Thomas Miller, Alexander K. Y. Tam, Robert Marangell, Martin Wechselberger, Bronwyn H. Bradshaw-Hajek
{"title":"具有负扩散性的反应-扩散方程的冲击前解析解","authors":"Thomas Miller, Alexander K. Y. Tam, Robert Marangell, Martin Wechselberger, Bronwyn H. Bradshaw-Hajek","doi":"10.1111/sapm.12685","DOIUrl":null,"url":null,"abstract":"<p>Reaction–diffusion equations (RDEs) model the spatiotemporal evolution of a density field <span></span><math>\n <semantics>\n <mrow>\n <mi>u</mi>\n <mo>(</mo>\n <mi>x</mi>\n <mo>,</mo>\n <mi>t</mi>\n <mo>)</mo>\n </mrow>\n <annotation>$u({x},t)$</annotation>\n </semantics></math> according to diffusion and net local changes. Usually, the diffusivity is positive for all values of <span></span><math>\n <semantics>\n <mi>u</mi>\n <annotation>$u$</annotation>\n </semantics></math>, which causes the density to disperse. However, RDEs with partially negative diffusivity can model aggregation, which is the preferred behavior in some circumstances. In this paper, we consider a nonlinear RDE with quadratic diffusivity <span></span><math>\n <semantics>\n <mrow>\n <mi>D</mi>\n <mo>(</mo>\n <mi>u</mi>\n <mo>)</mo>\n <mo>=</mo>\n <mo>(</mo>\n <mi>u</mi>\n <mo>−</mo>\n <mi>a</mi>\n <mo>)</mo>\n <mo>(</mo>\n <mi>u</mi>\n <mo>−</mo>\n <mi>b</mi>\n <mo>)</mo>\n </mrow>\n <annotation>$D(u) = (u - a)(u - b)$</annotation>\n </semantics></math> that is negative for <span></span><math>\n <semantics>\n <mrow>\n <mi>u</mi>\n <mo>∈</mo>\n <mo>(</mo>\n <mi>a</mi>\n <mo>,</mo>\n <mi>b</mi>\n <mo>)</mo>\n </mrow>\n <annotation>$u\\in (a,b)$</annotation>\n </semantics></math>. We use a nonclassical symmetry to construct analytic receding time-dependent, colliding wave, and receding traveling wave solutions. These solutions are multivalued, and we convert them to single-valued solutions by inserting a shock. We examine properties of these analytic solutions including their Stefan-like boundary condition, and perform a phase plane analysis. We also investigate the spectral stability of the <span></span><math>\n <semantics>\n <mrow>\n <mi>u</mi>\n <mo>=</mo>\n <mn>0</mn>\n </mrow>\n <annotation>$u = 0$</annotation>\n </semantics></math> and <span></span><math>\n <semantics>\n <mrow>\n <mi>u</mi>\n <mo>=</mo>\n <mn>1</mn>\n </mrow>\n <annotation>$u = 1$</annotation>\n </semantics></math> constant solutions, and prove for certain <span></span><math>\n <semantics>\n <mi>a</mi>\n <annotation>$a$</annotation>\n </semantics></math> and <span></span><math>\n <semantics>\n <mi>b</mi>\n <annotation>$b$</annotation>\n </semantics></math> that receding traveling waves are spectrally stable. In addition, we introduce a new shock condition where the diffusivity and flux are continuous across the shock. For diffusivity symmetric about the midpoint of its zeros, this condition recovers the well-known equal-area rule, but for nonsymmetric diffusivity it results in a different shock position.</p>","PeriodicalId":2,"journal":{"name":"ACS Applied Bio Materials","volume":null,"pages":null},"PeriodicalIF":4.6000,"publicationDate":"2024-03-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1111/sapm.12685","citationCount":"0","resultStr":"{\"title\":\"Analytic shock-fronted solutions to a reaction–diffusion equation with negative diffusivity\",\"authors\":\"Thomas Miller, Alexander K. Y. Tam, Robert Marangell, Martin Wechselberger, Bronwyn H. Bradshaw-Hajek\",\"doi\":\"10.1111/sapm.12685\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>Reaction–diffusion equations (RDEs) model the spatiotemporal evolution of a density field <span></span><math>\\n <semantics>\\n <mrow>\\n <mi>u</mi>\\n <mo>(</mo>\\n <mi>x</mi>\\n <mo>,</mo>\\n <mi>t</mi>\\n <mo>)</mo>\\n </mrow>\\n <annotation>$u({x},t)$</annotation>\\n </semantics></math> according to diffusion and net local changes. Usually, the diffusivity is positive for all values of <span></span><math>\\n <semantics>\\n <mi>u</mi>\\n <annotation>$u$</annotation>\\n </semantics></math>, which causes the density to disperse. However, RDEs with partially negative diffusivity can model aggregation, which is the preferred behavior in some circumstances. In this paper, we consider a nonlinear