Solid-state microrefrigeration in conjonction with liquid cooling

Y. Ezzahri, A. Shakouri
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Abstract

Thermal design requirements are mostly driven by the peak temperatures. Reducing or eliminating hot spots could alleviate the design requirement for the whole package. Combination of solid-state and liquid cooling will allow removal of both hot spots and background heating. In this paper, we analyze the performance of thin film Bi2Te3 microcooler and the 3D SiGe based microrefrigerator and optimize the maximum cooling and cooling power density in the presence of flow. Liquid flow and heat transfer coefficient will change the background temperature of the chip but they also affect the performance of the solid-state coolers used to remove hot spots. Both Peltier cooling at interfaces and Joule heating inside the device could be affected by the fluid flow. We analyze conventional Peltier coolers as well as 3D coolers. We study the impact of various parameters such as thermoelectric leg thickness, thermal interface resistances, and geometry factor on the overall system performance. We find that the cooling of conventional Peltier cooler is significantly reduced in the presence of fluid flow. On the other hand, 3D SiGe can be effective to remove high power density hot spots up to 500 W/cm2. 3D microrefrigerators can have a significant impact if the thermoelectric figure-of-Thermal design requirements are mostly driven by the peak temperatures. Reducing or eliminating hot spots could alleviate the design requirement for the whole package. Combination of solid-state and liquid cooling will allow removal of both hot spots and background heating. In this paper, we analyze the performance of thin film Bi2Te3 microcooler and the 3D SiGe based microrefrigerator and optimize the maximum cooling and cooling power density in the presence of flow. Liquid flow and heat transfer coefficient will change the background temperature of the chip but they also affect the performance of the solid-state coolers used to remove hot spots. Both Peltier cooling at interfaces and Joule heating inside the device could be affected by the fluid flow. We analyze conventional Peltier coolers as well as 3D coolers. We study the impact of various parameters such as thermoelectric leg thickness, thermal interface resistances, and geometry factor on the overall system performance. We find that the cooling of conventional Peltier cooler is significantly reduced in the presence of fluid flow. On the other hand, 3D SiGe can be effective to remove high power density hot spots up to 500 W/cm2. 3D microrefrigerators can have a significant impact if the thermoelectric figure-of-merit, ZT, could reach 0.5 for a material grown on silicon substrate. It is interesting to note that there is an optimum microrefrigerator active region thickness that gives the maximum localized cooling. For liquid heat transfer coefficient between 5000 and 20000 W/m2/K, the optimum is found to be between 10 and 20 mum.merit, ZT, could reach 0.5 for a material grown on silicon substrate. It is interesting to note that there is an optimum microrefrigerator active region thickness that gives the maximum localized cooling. For liquid heat transfer coefficient between 5000 and 20000 W/m2/K, the optimum is found to be between 10 and 20 mum.
与液体冷却相结合的固态微制冷
热设计要求主要由峰值温度驱动。减少或消除热点可以减轻对整个封装的设计要求。将固态和液态冷却结合起来,可以消除热点和背景加热。本文分析了薄膜 Bi2Te3 微冷却器和基于三维 SiGe 的微制冷器的性能,并优化了流动情况下的最大冷却和冷却功率密度。液体流动和传热系数会改变芯片的背景温度,但也会影响用于消除热点的固态制冷器的性能。界面处的珀尔帖冷却和器件内部的焦耳加热都会受到液体流动的影响。我们分析了传统的珀尔帖冷却器和 3D 冷却器。我们研究了热电腿厚度、热界面电阻和几何系数等各种参数对整个系统性能的影响。我们发现,在有流体流动的情况下,传统珀尔帖冷却器的冷却效果明显降低。另一方面,三维 SiGe 可以有效消除高达 500 W/cm2 的高功率密度热点。如果热电热图设计要求主要由峰值温度驱动,那么三维微型制冷器就会产生重大影响。减少或消除热点可以减轻对整个封装的设计要求。将固态和液态冷却相结合,可以消除热点和背景加热。本文分析了薄膜 Bi2Te3 微冷却器和基于三维 SiGe 的微制冷器的性能,并优化了流动情况下的最大冷却和冷却功率密度。液体流动和传热系数会改变芯片的背景温度,但也会影响用于消除热点的固态制冷器的性能。界面处的珀尔帖冷却和器件内部的焦耳加热都会受到液体流动的影响。我们分析了传统的珀尔帖冷却器和 3D 冷却器。我们研究了热电腿厚度、热界面电阻和几何系数等各种参数对整个系统性能的影响。我们发现,在有流体流动的情况下,传统珀尔帖冷却器的冷却效果明显降低。另一方面,三维 SiGe 可以有效消除高达 500 W/cm2 的高功率密度热点。如果在硅衬底上生长的材料的热电效应系数(ZT)能达到 0.5,三维微型制冷器就能产生重大影响。值得注意的是,有一个最佳的微制冷器活性区厚度,可以提供最大的局部冷却效果。对于液体传热系数在 5000 到 20000 W/m2/K 之间的情况,最佳厚度为 10 到 20 mum.mer。值得注意的是,有一个最佳的微制冷器活性区厚度,可以提供最大的局部冷却效果。对于液体传热系数在 5000 和 20000 W/m2/K 之间的情况,最佳厚度为 10 至 20 μm。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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