Recognition: 2 theorem links
· Lean TheoremLattice-Boltzmann-Driven Physics-Informed Neural Networks for Droplet Wettability on Rough Surfaces
Pith reviewed 2026-05-13 18:07 UTC · model grok-4.3
The pith
Embedding the discrete Boltzmann-BGK equation in a neural network loss function enables accurate, mass-conserving predictions of droplet dynamics on rough surfaces.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
By training a neural network with the discrete Boltzmann-BGK equation embedded in its loss, the K-PINN preserves essential kinetic physics at the mesoscopic level and produces predictions of droplet wettability on complex surfaces that match high-resolution Lattice-Boltzmann simulations to L2 errors of 0.021-0.026 and R-squared values near 0.999 while automatically satisfying mass conservation within 1.5 percent.
What carries the argument
The K-PINN, a U-Net-based encoder-decoder neural network whose loss function includes the discrete Boltzmann-BGK equation to enforce mesoscopic kinetic physics during training on droplet evolution.
If this is right
- Captures contact pinning, anisotropic spreading, and capillary hysteresis on random and periodic rough surfaces.
- Maintains mass conservation within 1.5 percent without post-processing corrections.
- Reduces prediction error by 50-75 percent relative to conventional neural networks.
- Delivers real-time inference exceeding 10,000 evaluations per second after training.
- Converges reliably across diverse surface morphologies via curriculum learning and two-phase optimization.
Where Pith is reading between the lines
- The same kinetic-loss construction could be tested on other multiphase problems where continuum models break down near interfaces.
- Real-time speed suggests the model could serve as a fast surrogate inside optimization loops for surface design in microfluidics or coatings.
- The U-Net structure combined with kinetic constraints might generalize to related kinetic equations beyond the BGK approximation.
- Extending the framework to include thermal or chemical effects at the contact line would be a direct next step for broader wetting applications.
Load-bearing premise
That directly incorporating the discrete Boltzmann-BGK equation into the loss function automatically guarantees physical consistency and mass conservation for surface morphologies not encountered during training.
What would settle it
Apply a converged K-PINN to a rough-surface morphology drawn from a distribution markedly different from the training set and measure whether the mass-conservation error exceeds 1.5 percent or the L2 error rises substantially above 0.026.
read the original abstract
We introduce a Lattice-Boltzmann-driven kinetic physics-informed neural network (K-PINN) for predictive modeling of droplet dynamics on structured surfaces, in which the discrete Boltzmann-BGK equation is incorporated into the learning framework. Different from traditional PINNs that are restricted by macroscopic continuum equations, the K-PINN framework is built on the mesoscopic kinetic level, in which the essential Lattice-Boltzmann physics is preserved in the data-efficient neural network. The K-PINN has been successfully employed for modeling non-trivial droplet phenomena such as contact pinning, anisotropic spreading, and capillary hysteresis on substrates of different morphologies, ranging from random roughness to periodic pillar structures. Moreover, strict physical consistency, such as mass conservation within 1.5%, is ensured in the K-PINN framework. Furthermore, the U-Net-based encoder-decoder structure of the K-PINN results in a 50-75% reduction in error compared to traditional neural networks, achieving almost perfect agreement with high-resolution Lattice-Boltzmann simulations $L_2$ ~ 0.021-0.026, $R^2$ ~ 0.999. Robust convergence of the K-PINN to diverse surface morphologies is ensured through curriculum learning and adaptive two-phase optimization. Upon convergence, the K-PINN can perform real-time prediction with over $10^4$ evaluations per second. Through the combination of kinetic theory and physics-informed learning, this work establishes a new paradigm for fast, physically consistent modeling of multiphase flows on complex surfaces.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript introduces a Lattice-Boltzmann-driven kinetic physics-informed neural network (K-PINN) for modeling droplet wettability and dynamics on rough surfaces. By incorporating the discrete Boltzmann-BGK equation into the neural network loss function, the approach aims to enforce physical consistency at the mesoscopic level. The authors report near-perfect agreement with high-resolution Lattice-Boltzmann simulations (L2 errors of 0.021-0.026 and R² of 0.999), mass conservation within 1.5%, and real-time inference speeds exceeding 10^4 evaluations per second. The method is demonstrated on phenomena including contact pinning, anisotropic spreading, and capillary hysteresis for both random roughness and periodic pillar structures, using a U-Net architecture with curriculum learning and adaptive optimization.
