Pub Date : 2024-07-15DOI: 10.1016/j.compfluid.2024.106370
Bao-Shan Wang , Naveen Kumar Garg
We propose third-order A-WENO finite difference schemes that are based on the recently introduced first-order numerical schemes in [N. K. Garg et al., Journal of Computational Physics, 407(2020)] for the systems of compressible Euler equations of gas dynamics. The convective components of these schemes (fluxes), both in one- and multi-dimensions, are free from complicated Riemann solvers. Third-order characteristic-wise WENO-Z interpolations are employed to obtain the third-order point values required for the numerical fluxes. To demonstrate the robustness and accuracy of the resulting schemes, we compare the numerical results with local Lax–Friedrichs (LLF) and Harten–Lax–van Leer (HLL) fluxes on various one- and two-dimensional examples. The obtained results outperform LLF and HLL fluxes in terms of enhancing the resolution of contact waves, especially near isolated steady and moving contact discontinuities, as well as in accurately resolving high-frequency waves in one dimension (1-D) and the small-scale structures in two dimensions (2-D).
{"title":"Third-order numerical scheme for Euler equations of gas dynamics using Jordan canonical based splitting flux","authors":"Bao-Shan Wang , Naveen Kumar Garg","doi":"10.1016/j.compfluid.2024.106370","DOIUrl":"10.1016/j.compfluid.2024.106370","url":null,"abstract":"<div><p>We propose third-order A-WENO finite difference schemes that are based on the recently introduced first-order numerical schemes in [N. K. Garg et al., Journal of Computational Physics, 407(2020)] for the systems of compressible Euler equations of gas dynamics. The convective components of these schemes (fluxes), both in one- and multi-dimensions, are free from complicated Riemann solvers. Third-order characteristic-wise WENO-Z interpolations are employed to obtain the third-order point values required for the numerical fluxes. To demonstrate the robustness and accuracy of the resulting schemes, we compare the numerical results with local Lax–Friedrichs (LLF) and Harten–Lax–van Leer (HLL) fluxes on various one- and two-dimensional examples. The obtained results outperform LLF and HLL fluxes in terms of enhancing the resolution of contact waves, especially near isolated steady and moving contact discontinuities, as well as in accurately resolving high-frequency waves in one dimension (1-D) and the small-scale structures in two dimensions (2-D).</p></div>","PeriodicalId":287,"journal":{"name":"Computers & Fluids","volume":"281 ","pages":"Article 106370"},"PeriodicalIF":2.5,"publicationDate":"2024-07-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141712072","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-11DOI: 10.1016/j.compfluid.2024.106364
A. Beccantini , C. Corre , S. Gounand , C.-H. Phan
An artificial compressibility approach is proposed to compute the solution of the compressible equations in the low Mach number limit, in closed domain with moving boundaries. The low Mach number stiffness is reduced by introducing an artificial sound speed, much lower than the physical one. This allows to avoid both the acoustic time step restriction and the loss of accuracy of classical compressible solvers, without solving a Poisson equation for the pressure or using the time-implicit discretization of the Turkel-type preconditioning technique. Moreover the proposed formulation involves the conservative variables plus the dynamic pressure, which facilitates the implementation of the approach in classical CFD codes for compressible flows. The numerical experiments presented show that the approach is both accurate and CPU efficient.
