Mathematical Fluid Dynamics: Theory, Analysis and Emerging Trends

A special issue of Mathematics (ISSN 2227-7390). This special issue belongs to the section "E: Applied Mathematics".

Deadline for manuscript submissions: 28 August 2026 | Viewed by 1030

Special Issue Editor


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Guest Editor
Department of Mechanical Engineering, Ishinomaki Senshu University, Fukuoka University, Fukuoka 986-8580, Japan
Interests: energy engineering; fluid numerical simulation; artificial intelligence

Special Issue Information

Dear Colleagues,

This Special Issue explores the mathematical essence of fluid motion through rigorous analysis, geometric reasoning, and modern data-driven methodologies. It seeks to illuminate how the foundational equations of continuum mechanics—most notably the Navier–Stokes and Euler equations—continue to pose profound challenges concerning existence, regularity, and singularity formation, while also inspiring new analytical and computational paradigms.

The Issue highlights advances in the mathematical theory of turbulence, the energy cascade across scales, and the analysis of free-boundary, multiphase, and magnetohydrodynamic (MHD) systems. Emphasis is placed on frameworks that integrate functional and harmonic analysis, stochastic formulations, and variational or geometric principles, thereby extending the reach of classical fluid theory. Moreover, the Issue welcomes mathematically grounded approaches to physics-informed and machine-learning-assisted modeling, which reconcile data adaptability with physical and analytical integrity. Collectively, these contributions aim to redefine the modern landscape of mathematical fluid dynamics, revealing how timeless equations give rise to new structures, symmetries, and pathways toward a deeper understanding of fluid motion in both nature and computation.

Prof. Dr. Shin'ichi Inage
Guest Editor

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Keywords

  • Navier–Stokes equations
  • regularity and singularity
  • turbulence and energy cascade
  • free-boundary problems
  • multiphase and MHD flows
  • geometric and variational formulations
  • data-driven and physics-informed modeling

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Published Papers (2 papers)

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Research

17 pages, 284 KB  
Article
Linear Hamiltonian Vector Fields on Lie Groups
by Víctor Ayala and María Luisa Torreblanca Todco
Mathematics 2026, 14(6), 994; https://doi.org/10.3390/math14060994 - 14 Mar 2026
Viewed by 299
Abstract
Linear vector fields on Lie groups constitute a fundamental class of dynamical systems, as their flows are one-parameter subgroups of automorphisms and their infinitesimal behavior is entirely determined by derivations of the Lie algebra. When a Lie group is endowed with a Hamiltonian-type [...] Read more.
Linear vector fields on Lie groups constitute a fundamental class of dynamical systems, as their flows are one-parameter subgroups of automorphisms and their infinitesimal behavior is entirely determined by derivations of the Lie algebra. When a Lie group is endowed with a Hamiltonian-type geometric structure, a natural problem is to determine whether such linear dynamics admit a global variational realization, and how such realizations can be interpreted in terms of reduced models of fluid motion. In the even-dimensional case, where the Lie group carries a symplectic structure, we establish a complete global criterion for the existence of Hamiltonians generating linear symplectic vector fields. The problem reduces to a single global obstruction: the de Rham cohomology class of the 1-form ιXω. Thus, every linear symplectic vector field on a simply connected Lie group is globally Hamiltonian, and when the obstruction vanishes, we provide an explicit constructive procedure to recover the Hamiltonian. On the affine group Aff+(1), this yields a fully explicit, finite-dimensional Hamiltonian model of a 1D ideal fluid with affine symmetries. We then treat odd-dimensional Lie groups, where symplectic geometry is unavailable. Using contact geometry as the canonical replacement, we prove a Hamiltonian lifting theorem ensuring the existence and uniqueness of the associated dynamics. The Reeb vector field appears as a distinguished vertical direction resolving the ambiguities of degenerate Hamiltonian systems. On the Heisenberg group H3, this gives a fully explicit contact Hamiltonian model of an effective non-conservative fluid mode. Finally, we interpret symplectic and contact theories within a unified geometric framework and discuss their relevance to geometric formulations of ideal (symplectic) and effective (contact) fluid equations on Lie groups. Full article
(This article belongs to the Special Issue Mathematical Fluid Dynamics: Theory, Analysis and Emerging Trends)
44 pages, 940 KB  
Article
A Two-Level Relative-Entropy Theory for Isotropic Turbulence Spectra: Fokker–Planck Semigroup Irreversibility and WKB Selection of Dissipation Tails
by Shin-ichi Inage
Mathematics 2026, 14(4), 620; https://doi.org/10.3390/math14040620 - 10 Feb 2026
Viewed by 435
Abstract
We propose a two-level theory that connects Lin-equation-based dynamical coarse-graining of the turbulence cascade with an information-theoretic selection principle in logarithmic wavenumber space. This framework places the dissipation-range spectral shape on a verifiable logical basis rather than on ad hoc fitting. At the [...] Read more.
We propose a two-level theory that connects Lin-equation-based dynamical coarse-graining of the turbulence cascade with an information-theoretic selection principle in logarithmic wavenumber space. This framework places the dissipation-range spectral shape on a verifiable logical basis rather than on ad hoc fitting. At the first (dynamical) level, we formulate an autonomous conservative Fokker–Planck equation for the normalized density and probability current. Under sufficient boundary decay and a strictly positive effective diffusion, the sign-reversed Kullback–Leibler divergence is shown to be a Lyapunov functional, yielding a rigorous H-theorem and fixing the arrow of time in scale space. At the second (selection) level, the dissipation range is treated as a stationary boundary-value problem for an open system by introducing a killing term for an unnormalized scale density. A WKB (Liouville–Green) analysis restricts the admissible tail to a stretched-exponential form and links the tail exponent to the high-wavenumber scaling of the effective diffusion. The exponential prefactor is fixed by dissipation-rate consistency, and the remaining degree of freedom is determined by one-dimensional Kullback–Leibler minimization (Hyper-MaxEnt) against a globally constructed reference distribution. The resulting exponent range is validated against the high-resolution DNS spectra reported in the literature. Full article
(This article belongs to the Special Issue Mathematical Fluid Dynamics: Theory, Analysis and Emerging Trends)
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