New Papers in Fluid Mechanics

Author(s): Alexei A. Mailybaev

Spontaneous stochasticity—persistent randomness in the limit of vanishing noise and viscosity—has been observed in turbulence models, yet its universality lacked a theoretical explanation. We develop a renormalization-group (RG) framework for the fluctuating Sabra shell model, showing that the ideal turbulent dynamics is governed by a fixed-point RG attractor. This approach explains universality across dissipation and noise mechanisms and predicts a complex RG eigenvalue responsible for the slow, oscillatory convergence observed numerically.

[Phys. Rev. Fluids 11, 034605] Published Thu Mar 05, 2026

Author(s): Sthavishtha R. Bhopalam, Ruben Juanes, and Hector Gomez

Droplet transport in deformable constrictions is important in microfluidics, enhanced oil recovery, biomedical systems, and surface-acoustic-wave-driven platforms. We study how actuation controls droplet motion in a constricted deformable tube using high resolution multicomponent fluid-structure interaction simulations. We show that oscillatory traction on the tube walls exhibits resonance, i.e., the droplet’s mobilization time is minimized when the traction frequency nears the tube’s natural frequency. However, actuation via oscillatory fluid forcing exhibits no such resonance. Our findings provide design guidelines for tunable, actuation-controlled droplet motion in soft confined geometries.

[Phys. Rev. Fluids 11, 033601] Published Tue Mar 03, 2026

Author(s): F. Novotný, M. Talíř, E. Varga, and L. Skrbek

Temporal decay of rotating turbulent thermal counterflow of He II is probed by second sound and found to display interesting new features. Two effects are observed, acting against each other and affecting the late temporal decay of vortex line density, L(t). The first one is gradual decrease of the decay exponent of the power law L(t), confirming that turbulent thermal counterflow under rotation acquires 2D features. The second one is the influence of the effective Ekman layer built within the effective quantum Ekman time. For increasing rotation rates, L(t) gradually ceases to display a clear power law. Instead, rounded and ever steeper decays occur, gradually shifted toward shorter times.

[Phys. Rev. Fluids 11, 034603] Published Tue Mar 03, 2026

Author(s): A. V. Kopyev, V. A. Sirota, A. S. Il'yn, and K. P. Zybin

We develop the Kazantsev theory of small-scale dynamo generation at small Prandtl numbers near the generation threshold and restore the concordance between the theory and numerical simulations: the theory predicted a power-law decay below the threshold, while simulations demonstrate exponential deca…

[Phys. Rev. E 113, 035101] Published Mon Mar 02, 2026

Author(s): Ruifeng Yuan and Lei Wu

Smaller gas-solid contact area or smaller bifurcation angle? What happens when inlet and outlet conditions are exchanged? This study employs topology optimization to investigate optimal manifold configurations across gas rarefaction regimes and uncovers two counterintuitive phenomena: a wetted-area minimum in the slip regime and inlet–outlet reciprocity in free-molecular flows. These findings provide crucial guidance for microfluidic and vacuum system applications.

[Phys. Rev. Fluids 11, 033401] Published Mon Mar 02, 2026

Author(s): Ashish S. Nair, Narendra Singh, Marco Panesi, Justin Sirignano, and Jonathan F. MacArt

Hypersonic boundary layers in the transition–continuum regime (Knudsen number Kn ≈ 0.1–10) challenge Navier–Stokes solvers due to the breakdown of transport laws and slip/jump wall conditions. We embed physics-constrained neural closures for viscous stress and heat flux directly in the partial differential equations and train them using adjoint-computed gradients to match direct simulation Monte Carlo target data. A distribution-function wall model built from mixtures of skewed Gaussians replaces empirical slip-velocity models, substantially improving bulk flow and boundary-layer predictions and generalizing across unseen Mach numbers, Knudsen numbers, and geometries.