{"title":"An artificial compressibility approach to solve low Mach number flows in closed domains","authors":"A. Beccantini , C. Corre , S. Gounand , C.-H. Phan","doi":"10.1016/j.compfluid.2024.106364","DOIUrl":"10.1016/j.compfluid.2024.106364","url":null,"abstract":"<div><p>An artificial compressibility approach is proposed to compute the solution of the compressible equations in the low Mach number limit, in closed domain with moving boundaries. The low Mach number stiffness is reduced by introducing an artificial sound speed, much lower than the physical one. This allows to avoid both the acoustic time step restriction and the loss of accuracy of classical compressible solvers, without solving a Poisson equation for the pressure or using the time-implicit discretization of the Turkel-type preconditioning technique. Moreover the proposed formulation involves the conservative variables plus the dynamic pressure, which facilitates the implementation of the approach in classical CFD codes for compressible flows. The numerical experiments presented show that the approach is both accurate and CPU efficient.</p></div>","PeriodicalId":287,"journal":{"name":"Computers & Fluids","volume":"280 ","pages":"Article 106364"},"PeriodicalIF":2.5,"publicationDate":"2024-07-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0045793024001968/pdfft?md5=3c1e8f8f18e0eb1776c399c9dc23ba2d&pid=1-s2.0-S0045793024001968-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141629805","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
<div><p>It is attempted earnestly to elucidate the mechanism of collision and drainage of liquid mass around the spherical substrate suspended within the hollow cylinder using Gerris open-source code by employing Volume of Fluid (VOF) methodology. Various influencing parameters, namely, sphere-to-droplet diameter ratio <span><math><mrow><mo>(</mo><mrow><msub><mi>D</mi><mi>s</mi></msub><mo>/</mo><msub><mi>D</mi><mi>o</mi></msub></mrow><mo>)</mo></mrow></math></span>, Weber number<span><math><mrow><mspace></mspace><mo>(</mo><mrow><mi>W</mi><mi>e</mi></mrow><mo>)</mo></mrow></math></span>, Ohnesorge number <span><math><mrow><mo>(</mo><mrow><mi>O</mi><mi>h</mi></mrow><mo>)</mo></mrow></math></span>, and Bond number<span><math><mrow><mo>(</mo><mrow><mi>B</mi><mi>o</mi></mrow><mo>)</mo></mrow></math></span> are employed to observe the drainage mechanism through the constricted path. The pattern of the interfacial morphology of droplet collision and drainage mechanism is presented using numerical contours. It is important to mention herein that the droplet undergoes several important stages like collision, cap formation, engulfment, drainage, and pinch-off. The passage between the sphere and the cylinder is sufficiently wider at a lower value of <span><math><mrow><msub><mi>D</mi><mi>s</mi></msub><mo>/</mo><msub><mi>D</mi><mi>o</mi></msub></mrow></math></span> due to which the liquid mass is drained out completely without any hindrance. The drainage process becomes considerably faster at a higher <span><math><mrow><mi>W</mi><mi>e</mi></mrow></math></span> compared to a lower <span><math><mrow><mi>W</mi><mi>e</mi></mrow></math></span>. In addition, the flow of liquid mass through the passage gets delayed at a greater <span><math><mrow><mi>O</mi><mi>h</mi></mrow></math></span> than a lower <span><math><mrow><mi>O</mi><mi>h</mi></mrow></math></span> assuming a given value of <span><math><mrow><mi>W</mi><mi>e</mi></mrow></math></span> and <span><math><mrow><msub><mi>D</mi><mi>s</mi></msub><mo>/</mo><msub><mi>D</mi><mi>o</mi></msub></mrow></math></span>. The liquid drop requires less time to pass through the constricted path at lower <span><math><mrow><mi>B</mi><mi>o</mi></mrow></math></span> for a given value of <span><math><mrow><msub><mi>D</mi><mi>s</mi></msub><mo>/</mo><msub><mi>D</mi><mi>o</mi></msub></mrow></math></span> and <span><math><mrow><mi>W</mi><mi>e</mi></mrow></math></span>. We have also attempted to quantify the drainage of liquid volume passes through the passage, which is denoted as <span><math><mrow><mo>(</mo><mrow><msup><mrow><mi>Q</mi></mrow><mo>*</mo></msup><mo>=</mo><mi>Q</mi><mo>/</mo><msub><mi>Q</mi><mi>o</mi></msub></mrow><mo>)</mo></mrow></math></span>. One can notice the increasing pattern of <span><math><mrow><mi>Q</mi><mo>/</mo><msub><mi>Q</mi><mi>o</mi></msub></mrow></math></span> with continuous progress of time stamp for all cases of <span><math><mrow><msub><mi>D</mi><mi>s</mi></msub><mo>/</mo><msub><mi>D</mi><mi>o</mi></msub
本研究采用流体体积(VOF)方法,使用 Gerris 开源代码,认真尝试阐明悬浮在空心圆柱体内的球形基质周围的液块碰撞和排水机制。采用各种影响参数,即球体与液滴直径比 (Ds/Do)、韦伯数 (We)、奥内索格数 (Oh) 和邦德数 (Bo),来观察通过收缩路径的排水机制。液滴碰撞和排水机制的界面形态是通过数值等值线呈现的。在此有必要提及液滴经历的几个重要阶段,如碰撞、帽形成、吞噬、排水和夹断。当 Ds/Do 值较低时,球体和圆柱体之间的通道足够宽,因此液滴可以毫无阻碍地完全排出。与较低的 We 值相比,较高的 We 值下的排液过程要快得多。此外,在给定 We 和 Ds/Do 值的情况下,Oh 越大,液流通过通道的时间越短。在给定 Ds/Do 和 We 值的情况下,当 Bo 值较低时,液滴通过收缩路径所需的时间较短。我们还尝试量化通过通道的液体体积排水量,即(Q*=Q/Qo)。我们可以注意到,在 We 值固定的情况下,在所有 Ds/Do 条件下,Q/Qo 都会随着时间戳的推移而增加。
