基于热阻调控方法的低温光学系统二级温区传热特性分析

Analysis of heat transfer characteristics of 2nd temperature zone of cryogenic optical system with thermal resistance control method

  • 摘要: 为了实现低温光学系统二级温区的精准控温,同时不引入额外的热负载,提出了一种热阻调控方法,建立了应用于该方法的一维数学模型,运用该数学模型研究了不同真空腔温度条件下不同热阻参数(不同材料参数和几何参数)对二级温区达到热平衡后温度水平和漏热量的影响,同时将该方法和传统的电加热调控方法进行了比较。研究结果表明:当真空腔温度为定值时,随着热阻的增大,二级温区温度升高,漏热量减小;当热阻为定值时,随着真空腔温度的升高,二级温区温度升高,漏热量增大。在文中的研究工况下,当真空腔温度为253.15 K时,二级温区温度水平调节范围为111.1~185.2 K,相应的漏热量从1.75 W减小至1.10 W;当真空腔温度为293.15 K时,温度水平调节范围为120.9~219.4 K,相应的漏热量从2.58 W减小至1.57 W。电加热调控方法使二级温区热负载达到了16.8 W,是热阻调控方法的11倍左右(真空腔温度为293.15 K,二级温区目标温度为220 K左右),随着二级温区温度的升高,电加热调控方法使得系统热负载增大,热阻调控方法与之相反。热阻调控方法使低温光学系统热负载一直处于较低的水平,同时可减少系统对电功率和散热资源的需求。研究结果可为空间应用中的类似低温光学设计提供参考。

     

    Abstract:
    Objective Adjusting the temperature of 2nd temperature zone of cryogenic optical system by applying the electrical heating control method will increase heat load on cryocooler, increase needs for electric power and heat dissipation resources of cryocooler, even decrease dependability of cryocooler in space application. When the cryogenic optical system in space payload is applicated on-orbit, a method without extra heat load on cryogenic optical system, which controlling the temperature of 2nd temperature zone accurately, is urgently needed under the condition of limited electric power and heat dissipation resource on the satellites.
    Methods In view of the above problems, thermal resistance control method was proposed to adjust the temperature of 2nd temperature zone of cryogenic optical system in this study. A mechanical structure used for thermal resistance control, consisted of screw, screw sleeve and heat insulated pad, was designed (Fig.2), which based on the model of dual-temperature zone of cryogenic optical system (Fig.1). A one dimensional (1D) mathematical model was developed based on this mechanical structure. The mathematical model was used to investigate heat balance temperature level and heat leakage of 2nd temperature zone. The effects of material parameters such as TC4 and 4J36 and geometric parameters such as length of screw, height of heat insulated pad, height of screw sleeve and thickness of heat insulated pad were investigated. Meanwhile, different temperature conditions of vacuum chamber were considered.
    Results and Discussions The experiment results show that the temperature fluctuation of 2nd temperature zone is smaller than ±0.5 ℃ within 4 hours in a row, which can be determined that the condition of thermal equilibrium is acquired. Different environmental temperature and different thermal resistance lead to the difference of heat balance temperature of 2nd temperature zone, which verifies the feasibility of thermal resistance method (Fig.5). The computed results of 1D mathematical model are in good agreement with the experimental data. The maximum deviation between the computed results and the experiment results is only 1.6% (Fig.6-7), which proved the reliability of the calculation method in this paper. Users can obtain more parameters of thermal resistance based on different temperatures of 2nd temperature zone by using above mathematical model. When the thermal resistance is taken constant, the temperature of 2nd temperature zone increases with increasing the temperature of vacuum chamber, which is result of increasing heat leakage caused by increasing environmental temperature. When the temperature of vacuum chamber is taken constant, the temperature of 2nd temperature zone increases with increasing length of screw, decreasing thickness of heat insulated pad and decreasing thermal conductivity, but heat leakage decreases. When the temperature of vacuum chamber is 253.15 K, the adjustment range of the temperature of 2nd temperature zone is 111.1-185.2 K, and the corresponding heat leakage decreases from 1.75 W to 1.1 W. When the temperature of vacuum chamber is 293.15 K, the adjustment range of the temperature of 2nd temperature zone is 120.9-219.4 K, and the corresponding heat leakage decreases from 2.58 W to 1.57 W (Fig.8-Fig.11). According to the above results, there is no extra heat load on cryogenic optical system with thermal resistance control method. The effect of heat load on 2nd temperature zone with the electrical heating control method and thermal resistance control method is calculated and compared, while the temperature of vacuum chamber is 293.15 K. With the raising of target temperature of 2nd temperature zone, heat load on 2nd temperature zone decreases with thermal resistance control method, but increases with electrical heating control method. When the temperature of vacuum chamber is around 220 K, the heat load on 2nd temperature zone is 16.8 W with electrical heating control method, which is nearly 11 times higher than that with thermal resistance control method (Fig.12).
    Conclusions Users can select the parameters of thermal resistance they need according to the appointed temperature of vacuum chamber and temperature of 2nd temperature zone. The cryocooler’s needs for electric power resources and heat dissipation resources can be reduced by using thermal resistance control method compared with electrical heating control method. This study may provide a reference for the thermal design of similar cryogenic optical system in space application.

     

/

返回文章
返回