Pub Date : 2024-03-06DOI: 10.1016/j.cryogenics.2024.103825
Yifeng Li, Shaotao Dai, Tao Ma, Lei Hu
superconducting material has a wide range of application prospects for its high transition temperature, favorable structural characteristics and low cost. When using to produce superconducting energy storage magnets, it is necessary to twist superconducting wires into cables to increase their current carrying capacity. One typical cable is made of 6 superconducting wires wrapped around 1 central copper wire, forming a (6+1) structure. coils used for energy storage require solid impregnation and can be cooled by liquid hydrogen or solid nitrogen. Due to the need for fast charging and discharging of energy storage coils and low thermal conductivity of commonly used epoxy resin impregnation and solid nitrogen, it is necessary to consider the temperature variation characteristics caused by AC loss and eddy current loss during operation process. A coil with 8 turns in each layer and 4 layers is simulated using the (6+1)-structure cable. In order to obtain better temperature distribution results while reducing the time required for simulation operation, the simulation time is set to 1 s. The impact of epoxy resin properties and surrounding environments on the coil are then analyzed. The results indicate that increasing the thermal conductivity of epoxy resin can significantly reduce the maximum temperature of the coil, while only changing the cooling method is unhelpful in dealing with the problem of local overheating of the coil.
{"title":"Analysis of heat transfer characteristics of (6+1)-structure MgB2 cable","authors":"Yifeng Li, Shaotao Dai, Tao Ma, Lei Hu","doi":"10.1016/j.cryogenics.2024.103825","DOIUrl":"10.1016/j.cryogenics.2024.103825","url":null,"abstract":"<div><p><span><math><mrow><mi>Mg</mi></mrow><msub><mrow><mi>B</mi></mrow><mrow><mn>2</mn></mrow></msub></math></span> superconducting material has a wide range of application prospects for its high transition temperature, favorable structural characteristics and low cost. When using <span><math><mrow><mi>Mg</mi></mrow><msub><mrow><mi>B</mi></mrow><mrow><mn>2</mn></mrow></msub></math></span> to produce superconducting energy storage magnets, it is necessary to twist superconducting wires into cables to increase their current carrying capacity. One typical cable is made of 6 <span><math><mrow><mi>Mg</mi></mrow><msub><mrow><mi>B</mi></mrow><mrow><mn>2</mn></mrow></msub></math></span> superconducting wires wrapped around 1 central copper wire, forming a (6+1) structure. <span><math><mrow><mi>Mg</mi></mrow><msub><mrow><mi>B</mi></mrow><mrow><mn>2</mn></mrow></msub></math></span> coils used for energy storage require solid impregnation and can be cooled by liquid hydrogen or solid nitrogen. Due to the need for fast charging and discharging of energy storage coils and low thermal conductivity of commonly used epoxy resin impregnation and solid nitrogen, it is necessary to consider the temperature variation characteristics caused by AC loss and eddy current loss during operation process. A coil with 8 turns in each layer and 4 layers is simulated using the (6+1)-structure cable. In order to obtain better temperature distribution results while reducing the time required for simulation operation, the simulation time is set to 1 s. The impact of epoxy resin properties and surrounding environments on the coil are then analyzed. The results indicate that increasing the thermal conductivity of epoxy resin can significantly reduce the maximum temperature of the coil, while only changing the cooling method is unhelpful in dealing with the problem of local overheating of the coil.</p></div>","PeriodicalId":10812,"journal":{"name":"Cryogenics","volume":null,"pages":null},"PeriodicalIF":2.1,"publicationDate":"2024-03-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140075416","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-03-03DOI: 10.1016/j.cryogenics.2024.103822
Jun Tan , Zhengjun Shi , Renjun Xue , Han Tan , Yujia Zhai , Shiguang Wu , Dong Ma , Dirui Wu , Haizheng Dang
This paper focuses on the remote cryogenic helium circulating system for cooling the 10-Mvar class HTS DSC. The cryogenic system is an upgraded version to provide a cooling power about 200 W@20 K. Six cryogenic cryocoolers are employed as the cold source. Two cryogenic helium blowers are used to overcome the pressure drop. Circulating loop is divided into two branches, of each three coolers are installed in parallel and then as a whole connected to a helium blower in series. The detailed design, structure parameters, and optimization of the cooling system were described as well. In the experimental tests coupled with the rotor section of 10-Mvar HTS DSC, the magnet was firstly pre-cooled to about 110 K with liquid nitrogen, and then further cooled to around 34.5 K by the circulating helium gas. In the near future, the 10-Mvar class HTS DSC will be installed, tested and integrated into the power grid for practical application.