{"title":"Mechanism of collision and drainage of liquid droplet around sphere placed within a hollow cylinder","authors":"Prakasha Chandra Sahoo , Jnana Ranjan Senapati , Basanta Kumar Rana","doi":"10.1016/j.compfluid.2024.106365","DOIUrl":"10.1016/j.compfluid.2024.106365","url":null,"abstract":"<div><p>It is attempted earnestly to elucidate the mechanism of collision and drainage of liquid mass around the spherical substrate suspended within the hollow cylinder using Gerris open-source code by employing Volume of Fluid (VOF) methodology. Various influencing parameters, namely, sphere-to-droplet diameter ratio <span><math><mrow><mo>(</mo><mrow><msub><mi>D</mi><mi>s</mi></msub><mo>/</mo><msub><mi>D</mi><mi>o</mi></msub></mrow><mo>)</mo></mrow></math></span>, Weber number<span><math><mrow><mspace></mspace><mo>(</mo><mrow><mi>W</mi><mi>e</mi></mrow><mo>)</mo></mrow></math></span>, Ohnesorge number <span><math><mrow><mo>(</mo><mrow><mi>O</mi><mi>h</mi></mrow><mo>)</mo></mrow></math></span>, and Bond number<span><math><mrow><mo>(</mo><mrow><mi>B</mi><mi>o</mi></mrow><mo>)</mo></mrow></math></span> are employed to observe the drainage mechanism through the constricted path. The pattern of the interfacial morphology of droplet collision and drainage mechanism is presented using numerical contours. It is important to mention herein that the droplet undergoes several important stages like collision, cap formation, engulfment, drainage, and pinch-off. The passage between the sphere and the cylinder is sufficiently wider at a lower value of <span><math><mrow><msub><mi>D</mi><mi>s</mi></msub><mo>/</mo><msub><mi>D</mi><mi>o</mi></msub></mrow></math></span> due to which the liquid mass is drained out completely without any hindrance. The drainage process becomes considerably faster at a higher <span><math><mrow><mi>W</mi><mi>e</mi></mrow></math></span> compared to a lower <span><math><mrow><mi>W</mi><mi>e</mi></mrow></math></span>. In addition, the flow of liquid mass through the passage gets delayed at a greater <span><math><mrow><mi>O</mi><mi>h</mi></mrow></math></span> than a lower <span><math><mrow><mi>O</mi><mi>h</mi></mrow></math></span> assuming a given value of <span><math><mrow><mi>W</mi><mi>e</mi></mrow></math></span> and <span><math><mrow><msub><mi>D</mi><mi>s</mi></msub><mo>/</mo><msub><mi>D</mi><mi>o</mi></msub></mrow></math></span>. The liquid drop requires less time to pass through the constricted path at lower <span><math><mrow><mi>B</mi><mi>o</mi></mrow></math></span> for a given value of <span><math><mrow><msub><mi>D</mi><mi>s</mi></msub><mo>/</mo><msub><mi>D</mi><mi>o</mi></msub></mrow></math></span> and <span><math><mrow><mi>W</mi><mi>e</mi></mrow></math></span>. We have also attempted to quantify the drainage of liquid volume passes through the passage, which is denoted as <span><math><mrow><mo>(</mo><mrow><msup><mrow><mi>Q</mi></mrow><mo>*</mo></msup><mo>=</mo><mi>Q</mi><mo>/</mo><msub><mi>Q</mi><mi>o</mi></msub></mrow><mo>)</mo></mrow></math></span>. One can notice the increasing pattern of <span><math><mrow><mi>Q</mi><mo>/</mo><msub><mi>Q</mi><mi>o</mi></msub></mrow></math></span> with continuous progress of time stamp for all cases of <span><math><mrow><msub><mi>D</mi><mi>s</mi></msub><mo>/</mo><msub><mi>D</mi><mi>o</mi></msub","PeriodicalId":287,"journal":{"name":"Computers & Fluids","volume":"281 ","pages":"Article 106365"},"PeriodicalIF":2.5,"publicationDate":"2024-07-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141701950","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-11DOI: 10.1016/j.compfluid.2024.106368
Yiming Qi , Jie Shen , Lian-Ping Wang , Zhaoli Guo
Recently, Qi et al. (2022) and Guo et al. (2023) proposed two alternative designs of an efficient mesoscopic method using the total-energy double-distribution-function (DDF) formulation, hereafter referred to as the Qi model and the Guo model. The two models share the same advantage of using only 40 discrete particle velocities to fully reproduce the Navier–Stokes-Fourier (NSF) system. However, the Guo model is based on a more rigorous kinetic consideration, while the Qi model relies on a more general design of the source term to allow for adjustable bulk-to-shear viscosity ratio. In this paper, we derive lifting relations for the Qi model based on two alternative approaches, namely, the Hermite expansion and the Chapman–Enskog expansion, which can be used to construct the boundary and initial conditions for the mesoscopic method. For three-dimensional compressible turbulence simulations, including compressible decaying homogeneous isotropic turbulence and Taylor–Green vortex flows, the derived two sets of lifting relations are applied to the initialization distribution function to study their impacts. Interestingly, for the Qi model, the two sets of lifting relations yield the same results without numerical artifacts, whereas for the Guo model, an appropriate lifting relation must be specified to avoid numerical artifacts resulting from the flow initialization (Qi et al., 2023).
