Rotation and translation of a long curved fiber
๐จ new paper alert ๐จ
1/3 ๐ Measuring experimentally the dispersion of #microplastic #fibres in turbulent flows is incredibly challenging, due to their small size. However, experiments are key to develop reliable models to predict the fate of microplastics in #environmental #flows.
06.05.2025 08:19 โ ๐ 6 ๐ 1 ๐ฌ 1 ๐ 0
๐งต3/6 Here we provide an efficient and parallel #open #source code to analyze these problems. We extend the simulation capabilities of the Advanced Finite Difference solver AFiD, developed at @poftwente.bsky.social, and we focus on the simulation of strongly convective Darcy flows.
20.03.2025 08:14 โ ๐ 0 ๐ 1 ๐ฌ 1 ๐ 0
Evolution of a Rayleigh-Taylor instability in a porous - 3D visualization of the concentration field.
๐จ PAPER ALERT ๐จ Comput. Phys. Commun.
๐งต1/6 We present the code AFiD-Darcy, designed for massively parallel numerical simulations of convective porous media flows. Thanks to Guru Sreevanshu Yerragolam, Detlef Lohse and Roberto Verzicco for the great collaboration at @poftwente.bsky.social
20.03.2025 08:14 โ ๐ 5 ๐ 1 ๐ฌ 1 ๐ 0
CoCalc -- JFM-Notebooks
CoCalc Share Server
This is our first paper with a JFM Notebookโan excellent initiative by J. Fluid Mech. to host interactive code and data. It greatly enhances reproducibility and transparency in fluid dynamics researchโa commendable step forward.
cocalc.com/Cambridge/S0...
22.02.2025 09:45 โ ๐ 1 ๐ 1 ๐ฌ 0 ๐ 0
[SM1]: The role of viscosity on drop impact forces
The case shown here is We = 40, Oh = 0.0025. Paper: https://doi.org/10.48550/arXiv.2311.03012 Full description: Comparison of the drop impact force $F(t)$ obtained from experiments and simulations for the three typical cases with impact velocity $V_0 = 1.2\,\si{\meter}/\si{\second}, 0.97\,\si{\meter}/\si{\second}, 0.96\,\si{\meter}/\si{\second}$, diameter $D_0 = 2.05\,\si{\milli\meter}, 2.52\,\si{\milli\meter}, 2.54\,\si{\milli\meter}$, surface tension $\gamma = 72\,\si{\milli\newton}/\si{\meter}, 61\,\si{\milli\newton}/\si{\meter}, 61\,\si{\milli\newton}/\si{\meter}$ and viscosity $\eta_d = 1\,\si{\milli\pascal\second}, 25.3\,\si{\milli\pascal\second}, 80.2\,\si{\milli\pascal\second}$. These parameter give $Oh = 0.0025, 0.06, 0.2$ and $We = 40$. For the three cases, the two peak amplitudes, $F_1/(\rho_dV_0^2D_0^2) \approx$ 0.82, 0.92, 0.99 at $t_1 \approx 0.03\sqrt{\rho_dD_0^3/\gamma}$ and $F_2/(\rho_dV_0^2D_0^2) \approx$ 0.37, 0.337, 0.1 at $t_2 \approx 0.42\sqrt{\rho_dD_0^3/\gamma}$, characterize the inertial shock from impact and the Worthington jet before takeoff, respectively. The drop reaches the maximum spreading at $t_{\text{max}}$ when it momentarily stops and retracts until $0.8\sqrt{\rho_dD_0^3/\gamma}$ when the drop takes off ($F = 0$). The black and gray dashed lines in panel (a) mark $F = 0$ and the resolution $F = 0.5\,\si{\milli\newton}$ of our piezoelectric force transducer, respectively. We stress the excellent agreement between experiments and simulations without any free parameters. The left part of each numerical snapshot shows (on a $\log_{10}$ scale) the dimensionless local viscous dissipation function $\tilde{\xi}_\eta \equiv \xi_\eta D_0/\left(\rho_dV_0^3\right) = 2Oh\left(\boldsymbol{\tilde{\mathcal{D}}:\tilde{\mathcal{D}}}\right)$, where $\boldsymbol{\mathcal{D}}$ is the symmetric part of the velocity gradient tensor, and the right part the velocity field magnitude normalized with the impact velocity.
๐ข Checkout our work in J. Fluid Mech. (bit.ly/3QuxMgE) on how viscosity alters drop-impact forces. Together with Bin Zhang, Cunjing Lv, & Detlef Lohse. The first and second force peaks emerge from distinct flow mechanismsโone at impact, another at take-off. @poftwente.bsky.social bit.ly/4gUvD8P
22.02.2025 09:39 โ ๐ 13 ๐ 2 ๐ฌ 1 ๐ 1
Congratulations, Giulia Piumini, for successfully defending her thesis: Fluid structure interaction of turbulent flows with complex-shape bodies. tinyurl.com/26dd34j2.