{"title":"Remote cryogenic helium gas circulating cooling system for a 10-Mvar class HTS dynamic synchronous condenser","authors":"Jun Tan , Zhengjun Shi , Renjun Xue , Han Tan , Yujia Zhai , Shiguang Wu , Dong Ma , Dirui Wu , Haizheng Dang","doi":"10.1016/j.cryogenics.2024.103822","DOIUrl":"https://doi.org/10.1016/j.cryogenics.2024.103822","url":null,"abstract":"<div><p>This paper focuses on the remote cryogenic helium circulating system for cooling the 10-Mvar class HTS DSC. The cryogenic system is an upgraded version to provide a cooling power about 200 W@20 K. Six cryogenic cryocoolers are employed as the cold source. Two cryogenic helium blowers are used to overcome the pressure drop. Circulating loop is divided into two branches, of each three coolers are installed in parallel and then as a whole connected to a helium blower in series. The detailed design, structure parameters, and optimization of the cooling system were described as well. In the experimental tests coupled with the rotor section of 10-Mvar HTS DSC, the magnet was firstly pre-cooled to about 110 K with liquid nitrogen, and then further cooled to around 34.5 K by the circulating helium gas. In the near future, the 10-Mvar class HTS DSC will be installed, tested and integrated into the power grid for practical application.</p></div>","PeriodicalId":10812,"journal":{"name":"Cryogenics","volume":null,"pages":null},"PeriodicalIF":2.1,"publicationDate":"2024-03-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140051949","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-03-02DOI: 10.1016/j.cryogenics.2024.103824
Li Mei, Chang Zhengze, Zhu Keyu, Han Ruixiong, Ye Rui, Sun Liangrui, Sang Minjing, Jiang Yongcheng, Li Shaopeng, Zhai Jiyuan, Sha Peng, Li Xiaoping, Ge Rui
Superconducting cavity is the key equipment of the superconducting accelerator, which provides higher acceleration voltage and higher frequency power per unit length, and saves equipment space. Superconducting cavities need to be gradually cooled from ambient temperature (300 K) to the superconducting temperature (4.2 K or below) during the test and operation. The temperature difference on the cavity must be strictly limited during the cooldown process to prevent excessive thermal stress on the surface of the superconducting cavity. Since this cooldown process for the superconducting cavity is a typical large hysteresis, non-linear process that is difficult to control automatically using decoupled proportion integral derivative (PID) methods directly, a less efficient manual control scheme is normally adopted. In this paper, 3D numerical simulation, 1D pipe and 0D tank model with artificial neural network (ANN) were combined to generate a two-layer surrogate model that can balance computational accuracy and speed, to improve the automation and cooling efficiency of the superconducting cavity cooldown process. In order to achieve automatic control of the cooling procedure for the superconducting cavity, a model predictive control (MPC) approach was also built on the basis of this two-layer surrogate model. According to the results of the experiment test, the improved method could realize a quick and smooth cooldown process of the superconducting cavity, during which the temperature difference on the cavity could satisfy the requirements. Additionally, the improved automatic cooldown method was more adaptable and saved 29 % more time than the original manual control method. The foundation for a more intelligent automated control of future large cryogenic systems or other system with the large hysteresis, non-linear properties, was laid.