{"title":"Lifting relations for a generalized total-energy double-distribution-function kinetic model and their impact on compressible turbulence simulation","authors":"Yiming Qi , Jie Shen , Lian-Ping Wang , Zhaoli Guo","doi":"10.1016/j.compfluid.2024.106368","DOIUrl":"10.1016/j.compfluid.2024.106368","url":null,"abstract":"<div><p>Recently, Qi et al. (2022) and Guo et al. (2023) proposed two alternative designs of an efficient mesoscopic method using the total-energy double-distribution-function (DDF) formulation, hereafter referred to as the Qi model and the Guo model. The two models share the same advantage of using only 40 discrete particle velocities to fully reproduce the Navier–Stokes-Fourier (NSF) system. However, the Guo model is based on a more rigorous kinetic consideration, while the Qi model relies on a more general design of the source term to allow for adjustable bulk-to-shear viscosity ratio. In this paper, we derive lifting relations for the Qi model based on two alternative approaches, namely, the Hermite expansion and the Chapman–Enskog expansion, which can be used to construct the boundary and initial conditions for the mesoscopic method. For three-dimensional compressible turbulence simulations, including compressible decaying homogeneous isotropic turbulence and Taylor–Green vortex flows, the derived two sets of lifting relations are applied to the initialization distribution function to study their impacts. Interestingly, for the Qi model, the two sets of lifting relations yield the same results without numerical artifacts, whereas for the Guo model, an appropriate lifting relation must be specified to avoid numerical artifacts resulting from the flow initialization (Qi et al., 2023).</p></div>","PeriodicalId":287,"journal":{"name":"Computers & Fluids","volume":"280 ","pages":"Article 106368"},"PeriodicalIF":2.5,"publicationDate":"2024-07-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141637544","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-11DOI: 10.1016/j.compfluid.2024.106366
David Gabriel Harispe, Pablo A. Kler
Droplet-based microfluidics gained significant attention for its high technological impact in various fields like (bio)analysis and (bio)synthesis. Precise and controlled droplet size is critical, for the encapsulated products, or the yield of chemical reactions. In a broad range of experimental parameters, the understanding of how droplets form, interact and move with accurate predictive models is crucial. In this work, numerical prototypes of droplet generators were made with Basilisk, an open source software for solving partial differential equations on adaptive Cartesian meshes including grid adaptation and scalability for High-Performance Computing (HPC). This research aims to analyze and compare the obtained droplets against existing experimental data. The evaluation involves qualitative and quantitative comparisons, considering various channel geometries, flow rates, and rheological conditions. The validation of the proposed tool in terms of accuracy and computational performance, enable us to offer to the microfluidics community a reliable tool to design and optimize droplet generators.
