欢迎登录材料期刊网

材料期刊网

高级检索

通过回热器数值计算程序REGEN深入理解回热器模型,计算回热器内部各项损失.基于各参数间的强弱关系讨论了回热器的优化设计流程.在此基础上,针对35 K、60 K和80 K温区及30~300 Hz频率,给出了回热器中质量流量、长度、填料以及充气压力对制冷效率COP的影响关系图,以期对回热器的工程实践提供指导.

Based on regenerator program REGEN,deep understanding of the regenerator was gained,and various kinds of losses inside a regenerator were calculated.An optimization design process was proposed based on dependency relationships between different parameters.On this basis,optimization calculations were carried out,variations of COP along with mass flow rate,regenerator length,matrix and charging pressure were obtained with the frequency from 30 to 300 Hz for 35 K,60 K and 80 K cold temperature respectively.This is expected to provide convenient reference for practical design of regenerators.

参考文献

[1] Radebaugh, R .Cryocoolers: the state of the art and recent developments[J].Journal of Physics. Condensed Matter,2009(16):164219:1-164219:9.
[2] B. Wang;Z.H. Gan .A critical review of liquid helium temperature high frequency pulse tube cryocoolers for space applications[J].Progress in aerospace sciences,2013(Aug.):43-70.
[3] H.J.M. ter Brake;G.F.M. Wiegerinck .Low-power cryocooler survey[J].Cryogenics,2002(11):705-718.
[4] 杨鲁伟,Thummes Guenter.单级高频脉冲管制冷机研究[J].工程热物理学报,2007(01):24-26.
[5] Vanapalli S;Lewis M;Gan Z;Radebaugh R .120 Hz pulse tube cryocooler for fast cooldown to 50 K[J].Applied physics letters,2007(7):72504-1-72504-3-0.
[6] Dai W;Yu GY;Zhu SL;Luo EC .300 Hz thermoacoustically driven pulse tube cooler for temperature below 100 K[J].Applied physics letters,2007(2):24104-1-24104-3-0.
[7] Zhi-hua GAN,Guo-jun LIU,Ying-zhe WU,Qiang CAO,Li-min QIU,Guo-bang CHEN,J.M.PFOTENHAUER.Study on a 5.0 W/80 K single stage Stirling type pulse tube cryocooler[J].浙大学报(英文版)(A辑:应用物理和工程),2008(09):1277-1282.
[8] Z.H. Gan;B.Y. Fan;Y.Z. Wu;L.M. Qiu;X.J. Zhang;G.B. Chen .A two-stage Stirling-type pulse tube cryocooler with a cold inertance tube[J].Cryogenics,2010(6/7):426-431.
上一张 下一张
上一张 下一张
计量
  • 下载量()
  • 访问量()
文章评分
  • 您的评分:
  • 1
    0%
  • 2
    0%
  • 3
    0%
  • 4
    0%
  • 5
    0%