超导腔是超导加速器的关键设备,它能在单位长度上提供更高的加速电压和更高的频率功率,并节省设备空间。在测试和运行过程中,超导腔需要从环境温度(300 K)逐渐冷却到超导温度(4.2 K 或以下)。在冷却过程中,必须严格限制腔体上的温差,以防止超导腔体表面产生过大的热应力。由于超导腔的冷却过程是一个典型的大滞后、非线性过程,难以直接使用解耦比例积分导数(PID)方法进行自动控制,因此通常采用效率较低的手动控制方案。本文将三维数值模拟、一维管道和零维水箱模型与人工神经网络(ANN)相结合,生成了一种能兼顾计算精度和速度的双层代用模型,以提高超导空腔冷却过程的自动化程度和冷却效率。为了实现超导腔冷却过程的自动控制,还在该双层代用模型的基础上建立了模型预测控制(MPC)方法。实验测试结果表明,改进后的方法可以实现快速平稳的超导腔体冷却过程,冷却过程中腔体上的温差可以满足要求。此外,改进后的自动冷却方法适应性更强,比原来的手动控制方法节省了 29% 的时间。这为未来大型低温系统或其他具有大滞后、非线性特性的系统实现更智能的自动控制奠定了基础。
{"title":"Automation of superconducting cavity cooldown process using two-layer surrogate model and model predictive control method","authors":"Li Mei, Chang Zhengze, Zhu Keyu, Han Ruixiong, Ye Rui, Sun Liangrui, Sang Minjing, Jiang Yongcheng, Li Shaopeng, Zhai Jiyuan, Sha Peng, Li Xiaoping, Ge Rui","doi":"10.1016/j.cryogenics.2024.103824","DOIUrl":"https://doi.org/10.1016/j.cryogenics.2024.103824","url":null,"abstract":"<div><p>Superconducting cavity is the key equipment of the superconducting accelerator, which provides higher acceleration voltage and higher frequency power per unit length, and saves equipment space. Superconducting cavities need to be gradually cooled from ambient temperature (300 K) to the superconducting temperature (4.2 K or below) during the test and operation. The temperature difference on the cavity must be strictly limited during the cooldown process to prevent excessive thermal stress on the surface of the superconducting cavity. Since this cooldown process for the superconducting cavity is a typical large hysteresis, non-linear process that is difficult to control automatically using decoupled proportion integral derivative (PID) methods directly, a less efficient manual control scheme is normally adopted. In this paper, 3D numerical simulation, 1D pipe and 0D tank model with artificial neural network (ANN) were combined to generate a two-layer surrogate model that can balance computational accuracy and speed, to improve the automation and cooling efficiency of the superconducting cavity cooldown process. In order to achieve automatic control of the cooling procedure for the superconducting cavity, a model predictive control (MPC) approach was also built on the basis of this two-layer surrogate model. According to the results of the experiment test, the improved method could realize a quick and smooth cooldown process of the superconducting cavity, during which the temperature difference on the cavity could satisfy the requirements. Additionally, the improved automatic cooldown method was more adaptable and saved 29 % more time than the original manual control method. The foundation for a more intelligent automated control of future large cryogenic systems or other system with the large hysteresis, non-linear properties, was laid.</p></div>","PeriodicalId":10812,"journal":{"name":"Cryogenics","volume":null,"pages":null},"PeriodicalIF":2.1,"publicationDate":"2024-03-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140042833","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-03-02DOI: 10.1016/j.cryogenics.2024.103818
Dirui Wu , Shiguang Wu , Jun Tan , Han Tan , Renjun Xue , Yujia Zhai , Dong Ma , Shuting Lu , Haizheng Dang
The gas gap heat switch (GGHS) used for controlling heat transfer between different stages can be an important component for the precooling process of some dilution refrigerators. In this paper, a novel circuit GGHS is a rotationally symmetric heat switch assembly with annular fin arrangements to strengthen the heat-transferring effect. A numerical model considering 4He actual gas properties is proposed to investigate the heat transfer characteristics in the circuit GGHS, in which the effects of charge pressure, cold end temperature, thickness and length of walls on the mean thermal conductance (MTC) are studied. Simulation results show that the MTC increases with the growing cold end temperature, wall thickness, and length, respectively. Given the pressure of 10 kPa, cold end temperature of 4.2 K, wall thickness of 0.97 mm, and wall height of 66 mm, the theoretical MTC is 0.828 W/K. Experimental results indicate that the proposed simulation model is reasonable. Furthermore, the increment of the MTC decreases with the growing temperature. The GGHS used in experiments had a cold end temperature of 4 K, wall thickness of 0.65 mm, and wall height of 33 mm; the measured MTC was 0.219 W/K. Only when the temperature is above 10 K does the charge pressure have a pronounced effect on the MTC. This study provides helpful theoretical guidance for the design and optimization of the circuit GGHS.