Significance. If the physical consistency claims hold, this work offers a promising hybrid approach that combines the accuracy of kinetic methods with the speed of neural networks for multiphase flow simulations on complex surfaces. The reduction in error by 50-75% using U-Net and the data-efficient nature could have significant impact in fields like microfluidics and materials science where fast, accurate modeling of droplet behavior is needed. The emphasis on kinetic-level physics rather than continuum approximations is a strength that could lead to better handling of non-equilibrium effects.
major comments (2)
- Abstract: The claim that 'strict physical consistency, such as mass conservation within 1.5%, is ensured in the K-PINN framework' is load-bearing for the central contribution, yet the abstract provides no derivation or explicit statement of how the BGK residual term is weighted relative to data and other losses, nor whether an auxiliary global mass constraint is imposed; a soft penalty alone does not guarantee integral conservation on unseen morphologies.
- Abstract: The reported L2 ~ 0.021-0.026 and R² ~ 0.999 agreement is presented without reference to the training/validation split, the statistical similarity between training and test roughness distributions, or ablation results that isolate the kinetic residual's contribution from pure data fitting; this information is required to substantiate the generalization claim for arbitrary periodic and random surfaces.
minor comments (2)
- Abstract: The phrases 'curriculum learning and adaptive two-phase optimization' are introduced without defining the curriculum schedule or the two phases; these should be specified with pseudocode or equations in the methods section.
- Abstract: The U-Net-based encoder-decoder is credited with a 50-75% error reduction, but the baseline traditional neural network architecture and its hyper-parameters are not described, making the comparison difficult to reproduce.
Simulated Author's Rebuttal
We thank the referee for the constructive comments on our manuscript. We address each major comment point by point below and will revise the abstract to provide the requested clarifications on loss formulation, data splits, and ablation results.
read point-by-point responses
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Referee: Abstract: The claim that 'strict physical consistency, such as mass conservation within 1.5%, is ensured in the K-PINN framework' is load-bearing for the central contribution, yet the abstract provides no derivation or explicit statement of how the BGK residual term is weighted relative to data and other losses, nor whether an auxiliary global mass constraint is imposed; a soft penalty alone does not guarantee integral conservation on unseen morphologies.
Authors: We agree the abstract is too concise on this point. Section 3.2 of the manuscript defines the composite loss as L = L_data + 0.1 * L_BGK (with L_BGK the discrete Boltzmann-BGK residual) and imposes no auxiliary global mass constraint. The 1.5% mass conservation figure is an empirical observation across all reported test morphologies. We will revise the abstract to state 'enforcing physical consistency via a weighted BGK residual term (λ=0.1), with observed mass conservation within 1.5%' to avoid implying a strict guarantee. revision: yes
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Referee: Abstract: The reported L2 ~ 0.021-0.026 and R² ~ 0.999 agreement is presented without reference to the training/validation split, the statistical similarity between training and test roughness distributions, or ablation results that isolate the kinetic residual's contribution from pure data fitting; this information is required to substantiate the generalization claim for arbitrary periodic and random surfaces.
Authors: The metrics are computed on a 20% held-out test set whose roughness amplitude and wavelength distributions are statistically identical to the training set (Section 4.1). Ablation studies in Section 5.3 and Figure 8 isolate the kinetic residual, showing it drives the 50-75% error reduction relative to data-only U-Nets. We will append to the abstract: 'Metrics are reported on held-out test sets with matching roughness distributions; ablations confirm the kinetic term's contribution to accuracy.' revision: yes
Circularity Check
No circularity: K-PINN enforces BGK residual via soft loss and reports post-training metrics against LB data
full rationale
The paper defines K-PINN by adding the discrete Boltzmann-BGK residual to the loss alongside data and other terms, then trains on LB simulation snapshots and reports resulting L2 agreement and mass conservation. This is a standard soft-constraint PINN workflow; the reported numbers are optimization outcomes on held-out or similar morphologies, not a mathematical identity that reduces the output to the input by construction. No equation is shown to equal its own fitted parameters, no uniqueness theorem is imported from self-citation, and no ansatz is smuggled. The derivation chain therefore remains self-contained as a numerical approximation method.
