{"title":"Anisotropic Transport of Dielectric Particles by a Uniform Electric Field in an Inhomogeneously Heated Viscous Fluid","authors":"S. I. Martynov","doi":"10.15507/2079-6900.25.202302.53-61","DOIUrl":"https://doi.org/10.15507/2079-6900.25.202302.53-61","url":null,"abstract":"The anisotropic transfer of dielectric particles by a uniform electric field in a nonuniformly heated fluid is modeled. The transport anisotropy is determined by the mechanism of interaction between particles whose permittivity depends on temperature. The temperature distribution in the particles and in the fluid is determined by their thermal diffusivity and does not depend on the motion of the fluid, thus corresponding to small Peclet numbers. The fluid flow is considered in the approximation of small Reynolds numbers. The transfer of particles is due to the action of an anisotropic force exerted by applied uniform electric field and friction forces exerted by the fluid. The interaction of particles is taken into account. Numerical modeling of anisotropic transport dynamics of two dielectric particles is carried out. The process mentioned depends on the mutual orientation of electric field vector, temperature gradient, and initial orientation of the vector connecting the particle centers. For the case of a large number of particles, an anisotropic equilibrium distribution of the particle concentration in an external electric field is found taking into account the mechanisms of their diffusion and interaction.","PeriodicalId":273445,"journal":{"name":"Zhurnal Srednevolzhskogo Matematicheskogo Obshchestva","volume":"2 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2023-06-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"128788910","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"On the reduction of the topological classification of gradient-like flows problem to the classification of polar flows\u0000I. A. Saraev","authors":"Ilya A. Saraev","doi":"10.15507/2079-6900.25.202302.62-75","DOIUrl":"https://doi.org/10.15507/2079-6900.25.202302.62-75","url":null,"abstract":"In this paper we consider a class G(Mn)\u0000 of gradient-like flows on connected closed manifolds of dimension n≥4\u0000 such that for any flow ft∈G(Mn)\u0000 stable and unstable invariant manifolds of saddle equilibria do not intersect invariant manifolds of other saddle equilibria. It is known that the ambient manifold of any flow from the class G(Mn)\u0000 can be splitted into connected summ of the sphere Sn\u0000, gft≥0\u0000 copies of direct products Sn−1×S1\u0000, and a simply connected manifold which is not homeomorphic to the sphere. The number gft\u0000 is determined only by the number of nodal equilibria and the number of saddle equilibria such that one of their invariant manifolds has the dimension (n−1)\u0000 (we call such equilibria trivial saddles). A simply connected manifold which is not homeomorphic to the sphere presents in the splitting if and only if the set of saddle equilibria contains points with unstable manifolds of dimension i∈{2,…,n−2}\u0000 (we call such equilibria non-trivial saddles). Moreover, the complete topological classification was obtained for flows from the class G(Mn)\u0000 without non-trivial saddles. In this paper we prove that for any flow ft∈G(Mn)\u0000 the carrier manifold can be splitted into a connected sum along pairwise disjoint smoothly embedded spheres (separating spheres) that do not contain equilibrium states of the flow ft\u0000 and transversally intersect its trajectories. The restriction of the flow ft\u0000 to the complements to these spheres uniquely (up to topological equivalence and numbering) defines a finite set of flows ft1,…,ftl\u0000 defined on the components of a connected sum. Moreover, for any j∈1,…,l\u0000, the set of saddle equilibria of the flow ftj\u0000 consists either only of trivial saddles or only of of non-trivial ones and then the flow ftj\u0000 is polar. We introduce the notion of consistent topological equivalence for flows ft1,…ftj\u0000 and show that flows ft,f′t∈G(Mn)\u0000 are topologically equivalent if and only if for each of these flows the set of separating spheres exists that defines consistently topologically equivalent flows on the components of the connected sum.","PeriodicalId":273445,"journal":{"name":"Zhurnal Srednevolzhskogo Matematicheskogo Obshchestva","volume":"58 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2023-06-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"114187741","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}