{"id":145348,"date":"2026-07-01T09:00:07","date_gmt":"2026-07-01T01:00:07","guid":{"rendered":"https:\/\/www.curtin.edu.au\/research\/?post_type=hdr-r-projects&#038;p=145348"},"modified":"2026-07-01T09:00:11","modified_gmt":"2026-07-01T01:00:11","slug":"modelling-oxide-skin-rupture-in-liquid-metal-vortex-fluidic-reactors","status":"publish","type":"hdr-r-projects","link":"https:\/\/www.curtin.edu.au\/research\/hdr-r-projects\/modelling-oxide-skin-rupture-in-liquid-metal-vortex-fluidic-reactors\/","title":{"rendered":"Modelling Oxide-Skin Rupture in Liquid-Metal Vortex-Fluidic Reactors"},"content":{"rendered":"\n<p class=\"wp-block-paragraph\">This project develops a three-level mathematical framework to solve the &#8220;no-go&#8221; paradox of the Liquid-Metal Vortex-Fluidic Device (LM-VFD), where standard centrifugal forces are theoretically 1,000 times too weak to break the metal&#8217;s protective oxide skin. By building a hierarchy of models, we aim to identify a &#8220;triple-mechanism bridge&#8221; comprising capillary stress from microscopic spikes, wave-mode collisions, and Marangoni surface-tension gradients. Preliminary analysis shows that these factors interact to amplify local stress, suggesting a productivity optimum at high RPM. Our framework will shift the experimental focus to measuring the stress-concentration factor ($k_{sc}$) as the primary driver of the reactor\u2019s high-throughput performance.<\/p>\n\n\n\n<p class=\"has-intro-font-size wp-block-paragraph\">Aims<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">The primary aim of this project is to resolve the fundamental &#8220;no-go&#8221; paradox of the Liquid-Metal Vortex-Fluidic Device (LM-VFD) by identifying the exact physical mechanisms that allow for high-throughput material production. While standard centrifugal theory suggests that the forces generated within the spinning thin film are three orders of magnitude too weak to rupture the metal&#8217;s protective oxide skin, real-world results prove otherwise. This research aims to bridge that gap by developing a three-level model hierarchy\u2014ranging from scaling laws to a population ensemble simulator\u2014to accurately map the reactor&#8217;s operating landscape.<\/p>\n\n\n\n<p class=\"has-intro-font-size wp-block-paragraph\">Objectives<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Implement a coupled wave-stress and oxide-Markov simulator (Level 2) to quantitatively confirm the inadequacy of mean-field azimuthal modes in breaking the oxide skin. Validate a three-mechanism hypothesis\u2014incorporating spicular tip-radius sharpening, wave-mode collision impacts, and Marangoni surface-tension gradients\u2014to explain how local stress is multiplied by a factor of $10^3$. Utilise a Lagrangian Monte Carlo ensemble (Level 3) to refine productivity predictions by accounting for the distinct behaviours of freshly-ruptured versus aged-ruptured cells. Build and verify a computational framework using Python\/Julia to ensure all solver outputs are agnostic and accurate to a precision of $10^{-4}$.<\/p>\n\n\n\n<p class=\"has-intro-font-size wp-block-paragraph\">Significance<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">This research is significant because it fundamentally reorients the scientific understanding of liquid-metal reactors from a focus on bulk material properties to the study of stress-concentration factors ($k_{sc}$). By identifying that the productivity optimum occurs at high RPM due to specific &#8220;force multipliers,&#8221; the framework will provide a predictive tool that matches empirical data from high-throughput labs. Furthermore, the project\u2019s sensitivity analysis identifies $k_{sc}$ as the highest-leverage parameter for future optimisation, effectively setting a new experimental agenda focused on high-speed video correlation and Marangoni differentials rather than simple yield strength.<\/p>\n\n\n\n<p class=\"has-intro-font-size wp-block-paragraph\">Ideal Candidate<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">We are seeking a highly motivated HDR candidate with a strong foundation in numerical analysis and computational physics. The ideal applicant should possess advanced skills in Julia or Python, with a demonstrated ability to build and verify robust code. Familiarity with fluid dynamics, dimensionless scaling, or stochastic modelling (e.g., Monte Carlo methods) is highly desired. Candidates must have excellent analytical problem-solving skills to navigate complex multiphysics simulations and collaborate effectively with leading scientists at UWA. Additionally, the applicants should meet the eligibility criteria for entry into a PhD program at Curtin University.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">This project is open to International and Domestic applicants.<\/p>\n\n\n\n<p class=\"has-intro-font-size wp-block-paragraph\">Scholarship<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">If you are identified as the preferred candidate for this project, you may be considered for an <a href=\"https:\/\/www.curtin.edu.au\/study\/scholarships\/research-training-program-rtp-scholarships\/\" rel=\"noreferrer noopener\" target=\"_blank\">RTP scholarship<\/a>.<\/p>\n\n\n\n<p class=\"has-intro-font-size wp-block-paragraph\">Enquires and How to Apply<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">For enquires about this opportunity contact Professor Victor Calo at <a href=\"mailto:victor.calo@curtin.edu.au\">victor.calo@curtin.edu.au<\/a><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">To formally apply submit an <a href=\"https:\/\/forms.curtin.edu.au\/Produce\/Form\/External%20Forms\/Graduate%20Research\/\" target=\"_blank\" rel=\"noreferrer noopener\">Expression of Interest<\/a> to Professor Victor Calo during the Central Scholarship round (July 1st &#8211; July 31st 2026)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><\/p>\n","protected":false},"author":124,"featured_media":0,"template":"","faculties":[51],"hdr_types":[5487],"research_areas":[39],"class_list":["post-145348","hdr-r-projects","type-hdr-r-projects","status-publish","hentry","faculties-science-and-engineering","hdr_types-rtp-scholarship","research_areas-energy-transition"],"acf":false,"featured_image":false,"_links":{"self":[{"href":"https:\/\/www.curtin.edu.au\/research\/wp-json\/wp\/v2\/hdr-r-projects\/145348","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.curtin.edu.au\/research\/wp-json\/wp\/v2\/hdr-r-projects"}],"about":[{"href":"https:\/\/www.curtin.edu.au\/research\/wp-json\/wp\/v2\/types\/hdr-r-projects"}],"author":[{"embeddable":true,"href":"https:\/\/www.curtin.edu.au\/research\/wp-json\/wp\/v2\/users\/124"}],"version-history":[{"count":0,"href":"https:\/\/www.curtin.edu.au\/research\/wp-json\/wp\/v2\/hdr-r-projects\/145348\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.curtin.edu.au\/research\/wp-json\/wp\/v2\/media?parent=145348"}],"wp:term":[{"taxonomy":"faculties","embeddable":true,"href":"https:\/\/www.curtin.edu.au\/research\/wp-json\/wp\/v2\/faculties?post=145348"},{"taxonomy":"hdr_types","embeddable":true,"href":"https:\/\/www.curtin.edu.au\/research\/wp-json\/wp\/v2\/hdr_types?post=145348"},{"taxonomy":"research_areas","embeddable":true,"href":"https:\/\/www.curtin.edu.au\/research\/wp-json\/wp\/v2\/research_areas?post=145348"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}