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Experimental investigation of a single plate thermoacoustic refrigerator.

机译:单板热声制冷机的实验研究。

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摘要

Thermoacoustic refrigeration was developed during the past two decades as a new, environmentally safe refrigeration technology. The operation of thermoacoustic refrigerators employs acoustic power to pump heat from a cold to a hot temperature reservoir. The disadvantage of such devices is that, because of the poor performance of their individual components, the acoustic driver and heat exchangers, the efficiencies achieved up to date are lower when compared to commercially available refrigerators. The poor performance of the heat exchangers can be attributed to the fact that in thermoacoustic refrigerators the physical situation is characterized by oscillating flow with zero mean velocity. For such situations heat transfer has not yet been completely understood, and conventional heat exchanger design methods are not applicable.; One objective of the present thesis was to gain better insight into the heat transfer in oscillatory flows. In order to achieve this goal the oscillating temperature fields and time averaged heat fluxes in a thermoacoustic refrigerator model were measured applying holographic interferometry (HI) combined with high-speed cinematography. To apply HI to temperature measurements in an acoustic field two new evaluation procedures that account for acoustic pressure variations were developed. The procedures were verified by comparing temperature measurements obtained with the new evaluation procedures to theory. The temperature and heat flux measurements revealed unexpected heat transfer behavior: heat flow from the colder working fluid to a heated plate at the edge of the plate was detected. Through the energy balance this heat transfer into the plate could be related to the thermoacoustic effect. In addition to revealing this unexpected behavior, the thermoacoustic effect was visualized through the temperature measurements.; Additionally, a design optimization algorithm for thermoacoustic refrigerators was developed. Through a first law analysis four main modules of the refrigerator were identified: (i) acoustic driver, (ii) resonance tube, (iii) heat exchangers and thermoacoustic core. To find a global performance maximum of the thermoacoustic refrigerator, viewed as a thermodynamic system, the analysis suggests separate optimization of these four main modules. From the linear theory 19 independent design parameters, relevant for the optimization of the thermoacoustic core, were identified. By introducing new scaling arguments it was possible to reduce the number of parameters to 10. Performance calculations of the thermoacoustic core predict limiting values of 40% to 50% of Carnot's efficiency.; With the two new evaluation procedures for HI this dissertation provides a novel contribution to the field of metrology, and with the measurements of the temperature fields and heat fluxes as well as with the design algorithm and the optimization scheme new contributions to the field of thermoacoustics.
机译:在过去的二十年中,热声制冷是一种新的,对环境安全的制冷技术。热声制冷机的运行利用声能将热量从冷库抽到热库中。这种设备的缺点在于,由于它们的各个部件,声学驱动器和热交换器的性能较差,因此与商用冰箱相比,迄今为止实现的效率较低。热交换器的不良性能可以归因于以下事实:在热声制冷机中,物理情况的特征在于平均流速为零的振荡流。对于这种情况,尚未完全了解热传递,并且传统的热交换器设计方法不适用。本论文的目的之一是更好地了解振荡流中的热传递。为了实现此目标,使用全息干涉术(HI)与高速摄影相结合的方法,测量了热声制冷机模型中的振荡温度场和时间平均热通量。为了将HI应用于声场中的温度测量,开发了两个新的评估程序来解决声压变化。通过将使用新评估程序获得的温度测量值与理论值进行比较,对程序进行了验证。温度和热通量的测量结果显示出出乎意料的热传递行为:检测到从较冷的工作流体到板边缘的加热板的热流。通过能量平衡,热传递到板中可能与热声效应有关。除了揭示这种意外行为外,还通过温度测量将热声效果可视化。此外,开发了一种热声冰箱的设计优化算法。通过第一定律分析,确定了冰箱的四个主要模块:(i)声驱动器,(ii)共振管,(iii)热交换器和热声芯。为了找到被视为热力学系统的热声制冷机的整体性能最大化,分析建议对这四个主要模块进行单独优化。根据线性理论,确定了19个独立的设计参数,这些参数与热声芯的优化有关。通过引入新的缩放参数,可以将参数的数量减少到10。热声芯的性能计算预测出卡诺效率的40%至50%的极限值。借助HI的两种新的评估程序,本论文为计量学领域做出了新的贡献,随着温度场和热通量的测量以及设计算法和优化方案对热声学领域的新贡献。

著录项

  • 作者

    Wetzel, Martin Josef.;

  • 作者单位

    The Johns Hopkins University.;

  • 授予单位 The Johns Hopkins University.;
  • 学科 Engineering Mechanical.; Applied Mechanics.
  • 学位 Ph.D.
  • 年度 1999
  • 页码 175 p.
  • 总页数 175
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 机械、仪表工业;应用力学;
  • 关键词

  • 入库时间 2022-08-17 11:48:01

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