{"title":"Accurate numerical prototypes of microfluidic droplet generators with open source tools","authors":"David Gabriel Harispe, Pablo A. Kler","doi":"10.1016/j.compfluid.2024.106366","DOIUrl":"10.1016/j.compfluid.2024.106366","url":null,"abstract":"<div><p>Droplet-based microfluidics gained significant attention for its high technological impact in various fields like (bio)analysis and (bio)synthesis. Precise and controlled droplet size is critical, for the encapsulated products, or the yield of chemical reactions. In a broad range of experimental parameters, the understanding of how droplets form, interact and move with accurate predictive models is crucial. In this work, numerical prototypes of droplet generators were made with Basilisk, an open source software for solving partial differential equations on adaptive Cartesian meshes including grid adaptation and scalability for High-Performance Computing (HPC). This research aims to analyze and compare the obtained droplets against existing experimental data. The evaluation involves qualitative and quantitative comparisons, considering various channel geometries, flow rates, and rheological conditions. The validation of the proposed tool in terms of accuracy and computational performance, enable us to offer to the microfluidics community a reliable tool to design and optimize droplet generators.</p></div>","PeriodicalId":287,"journal":{"name":"Computers & Fluids","volume":"281 ","pages":"Article 106366"},"PeriodicalIF":2.5,"publicationDate":"2024-07-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141690274","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-11DOI: 10.1016/j.compfluid.2024.106363
Yin Zhang , Yujie Zhu , Zhensheng Sun , Siye Li , Yu Hu , Xuefeng Xia , Wei Zhang
A numerical scheme with good spectral properties is important for the simulation of compressible flows with various of length scales for fine flow scales resolving. The MDAD-HY scheme (Li et al., 2022) using a discontinuity detector and scale sensor achieves the minimized dispersion and adaptive dissipation property. However, the discontinuity detector is devised based on the ratio of the 1st-order and 2nd-order derivatives on two sides of the interface introducing excessive numerical cost. To address this issue, an efficient hybrid WENO scheme with minimized dispersion and adaptive dissipation properties is proposed in this work. Based on the characteristic-decomposition approach, the numerical flux of the present hybrid scheme is achieved by switching between the linear MDAD scheme and the MDAD-WENO scheme according to a new efficient non-dimensional discontinuity detector. The linear flux is reconstructed in a component-wise method to decrease the characteristic-projection operations. To further improve the spectral property of the present scheme, an adaptive parameter controlling the contribution of the optimal linear scheme according to the discontinuity indicator is introduced. Several benchmark test cases involving broadband of length scales and discontinuities are adopted to verify the efficiency and the high-resolution capability of the present scheme.
{"title":"An efficient hybrid WENO scheme with minimized dispersion and adaptive dissipation properties for compressible flows","authors":"Yin Zhang , Yujie Zhu , Zhensheng Sun , Siye Li , Yu Hu , Xuefeng Xia , Wei Zhang","doi":"10.1016/j.compfluid.2024.106363","DOIUrl":"10.1016/j.compfluid.2024.106363","url":null,"abstract":"<div><p>A numerical scheme with good spectral properties is important for the simulation of compressible flows with various of length scales for fine flow scales resolving. The MDAD-HY scheme (Li et al., 2022) using a discontinuity detector and scale sensor achieves the minimized dispersion and adaptive dissipation property. However, the discontinuity detector is devised based on the ratio of the 1st-order and 2nd-order derivatives on two sides of the interface introducing excessive numerical cost. To address this issue, an efficient hybrid WENO scheme with minimized dispersion and adaptive dissipation properties is proposed in this work. Based on the characteristic-decomposition approach, the numerical flux of the present hybrid scheme is achieved by switching between the linear MDAD scheme and the MDAD-WENO scheme according to a new efficient non-dimensional discontinuity detector. The linear flux is reconstructed in a component-wise method to decrease the characteristic-projection operations. To further improve the spectral property of the present scheme, an adaptive parameter controlling the contribution of the optimal linear scheme according to the discontinuity indicator is introduced. Several benchmark test cases involving broadband of length scales and discontinuities are adopted to verify the efficiency and the high-resolution capability of the present scheme.</p></div>","PeriodicalId":287,"journal":{"name":"Computers & Fluids","volume":"280 ","pages":"Article 106363"},"PeriodicalIF":2.5,"publicationDate":"2024-07-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141637545","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-10DOI: 10.1016/j.compfluid.2024.106362
Yong-Dong Liang , Zhi-Hui Li , Jie Liang , Jia-Zhi Hu
To study the influence of energy accommodation of scattering gas molecules on flow fields during large expired spacecraft reentry, a more elaborated gas-surface interaction model, compared with full Maxwellian diffuse model, is employed in implicit algorithms based on Boltzmann model equation. The characteristic distributions around cylinder at different fluid regimes are accordingly obtained by implicit algorithms, Navier-Stokes solver and DSMC ((Direct Simulation Monte Carlo) method. And the consistency of these results is verified. It is confirmed that present algorithms are capable of solving external flow problems covering various fluid regimes. Then the simulation results see that under current conditions set in the paper, pressure and temperature are proportional to wall activation (, is surface temperature, denotes as free stream temperature), but their amplitudes alter with at different fluid regimes. As for the effects of energy accommodation coefficients (), both pressure and temperature profiles vary in a linear way with . However, the variation ranges of these parameters are diverse with regard to different fluid regimes. These observations are favor to the construction of efficient forecasting software, which could predict the flight path of large defunct spacecraft. In this forecasting software, the external ballistics computations and aerothermodynamic simulations are synchronously carried out.