{"title":"Numerical simulation and experimental validation of the heat transfer characteristics in a circuit gas gap heat switch for the dilution refrigerator","authors":"Dirui Wu , Shiguang Wu , Jun Tan , Han Tan , Renjun Xue , Yujia Zhai , Dong Ma , Shuting Lu , Haizheng Dang","doi":"10.1016/j.cryogenics.2024.103818","DOIUrl":"https://doi.org/10.1016/j.cryogenics.2024.103818","url":null,"abstract":"<div><p>The gas gap heat switch (GGHS) used for controlling heat transfer between different stages can be an important component for the precooling process of some dilution refrigerators. In this paper, a novel circuit GGHS is a rotationally symmetric heat switch assembly with annular fin arrangements to strengthen the heat-transferring effect. A numerical model considering <sup>4</sup>He actual gas properties is proposed to investigate the heat transfer characteristics in the circuit GGHS, in which the effects of charge pressure, cold end temperature, thickness and length of walls on the mean thermal conductance (MTC) are studied. Simulation results show that the MTC increases with the growing cold end temperature, wall thickness, and length, respectively. Given the pressure of 10 kPa, cold end temperature of 4.2 K, wall thickness of 0.97 mm, and wall height of 66 mm, the theoretical MTC is 0.828 W/K. Experimental results indicate that the proposed simulation model is reasonable. Furthermore, the increment of the MTC decreases with the growing temperature. The GGHS used in experiments had a cold end temperature of 4 K, wall thickness of 0.65 mm, and wall height of 33 mm; the measured MTC was 0.219 W/K. Only when the temperature is above 10 K does the charge pressure have a pronounced effect on the MTC. This study provides helpful theoretical guidance for the design and optimization of the circuit GGHS.</p></div>","PeriodicalId":10812,"journal":{"name":"Cryogenics","volume":null,"pages":null},"PeriodicalIF":2.1,"publicationDate":"2024-03-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140042838","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Global Change Observation Mission – Climate (GCOM-C) “Shikisai”, a satellite designed to observe global climate change, was launched from Tanegashima Space Center on December 23, 2017 by an H2A launch vehicle. The Second-generation GLobal Imager (SGLI) on GCOM-C is a multi-channel optical sensor for observing aerosols, vegetation, and temperatures. Through long-term monitoring, our understanding of climate change mechanisms will be improved. The infrared scanner (IRS) on SGLI has a Thermal InfraRed (TIR) detector requested to operate at 55 K. A Cooler Dewar Assembly (CDA) developed to keep the detector at 55 K is designed to minimize the heat load for the small cooler. The detector is supported on a thermal isolator made of Glass FRP and is thermally connected to the cooler by flexible thermal link. The Cooler Control Electronics (CCE) uses a heater to compensate heat load fluctuations, thereby maintaining temperature and stability. The heater power decreases gradually during five years, consequently decreasing the cooling power. Despite that cooler degradation, the detector temperature has been maintained at 55 ± 0.1 K for 5 years in orbit and has continued operating with 36 W power consumption. This paper describes the cooler Dewar Assembly and its five years of operation in orbit.