[Phys. Rev. Fluids 11, 033402] Published Mon Mar 02, 2026

Author(s): Thomas Boeck

Wall-attached Rayleigh-Bénard convection arises in the presence of a damping body force, e.g. the Coriolis or Lorentz force, when this force is less effective near a lateral boundary than in the bulk. The shape of the container is important in this context. A numerical linear stability analysis of Rayleigh-Bénard magnetoconvection in a wide rectangular container with a vertical magnetic field and electrically insulating walls shows that the least stable mode of convection becomes localized in the corners rather than spread out over the whole circumference of the container. This corner mode has a similar dependence on the magnetic field strength as the ordinary wall-attached mode.

[Phys. Rev. Fluids 11, 033501] Published Mon Mar 02, 2026

Author(s): Abdallah Daddi-Moussa-Ider, Jakob Mihatsch, Michael J. Mitchell, Elsen Tjhung, and Andreas M. Menzel

Wedge-shaped confinements are increasingly relevant in low-Reynolds-number microfluidics, yet existing Green’s functions describe only flows driven by point forces. We derive the flow induced by localized torques using a Fourier–Kontorovich–Lebedev framework combined with the Papkovich–Neuber representation. The resulting solutions reveal how geometric asymmetry couples rotation and translation and yield the full torque– mobility tensor. These analytical results provide predictive tools for controlling particle motion in confined microfluidic systems.

[Phys. Rev. Fluids 11, 034101] Published Mon Mar 02, 2026

Author(s): Yutaro Motoori, Pierre Bragança, and Susumu Goto

We introduce a simple method to objectively identify the axes of coherent vortices in turbulence using only the velocity-gradient tensor. The method is readily applicable to experimental data. As an example, applying it to stereo-PIV measurements of a wind-tunnel turbulent boundary layer, we quantitatively show that boundary-layer-scale vortices form hairpin shapes.

[Phys. Rev. Fluids 11, 034601] Published Mon Mar 02, 2026

Author(s): Francesca De Serio

In rotating geophysical flows, turbulence can either drive small-scale mixing or build large-scale coherent eddies. Here, a very large rotating-tank jet experiment with planar particle imaging velocimetry (PIV) is used to map the local energy flux across scales. The results show that stress–strain alignment and a local jet Rossby number organize where and how long inverse energy-cascade patches appear. This identifies a local control parameter for steering energy pathways in jet-like environmental flows.

[Phys. Rev. Fluids 11, 034602] Published Mon Mar 02, 2026

Author(s): Martin Heinrich, Michael Döllinger, and Rüdiger Schwarze

The atomization of airway mucus during speech is a primary mechanism for airborne disease transmission, yet the multiphase dynamics within the vocal folds remain largely uncharacterized. This study presents a Volume-of-Fluid CFD model to simulate the stretching and rupture of mucus bridges during phonation. Results show that small-scale surface perturbations seed realistic breakup patterns and that the bridge ruptures at a dynamic aspect ratio of approximately 20, far exceeding the quasi-static Rayleigh-Plateau stability limit. Higher transglottal pressures accelerate rupture, linking phonation intensity to aerosol generation.

[Phys. Rev. Fluids 11, 023103] Published Fri Feb 27, 2026

Author(s): Seema Chahal and Brato Chakrabarti

Active Stokesian suspensions are conventionally understood to generate dipolar stresses that destabilize aligned states in the bulk and drive systemwide spatiotemporally chaotic flows. Here, we report dynamics in suspensions of torque-driven spinning chiral particles that exhibit a distinct and prev…

[Phys. Rev. E 113, L023101] Published Thu Feb 26, 2026

Author(s): Thomas Bergier, Stéphane Jamme, Jérémie Gressier, Romain Gojon, and Laurent Joly

We study how the presence of a moderate sweep angle affects the behavior of shock/boundary layer interactions by means of wall-resolved Large Eddy Simulations. Several sweep angles up to 40deg are investigated. The mean properties of the flow are first reported, before analyzing the unsteady dynamics of the interaction. Intermediate frequencies at the separation location appear when sweep is present. They are related to spanwise-travelling structures detected around the interaction region.

