Droplet Hamilton Dynamics 1: the rolling angle of a water droplet on an inclined surface

preprint OA: closed CC-BY-4.0
📄 Open PDF Full text JSON View at publisher

Abstract

Abstract The rolling angle calculation of a water droplet on an inclined surface is not only an everyday phenomenon but also forms an essential part of many industrial processes. Previous researchers always used Newtonian mechanics (the vector mechanics) to set up the differential equation by analyzing the forces affecting on the droplet on an inclined surface and get the rolling angle. Here, by constructing the single-valued mapping from the droplet mass center motion parameters to the moving droplet body, we use the Hamilton's principle (the energy method) and the Karush-Kuhn-Tucher (KKT) theory to set up Euler equation sets of mass center motions. In initial conditions of “sphere shape-zero velocity”, we solve Euler equation sets and gain the droplet mass center motion equations. By judging whether the singularities (velocity zero points) exist or not in the phase space of mass center motions, we judge the droplet “is pinned” or “continuously rolls” on the inclined surface. Finally, we calculate out the critical tilt angle of the inclined surface, which just makes the droplet “continuously roll”, as the droplet rolling angle. Our results from the energy method can also improve analyzing the kinetic behaviors of droplets in multi-physical fields, such as phase-change droplets, triboelectrically induced electrostatic droplets and polar droplets in fixed electrostatic fields.
Full text 14,658 characters · extracted from preprint-html · click to expand
Droplet Hamilton Dynamics 1: the rolling angle of a water droplet on an inclined surface | Research Square window.SnipcartSettings = { analytics: { enabled: false } }; (function() { var accessVector = localStorage.getItem('access_vector') || ''; window.dataLayer = window.dataLayer || []; if (accessVector) { window.dataLayer.push({ user: { profile: { profileInfo: { snid: accessVector } } } }); } })(); (function(w,d,s,l,i){w[l]=w[l]||[];w[l].push({'gtm.start':new Date().getTime(),event:'gtm.js'});var f=d.getElementsByTagName(s)[0],j=d.createElement(s),dl=l!='dataLayer'?'&l='+l:'';j.async=true;j.src='https://www.googletagmanager.com/gtm.js?id='+i+dl;f.parentNode.insertBefore(j,f);})(window,document,'script','dataLayer','GTM-K279D39R'); Browse Preprints In Review Journals COVID-19 Preprints AJE Video Bytes Research Tools Research Promotion AJE Professional Editing AJE Rubriq About Preprint Platform In Review Editorial Policies Our Team Advisory Board Help Center Sign In Submit a Preprint Cite Share Download PDF Article Droplet Hamilton Dynamics 1: the rolling angle of a water droplet on an inclined surface Jian Dong, Bilong Liu, Dezhao Li, Da-peng Tan This is a preprint; it has not been peer reviewed by a journal. https://doi.org/ 10.21203/rs.3.rs-8817038/v1 This work is licensed under a CC BY 4.0 License Status: Posted Version 1 posted You are reading this latest preprint version Abstract The rolling angle calculation of a water droplet on an inclined surface is not only an everyday phenomenon but also forms an essential part of many industrial processes. Previous researchers always used Newtonian mechanics (the vector mechanics) to set up the differential equation by analyzing the forces affecting on the droplet on an inclined surface and get the rolling angle. Here, by constructing the single-valued mapping from the droplet mass center motion parameters to the moving droplet body, we use the Hamilton's principle (the energy method) and the Karush-Kuhn-Tucher (KKT) theory to set up Euler equation sets of mass center motions. In initial conditions of “sphere shape-zero velocity”, we solve Euler equation sets and gain the droplet mass center motion equations. By judging whether the singularities (velocity zero points) exist or not in the phase space of mass center motions, we judge the droplet “is pinned” or “continuously rolls” on the inclined surface. Finally, we calculate out the critical tilt angle of the inclined surface, which just makes the droplet “continuously roll”, as the droplet rolling angle. Our results from the energy method can also improve analyzing the kinetic behaviors of droplets in multi-physical