全球变化观测任务-气候(GCOM-C)"敷世 "号卫星是一颗旨在观测全球气候变化的卫星,于2017年12月23日由H2A运载火箭从种子岛航天中心发射升空。GCOM-C卫星上的第二代气溶胶成像仪(SGLI)是一个多通道光学传感器,用于观测气溶胶、植被和温度。通过长期监测,我们将加深对气候变化机制的了解。SGLI 上的红外扫描仪(IRS)有一个热红外(TIR)探测器,要求在 55 K 的温度下工作。为使探测器保持在 55 K 的温度,设计了一个冷却器杜瓦组件(CDA),以尽量减少小型冷却器的热负荷。探测器由玻璃纤维增强塑料制成的热隔离器支撑,并通过柔性热连接与冷却器热连接。冷却器控制电子装置(CCE)使用加热器补偿热负荷波动,从而保持温度和稳定性。加热器的功率在五年内逐渐降低,冷却功率也随之降低。尽管冷却器出现了退化,但探测器的温度在轨道上仍保持在 55 ± 0.1 K 的水平达 5 年之久,并以 36 W 的功耗持续运行。本文介绍了冷却器杜瓦组件及其在轨运行五年的情况。
{"title":"Five year operation of a cooler Dewar assembly for infrared scanner on board GCOM-C","authors":"Ken'ichi Kanao , Kiyomi Otsuka , Shoji Tsunematsu , Takahiro Amano , Kazuhiro Tanaka","doi":"10.1016/j.cryogenics.2024.103823","DOIUrl":"10.1016/j.cryogenics.2024.103823","url":null,"abstract":"<div><p>Global Change Observation Mission – Climate (GCOM-C) “Shikisai”, a satellite designed to observe global climate change, was launched from Tanegashima Space Center on December 23, 2017 by an H2A launch vehicle. The Second-generation GLobal Imager (SGLI) on GCOM-C is a multi-channel optical sensor for observing aerosols, vegetation, and temperatures. Through long-term monitoring, our understanding of climate change mechanisms will be improved. The infrared scanner (IRS) on SGLI has a Thermal InfraRed (TIR) detector requested to operate at 55 K. A Cooler Dewar Assembly (CDA) developed to keep the detector at 55 K is designed to minimize the heat load for the small cooler. The detector is supported on a thermal isolator made of Glass FRP and is thermally connected to the cooler by flexible thermal link. The Cooler Control Electronics (CCE) uses a heater to compensate heat load fluctuations, thereby maintaining temperature and stability. The heater power decreases gradually during five years, consequently decreasing the cooling power. Despite that cooler degradation, the detector temperature has been maintained at 55 ± 0.1 K for 5 years in orbit and has continued operating with 36 W power consumption. This paper describes the cooler Dewar Assembly and its five years of operation in orbit.</p></div>","PeriodicalId":10812,"journal":{"name":"Cryogenics","volume":null,"pages":null},"PeriodicalIF":2.1,"publicationDate":"2024-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140092423","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-03-01DOI: 10.1016/j.cryogenics.2024.103817
R. Beckmüller , I.H. Bell , M. Thol , E.W. Lemmon , R. Span
In this work, new equations of state for the binary mixtures H2 + Ar, H2 + He, and H2 + Ne are presented. The equations are formulated in terms of the reduced Helmholtz energy and allow for the calculation of all thermodynamic properties over the entire fluid surface including the gas phase, liquid phase, supercritical region, and equilibrium states. The models are validated by comparisons with experimental data and their physical behavior is analyzed. Furthermore, the new equations of state are compared to other state-of-the-art models from the literature.
本研究提出了 H2 + Ar、H2 + He 和 H2 + Ne 二元混合物的新状态方程。这些方程是根据还原亥姆霍兹能制定的,可以计算整个流体表面的所有热力学性质,包括气相、液相、超临界区和平衡态。这些模型通过与实验数据的比较得到了验证,并对其物理行为进行了分析。此外,还将新的状态方程与文献中其他最先进的模型进行了比较。
{"title":"New fundamental equations of state for binary hydrogen mixtures containing argon, helium, and neon","authors":"R. Beckmüller , I.H. Bell , M. Thol , E.W. Lemmon , R. Span","doi":"10.1016/j.cryogenics.2024.103817","DOIUrl":"10.1016/j.cryogenics.2024.103817","url":null,"abstract":"<div><p>In this work, new equations of state for the binary mixtures H<sub>2</sub> + Ar, H<sub>2</sub> + He, and H<sub>2</sub> + Ne are presented. The equations are formulated in terms of the reduced Helmholtz energy and allow for the calculation of all thermodynamic properties over the entire fluid surface including the gas phase, liquid phase, supercritical region, and equilibrium states. The models are validated by comparisons with experimental data and their physical behavior is analyzed. Furthermore, the new equations of state are compared to other state-of-the-art models from the literature.</p></div>","PeriodicalId":10812,"journal":{"name":"Cryogenics","volume":null,"pages":null},"PeriodicalIF":2.1,"publicationDate":"2024-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0011227524000377/pdfft?md5=e5033ac8ab59c114abe4d73a896a69ca&pid=1-s2.0-S0011227524000377-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140084947","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-02-28DOI: 10.1016/j.cryogenics.2024.103819
Wanyin Zhao , Jijun Xin , Chuanjun Huang , Wei Wang , Zhichun Fang , Qichen Wang , Chundong Wang , Liguo Wang , Hengcheng Zhang , Fuzhi Shen , Wentao Sun , Yuan Zhou , Laifeng Li