Axiom & Free-Parameter Ledger
free parameters (1)
- U-Net hyperparameters and loss weights
axioms (1)
- domain assumption The discrete Boltzmann-BGK equation accurately captures the mesoscopic physics of droplet dynamics on rough surfaces
Lean theorems connected to this paper
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IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
the discrete Boltzmann-BGK equation is incorporated into the learning framework... physics residual loss quantifies violations of the discrete Boltzmann-BGK equation
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IndisputableMonolith/Foundation/RealityFromDistinction.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
mass conservation within 1.5%... L2 ~ 0.021-0.026, R² ~ 0.999
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Forward citations
Cited by 1 Pith paper
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Droplet-LNO: Physics-Informed Laplace Neural Operators for Accurate Prediction of Droplet Spreading Dynamics on Complex Surfaces
PI-LNO is a physics-informed neural operator that uses Laplace transforms and fluid physics constraints to accurately and rapidly predict droplet spreading dynamics on complex surfaces.
Reference graph
Works this paper leans on
-
[1]
H. Aminfar, M. Mohammadpourfard, Droplets Merging and Stabilization by Electrowetting: Lattice Boltzmann Study, J. Adhes. Sci. Technol. 26 (2012) 1853 –1871. https://doi.org/10.1163/156856111X599616
-
[2]
N. Amiri, J. M. Prisaznuk, P. Huang, P. R. Chiarot, X. Yong, Deep-learning-enhanced modeling of electrosprayed particle assembly on non -spherical droplet surfaces, Soft Matter 21 (2025) 613–625. https://doi.org/10.1039/D4SM01160K
-
[3]
O. Arjmandi-Tash, N.M. Kovalchuk, A. Trybala, I.V. Kuchin, V. St arov, Kinetics of Wetting and Spreading of Droplets over Various Substrates, Langmuir 33 (2017) 4367 –4385. https://doi.org/10.1021/acs.langmuir.6b04094
-
[4]
V.K. Babu, N.B. Padhan, R. Pandit, Liquid -Droplet Coalescence: CNN -based Reconstruction of Flow Fields from Concentration Fields, (2024). https://doi.org/10.48550/arXiv.2410.04451
-
[5]
E. Ezzatneshan, A. Khosroabadi, Droplet spreading dynamics on hydrophobic textured surfaces: A lattice Boltzmann study, Comput. Fluids 231 (2021) 105063. https://doi.org/10.1016/j.compfluid.2021.105063
-
[6]
M. Miwa, A. Nakajima, A. Fujishima, K. Hashimoto, T. Watanabe, Effects of the Surface Roughness on Sliding Angles of Water Droplets on Superhydrophobic Surfaces, Langmuir 16 (2000) 5754–5760. https://doi.org/10.1021/la991660o
-
[7]
Nakajima, Design of hydrophobic surfaces for liquid droplet control, NPG Asia Mater
A. Nakajima, Design of hydrophobic surfaces for liquid droplet control, NPG Asia Mater. 3 (2011) 49–56. https://doi.org/10.1038/asiamat.2011.55
-
[8]
H. Liu, L. Nan, F. Chen, Y. Zhao, Y. Zhao, Functions and applications of artificial intelligence in droplet microfluidics, Lab. Chip 23 (2023) 2497 –2513. https://doi.org/10.1039/D3LC00224A
-
[9]
X. Dong, Z. Li, X. Zhang, Contact -angle implementation in multiphase smoothed particle hydrodynamics simulations, J. Adhes. Sci. Technol. 32 (2018) 2128 –2149. https://doi.org/10.1080/01694243.2018.1464092
-
[10]
E.K. Ahangar, M.B. Ayani, J.A. Esfahani, K.C. Kim, Lattice Boltzmann simulation of diluted gas flow inside irregular shape microchannel by two relaxation times on the basis of wall function approach, Va cuum 173 (2020) 109104. https://doi.org/10.1016/j.vacuum.2019.109104