{"title":"The effects of energy accommodation of reflected gas molecules on flow structures during expired spacecraft reentry","authors":"Yong-Dong Liang , Zhi-Hui Li , Jie Liang , Jia-Zhi Hu","doi":"10.1016/j.compfluid.2024.106362","DOIUrl":"10.1016/j.compfluid.2024.106362","url":null,"abstract":"<div><p>To study the influence of energy accommodation of scattering gas molecules on flow fields during large expired spacecraft reentry, a more elaborated gas-surface interaction model, compared with full Maxwellian diffuse model, is employed in implicit algorithms based on Boltzmann model equation. The characteristic distributions around cylinder at different fluid regimes are accordingly obtained by implicit algorithms, Navier-Stokes solver and DSMC ((Direct Simulation Monte Carlo) method. And the consistency of these results is verified. It is confirmed that present algorithms are capable of solving external flow problems covering various fluid regimes. Then the simulation results see that under current conditions set in the paper, pressure and temperature are proportional to wall activation (<span><math><mrow><mi>ω</mi><mo>=</mo><mrow><msub><mi>T</mi><mi>w</mi></msub><mo>/</mo><msub><mi>T</mi><mi>∞</mi></msub></mrow></mrow></math></span>, <span><math><msub><mi>T</mi><mi>w</mi></msub></math></span> is surface temperature, <span><math><msub><mi>T</mi><mi>∞</mi></msub></math></span> denotes as free stream temperature), but their amplitudes alter with <span><math><mi>ω</mi></math></span> at different fluid regimes. As for the effects of energy accommodation coefficients (<span><math><msub><mi>α</mi><mi>e</mi></msub></math></span>), both pressure and temperature profiles vary in a linear way with <span><math><msub><mi>α</mi><mi>e</mi></msub></math></span>. However, the variation ranges of these parameters are diverse with regard to different fluid regimes. These observations are favor to the construction of efficient forecasting software, which could predict the flight path of large defunct spacecraft. In this forecasting software, the external ballistics computations and aerothermodynamic simulations are synchronously carried out.</p></div>","PeriodicalId":287,"journal":{"name":"Computers & Fluids","volume":"281 ","pages":"Article 106362"},"PeriodicalIF":2.5,"publicationDate":"2024-07-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141694041","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The numerical treatment of fluid–particle systems is a very challenging problem because of the complex coupling phenomena occurring between the two phases. Although an accurate mathematical modelling is available to address this kind of applications, the computational cost of the numerical simulations is very expensive. The use of the most modern high performance computing infrastructures could help to mitigate such an issue but not completely to fix it. In this work we develop a non intrusive data-driven reduced order model (ROM) for Computational Fluid Dynamics (CFD) - Discrete Element Method (DEM) simulations. The ROM is built using the proper orthogonal decomposition (POD) for the computation of the reduced basis space and the Long Short-Term Memory (LSTM) network for the computation of the reduced coefficients. We are interested to deal both with system identification and prediction. The most relevant novelties rely on (i) a filtering procedure of the full order snapshots to reduce the dimensionality of the reduced problem and (ii) a preliminary treatment of the particle phase. The accuracy of our ROM approach is assessed against the classic Goldschmidt fluidized bed benchmark problem. Finally, we also provide some insights about the efficiency of our ROM approach.