In large-scale, high-field superconducting magnets used for magnetic confinement fusion, high energy accelerators, and magnetic resonance imaging, the insulating system made from glass fiber reinforced resin-based composites is the key component, which mainly plays the role of mechanical support, fixing and protecting superconducting conductors, as well as electrical insulation. Vacuum Pressure Impregnation (VPI) approach is widely used in the manufacturing of the insulation system. The second curing cycle is generally required after the first VPI and curing process. For example, after the superconducting coil is cured in the mold, the de-molding process requires the superconducting coil to be reheated according the curing temperature. Moreover, for large-scale superconducting magnets, the superconducting coil needs to undergo a second VPI process after the first VPI process to fix the coil in the coil case. In this work, the tensile and shear properties of pure epoxy resin and the glass fiber reinforced resin-based composite, were investigated at both room and cryogenic temperatures and the effect of the second curing cycle on the mechanical properties was analyzed. Additionally, the strain evolution of the Nb-Ti superconducting coil during the second curing cycle was measured using the Fiber Bragg Grating (FBG) sensors embedded in the composite. The results indicate that the second curing cycle will not introduce additional strain to the previously cured resin matrix, but the defective or weak parts of the resin matrix may be affected by the new added epoxy resin and a little extra strain has been observed.
{"title":"Effect of the second curing cycle on performance of superconducting magnet insulating system","authors":"Wanyin Zhao , Jijun Xin , Chuanjun Huang , Wei Wang , Zhichun Fang , Qichen Wang , Chundong Wang , Liguo Wang , Hengcheng Zhang , Fuzhi Shen , Wentao Sun , Yuan Zhou , Laifeng Li","doi":"10.1016/j.cryogenics.2024.103819","DOIUrl":"https://doi.org/10.1016/j.cryogenics.2024.103819","url":null,"abstract":"<div><p>In large-scale, high-field superconducting magnets used for magnetic confinement fusion, high energy accelerators, and magnetic resonance imaging, the insulating system made from glass fiber reinforced resin-based composites is the key component, which mainly plays the role of mechanical support, fixing and protecting superconducting conductors, as well as electrical insulation. Vacuum Pressure Impregnation (VPI) approach is widely used in the manufacturing of the insulation system. The second curing cycle is generally required after the first VPI and curing process. For example, after the superconducting coil is cured in the mold, the de-molding process requires the superconducting coil to be reheated according the curing temperature. Moreover, for large-scale superconducting magnets, the superconducting coil needs to undergo a second VPI process after the first VPI process to fix the coil in the coil case. In this work, the tensile and shear properties of pure epoxy resin and the glass fiber reinforced resin-based composite, were investigated at both room and cryogenic temperatures and the effect of the second curing cycle on the mechanical properties was analyzed. Additionally, the strain evolution of the Nb-Ti superconducting coil during the second curing cycle was measured using the Fiber Bragg Grating (FBG) sensors embedded in the composite. The results indicate that the second curing cycle will not introduce additional strain to the previously cured resin matrix, but the defective or weak parts of the resin matrix may be affected by the new added epoxy resin and a little extra strain has been observed.</p></div>","PeriodicalId":10812,"journal":{"name":"Cryogenics","volume":null,"pages":null},"PeriodicalIF":2.1,"publicationDate":"2024-02-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140000288","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-02-24DOI: 10.1016/j.cryogenics.2024.103810
Yue Wu , Liye Xiao , Siyuan Han , Jiamin Chen
Tunnel magnetoresistance (TMR), recognized for its high sensitivity and low power consumption, holds significant promise in the domain of weak magnetic field detection. Using superconducting materials as magnetic concentrators can achieve several hundred to even a thousandfold amplification of magnetic fields, making it one of the most effective approaches to enhance the magnetic field resolution of TMR sensors. This paper utilized the flip-chip bonding process to integrate TMR with the high-temperature superconductor YBCO (YBa2Cu3O7-δ), and successfully developed TMR-YBCO composite magnetic sensor. Building upon this foundation, through optimization of the fabrication process and the pioneering use of a structural design incorporating the filling of annular holes with superconducting concentrators, the sensitivity of the sensor was further enhanced. Finally, the magnetic field resolution was increased by 1030 times compared to TMR sensors, reached to 2.9pT/Hz1/2 at 1 Hz. Simultaneously, results from frequency band testing indicated excellent frequency band characteristics, with a frequency response range exceeding kHz.