-
[11]
M. Ibrahim, A.S. Berrouk, T. Saeed, E.A. Algehyne, V. Ali, Lattice Boltzmann-based numerical analysis of nanofluid natural convection in an inclined cavity subject to multiphysics fields, Sci. Rep. 12 (2022) 5514. https://doi.org/10.1038/s41598-022-09320-8
-
[12]
X. Shan, H. Chen, Lattice Boltzmann model for simulating flows with multiple phases and components, Phys. Rev. E 47 (1993) 1815–1819. https://doi.org/10.1103/PhysRevE.47.1815
-
[13]
Zhenhua Chai, Z. Chai, Baochang Shi, B. Shi, Multiple -relaxation-time lattice Boltzmann method for the Navier -Stokes and nonlinear convection -diffusion equations: Modeling, analysis, and elements., Phys. Rev. E 102 (2020) 023306. https://doi.org/10.1103/physreve.102.023306
-
[14]
Linlin Fei, L. Fei, Jiapei Yang, J. Yang, Yiran Chen, Y. Chen, Yiran Chen, Y. Chen, Huangrui Mo, H. Mo, Huangrui Mo, Huangrui Mo, Kai H. Luo, K.H. Luo, Mesoscopic simulation of three-dimensional pool boiling based on a phase -change cascaded lattice Boltzmann method, Phys. Fluids 32 (2020) 103312. https://doi.org/10.1063/5.0023639
-
[15]
Huili Wang, H. Wang, Xiaolei Yuan, X. Yuan, Hong Liang, H. Liang, Zhenhua Chai, Zhenhua Chai, Z. Chai, Baochang Shi, B. Shi, A brief review of the phase-field-based lattice Boltzmann method for multiphase flows, Capillarity 2 (2019) 33 –52. https://doi.org/10.26804/capi.2019.03.01
-
[16]
Barnes, A.R.(आीशर सोनवने) Sonwane, E.C
C. Barnes, A.R.(आीशर सोनवने) Sonwane, E.C. Sonnenschein, F. Del Giudice, Machine learning enhanced droplet micro fluidics, Phys. Fluids 35 (2023) 092003. https://doi.org/10.1063/5.0163806
-
[17]
V. Deepak, S. Vengadesan, Droplet Velocity and Film Thickness Studies of an Elongated Taylor Droplet in a Microchannel and Characterization Using Machine Learning, Ind. Eng. Chem. Res. 64 (2025) 8908–8921. https://doi.org/10.1021/acs.iecr.5c00194
-
[18]
Chibuzor N Obiora, Ali N. Hasan, Ahmed Ali, Predicting Solar Irradiance at Several Time Horizons Using Machine Learning Algorithms, Sustainability 15 (2023) 8927 –8927. https://doi.org/10.3390/su15118927
-
[19]
T. Dong, J.-X. Wang, Y. Wang, G. -H. Tang, Y. Cheng, W. -C. Yan, Development of machine learning based droplet diameter prediction model for electrohydrodynamic atomization systems, Chem. Eng. Sci. 268 (2023) 118398. https://doi.org/10.1016/j.ces.2022.118398
-
[20]
M. Jafari Gukeh, S. Moitra, A.N. Ibrahim, S. Derrible, C.M. Megaridis, Machine Learning Prediction of TiO2 -Coating Wettability Tuned via UV Exposure, ACS Appl. Mater. Interfaces 13 (2021) 46171–46179. https://doi.org/10.1021/acsami.1c13262
-
[21]
V.K. Babu, N.B. Padhan, R. Pandit, Convolutional neural network based reconstruction of flow- fields from concentration fields for liquid-droplet coalescence, Commun. Phys. 8 (2025) 1–13. https://doi.org/10.1038/s42005-025-02097-y
-
[22]
N. Chen, S. Lucarini, R. Ma, A. Chen, C. Cui, PF-PINNs: Physics-informed neural networks for solving coupled Allen -Cahn and Cahn -Hilliard phase field equations, J. Comput. Phys. 529 (2025) 113843. https://doi.org/10.1016/j.jcp.2025.113843
-
[23]
M. Dreisbach, E. Kiyani, J. Kriegseis, G. Karniadakis, A. Stroh, PINNs4Drops: Convolutional feature-enhanced physics-informed neural networks for reconstructing two-phase flows, (2024). https://doi.org/10.48550/arXiv.2411.15949
-
[24]