流体-粒子系统的数值处理是一个非常具有挑战性的问题,因为两相之间存在复杂的耦合现象。虽然有精确的数学模型可以解决这类应用问题,但数值模拟的计算成本非常昂贵。使用最先进的高性能计算基础设施有助于缓解这一问题,但不能完全解决。在这项工作中,我们为计算流体动力学(CFD)- 离散元素法(DEM)模拟开发了一种非侵入式数据驱动的减阶模型(ROM)。该模型采用适当的正交分解(POD)来计算还原基空间,并采用长短期记忆(LSTM)网络来计算还原系数。我们对系统识别和预测都很感兴趣。最重要的新颖之处在于:(i) 对全阶快照进行过滤,以降低简化问题的维度;(ii) 对粒子阶段进行初步处理。我们根据经典的 Goldschmidt 流化床基准问题对 ROM 方法的准确性进行了评估。最后,我们还就 ROM 方法的效率提出了一些见解。
{"title":"An LSTM-enhanced surrogate model to simulate the dynamics of particle-laden fluid systems","authors":"Arash Hajisharifi , Rahul Halder , Michele Girfoglio , Andrea Beccari , Domenico Bonanni , Gianluigi Rozza","doi":"10.1016/j.compfluid.2024.106361","DOIUrl":"https://doi.org/10.1016/j.compfluid.2024.106361","url":null,"abstract":"<div><p>The numerical treatment of fluid–particle systems is a very challenging problem because of the complex coupling phenomena occurring between the two phases. Although an accurate mathematical modelling is available to address this kind of applications, the computational cost of the numerical simulations is very expensive. The use of the most modern high performance computing infrastructures could help to mitigate such an issue but not completely to fix it. In this work we develop a non intrusive data-driven reduced order model (ROM) for Computational Fluid Dynamics (CFD) - Discrete Element Method (DEM) simulations. The ROM is built using the proper orthogonal decomposition (POD) for the computation of the reduced basis space and the Long Short-Term Memory (LSTM) network for the computation of the reduced coefficients. We are interested to deal both with system identification and prediction. The most relevant novelties rely on (i) a filtering procedure of the full order snapshots to reduce the dimensionality of the reduced problem and (ii) a preliminary treatment of the particle phase. The accuracy of our ROM approach is assessed against the classic Goldschmidt fluidized bed benchmark problem. Finally, we also provide some insights about the efficiency of our ROM approach.</p></div>","PeriodicalId":287,"journal":{"name":"Computers & Fluids","volume":"280 ","pages":"Article 106361"},"PeriodicalIF":2.5,"publicationDate":"2024-07-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141607102","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-02DOI: 10.1016/j.compfluid.2024.106360
Christina Kolokotronis, Brian C. Vermeire
This work introduces two new non-dimensional gradient-based adaptation indicators for feature-based polynomial adaptation with high-order unstructured methods when used for turbulent flows. Recently, the Flux Reconstruction (FR) approach has been introduced as a unifying framework for high-order unstructured spatial discretizations. To achieve high-order accuracy, FR utilizes an element-wise polynomial representation of the solution. In the current work, we consider three indicators for local adaptation of this polynomial degree. One, introduced previously, uses a non-dimensional maximal vorticity norm. Two new indicators are then introduced using the Frobenius norm of the velocity gradient, and the eigenvalue modulus of the velocity gradient, both normalized by the maximum local grid spacing and free stream velocity. These feature-based methods are simple to implement and have the potential to track small-scale turbulent structures that arise in scale-resolving simulations, such as Direct Numerical Simulation (DNS) and Large Eddy Simulation (LES). The vorticity, gradient, and eigenvalue-based polynomial adaptation strategies with the FR approach are used to solve the compressible Navier–Stokes equations. DNS simulations are performed for unsteady laminar flow over a two-dimensional circular cylinder, turbulent flow over a three-dimensional sphere, and massively separated flow over a Martian helicopter rotor airfoil section. Results show a reduction in computational cost, with approximately one-quarter of the number of degrees of freedom relative to a non-adaptive case. The Frobenius norm method performs consistently well for all applications, and is identified as being a preferred method when compared to the vorticity and maximum eigenvalue approaches.
