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A novel coupling configuration for thermoacoustically-driven pulse tube coolers: Acoustic amplifier

机译:用于热声驱动脉冲管冷却器的新型耦合配置:声学放大器

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摘要

Thermoacoustically-driven pulse tube cooler can provide cryogenic cooling power with no moving components. Up to now, pulse tube cooler is directly coupled with the thermoacoustic engine and obtainable pressure ratio for the pulse tube cooler is limited by the capability of the thermoacoustic engine. The authors propose here the concept of acoustic amplifier, which is actually a long tube connecting the engine with the pulse tube cooler. Theoretical calculation shows that suitable length and diameter of the tube can lead to a pressure wave amplification effect which means that pressure wave amplitude coming from the thermoacoustic engine can be much amplified to drive the pulse tube cooler. Based on this, a 2.8 m long copper tube with 8 mm inner diameter is used as the acoustic amplifier in experiments. The experimental results show that due to the amplification effect, pressure wave amplitude at the inlet of the pulse tube cooler is over 2.5 times of that at the engine outlet. Typically, with 1.67 kW heating power, the pressure ratio provided by the engine is 1.11 while at the inlet of the pulse tube cooler the pressure ratio is 1.32, which leads to a lowest no-load temperature of 65.7 K.
机译:由热声驱动的脉冲管冷却器可提供低温冷却能力,而无需移动组件。迄今为止,脉冲管冷却器直接与热声发动机耦合,并且脉冲管冷却器可获得的压力比受热声发动机的能力限制。作者在这里提出了声放大器的概念,它实际上是连接发动机和脉冲管冷却器的长管。理论计算表明,合适的管长和管径可导致压力波放大效果,这意味着来自热声引擎的压力波振幅可被大大放大以驱动脉冲管冷却器。基于此,实验中使用了一根2.8 m长,内径为8 mm的铜管作为声放大器。实验结果表明,由于放大作用,脉冲管冷却器入口处的压力波振幅是发动机出口处的压力波振幅的2.5倍以上。通常,以1.67 kW的加热功率,发动机提供的压力比为1.11,而在脉冲管冷却器的进口处,压力比为1.32,这导致最低的空载温度为65.7K。

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