fields, such as phase-change droplets, triboelectrically induced electrostatic droplets and polar droplets in fixed electrostatic fields. Physical sciences/Physics/Fluid dynamics Physical sciences/Materials science/Soft materials/Fluids the rolling angle calculation the single-valued mapping the Hamilton's principle the Karush-Kuhn-Tucher (KKT) theory the singularities the phase space Full Text Additional Declarations There is NO Competing Interest. Tables 2 and 3 are available in the Supplementary Files section. Supplementary Files NPSI5final.docx Supplementary Information for Droplet Hamilton Dynamics 1: the rolling angle of a water droplet on an inclined surface Table2PDMSfinal.xlsx Table2 Table3.xlsx Table3 Partialexperimentalvideos.mp4 The motion of liquid droplets on the surface under high-speed cameras code.docx Supplementary code for Droplet Hamilton Dynamics 1: the rolling angle of a water droplet on an inclined surface NPSIfinal.docx Supplementary Information for Droplet Hamilton Dynamics 1: the rolling angle of a water droplet on an inclined surface Cite Share Download PDF Status: Posted Version 1 posted You are reading this latest preprint version Research Square lets you share your work early, gain feedback from the community, and start making changes to your manuscript prior to peer review in a journal. As a division of Research Square Company, we’re committed to making research communication faster, fairer, and more useful. We do this by developing innovative software and high quality services for the global research community. Our growing team is made up of researchers and industry professionals working together to solve the most critical problems facing scientific publishing. Also discoverable on Platform About Our Team In Review Editorial Policies Advisory Board Help Center Resources Author Services Accessibility API Access RSS feed Manage Cookie Preferences © Research Square 2026 | ISSN 2693-5015 (online) Privacy Policy Terms of Service Do Not Sell My Personal Information {"props":{"pageProps":{"initialData":{"identity":"rs-8817038","acceptedTermsAndConditions":true,"allowDirectSubmit":true,"archivedVersions":[],"articleType":"Article","associatedPublications":[],"authors":[{"id":588339932,"identity":"868eb166-b837-4e8d-8c6d-da7141d40287","order_by":0,"name":"Jian Dong","email":"data:image/png;base64,iVBORw0KGgoAAAANSUhEUgAAAZAAAAAyAQMAAABI0h/eAAAABlBMVEX///8AAABVwtN+AAAACXBIWXMAAA7EAAAOxAGVKw4bAAAA2ElEQVRIie3SMQrCMBiG4S8EOv3SNYPoFdrJQdGrKIKO4uJcEXTpASL2EB4hEnAqdRV0UFwVHF0EY91NRsG8Swj8DwkhgM/3kymAqAWWvDeBG2EJ0cAQ7kzMMEGb1ZXUp3njdK3uOlyOFO4TjXCV2I7I42lGB85kH0wWGuKovhOOPJ4RHYI34ZW5RiS630nwIQWV5OlC6EOUKAlzIQLb8TKjfsTSS7RJiyGJvYXUpV7fb2m7Ey9659Nj0qyF0kIglHm2FIiT8iOYm1oLzSge5jj7qM/n8/1rLypgQH/9C4CbAAAAAElFTkSuQmCC","orcid":"","institution":"zhejiang university of technology","correspondingAuthor":true,"prefix":"","firstName":"Jian","middleName":"","lastName":"Dong","suffix":""},{"id":588339933,"identity":"69bfaca9-3f95-4bf2-91ed-741e236a71a3","order_by":1,"name":"Bilong Liu","email":"","orcid":"","institution":"","correspondingAuthor":false,"prefix":"","firstName":"Bilong","middleName":"","lastName":"Liu","suffix":""},{"id":588339934,"identity":"a166cb48-740b-4751-b08c-2b7dc8eaf846","order_by":2,"name":"Dezhao Li","email":"","orcid":"","institution":"zhejiang university of technology","correspondingAuthor":false,"prefix":"","firstName":"Dezhao","middleName":"","lastName":"Li","suffix":""},{"id":588339935,"identity":"fc3f342f-7d24-4500-848f-206b3d6ec8d4","order_by":3,"name":"Da-peng Tan","email":"","orcid":"","institution":"zhejiang university of technology","correspondingAuthor":false,"prefix":"","firstName":"Da-peng","middleName":"","lastName":"Tan","suffix":""}],"badges":[],"createdAt":"2026-02-07 16:55:20","currentVersionCode":1,"declarations":"","doi":"10.21203/rs.3.rs-8817038/v1","doiUrl":"https://doi.org/10.21203/rs.3.rs-8817038/v1","draftVersion":[],"editorialEvents":[],"editorialNote":"","failedWorkflow":false,"files":[{"id":104397556,"identity":"7a7da71d-7525-43c5-9c03-bc979a08a84b","added_by":"auto","created_at":"2026-03-11 