这项工作介绍了两种新的基于梯度的非维度适应指标,用于在湍流中使用基于特征的多项式适应和高阶非结构化方法。最近,流量重构(FR)方法被引入作为高阶非结构化空间离散的统一框架。为了达到高阶精度,FR 采用了元素多项式表示解法。在当前的工作中,我们考虑了对多项式度进行局部调整的三个指标。其中一个是之前介绍过的,使用非维度最大涡度规范。之后,我们又引入了两个新指标,分别使用速度梯度的弗罗贝尼斯规范和速度梯度的特征值模量,这两个指标都根据最大局部网格间距和自由流速度进行了归一化处理。这些基于特征的方法简单易用,可用于跟踪尺度分辨率模拟(如直接数值模拟(DNS)和大涡模拟(LES))中出现的小尺度湍流结构。涡度、梯度和基于特征值的多项式适应策略与 FR 方法被用于求解可压缩纳维-斯托克斯方程。对二维圆柱体上的非稳态层流、三维球体上的湍流和火星直升机转子翼面截面上的大规模分离流进行了 DNS 模拟。结果表明,与非自适应情况相比,计算成本降低了,自由度数量减少了约四分之一。弗罗贝尼斯准则法在所有应用中都表现出色,与涡度和最大特征值法相比,弗罗贝尼斯准则法被认为是一种首选方法。
{"title":"Gradient-based polynomial adaptation indicators for high-order methods","authors":"Christina Kolokotronis, Brian C. Vermeire","doi":"10.1016/j.compfluid.2024.106360","DOIUrl":"https://doi.org/10.1016/j.compfluid.2024.106360","url":null,"abstract":"<div><p>This work introduces two new non-dimensional gradient-based adaptation indicators for feature-based polynomial adaptation with high-order unstructured methods when used for turbulent flows. Recently, the Flux Reconstruction (FR) approach has been introduced as a unifying framework for high-order unstructured spatial discretizations. To achieve high-order accuracy, FR utilizes an element-wise polynomial representation of the solution. In the current work, we consider three indicators for local adaptation of this polynomial degree. One, introduced previously, uses a non-dimensional maximal vorticity norm. Two new indicators are then introduced using the Frobenius norm of the velocity gradient, and the eigenvalue modulus of the velocity gradient, both normalized by the maximum local grid spacing and free stream velocity. These feature-based methods are simple to implement and have the potential to track small-scale turbulent structures that arise in scale-resolving simulations, such as Direct Numerical Simulation (DNS) and Large Eddy Simulation (LES). The vorticity, gradient, and eigenvalue-based polynomial adaptation strategies with the FR approach are used to solve the compressible Navier–Stokes equations. DNS simulations are performed for unsteady laminar flow over a two-dimensional circular cylinder, turbulent flow over a three-dimensional sphere, and massively separated flow over a Martian helicopter rotor airfoil section. Results show a reduction in computational cost, with approximately one-quarter of the number of degrees of freedom relative to a non-adaptive case. The Frobenius norm method performs consistently well for all applications, and is identified as being a preferred method when compared to the vorticity and maximum eigenvalue approaches.</p></div>","PeriodicalId":287,"journal":{"name":"Computers & Fluids","volume":"280 ","pages":"Article 106360"},"PeriodicalIF":2.5,"publicationDate":"2024-07-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0045793024001920/pdfft?md5=c059e203b4c7d93a0ea755a7cfe90303&pid=1-s2.0-S0045793024001920-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141607104","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-29DOI: 10.1016/j.compfluid.2024.106349
A. Navas-Montilla, J. Guallart, P. Solán-Fustero, P. García-Navarro
This paper focuses on the design and analysis of very high-order finite volume methods for the computation of simplified meso- and micro-scale atmospheric flows. In a dry atmosphere, these flows can be represented by the Euler equations with a gravitational source term. Two different approaches are considered here. While one of the approaches is fully conservative for the total energy, the other is formulated in a non-conservative form. The main focus of the paper is to analyze the performance of such models in combination with the traditional WENO reconstruction and the novel TENO reconstruction by examining the spectral properties of these reconstruction methods. The overarching goal is to determine whether the combination of these models and numerical schemes can be used to build an implicit Large Eddy Simulation framework, shedding light on their potential advantages or limitations in representing under-resolved atmospheric processes in the meso- and micro-scales.
{"title":"Exploring the potential of TENO and WENO schemes for simulating under-resolved turbulent flows in the atmosphere using Euler equations","authors":"A. Navas-Montilla, J. Guallart, P. Solán-Fustero, P. García-Navarro","doi":"10.1016/j.compfluid.2024.106349","DOIUrl":"https://doi.org/10.1016/j.compfluid.2024.106349","url":null,"abstract":"<div><p>This paper focuses on the design and analysis of very high-order finite volume methods for the computation of simplified meso- and micro-scale atmospheric flows. In a dry atmosphere, these flows can be represented by the Euler equations with a gravitational source term. Two different approaches are considered here. While one of the approaches is fully conservative for the total energy, the other is formulated in a non-conservative form. The main focus of the paper is to analyze the performance of such models in combination with the traditional WENO reconstruction and the novel TENO reconstruction by examining the spectral properties of these reconstruction methods. The overarching goal is to determine whether the combination of these models and numerical schemes can be used to build an implicit Large Eddy Simulation framework, shedding light on their potential advantages or limitations in representing under-resolved atmospheric processes in the meso- and micro-scales.</p></div>","PeriodicalId":287,"journal":{"name":"Computers & Fluids","volume":"280 ","pages":"Article 106349"},"PeriodicalIF":2.5,"publicationDate":"2024-06-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0045793024001816/pdfft?md5=0b226165687261fb653604b60e4ac2f2&pid=1-s2.0-S0045793024001816-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141541913","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}