RDE with quadratic diffusivity <span></span><math>\\n <semantics>\\n <mrow>\\n <mi>D</mi>\\n <mo>(</mo>\\n <mi>u</mi>\\n <mo>)</mo>\\n <mo>=</mo>\\n <mo>(</mo>\\n <mi>u</mi>\\n <mo>−</mo>\\n <mi>a</mi>\\n <mo>)</mo>\\n <mo>(</mo>\\n <mi>u</mi>\\n <mo>−</mo>\\n <mi>b</mi>\\n <mo>)</mo>\\n </mrow>\\n <annotation>$D(u) = (u - a)(u - b)$</annotation>\\n </semantics></math> that is negative for <span></span><math>\\n <semantics>\\n <mrow>\\n <mi>u</mi>\\n <mo>∈</mo>\\n <mo>(</mo>\\n <mi>a</mi>\\n <mo>,</mo>\\n <mi>b</mi>\\n <mo>)</mo>\\n </mrow>\\n <annotation>$u\\\\in (a,b)$</annotation>\\n </semantics></math>. We use a nonclassical symmetry to construct analytic receding time-dependent, colliding wave, and receding traveling wave solutions. These solutions are multivalued, and we convert them to single-valued solutions by inserting a shock. We examine properties of these analytic solutions including their Stefan-like boundary condition, and perform a phase plane analysis. We also investigate the spectral stability of the <span></span><math>\\n <semantics>\\n <mrow>\\n <mi>u</mi>\\n <mo>=</mo>\\n <mn>0</mn>\\n </mrow>\\n <annotation>$u = 0$</annotation>\\n </semantics></math> and <span></span><math>\\n <semantics>\\n <mrow>\\n <mi>u</mi>\\n <mo>=</mo>\\n <mn>1</mn>\\n </mrow>\\n <annotation>$u = 1$</annotation>\\n </semantics></math> constant solutions, and prove for certain <span></span><math>\\n <semantics>\\n <mi>a</mi>\\n <annotation>$a$</annotation>\\n </semantics></math> and <span></span><math>\\n <semantics>\\n <mi>b</mi>\\n <annotation>$b$</annotation>\\n </semantics></math> that receding traveling waves are spectrally stable. In addition, we introduce a new shock condition where the diffusivity and flux are continuous across the shock. For diffusivity symmetric about the midpoint of its zeros, this condition recovers the well-known equal-area rule, but for nonsymmetric diffusivity it results in a different shock position.</p>\",\"PeriodicalId\":2,\"journal\":{\"name\":\"ACS Applied Bio Materials\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":4.6000,\"publicationDate\":\"2024-03-21\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://onlinelibrary.wiley.com/doi/epdf/10.1111/sapm.12685\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"ACS Applied Bio Materials\",\"FirstCategoryId\":\"100\",\"ListUrlMain\":\"https://onlinelibrary.wiley.com/doi/10.1111/sapm.12685\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"MATERIALS SCIENCE, BIOMATERIALS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"ACS Applied Bio Materials","FirstCategoryId":"100","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1111/sapm.12685","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATERIALS SCIENCE, BIOMATERIALS","Score":null,"Total":0}
Analytic shock-fronted solutions to a reaction–diffusion equation with negative diffusivity
Reaction–diffusion equations (RDEs) model the spatiotemporal evolution of a density field according to diffusion and net local changes. Usually, the diffusivity is positive for all values of , which causes the density to disperse. However, RDEs with partially negative diffusivity can model aggregation, which is the preferred behavior in some circumstances. In this paper, we consider a nonlinear RDE with quadratic diffusivity that is negative for . We use a nonclassical symmetry to construct analytic receding time-dependent, colliding wave, and receding traveling wave solutions. These solutions are multivalued, and we convert them to single-valued solutions by inserting a shock. We examine properties of these analytic solutions including their Stefan-like boundary condition, and perform a phase plane analysis. We also investigate the spectral stability of the and constant solutions, and prove for certain and that receding traveling waves are spectrally stable. In addition, we introduce a new shock condition where the diffusivity and flux are continuous across the shock. For diffusivity symmetric about the midpoint of its zeros, this condition recovers the well-known equal-area rule, but for nonsymmetric diffusivity it results in a different shock position.