cuticle 发表于 2025-3-25 05:37:46
Theoretical and Numerical Study of Evaporation Effects in Spray Flamelet Modeling,t spray combustion are based on laminar gas flame structures neglecting the influence of spray evaporation in the laminar spray flamelet. In this work, a combined theoretical and numerical study of the impact of spray evaporation on the structure of laminar spray flames is presented. Numerical simullymphedema 发表于 2025-3-25 09:07:23
Large Eddy Simulation of Diluted Turbulent Spray Combustion Based on FGM Methodology: Effect of fuetion. To retrieve the flow, mixing and combustion proper-ties, an Eulerian-Lagrangian approach is adopted. The method includes a full two-way coupling between the interacting two phases in presence, while the evaporation process is described by a non-eqnilibrium vaporization model. The carrier phase教义 发表于 2025-3-25 13:46:16
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http://reply.papertrans.cn/32/3192/319108/319108_24.pngBrocas-Area 发表于 2025-3-25 22:58:09
978-3-319-35451-4Springer International Publishing Switzerland 2014鞠躬 发表于 2025-3-26 03:02:46
Experiments and Numerical Simulations of Turbulent Combustion of Diluted Sprays978-3-319-04678-5Series ISSN 1382-4309 Series E-ISSN 2215-1826Monolithic 发表于 2025-3-26 07:20:07
Performance of the Banking Sector in Greece, turbulent flame structure, auto-ignition and atomization with reference to well-characterized burners that could be implemented by modelers with relative ease. The discussion of turbulent combustion is limited to dilute sprays stabilized on a simple piloted burner. Attention is shifted to the struc注意力集中 发表于 2025-3-26 09:38:07
https://doi.org/10.1007/978-3-030-81018-4phase context, various choices for boundary conditions as well as modeling frameworks and formulations are evaluated. Both large eddy simulation (LES) and Reynolds-averaged Navier-Stokes (RANS) approaches showed the ability to capture droplet evolution with regards to mean and fluctuating velocities愤世嫉俗者 发表于 2025-3-26 14:17:29
http://reply.papertrans.cn/32/3192/319108/319108_29.png分散 发表于 2025-3-26 18:22:53
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