计算流体力学在燃烧室不同烈度燃烧模拟中的应用

A. Aravindkumar, Rajiv Kumar, Shorab Jain
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引用次数: 4

摘要

火灾场建模(计算流体力学)作为一种重要的设计工具,越来越受到人们的关注,以满足现代先进建筑的性能化火灾设计。本文介绍了计算流体力学(CFD)在Steckler实验数据池中预测火灾引起的速度和温度分布的应用。本文以不同火灾荷载下的试验数据为例进行了研究。在高度为2.8 m × 2.8 m × 2.18 m的室内进行了Steckler室火灾实验。舱门开口为0.74米× 1.83米,以满足通风条件。在房间中央的地板上冲洗一个多孔气体燃烧器,在隔间内直径为0.3m。根据上述实验数据,利用ANSYS CFX-5商用代码进行燃烧建模仿真研究。报道了31.6、62.9、105.3和158.0 kW不同强度火场模型与实验域的模拟结果对比。在模拟边界条件不变的情况下,仅改变火灾强度即可看出CFD工具的性能。对车门中心线温度、速度和房间角落温度进行了预测,并与实验数据和FDS进行了比较。计算结果与实验数据吻合较好。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Application of Computational Fluid Dynamics for Different Fire Strengths in a Compartment Using Combustion Modelling
Fire field modelling (Computation Fluid Dynamics) has become more and more attractive as a critical design tool to meet Performance-based fire design on advanced modern buildings. This paper describes the application of Computational Fluid Dynamics (CFD) to predict velocities and temperature distributions induced by a fire in a Steckler’s experimental data [1]. The experimental data of different fire loads is taken as case study for present investigation. The experiments of Steckler’s compartment fire were conducted to investigate fire-induced flows through the opening in a compartment of size 2.8 m × 2.8 m × 2.18 m (height). The compartment has a doorway opening of 0.74 m × 1.83 m to account the ventilation condition. A porous gas burner is flushed at the floor in the centre of the room with the diameter of 0.3m in the compartment. With the above experimental data, simulation studies were performed with combustion modelling using commercial code of ANSYS CFX-5. The comparison of simulation results of fire field models with experimental domain for different strengths of fire 31.6, 62.9, 105.3 and 158.0 kW is reported. The boundary conditions of the simulation are kept constant, only fire strength is changed to see the performance of the CFD tool. The door centreline temperature, velocities and room corner temperatures are predicted and compared with experimental data as well as with FDS. The results are in good agreement with the experimental data.
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