11:51:38","extension":"pdf","order_by":1,"title":"","display":"","copyAsset":false,"role":"manuscript-pdf","size":1002981,"visible":true,"origin":"","legend":"","description":"","filename":"NPmanuscriptfinal.pdf","url":"https://assets-eu.researchsquare.com/files/rs-8817038/v1_covered_beaab515-0ae0-486d-8569-90edd45b08d3.pdf"},{"id":102275887,"identity":"6f4b177f-94d8-4b48-a3fa-5d749863f99d","added_by":"auto","created_at":"2026-02-10 05:48:51","extension":"docx","order_by":1,"title":"","display":"","copyAsset":false,"role":"supplement","size":834226,"visible":true,"origin":"","legend":"Supplementary Information for Droplet Hamilton Dynamics 1: the rolling angle of a water droplet on an inclined surface","description":"","filename":"NPSI5final.docx","url":"https://assets-eu.researchsquare.com/files/rs-8817038/v1/87694fac30f3bf1f94450761.docx"},{"id":102275891,"identity":"af75a9bf-ba9b-45be-8bb5-a8d8678ccc98","added_by":"auto","created_at":"2026-02-10 05:48:51","extension":"xlsx","order_by":2,"title":"","display":"","copyAsset":false,"role":"supplement","size":2051855,"visible":true,"origin":"","legend":"Table2","description":"","filename":"Table2PDMSfinal.xlsx","url":"https://assets-eu.researchsquare.com/files/rs-8817038/v1/4279188e787d827e8fb85429.xlsx"},{"id":102275890,"identity":"5402c794-668c-44a8-a743-062e3f3d28c7","added_by":"auto","created_at":"2026-02-10 05:48:51","extension":"xlsx","order_by":3,"title":"","display":"","copyAsset":false,"role":"supplement","size":2056930,"visible":true,"origin":"","legend":"Table3","description":"","filename":"Table3.xlsx","url":"https://assets-eu.researchsquare.com/files/rs-8817038/v1/2a078155ce5a1127e6591236.xlsx"},{"id":102275893,"identity":"a624ebbe-c0e8-49d5-bcba-6e26091c6b32","added_by":"auto","created_at":"2026-02-10 05:48:52","extension":"mp4","order_by":4,"title":"","display":"","copyAsset":false,"role":"supplement","size":64019707,"visible":true,"origin":"","legend":"The motion of liquid droplets on the surface under high-speed cameras","description":"","filename":"Partialexperimentalvideos.mp4","url":"https://assets-eu.researchsquare.com/files/rs-8817038/v1/eaed2791fe678940aa33c47f.mp4"},{"id":102275889,"identity":"e81379db-abbf-4a45-8cb3-d54d68baf2ee","added_by":"auto","created_at":"2026-02-10 05:48:51","extension":"docx","order_by":5,"title":"","display":"","copyAsset":false,"role":"supplement","size":73962,"visible":true,"origin":"","legend":"Supplementary code for Droplet Hamilton Dynamics 1: the rolling angle of a water droplet on an inclined surface","description":"","filename":"code.docx","url":"https://assets-eu.researchsquare.com/files/rs-8817038/v1/f59c26367f6ecd22eb017244.docx"},{"id":102275888,"identity":"08557901-aa5c-4e20-8f03-0dd3e6db496f","added_by":"auto","created_at":"2026-02-10 05:48:51","extension":"docx","order_by":6,"title":"","display":"","copyAsset":false,"role":"supplement","size":834114,"visible":true,"origin":"","legend":"Supplementary Information for Droplet Hamilton Dynamics 1: the rolling angle of a water droplet on an inclined surface","description":"","filename":"NPSIfinal.docx","url":"https://assets-eu.researchsquare.com/files/rs-8817038/v1/b29393aaf3d4ba818ee84838.docx"}],"financialInterests":"\u003cp\u003eThere is \u003cstrong\u003eNO\u003c/strong\u003e Competing Interest.\u003c/p\u003e\n\u003cp\u003eTables 2 and 3 are available in the Supplementary Files section.\u003c/p\u003e","formattedTitle":"Droplet Hamilton Dynamics 1: the rolling angle of a water droplet on an inclined surface","fulltext":[],"fulltextSource":"","fullText":"","funders":[],"hasAdminPriorityOnWorkflow":false,"hasManuscriptDocX":false,"hasOptedInToPreprint":true,"hasPassedJournalQc":"","hasAnyPriority":true,"hideJournal":true,"highlight":"","institution":"","isAcceptedByJournal":false,"isAuthorSuppliedPdf":true,"isDeskRejected":"","isHiddenFromSearch":false,"isInQc":false,"isInWorkflow":false,"isPdf":true,"isPdfUpToDate":true,"isWithdrawnOrRetracted":false,"journal":{"display":true,"email":"[email protected]","identity":"researchsquare","isNatureJournal":false,"hasQc":true,"allowDirectSubmit":true,"externalIdentity":"","sideBox":"","snPcode":"","submissionUrl":"/submission","title":"Research Square","twitterHandle":"researchsquare","acdcEnabled":true,"dfaEnabled":false,"editorialSystem":"","reportingPortfolio":"","inReviewEnabled":false,"inReviewRevisionsEnabled":true},"keywords":"the rolling angle calculation, the single-valued mapping, the Hamilton's principle, the Karush-Kuhn-Tucher (KKT) theory, the singularities, the phase space","lastPublishedDoi":"10.21203/rs.3.rs-8817038/v1","lastPublishedDoiUrl":"https://doi.org/10.21203/rs.3.rs-8817038/v1","license":{"name":"CC BY 4.0","url":"https://creativecommons.org/licenses/by/4.0/"},"manuscriptAbstract":"\u003cp\u003eThe rolling angle calculation of a water droplet on an inclined surface is not only an everyday phenomenon but also forms an essential part of many industrial processes. Previous researchers always used Newtonian mechanics (the vector mechanics) to set up the differential equation by analyzing the forces affecting on the droplet on an inclined surface and get the rolling angle. Here, by constructing the single-valued mapping from the droplet mass center motion parameters to the moving droplet body, we use the Hamilton's principle (the energy method) and the Karush-Kuhn-Tucher (KKT) theory to set up Euler equation sets of mass center motions. In initial conditions of “sphere shape-zero velocity”, we solve Euler equation sets and gain the droplet mass center motion equations. By judging whether the singularities (velocity zero points) exist or not in the phase space of mass center motions, we judge the droplet “is pinned” or “continuously rolls” on the inclined surface. Finally, we calculate out the critical tilt angle of the inclined surface, which just makes the droplet “continuously roll”, as the droplet rolling angle. Our results from the energy method can also improve analyzing the kinetic behaviors of droplets in multi-physical fields, such as phase-change droplets, triboelectrically induced electrostatic droplets and polar droplets in fixed electrostatic fields.\u003c/p\u003e","manuscriptTitle":"Droplet Hamilton Dynamics 1: the rolling angle of a water droplet on an inclined surface","msid":"","msnumber":"","nonDraftVersions":[{"code":1,"date":"2026-02-10 05:48:42","doi":"10.21203/rs.3.rs-8817038/v1","editorialEvents":[{"type":"communityComments","content":0}],"status":"published","journal":{"display":true,"email":"[email protected]","identity":"researchsquare","isNatureJournal":false,"hasQc":true,"allowDirectSubmit":true,"externalIdentity":"","sideBox":"","snPcode":"","submissionUrl":"/submission","title":"Research Square","twitterHandle":"researchsquare","acdcEnabled":true,"dfaEnabled":false,"editorialSystem":"","reportingPortfolio":"","inReviewEnabled":false,"inReviewRevisionsEnabled":true}}],"origin":"","ownerIdentity":"98aaa5e5-4275-468d-bfcf-c4e70521b620","owner":[],"postedDate":"February 10th, 2026","published":true,"recentEditorialEvents":[],"rejectedJournal":[],"revision":"","amendment":"","status":"posted","subjectAreas":[{"id":62591338,"name":"Physical sciences/Physics/Fluid dynamics"},{"id":62591339,"name":"Physical sciences/Materials science/Soft materials/Fluids"}],"tags":[],"updatedAt":"2026-02-22T20:15:24+00:00","versionOfRecord":[],"versionCreatedAt":"2026-02-10 05:48:42","video":"","vorDoi":"","vorDoiUrl":"","workflowStages":[]},"version":"v1","identity":"rs-8817038","journalConfig":"researchsquare"},"__N_SSP":true},"page":"/article/[identity]/[[...version]]","query":{"redirect":"/article/rs-8817038","identity":"rs-8817038","version":["v1"]},"buildId":"XKTyCvWXoU3ODBz1xrDgd","isFallback":false,"isExperimentalCompile":false,"dynamicIds":[84888],"gssp":true,"scriptLoader":[]}

Text is read by the "Ask this paper" AI Q&A widget below. Extraction quality varies by source — PMC NXML preserves structure cleanly, OA-HTML may include some navigation residue, and OA-PDF can have broken hyphenation. The publisher copy (via DOI) is the canonical version.

My notes (saved in your browser only)

Ask this paper AI returns verbatim quotes from the full text · source: preprint-html

Answers must be backed by verbatim quotes from this paper's full text. Hallucinated quotes are dropped automatically; if no verbatim passage answers the question, we say so. How this works

Citation neighborhood (no data yet)

We don't have any in-corpus citations linked to this paper yet. This is a recent paper (2026) — citers typically take a year or two to land, and the OpenAlex reference graph may still be filling in.

Source provenance

europepmc
last seen: 2026-05-20T01:45:00.602351+00:00
unpaywall
last seen: 2026-05-22T02:00:06.705733+00:00
License: CC-BY-4.0