微低温冷却器的高频回热器操作

R. Radebaugh, A. O'Gallagher
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引用次数: 51

摘要

斯特林和斯特林型脉冲管制冷机的尺寸主要取决于压力振荡器的尺寸。这种制冷机通常工作频率高达约60hz,冷端温度高于约60k。对于给定的功率输入,更高的工作频率将允许减小压力振荡器的尺寸和质量。然而,简单地提高工作频率会导致回热器损失很大。这里推导的简单解析方程显示了频率和压力的正确组合,以及优化的再生器几何形状,可以使再生器在高达1khz的频率下成功运行。在如此高的频率下,只有在压力约为5至8mpa,液压直径和长度非常小的情况下,才能实现高效的回热器运行。其他几何参数也必须针对这种条件进行优化。利用解析方程为参数的正确组合提供指导。本文用REGEN3.2软件对优化后的筛网再生器进行了60hz、400hz和1000hz运行的数值计算,结果表明,当平均压力为7mpa时,400 Hz和1000 Hz的性能系数分别约为60hz时的78%和68%,而60hz运行时的平均压力为2.5 MPa。平行管的1000hz性能系数与屏幕几何形状在60hz时的性能系数大致相同。与相同输入声功率的60 Hz情况相比,压缩机和冷端扫描体积在1000 Hz时减少了47倍,这可以为MEMS应用开发微低温冷却器。
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Regenerator Operation at Very High Frequencies for Microcryocoolers
The size of Stirling and Stirling‐type pulse tube cryocoolers is dominated by the size of the pressure oscillator. Such cryocoolers typically operate at frequencies up to about 60 Hz for cold‐end temperatures above about 60 K. Higher operating frequencies would allow the size and mass of the pressure oscillator to be reduced for a given power input. However, simply increasing the operating frequency leads to large losses in the regenerator. The simple analytical equations derived here show how the right combination of frequency and pressure, along with optimized regenerator geometry, can lead to successful regenerator operation at frequencies up to 1 kHz. Efficient regenerator operation at such high frequencies is possible only with pressures of about 5 to 8 MPa and with very small hydraulic diameters and lengths. Other geometrical parameters must also be optimized for such conditions. The analytical equations are used to provide guidance to the right combination of parameters. We give example numerical calculations with REGEN3.2 in the paper for 60 Hz, 400 Hz, and 1000 Hz operation of optimized screen regenerators and show that the coefficient of performance at 400 Hz and 1000 Hz is about 78 % and 68 %, respectively, of that for 60 Hz when an average pressure of 7 MPa is used with the higher frequency, compared with 2.5 MPa for 60 Hz operation. The 1000 Hz coefficient of performance for parallel tubes is about the same as that of the screen geometry at 60 Hz. The compressor and cold‐end swept volumes are reduced by a factor of 47 at 1000 Hz, compared with the 60 Hz case for the same input acoustic power, which can enable the development of microcryocoolers for MEMS applications.
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