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Using the inverse heat conduction problem and thermography for the determination of local heat transfer coefficients and fin effectiveness for longitudinal fins

机译:利用逆热传导问题和热成像技术确定纵向翅片的局部传热系数和翅片效能

摘要

Heat transfer is a physical process in which energy is exchanged. It occurs in numerous applications, such as production of electricity, building climatisation, food preparation,... Since energy consumption has increased tremendously in the last decades and this trend will continue, the concept of energy efficiency has become omnipresent. In electronics miniaturization has become a trend. Desktops, laptops, dvd-players, mp3-players, televisions,... are getting thinner and/or smaller. Together with the increase in work speed and capacity, these small dimensions cause the energy density of electronic components (chips, processors,. . . ) to intensify significantly. As the electric power supply for these components is converted into heat, the component temperature rises. Hence, large amount of electricity are dissipated in a small surface area and cause high heat fluxes in the electronic components. To prevent overheating (and therefore failure) of electronic components, efficient heat removal is necessary. A cheap and almost universally applicable method for the cooling of electronics uses air as coolant in combination with a heat sink. The heat sinks are placed on the electronic component in order to distribute the heat and to create a better heat transfer. A heat sink mostly consists of longitudinal fins. Fin shape adjustments can improve the heat transfer, without the need for an increase in fin volume. This dissertation is specifically aimed at the research on longitudinal fins. It takes off looking for a measurement method to determine the performance of longitudinal fins as well as possible performance improvements by adjustments to these fins. The developed technique offers a global examination with a performance parameter. Moreover, it creates the possibility to study local heat transfer effects. In this work, the technique is applied to longitudinal fins, specifically fins for the cooling of electronics, but can be extended to other fin types. Chapter one also provides a summary of previous research on longitudinal fins. The number of studies on local heat transfer coefficients is limited and these studies are often inaccurate. A study of different fin performance indicators was also made, whichindicated that the widely spread concept of fin efficiency is misleading, and a bad fin performance indicator. Nevertheless, many studies still aim for the highest possible fin efficiency, assuming this would guarantee the maximum heat transfer.A better, more reliable fin performance parameter is the fin effectiveness, or the performance ratio which is derived from it. As high fin effectiveness actually corresponds to a higher heat transfer, fin effectiveness was used as the fin performance indicator in this work. The developed measurement technique should not only be able to determine local heat transfer coefficients, it should also measure the fin effectiveness. To attain those goals, one has to determine the heat flux distribution in the fin. Normally, one does not measure heat fluxes, but temperatures, that make it possible to calculate the heat flux distribution. This requires a technique to accurately measure temperature profiles, and a numerical method to calculate the heat flux distribution from these measurements. This numerical method is developed in the second chapter. Determining heat fluxes from temperatures is known as the inverse heat conduction problem. This kind of problem is solved inversely. Whereas in a direct problem heat fluxes are imposed as boundary conditions and the temperature field is