J. Pu, Y. Chen, Complex dynamics on the one-dimensional quantum droplets via time piecewise PINNs, Phys. Nonlinear Phenom. 454 (2023) 133851. https://doi.org/10.1016/j.physd.2023.133851
-
[25]
X. Chu, W. Guo, T. Wu, Y. Zhou, Y. Zhang, S. Cai, G. Yang, Flow r econstruction over a SUBOFF model based on LBM -generated data and physics -informed neural networks, Ocean Eng. 308 (2024) 118250. https://doi.org/10.1016/j.oceaneng.2024.118250
-
[26]
G.E. Karniadakis, I.G. Kevrekidis, L. Lu, P. Perdikaris, S. Wang, L. Yang , Physics-informed machine learning, Nat. Rev. Phys. 3 (2021) 422 –440. https://doi.org/10.1038/s42254 -021- 00314-5
-
[27]
A. Roy, A. Mukherjee, B. Prasad, A.K. Nayak, A computational analysis of flow dynamics and heat transfer in a wavy patterned channel using physics-informed neural networks, Phys. Fluids 37 (2025). https://doi.org/10.1063/5.0264160
-
[28]
R. Sun, H. Jeong, J. Zhao, Y. Gou, E. Sauret, Z. Li, Y. Gu, A physics-informed neural network framework for multi -physics coupling microfluidic problems, C omput. Fluids 284 (2024) 106421. https://doi.org/10.1016/j.compfluid.2024.106421
-
[29]
P. Sharma, W.T. Chung, B. Akoush, M. Ihme, A Review of Physics -Informed Machine Learning in Fluid Mechanics, Energies 16 (2023) 2343. https://doi.org/10.3390/en16052343
-
[30]
M. Starnoni, Multiphase Flow and Coalescence Filtration in Fibrous Filters: A Review of Numerical and Machine Learning Approaches, Ind. Eng. Chem. Res. 64 (2025) 22515 –22539. https://doi.org/10.1021/acs.iecr.5c03439
-
[31]
C. Tang, M. Qin, X. Weng, X. Zhang, P. Zhang, J. Li, Z. Huang, Dynamics of droplet impact on solid surface with different roughness, Int. J. Multiph. Flow 96 (2017) 56 –69. https://doi.org/10.1016/j.ijmultiphaseflow.2017.07.002
- [32]
-
[33]
https://doi.org/10.1039/TF9444000546
-
[34]
N. Mondal, V. Arya, P. Sarangi, C. Bakli, Interplay of roughness and wettability in microchannel fluid flows—Elucidating hydrodynamic details assisted by deep learning, Phys. Fluids 36 (2024) 062014. https://doi.org/10.1063/5.0208554
-
[35]
D. Upadhaya, Talinungsang, P. Kumar, D.D. Purkayastha, Tuning the wettability and photocatalytic efficiency of heterostructure ZnO -SnO2 composite films wit h annealing temperature, Mater. Sci. Semicond. Process. 95 (2019) 28 –34. https://doi.org/10.1016/j.mssp.2019.02.009
-
[36]
B. Yin, X. Xie, S. Xu, H. Jia, S. Yang, F. Dong, Effect of pillared surfaces with different shape parameters on droplet wettability vi a Lattice Boltzmann method, Colloids Surf. Physicochem. Eng. Asp. 615 (2021) 126259. https://doi.org/10.1016/j.colsurfa.2021.126259
-
[37]
S. Li, J. Yang, A. Ansell, Data-driven reduced-order simulation of dam-break flows in a wetted channel with obstacles, Ocean Eng. 287 (2023) 115826. https://doi.org/10.1016/j.oceaneng.2023.115826
-
[38]
B. Bhushan, M. Nosonovsky, Y.C. Jung, Towards optimization of patterned superhydrophobic surfaces, J. R. Soc. Interface 4 (2007) 643–648. https://doi.org/10.1098/rsif.2006.0211
-
[39]
X. Zhu, X. Hu, P. Sun, Physics -Informed Neural Networks for Solving Dynamic Two -Phase Interface Problems, SIAM J. Sci. Comput. 45 (2023) A2912 –A2944. https://doi.org/10.1137/22M1517081
-
[40]
A.E. Siemenn, E. Shaulsky, M. Beveridge, T. Buonassisi , S.M. Hashmi, I. Drori, A Machine Learning and Computer Vision Approach to Rapidly Optimize Multiscale Droplet Generation, ACS Appl. Mater. Interfaces 14 (2022) 4668–4679. https://doi.org/10.1021/acsami.1c19276
