通过诱导湍流增强4孔芯砖蓄热器的传热

P. Ramakrishnan, A. S. Krishnan
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引用次数: 2

摘要

本文用计算流体力学方法研究了显热装置内的瞬态传热和流体流动。考虑的几何形状是一个长度为455mm,直径为43mm的圆柱体,由低碳钢材料制成。在孔隙度为0.4、进口速度为2m/s(质量流量为0.0035 kg/s)的条件下,利用商业CFD软件进行了数值研究。在CFD软件中,对孔尺寸为13.6mm的4孔芯砖加热器的三维几何模型进行建模、网格化和仿真。采用k-ε模型将流体流动视为不可压缩,并假设流体和固体的热物性保持不变。对储能系统的充放电时间等热性能进行了评价。对不同的导热系数进行了参数化研究,模拟了整个系统的轴向温度变化和压降。以输入温度为465K作为蓄热器的条件进行温度模拟。蓄热器的侧向和出口条件分别为绝热和常压条件。本文研究了有和无诱导体时流体在4孔芯砖上的流动,其中诱导体将层流诱导为湍流。因此,流体在层流状态下以低雷诺数流动,而在湍流状态下由于诱导剂的存在而向高雷诺数流动。分析了无诱导、各孔入口处诱导和各孔发展长度附近诱导的情况。对存在和不存在诱导体的情况进行了计算分析。
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Heat Transfer Enhancement in a 4-Holed Cored Brick Regenerator by Inducing Turbulence
The article reports on the transient heat transfer and fluid flow in the sensible heat storage device using Computational Fluid Dynamics. The geometry considered is a cylinder of 455mm length and 43mm diameter made up of mild steel material. Numerical investigations have been done for a porosity of 0.4 and inlet velocity of 2m/s which corresponds to mass flow rate of 0.0035 kg/s by use of commercial CFD software. In CFD software the three dimensional geometrical model of the cored brick heater was modelled, meshed and simulated for 4 holed cored brick which corresponds to the hole size of 13.6mm. The fluid flow was considered to be incompressible with k-ε model to predict turbulence, and the thermo-physical properties of fluid and solid were assumed to remain constant. Thermal performance of storage system such as charging and discharging time were evaluated. A parametric study was conducted for different thermal conductivity, to simulate axial temperature variation and pressure drop across the system. Temperature simulations are carried out by input as 465K as the condition in the regenerator. The lateral and outlet condition of the regenerator are given as adiabatic and atmospheric condition. This paper represents the fluid flow across the 4 hole cored brick with and without inducer, where the inducer induces the laminar flow to turbulent. Thus the fluid flows is at low Renoylds number in the laminar regime and due to the presence of the inducer the flow get transformed to higher Renoylds number in the turbulent regime. Analysis is made for without inducer, inducer at the entrance of each holes and inducer is just next to the developing length on each holes. Result of the computational analysis was made for cases with and without the presence of inducer.
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