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Comparison of finite element and finite volume methods for simulation of natural ventilation in greenhouses

机译:温室自然通风模拟的有限元和有限体积方法比较

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摘要

This article aims to contribute to the discussion on the efficiency of two different discretization methods used as computational fluid dynamics (CFD) solvers for the simulation of natural ventilation in greenhouses. The focus is not on a general use of CFD, but rather on its specific application to simulate airflow in naturally ventilated greenhouses. After a short review of the basic model and its extensions, we compare the accuracy and computational efficiency of two simulation codes based on the Finite Element Method (FEM) and the Finite Volume Method (FVM) for two-dimensional incompressible turbulent flow in naturally ventilated greenhouses. FVM software (ANSYS/FLUENT v 6.3.) is the most frequently used CFD code in ventilation research, but few papers using FEM software (ANSYS/FLOTRAN v. 11.0) have been published. CFD simulations have been compared to experimental data for 12 cases corresponding to three greenhouse types. The experimental greenhouses were chosen to represent a large range of ventilation situations: buoyancy effect in a mono-span greenhouse with adiabatic walls, buoyancy and wind effect in a multi-span greenhouse and ventilation in an Almeria-type greenhouse under conditions of large temperature gradient and high wind speeds. The data from simulations and field experiments were compared using different parameters to analyze the effectiveness of experimental data in the validations of CFD models.The possibility of repeating simulations with different discretization methods and commercial software has been tested, as well as the type of experimental data needed to ensure correct validation of CFD models for use in greenhouse ventilation studies. To this end, temperature distribution measurements are preferable to set-point measurements and the use of visualization techniques (laser sheets) or the measurement of velocity vectors (anemometer) are more indicative than ventilation rates.The computational capacity of these approaches has also been analyzed, comparing their performance in terms of the overall database space necessary to store the numerical models and the necessary CPU time to compute one step of the convergence process. On average, the FEM required twice as much computing time per cell and step as FVM, and the amount of required memory storage was approximately 10 times greater for the FEM. (C) 2010 Elsevier B.V. All rights reserved.
机译:本文旨在为讨论用作计算流体动力学(CFD)求解器的温室中自然通风的两种不同离散化方法的效率做出贡献。重点不在于CFD的一般用途,而在于其在自然通风的温室中模拟气流的特定应用。在简短回顾了基本模型及其扩展之后,我们比较了基于有限元方法(FEM)和有限体积方法(FVM)的两种模拟代码在自然通风条件下二维不可压缩湍流的准确性和计算效率温室。 FVM软件(ANSYS / FLUENT v 6.3。)是通气研究中最常用的CFD代码,但是使用FEM软件(ANSYS / FLOTRAN v。11.0)的论文很少。已将CFD模拟与对应于三种温室类型的12个案例的实验数据进行了比较。选择实验温室来代表大范围的通风情况:具有绝热壁的单跨温室的浮力效应,多跨温室的浮力和风效应以及温度梯度大的阿尔梅里亚型温室的通风和高风速。使用不同的参数对来自仿真和现场实验的数据进行比较,以分析CFD模型验证中实验数据的有效性。测试了使用不同离散化方法和商业软件重复进行仿真的可能性,以及实验数据的类型需要确保正确验证用于温室通风研究的CFD模型。为此,温度分布测量优于设定点测量,并且使用可视化技术(激光纸)或速度矢量的测量(风速计)比通风率更具指示性。还分析了这些方法的计算能力,根据存储数值模型所需的整体数据库空间和计算收敛过程的第一步所需的CPU时间,比较它们的性能。平均而言,FEM每个单元和每个步骤所需的计算时间是FVM的两倍,并且所需的内存存储量约为FEM的10倍。 (C)2010 Elsevier B.V.保留所有权利。

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