calculated from these conditions, in an inverse conduction problem the solution (temperature field) is known and the boundary conditions (heat fluxes) are determined from these temperatures. An introducing literature survey indicates that the inverse conduction problem is ill-posed and that it therefore can have several solutions. To obtain stable, physically correct solutions, mathematical methods are used. The second chapter offers a summary of the solution methods found in literature, which are all based on the minimization of a temperature functional. The inverse heat conduction problem studied in this work is three-dimensional, linear and steady state. Based on the summary of the different numerical techniques the most suitable methods are chosen. Two methods are taken into consideration: the steepest descent method (SDM) and the conjugate gradient method (CGM). Chapter two mathematically develops both of these similar techniques and writes the complete solution algorithm for both of them.These two solution algorithms are applied to some numerical test cases in chapter 3. The test cases consist of a rectangular longitudinal fin that partly covers a flat primary surface. Different heat transfer coefficient profiles are imposed on thefin walls and the primary surface. Using these boundary conditions, the temperature profiles on the same surfaces are calculated. These temperature profiles are considered as exact temperature measurements and are the boundary conditions for the inverse heat conduction problem. This inverse heat conduction problem is solved with both SDM and CGM. Afterwards, chapter three investigates the influenceof measurement errors on the measured temperature profiles for two different measurement accuracies: 0.1°C and 0.5°C. Apparently SDM and CGM have a comparable accuracy, but CGM converges much faster. The introduction of measurementerrors gives comparable results as in the ideal case of exact temperature measurements. Only at the edges the deviations increase significantly. Enlarging the measurement error from 0.1°C to 0.5°C does not lead to the expected drastic decrease in accuracy of the estimated profiles. The results are even comparable to the exact results. This indicates that the solution methods are not too sensitive to noise and thus suitable to process experimental measurement data. Relying on the results, CGM was chosen as solution method because of the faster convergence rate.Chapter 4 develops a measurement method using infrared thermography as measurement technique. Infrared thermography has the advantage that it is a noncontactingmethod. Thus the temperature field and measurement object are not disturbed by the measurement. Moreover, thermography makes it possible to get complete temperature profiles with a single measurement. The first part of the chapter explains some basic notions on radiation and thermography. Calibration methods are drawn up and applied. An error analysis is executed on the parameters that determine the incident radiation energy and on the camera specific properties, resulting in an uncertainty for the measured temperature values. The second part of the chapter explains the measurement setup. First the dimensionsof the studied fins are determined based on the Reynolds analogy and on data from literature. Subsequently, the composition of the experimental setup is described. A low speed wind tunnel is used to set the environmental conditions and vary the Reynlods number (Re), which allows examining the influence of Re on the fin effectiveness and local heat transfer coefficients. A heat source is placed at the bottom of the fin, in combination with a guard heater to limit uncontrolled temperature losses. The power of the heat source is based on the fin temperature that should be attained to perform the most