{"title":"Forced Burgers equation with sticky impulsion source","authors":"Florent Nzissila, Octave Moutsinga","doi":"10.1007/s13370-023-01150-9","DOIUrl":null,"url":null,"abstract":"<div><p>We consider the inviscid Burgers equation with force <span>\\(\\partial _t u+\\partial _x(u^2/2)=\\nu \\)</span>, where the discontinuities of initial datum <span>\\(u_0\\)</span> are interpreted as <i>force sources.</i> Thence, <span>\\(\\nu \\)</span> is the force of shocks in a sticky dynamics of (paradoxically) non accelerated particles, whose the mass distribution field is <span>\\(\\partial _xu\\)</span>. The force has its own dynamics of density field <span>\\(\\eta =u-w\\)</span> (the experienced impulsion), where <i>w</i> denotes the sticky particle velocity field. Along the sticky particle trajectory <span>\\(t\\mapsto X_t\\)</span>, the processes <span>\\(t\\mapsto \\eta (X_t,t),u(X_t,t),w(X_t,t)\\)</span> are backward martingales.</p></div>","PeriodicalId":46107,"journal":{"name":"Afrika Matematika","volume":null,"pages":null},"PeriodicalIF":0.9000,"publicationDate":"2023-12-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Afrika Matematika","FirstCategoryId":"1085","ListUrlMain":"https://link.springer.com/article/10.1007/s13370-023-01150-9","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATHEMATICS","Score":null,"Total":0}
引用次数: 0
Abstract
We consider the inviscid Burgers equation with force \(\partial _t u+\partial _x(u^2/2)=\nu \), where the discontinuities of initial datum \(u_0\) are interpreted as force sources. Thence, \(\nu \) is the force of shocks in a sticky dynamics of (paradoxically) non accelerated particles, whose the mass distribution field is \(\partial _xu\). The force has its own dynamics of density field \(\eta =u-w\) (the experienced impulsion), where w denotes the sticky particle velocity field. Along the sticky particle trajectory \(t\mapsto X_t\), the processes \(t\mapsto \eta (X_t,t),u(X_t,t),w(X_t,t)\) are backward martingales.