{"title":"TMR-high-temperature superconductor composite magnetic sensor and its performance optimization","authors":"Yue Wu , Liye Xiao , Siyuan Han , Jiamin Chen","doi":"10.1016/j.cryogenics.2024.103810","DOIUrl":"https://doi.org/10.1016/j.cryogenics.2024.103810","url":null,"abstract":"<div><p>Tunnel magnetoresistance (TMR), recognized for its high sensitivity and low power consumption, holds significant promise in the domain of weak magnetic field detection. Using superconducting materials as magnetic concentrators can achieve several hundred to even a thousandfold amplification of magnetic fields, making it one of the most effective approaches to enhance the magnetic field resolution of TMR sensors. This paper utilized the flip-chip bonding process to integrate TMR with the high-temperature superconductor YBCO (YBa2Cu3O7-δ), and successfully developed TMR-YBCO composite magnetic sensor. Building upon this foundation, through optimization of the fabrication process and the pioneering use of a structural design incorporating the filling of annular holes with superconducting concentrators, the sensitivity of the sensor was further enhanced. Finally, the magnetic field resolution was increased by 1030 times compared to TMR sensors, reached to 2.9pT/Hz1/2 at 1 Hz. Simultaneously, results from frequency band testing indicated excellent frequency band characteristics, with a frequency response range exceeding kHz.</p></div>","PeriodicalId":10812,"journal":{"name":"Cryogenics","volume":null,"pages":null},"PeriodicalIF":2.1,"publicationDate":"2024-02-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139992682","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-02-22DOI: 10.1016/j.cryogenics.2024.103808
Shixin Zhang , Zigang Deng , Zhichuan Huang , Haitao Li , Xucheng Zhou , Weihua Zhang
High-temperature superconducting (HTS) pinning magnetic levitation (maglev) has garnered significant attention in high-speed maglev transportation due to its inherent self-stability, low energy consumption, and absence of mechanical friction. Ensuring the safe and stable operation of HTS pinning maglev systems necessitates a dedicated focus on the performance and stability of HTS bulks levitated above the permanent magnetic guideway (PMG). Previous research has indicated that variations in the temperature within the HTS bulk can impact the levitation performance of the system. This temperature-related phenomenon occurs when the external magnetic field applied to the HTS bulk changes. However, it is noteworthy that previous levitation force tests for HTS magnetic levitation systems have been limited to quasi-static or low-speed studies. The exploration of dynamic levitation forces, particularly at high speeds, has remained constrained due to the associated high costs. Therefore, the objective of this study is to investigate dynamic levitation forces while the HTS pinning maglev system is in motion at high speeds, utilizing a self-developed ultra-high-speed maglev test rig. Initially, the relationship between the levitation force and the vertical displacement of the HTS pinning maglev system is examined based on quasi-static experiments. Subsequently, comparative studies are conducted to measure levitation forces at varying speeds. Finally, the correlation between running speed and dynamic levitation force is discussed. The investigation reveals that the levitation force experiences only a marginal decrease as the running speed increases. At a running speed of 240 km/h, the attenuation rate of the levitation force is approximately 2.478 %, demonstrating the commendable stability of HTS pinning maglev systems. The article concludes by presenting the dynamic levitation characteristics and their attenuation trends to speed. These findings can serve as valuable references for future design and practical implementation of HTS pinning maglev systems.