accurate temperature measurements with the infrared camera. The end of the chapter presents the different fin forms that will be studied: solid rectangular longitudinal fins and perforated fins with various numbers of perforations.The final chapter accomplishes the data reduction and presents the results. The temperature images, measured with the infrared camera during the experiments, are converted to a matrix with temperature values. This matrix can be used as aboundary condition for the inverse heat conduction problem that is solved with the developed solution method based on CGM. This solution makes it possible to determine the local heat fluxes and fin effectivenesss. The results obtained forthe rectangular longitudinal fins agree with data from literature. The local heat transfer coefficients indicate the expected trends, and even show the influence of a horseshoe vortex at the base of the fin. The results for the perforated fins show the influence of the perforations and of restarting the boundary layer: after a perforation higher local heat transfer coefficients are found. The comparison with valuesfrom literature confirms the obtained results. The results for fin effectiveness are not accurate enough to draw conclusions for this. To conclude, chapter 6 presents the most important findings and perspectives for future work.
机译:传热是交换能量的物理过程。它发生在许多应用中,例如电力生产,建筑气候变化,食品制备等。由于在过去的几十年中能源消耗量急剧增加,而且这种趋势还将继续,因此能源效率的概念已无处不在。在电子领域中,小型化已成为趋势。台式机,笔记本电脑,dvd播放器,mp3播放器,电视等越来越薄。随着工作速度和工作量的增加,这些小的尺寸导致电子组件(芯片,处理器等)的能量密度显着增强。随着这些组件的电源转换成热量,组件温度上升。因此,大量的电耗散在较小的表面积中并且在电子部件中引起高的热通量。为了防止电子组件过热(因此发生故障),必须有效地排热。一种便宜且几乎普遍适用的电子设备冷却方法是将空气作为冷却剂与散热器结合使用。散热器放置在电子组件上,以便散发热量并产生更好的热传递。散热器主要由纵向散热片组成。翅片形状的调整可以改善热传递,而无需增加翅片的体积。本文主要针对纵向鳍片的研究。它开始寻找一种确定纵向散热片性能的测量方法,以及通过调整这些散热片来改善性能的方法。所开发的技术可对性能参数进行全面检查。此外,它为研究局部传热效应提供了可能性。在这项工作中,该技术应用于纵向散热片,特别是用于冷却电子设备的散热片,但可以扩展到其他散热片类型。第一章还概述了以前对纵向鳍片的研究。关于局部传热系数的研究数量有限,而且这些研究往往不准确。还对不同的鳍片性能指标进行了研究,结果表明,广泛使用的鳍片效率概念具有误导性,并且鳍片性能指标不佳。尽管如此,许多研究仍以尽可能高的鳍片效率为目标,假设这将确保最大的传热效果。一个更好,更可靠的鳍片性能参数是鳍片的效率或由此得出的性能比。由于高翅片效率实际上对应于较高的热传递,因此在这项工作中将翅片效率用作翅片性能指标。发达的测量技术不仅应该能够确定局部传热系数,而且还应该测量散热片的有效性。为了实现这些目标,必须确定散热片中的热通量分布。通常,不测量热通量,而是测量温度,这使得可以计算热通量分布。这就需要一种能够精确测量温度分布的技术,以及一种通过这些测量来计算热通量分布的数值方法。在第二章中开发了这种数值方法。从温度确定热通量被称为逆导热问题。这种问题反过来解决了。在直接问题中,将热通量作为边界条件,并根据这些条件计算温度场,而在逆传导问题中,解(温度场)是已知的,并且边界条件(热通量)由这些温度确定。一项介绍性文献调查表明,逆传导问题是不适当的,因此可以有多种解决方案。为了获得稳定的,物理上正确的解决方案,使用了数学方法。第二章总结了文献中发现的解决方法,这些方法都是基于温度函数的最小化。在这项工作中研究的逆导热问题是三维,线性和稳态。基于不同数值技术的总结,选择了最合适的方法。考虑了两种方法:最速下降法(SDM)和共轭梯度法(CGM)。第二章在数学上开发了这两种相似的技术,并为它们编写了完整的求解算法。这两种求解算法在第三章中应用于一些数值测试用例。测试用例由矩形纵向鳍组成,部分覆盖了平坦的主表面。在翅片壁和主表面上施加了不同的传热系数分布。使用这些边界条件,计算相同表面上的温度曲线。这些温度曲线被认为是精确的温度测量值,并且是逆导热问题的边界条件。 SDM和CGM都解决了逆导热问题。然后,第三章研究了两种不同测量精度(0.1°C和0.5°C)下测量误差对测量温度曲线的影响。显然,SDM和CGM具有相当的精度,但是CGM收敛得更快。与精确温度测量的理想情况相比,测量误差的引入提供了可比的结果。仅在边缘处,偏差才会显着增加。将测量误差从0.1°C扩大到0.5°C不​​会导致预计轮廓精度的急剧下降。结果甚至与精确结果相当。这表明解决方案方法对噪声不太敏感,因此适合处理实验测量数据。根据该结果,由于收敛速度较快,因此选择CGM作为求解方法。第4章开发了一种以红外热成像为测量技术的测量方法。红外热成像的优势在于它是一种非接触式方法。因此,温度场和测量对象不受测量干扰。此外,热成像技术可以通过一次测量获得完整的温度曲线。本章的第一部分介绍了有关辐射和热成像的一些基本概念。制定并应用校准方法。对确定入射辐射能量的参数和摄像机的特定属性执行错误分析,从而导致所测温度值的不确定性。本章的第二部分介绍了测量设置。首先,根据雷诺兹类比和文献资料确定所研究鳍片的尺寸。随后,描述了实验装置的组成。使用低速风洞来设置环境条件并更改雷诺兹数(Re),这可以检查Re对鳍效率和局部传热系数的影响。一个热源被放置在散热片的底部,与保护加热器结合在一起以限制不受控制的温度损失。热源的功率取决于使用红外热像仪执行最精确的温度测量应达到的散热片温度。本章的最后介绍了将要研究的不同翅片形式:实心矩形纵向翅片和具有各种穿孔数量的穿孔翅片。最后一章完成了数据精简并给出了结果。在实验过程中用红外热像仪测量的温度图像将转换为具有温度值的矩阵。该矩阵可以用作反热传导问题的边界条件,该问题可以通过基于CGM的改进求解方法来解决。该解决方案使得确定局部热通量和散热片效率成为可能。矩形纵向鳍片获得的结果与文献数据吻合。局部传热系数表明了预期的趋势,甚至表明了翅片底部的马蹄涡的影响。穿孔鳍片的结果显示了穿孔和边界层重新开始的影响:穿孔后,发现较高的局部传热系数。与来自文献的值的比较证实了所获得的结果。鳍片有效性的结果不够准确,无法得出结论。总而言之,第6章介绍了未来工作中最重要的发现和观点。

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    Willockx Arnout;

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  • 年度 2009
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  • 原文格式 PDF
  • 正文语种 eng
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