Congratulations also to the promotion team: Detlef Lohse and Roberto Verzicco. #FluidDynamics #particles
30.01.2025 16:49 โ ๐ 5 ๐ 2 ๐ฌ 0 ๐ 0
โกTo clog or not to clog: @alvaromarin.bsky.social and Mathieu Souzy summarize how particle bridging drives clogging in noncohesive suspensionsโfrom arch formation at constrictions to fluid-induced stabilization and destabilization. @utwente.bsky.social @poftwente.bsky.social #clogging #fluiddynamics
25.01.2025 13:30 โ ๐ 4 ๐ 1 ๐ฌ 0 ๐ 0
Our Annual Review of Fluid Mechanics is now accessible for free! find out how to make a jellyfish smoothy ๐ชผ, or how to cross a river without a bridge ๐ชต... thanks @annualreviews.bsky.social for make this volume open!
www.annualreviews.org/content/jour...
24.01.2025 10:15 โ ๐ 17 ๐ 6 ๐ฌ 0 ๐ 1
Gallery of Fluid Motion
Delighted that our research on evaporating binary drops by Pim Dekker, Christian Diddens, and Detlef Lohse, studying non-monotonic surface tension and symmetry-breaking dynamics, was one of the the 2024 APS-DFD Milton van Dyke award winners.
arXiv: tinyurl.com/2c7v7lzc.
Video: tinyurl.com/2crhbjtp
11.12.2024 12:36 โ ๐ 5 ๐ 1 ๐ฌ 0 ๐ 1
๐ Just wrapped up an insightful seminar on microscale #Acoustofluidics with Henrik Bruus from Technical University of Denmark! Exploring the shift from traditional glass/silicon devices to innovative polymer-based solutions. @utwente.bsky.social
11.12.2024 12:20 โ ๐ 1 ๐ 1 ๐ฌ 0 ๐ 0
follow the work here: doi.org/10.1017/jfm....
06.12.2024 14:42 โ ๐ 4 ๐ 1 ๐ฌ 0 ๐ 0
Devaraj van der Meer from @poftwente.bsky.social @utwente.bsky.social explores the impact of boiling liquids on solid surfaces. Condensing vapor can create pressures far exceeding those in water-air scenarios. Fascinating implications for industrial applications! ๐ #FluidDynamics #Physics #APSDFD24
26.11.2024 18:33 โ ๐ 4 ๐ 1 ๐ฌ 0 ๐ 1
The Driscoll lab is an experimental physics lab at Northwestern University; our research lies at the junction between soft-matter physics and fluid dynamics.
(Carlowen = Carl + Owen, he/him) Physics Instructor at Johnston Community College. I've studied turbulence in the ocean, atmosphere, and planets!
Research unit on #physics and #mechanics of heterogeneous media
CNRS, ESPCI Paris-PSL, Sorbonne Universitรฉ, Universitรฉ Paris Citรฉ
France
Home: www.pmmh.espci.fr
๐ฆฃ: mathstodon.xyz/@PMMH_lab
The University of Twente is currently not actively using this Blueskye account.
The latest news in Physics, Computer Science, Engineering, Astronomy and Astrophysics from @cambridgeup.bsky.social
Oxford Fluid Dynamics Lab at the University of Oxford. Led by Prof. Alfonso Castrejon-Pita.
School of Engineering at Brown University, Fluids and Thermal Sciences
sites.brown.edu/harrislab
Curious soul who dreams in colour.
Fluid dynamicist working on turbulent multiphase flows with particles, bubbles, droplets, and heat, and including melting and dissolutionโฆ
Scientist and engineer, TU Wien ๐ฆ๐น๐ช๐บ
Visit my website https://marcodepaoli.com/
Author, aerospace engineer, science communicator. Writes with excessive enthusiasm about fluid physics at FYFD.
Assistant Professor @pcc-wur.bsky.social @w-u-r.bsky.social | Soft matter | Biophysics | Interfacial hydrodynamics | Cell mechanics
https://www.physm-lab.org
Assistant Professor in Soft Matter Physics at Aalto University, Finland | Forces and flow in mesoscale living, fluid, & soft matter | ERC StG laureate & Research Council of Finland Fellow | EPL co-editor
aalto.fi/living-matter
Lecturer in Applied & Computational Maths @ UCD
Turbulence | Phase change | Environmental Flows | Numerical Methods
Fluid dynamicistโฏ| Assistant Professor, Physics Department, Durham Universityโฏ| ex-PoF (Univ.โฏTwente)โฏ| IITRโฏalumโฏ| soft-matterโฏ&โฏnonโNewtonian flows (drops, bubbles, jets, sheets)โฏ|โฏ#FluidDynamicsโฏ#SoftMatterโฏ#Dropsโฏ#Bubblesโฏ#DNS
Fluid physicist ๐ง๐ฌ attempting to understand nature ๐ one epsilon more every day, because "Not only is the universe stranger than we imagine, it is stranger than we can imagine." (Sir Arthur Eddington๐ญ) https://marin-lab.com + pof.tnw.utwente.nl
Interested in science, engineering, higher education, global warming, fluid & solid mechanics, droplets and bubbles, acoustics, energetics, free code, sociology of science.