to record the evolution of the water droplet when the shock wave impacts it. Until \({T} \approx 2.5\), the qualitative and quantitative analyses of our frames show that the initial diameter as well as the Mach number studied have an apparent weak influence on the droplet dimensionless displacement. Beyond this time, the results for \({M}=10.6\) are more dispersed than the data for \({M}=4.3\) revealing a possible effect of the droplet size. One of the main results of this paper is that the droplet disappearance occurs at \({T}=[4.5\)–5.5] for \({M}=10.6\), while some mist is still present at \({T}>9\) for \({M}=4.3\). We note also that the droplet is always supersonic for \({M}=10.6\) whereas it becomes subsonic at \({T}\approx 3.5\) for \({M}=4.3\).
期刊介绍:
Shock Waves provides a forum for presenting and discussing new results in all fields where shock and detonation phenomena play a role. The journal addresses physicists, engineers and applied mathematicians working on theoretical, experimental or numerical issues, including diagnostics and flow visualization.
The research fields considered include, but are not limited to, aero- and gas dynamics, acoustics, physical chemistry, condensed matter and plasmas, with applications encompassing materials sciences, space sciences, geosciences, life sciences and medicine.
Of particular interest are contributions which provide insights into fundamental aspects of the techniques that are relevant to more than one specific research community.
The journal publishes scholarly research papers, invited review articles and short notes, as well as comments on papers already published in this journal. Occasionally concise meeting reports of interest to the Shock Waves community are published.