首页> 外文会议>ASME International Mechanical Engineering Congress and Exposition; 20041113-19; Anaheim,CA(US) >EXPANSION OF A MODIFIED TRANSIENT LIQUID CRYSTAL METHOD FOR THIN PLATES OF DIFFERENT MATERIALS
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EXPANSION OF A MODIFIED TRANSIENT LIQUID CRYSTAL METHOD FOR THIN PLATES OF DIFFERENT MATERIALS

机译:不同材料薄板的改进的瞬态液体晶体方法的扩展

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The purpose of this research is to apply a modified transient liquid crystal method to a thin flat plate to determine the local temperature distribution and heat transfer coefficient. This research examines three different plates: 1) 1/8 inch thick Plexiglas plate, 2) 1/2 inch thick Plexiglas plate, and 3) 1/8 inch thick aluminum plate. Each plate is approximately 6 inches in length by 3 inches in width. The temperature distributions on a flat plate are viewed over time using a liquid crystal thermography (LCT) technique. The plates are coated with a wide band liquid crystal (R30C5W) and fixed in a vertically oriented wind tunnel. For any thickness plate, the speed of the tunnel was adjusted for a Reynolds number within the range of approximately 22100 and 23100. For the theoretical analysis, the thin flat plate used a convective surface boundary condition and a 2-D transient finite-differencing conduction scheme. An initial local heat transfer coefficient distribution is selected based upon flat plate theory, and is used to calculate an initial streamwise temperature distribution. The local heat transfer coefficient distribution is readjusted until the theoretical temperature distribution matches the experimental temperature distribution over the center surface of the plate. This technique allows a wider application of transient LCT and for heat transfer coefficients to be mapped on thin surfaces of different materials.
机译:本研究的目的是将改进的瞬态液晶方法应用于薄平板,以确定局部温度分布和传热系数。这项研究检查了三种不同的板:1)1/8英寸厚的有机玻璃板,2)1/2英寸厚的有机玻璃板和3)1/8英寸厚的铝板。每个板的长度约为6英寸,宽度约为3英寸。使用液晶热成像(LCT)技术可以随时观察平板上的温度分布。这些板涂有宽带液晶(R30C5W),并固定在垂直方向的风洞中。对于任何厚度的板,将隧道的速度调整为雷诺数在大约22100和23100的范围内。为了进行理论分析,薄平板使用对流表面边界条件和二维瞬态有限差分传导方案。基于平板理论选择初始局部传热系数分布,并将其用于计算初始沿流的温度分布。重新调节局部传热系数分布,直到理论温度分布与板中心表面上的实验温度分布相匹配为止。此技术允许更广泛地应用瞬态LCT,并将传热系数映射到不同材料的薄表面上。

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