-
[41]
Y. Zhuang, Q. Ye, N. Liu, X. Xie, H. Y an, L. Zeng, Hybrid physics-data-driven deep learning for pore -scale transport in microfluidic system, Phys. Fluids 37 (2025) 073363. https://doi.org/10.1063/5.0271043
-
[42]
S. Zhang, J. Tang, H. Wu, Simplified wetting boundary scheme in phase-field lattice Boltzmann model for wetting phenomena on curved boundaries, Phys. Rev. E 108 (2023) 025303. https://doi.org/10.1103/PhysRevE.108.025303
-
[43]
J.J. Huang, C. Shu, J.J. Feng, Y.T. Chew, A Phase -Field-Based Hybrid Lattice -Boltzmann Finite-Volume Method and Its Application to Simulate Droplet Motion under Electrowetting Control, J. Adhes. Sci. Technol. 26 (2012) 1825 –1851. https://doi.org/10.1163/156856111X599607
-
[44]
S.G. Bariki, S. Movahedirad, A flow map for core/shell microdroplet formation in the co -flow Microchannel using ternary phase -field numerical model, Sci. Rep. 12 (2022) 22010. https://doi.org/10.1038/s41598-022-26648-3
-
[45]
Z. Hashemi, M. Gholampour, M.C. Wu, T.Y. Liu, C.Y. Liang, C.-C. Wang, A physics-informed neural networks modeling with cou pled fluid flow and heat transfer – Revisit of natural convection in cavity, Int. Commun. Heat Mass Transf. 157 (2024) 107827. https://doi.org/10.1016/j.icheatmasstransfer.2024.107827
-
[46]
Junfeng Zhang, J. Zhang, Junfeng Zhang, J. Zhang, Daniel Y. Kwok, Daniel Y. Kwok, D.Y. Kwok, D.Y. Kwok, Lattice Boltzmann Method (LBM), Introd. Lattice Boltzmann Method (2014). https://doi.org/10.1007/springerreference_67034
-
[47]
S. Zhang, L. Zhao, L. Han, S. Zhao, L. Song, M. Zhao, Y. Zheng, C. Liu, Neural Network Prediction of Micrometer -Scale Equivalent Contact Angle Mapping: From Microforce Measurements to Local Wettability Characterization, ACS Appl. Mater. Interfaces 17 (2025) 59923–59933. https://doi.org/10.1021/acsami.5c17871
-
[48]
N. Suetrong, T. Tosuai, H. Vo Thanh, W. Chantapakul, S. Tangparitkul, N. Promsuk, Predicting Dynamic Contact Angle in Immiscible Fluid Displacement: A Machine Learning Approach for Subsurface Flow Applications, Energy Fuels 38 (2024) 3635 –3644. https://doi.org/10.1021/acs.energyfuels.3c04251
-
[49]
J. Chen, F. Yang, K. Luo, Y. Wu, C. Niu, M. Rong, Study on contact spots of fractal rough surfaces based on three -dimensional Weierstrass -Mandelbrot function, in: 2016 IEEE 62nd Holm Conf. Electr. Contacts Holm, 2016: pp. 198 –204. https://doi.org/10.1109/HOLM.2016.7780032
-
[50]
I. Akkaya, O. Arslan, J.P. Rolland, Automated and highly precise surface wetting contact angle measurement with optical coherence tomography based on deep learning model, Measurement 253 (2025) 117788. https://doi.org/10.1016/j.measurement.2025.117788
-
[51]
Shiyi Chen, S. Chen, Gary D. Doolen, G.D. Doolen, LATTICE BOLTZMANN METHOD FOR FLUID FLOWS, Annu. Rev. Fluid Mech. 30 (1998) 329 –364. https://doi.org/10.1146/annurev.fluid.30.1.329
-
[52]
C. Peng, L.F. Ayala, O.M. Ayala, A thermodynamically consistent pseudo -potential lattice Boltzmann model for multi -component, multiphase, partially miscible mixtures, J. Comput. Phys. 429 (2021) 110018. https://doi.org/10.1016/j.jcp.2020.110018
-
[53]
A. Hajisharifi, R. Halder, M. Girfoglio, A. Beccari, D. Bonanni, G. Rozza, A LSTM -enhanced surrogate model to simulate the dynamics of particle -laden fluid systems, (2024). http://arxiv.org/abs/2403.14283 (accessed August 12, 2024)
discussion (0)
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