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International Journal of Thermal Sciences
Research Hotspot & Journal Scope - Boltzmann


International Journal of Thermal Sciences - DOI: 10.1016/J.IJTHERMALSCI.2018.08.039
An optimal two-relaxation-time lattice Boltzmann equation for solid-liquid phase change: The elimination of unphysical numerical diffusion

J. H. Lu · Haiyan Lei · C. S. Dai ·

Physics
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International Journal of Thermal Sciences - DOI: 10.1016/J.IJTHERMALSCI.2018.10.015
Lattice Boltzmann simulations of the double-diffusive natural convection and oscillation characteristics in an enclosure with Soret and Dufour effects

Hongtao Xu · Zhuqing Luo · Qin Lou · Shuanyang Zhang · Jun Wang ·

Physics
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International Journal of Thermal Sciences - DOI: 10.1016/J.IJTHERMALSCI.2018.09.025
Study of laminar natural convection in a vertical annulus with inner wall covered by a porous layer by using lattice Boltzmann method

Zuo Wang · Yan Liu · Jiazhong Zhang · Nannan Dang ·

Materials Science
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International Journal of Thermal Sciences - DOI: 10.1016/j.ijthermalsci.2019.106112
Lattice Boltzmann simulation of thermal flows with complex geometry using a single-node curved boundary condition

Shi Tao · Baiman Chen · Hanmin Xiao · Si-Min Huang ·

Physics
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International Journal of Thermal Sciences - DOI: 10.1016/J.IJTHERMALSCI.2019.02.015
An immersed boundary-lattice Boltzmann method for electro-thermo-convection in complex geometries

Yang Hu · Decai Li · Xiao-Dong Niu · Shi Shu ·

Physics
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Far from the particle, when the potential becomes lower than its thermal value \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${{\varphi }_{{\text{T}}}} = \frac{{kT}}{e}$$\end{document} (k is the Boltzmann constant, T is the temperature, and e is the elementary charge), the potential decreases exponentially irrespective of the counterion sizes: \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\psi \left( r \right) = \frac{{\varphi \left( r \right)}}{{{{\varphi }_{{\text{T}}}}}} = {{\psi }_{{{\text{eff}}}}}\frac{a}{r}\exp \left( { - \kappa \left( {r - a} \right)} \right),$$\end{document} where r is the distance from the particle center and κ is the reciprocal Debye radius.

Features of Electrical Double Layers Formed Around Strongly Charged Nanoparticles Immersed in an Electrolyte Solution. The Effect of Ion Sizes [10.1134/S1061933X19060048]


Besides, our results can be verified using the modified Stefan–Boltzmann law.

Modified fermion tunneling from higher-dimensional charged AdS black hole in massive gravity [10.1140/EPJC/S10052-019-6959-1]


The model was trained using iteration Boltzmann inversion and a new heuristically–determined, distance–dependent scaling function that dramatically reduces the iterations required.

Coarse–grained molecular modeling of the microphase structure of polyurea elastomer [10.1016/J.POLYMER.2019.04.039]


A pseudo-potential based single component multiphase Lattice Boltzmann flow solver was developed.

Development and application of a high density ratio pseudopotential based two-phase LBM solver to study cavitating bubble dynamics in pressure driven channel flow at low Reynolds number [10.1016/J.EUROMECHFLU.2018.12.004]


Results suggest that a size-modified Poisson-Boltzmann description of the electrolyte solution is sufficient to qualitatively reproduce the main experimental trends.

Continuum models of the electrochemical diffuse layer in electronic-structure calculations. [10.1063/1.5054588]



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