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Towards systematic approach to boundary conditions in mixture and multiphasic incompressible models: Maximum Entropy principle estimate

The result's identifiers

  • Result code in IS VaVaI

    <a href="https://www.isvavai.cz/riv?ss=detail&h=RIV%2F68407700%3A21340%2F23%3A00367597" target="_blank" >RIV/68407700:21340/23:00367597 - isvavai.cz</a>

  • Result on the web

    <a href="https://doi.org/10.1016/j.ijengsci.2023.103902" target="_blank" >https://doi.org/10.1016/j.ijengsci.2023.103902</a>

  • DOI - Digital Object Identifier

    <a href="http://dx.doi.org/10.1016/j.ijengsci.2023.103902" target="_blank" >10.1016/j.ijengsci.2023.103902</a>

Alternative languages

  • Result language

    angličtina

  • Original language name

    Towards systematic approach to boundary conditions in mixture and multiphasic incompressible models: Maximum Entropy principle estimate

  • Original language description

    The single continuum model formulation, no matter how complex the considered constitutive relations are, cannot describe important phenomena stemming from constituents' interactions. In contrast, mixture theory is a successful framework for providing thermodynamically con-sistent governing equations in the bulk allowing for the inclusion of details in the material structure and interactions. Despite its ubiquitous applications, a fundamental open problem, a framework for the assessment of boundary conditions, persisted.Our objective is to relate these boundary conditions of mixtures to those of a single continuum and, hence, derive their possible form. To obtain such an estimation, we suggest using the Maximum Entropy (MaxEnt) principle yielding the least biased estimate (when measured by the entropy) of the values of the state variables on the more detailed level based on the knowledge of the state on the less detailed level. In the case of mixtures, the total mixture quantities represent the less detailed description, whereas the quantities related to each phase of the mixture represent the more detailed level, and the mapping (projection) connecting the two levels usually follows from the conservation of total mixture quantities. Therefore, once we have entropy on the detailed level and the aforementioned projection, from the MaxEnt principle, we get the least biased estimate of the decomposition of the total mixture state variables into variables corresponding to each constituent.These estimates can be used to obtain the interfacial conditions between two mixtures: we consider the decomposition of the total mixture quantities to partial quantities on both sides of the interface independently and match the mixture quantities at the interface using classical boundary conditions for a single phase. In this way, we may connect the well-developed theory for single continuum boundary conditions to the boundary conditions in mixtures. The generality of such an approach

  • Czech name

  • Czech description

Classification

  • Type

    J<sub>imp</sub> - Article in a specialist periodical, which is included in the Web of Science database

  • CEP classification

  • OECD FORD branch

    10102 - Applied mathematics

Result continuities

  • Project

    <a href="/en/project/GA20-22092S" target="_blank" >GA20-22092S: Multiscale thermodynamics: boundary conditions, integration and applications</a><br>

  • Continuities

    P - Projekt vyzkumu a vyvoje financovany z verejnych zdroju (s odkazem do CEP)

Others

  • Publication year

    2023

  • Confidentiality

    S - Úplné a pravdivé údaje o projektu nepodléhají ochraně podle zvláštních právních předpisů

Data specific for result type

  • Name of the periodical

    International Journal of Engineering Science

  • ISSN

    0020-7225

  • e-ISSN

    1879-2197

  • Volume of the periodical

    191

  • Issue of the periodical within the volume

    103902

  • Country of publishing house

    US - UNITED STATES

  • Number of pages

    13

  • Pages from-to

  • UT code for WoS article

    001024479100001

  • EID of the result in the Scopus database

    2-s2.0-85163441657