[Phys. Rev. Fluids 11, 023401] Published Thu Feb 26, 2026

Author(s): K. Bhavsar, M. Stastna, and N. Castro-Folker

In fresh water between temperatures of 0 and 4 degrees Celsius, the equation of state (EOS) for density is nonlinear and the differences in density are extremely small. We call this the “cold water regime”. Using three-dimensional direct numerical simulations, we study the impact of the nonlinearity of the EOS on the development of the Kelvin-Helmholtz instability. We find that the nonlinear EOS displaces the pycnocline vertically above the shear layer which leads to differences in the onset of three-dimensional flow — both in terms of timing and scale. We further comment on how the extent of these differences changes under varying Prandtl and Reynolds numbers.

[Phys. Rev. Fluids 11, 023904] Published Wed Feb 25, 2026

Author(s): Haitao Zhu, Chenmingze Li, Long Chen, and Mingjiu Ni

Thermal convection under a horizontal magnetic field is known to promote quasi-two-dimensionalization, yet its impact on transport in strongly confined geometries is incompletely understood. Using three-dimensional simulations of low-Prandtl-number convection in a small-aspect-ratio cell, we reveal a transition from 3D cellular structures to quasi-2D rolls accompanied by regular/irregular flow reversals. Unlike classical roll breakup and reconnection, the reversals originate from mode competition within vertically stacked vortices. Unified transport scaling and an extension of elliptical instability theory quantitatively explain the observed dimensional transition and flow-state selection.

[Phys. Rev. Fluids 11, 023703] Published Mon Feb 23, 2026

Author(s): Hamid Reza Zandi Pour, Perry L. Johnson, and Michele Iovieno

The heat transfer in a turbulent thermal mixing layer of a fluid laden with inertial particles with finite heat capacity is investigated using direct numerical simulations. A reduced phase-space analysis, combined with a moment-of-total-enthalpy formulation, reveals how particle inertia and finite thermal response organize velocity–temperature correlations. These mechanisms lead to a self-similar regime in which particles dominate enthalpy transport, with maximum enhancement near a unity Stokes number. The results connect phase-space dynamics to global heat-transfer scaling in inhomogeneous turbulence.

[Phys. Rev. Fluids 11, 024308] Published Mon Feb 23, 2026

Author(s): Sandip Sarkar and Arnab Kumar De

The present reserch investigates two-dimensional numerical simulations of vortex-induced vibrations (VIV) of initially tandem circular cylinders with two degrees of freedom in both the streamwise and transverse directions, undergoing rigid collisions for varying mass ratios. The cylinders exhibit a natural tendency to reconfigure their mean positions into a side-by-side arrangement. As the mass ratio increases, the VIV dynamics progressively evolve from chaotic behavior toward more organized, periodic-like states.

[Phys. Rev. Fluids 11, 024702] Published Mon Feb 23, 2026

Author(s): J. R. Carpenter

The behavior of waves on a water surface is usually classified in terms of the different modes of oscillation that are present. However, for water that is flowing, this description alone will miss a vital part of the physics.

[Phys. Rev. Fluids 11, 024804] Published Mon Feb 23, 2026

Author(s): Eunhye An and Eric Johnsen

We investigate the effects of compressibility and geometry on turbulent/nonturbulent mixing in the absence of a mean shear. Focusing on initially homogeneous isotropic turbulence adjacent to a quiescent fluid in planar and cylindrical geometries, we theoretically predict the evolution of the mixing region width and turbulent kinetic energy and validate these predictions using direct numerical simulation. Compared to decaying homogeneous isotropic turbulence, we find that the decay rate is enhanced by dilatation due to energy transport to the nonturbulent region and by diverging geometries.

[Phys. Rev. Fluids 11, 024607] Published Fri Feb 20, 2026

Author(s): Gopal Verma and Wei Li

Particle motion at fluid interfaces is commonly governed by static capillary interactions, limiting active control. Here, we introduce a geometry-controlled capillary well formed by a neck-shaped meniscus around a vertically actuated rod, enabling reversible trapping and guided migration of particles. Elliptical rods generate anisotropic curvature landscapes that focus particles toward regions of maximum curvature, revealing an optimal aspect ratio for trapping efficiency. Theoretical predictions are validated through experiments and simulations.

[Phys. Rev. Fluids 11, 023903] Published Thu Feb 19, 2026