{"title":"Measurement of levitation force of high-temperature superconducting maglev under high-speed operation condition","authors":"Shixin Zhang , Zigang Deng , Zhichuan Huang , Haitao Li , Xucheng Zhou , Weihua Zhang","doi":"10.1016/j.cryogenics.2024.103808","DOIUrl":"10.1016/j.cryogenics.2024.103808","url":null,"abstract":"<div><p>High-temperature superconducting (HTS) pinning magnetic levitation (maglev) has garnered significant attention in high-speed maglev transportation due to its inherent self-stability, low energy consumption, and absence of mechanical friction. Ensuring the safe and stable operation of HTS pinning maglev systems necessitates a dedicated focus on the performance and stability of HTS bulks levitated above the permanent magnetic guideway (PMG). Previous research has indicated that variations in the temperature within the HTS bulk can impact the levitation performance of the system. This temperature-related phenomenon occurs when the external magnetic field applied to the HTS bulk changes. However, it is noteworthy that previous levitation force tests for HTS magnetic levitation systems have been limited to quasi-static or low-speed studies. The exploration of dynamic levitation forces, particularly at high speeds, has remained constrained due to the associated high costs. Therefore, the objective of this study is to investigate dynamic levitation forces while the HTS pinning maglev system is in motion at high speeds, utilizing a self-developed ultra-high-speed maglev test rig. Initially, the relationship between the levitation force and the vertical displacement of the HTS pinning maglev system is examined based on quasi-static experiments. Subsequently, comparative studies are conducted to measure levitation forces at varying speeds. Finally, the correlation between running speed and dynamic levitation force is discussed. The investigation reveals that the levitation force experiences only a marginal decrease as the running speed increases. At a running speed of 240 km/h, the attenuation rate of the levitation force is approximately 2.478 %, demonstrating the commendable stability of HTS pinning maglev systems. The article concludes by presenting the dynamic levitation characteristics and their attenuation trends to speed. These findings can serve as valuable references for future design and practical implementation of HTS pinning maglev systems.</p></div>","PeriodicalId":10812,"journal":{"name":"Cryogenics","volume":null,"pages":null},"PeriodicalIF":2.1,"publicationDate":"2024-02-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139954481","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-02-22DOI: 10.1016/j.cryogenics.2024.103807
Logan Kossel , John Pfotenhauer , Ali Kashani , Franklin Miller
Future space telescopes, such as those proposed for the Far-infrared Surveyor Mission, are expected to employ actively cooled optical arrays with a similar overall surface area compared to the James Webb Space Telescope. Therefore, there is a need for a cryogenic cooling system with a thermal bus architecture that can distribute cooling to these large optical arrays. Recent experimental research of helium Pulsating Heat Pipes (PHPs) has shown that helium PHPs can transfer heat over long distances (on the order of 2 m) with high efficiency, and also have the ability to act as a passive thermal switch upon the removal of the cooling source. PHPs’ high thermal performance, passive switching capability, low mass, and ease of manufacturing make them an appealing option compared to high-purity metal straps for a thermal bus architecture on large cryogenic space telescopes. A novel architecture for the thermal control of optical arrays is proposed utilizing unique configurations of helium pulsating heat pipes that minimize mass, maximize thermal performance, and reduce the risk of mission failure.
{"title":"A novel thermal bus architecture for large cryogenic space telescopes utilizing helium pulsating heat pipes","authors":"Logan Kossel , John Pfotenhauer , Ali Kashani , Franklin Miller","doi":"10.1016/j.cryogenics.2024.103807","DOIUrl":"10.1016/j.cryogenics.2024.103807","url":null,"abstract":"<div><p>Future space telescopes, such as those proposed for the Far-infrared Surveyor Mission, are expected to employ actively cooled optical arrays with a similar overall surface area compared to the James Webb Space Telescope. Therefore, there is a need for a cryogenic cooling system with a thermal bus architecture that can distribute cooling to these large optical arrays. Recent experimental research of helium Pulsating Heat Pipes (PHPs) has shown that helium PHPs can transfer heat over long distances (on the order of 2 m) with high efficiency, and also have the ability to act as a passive thermal switch upon the removal of the cooling source. PHPs’ high thermal performance, passive switching capability, low mass, and ease of manufacturing make them an appealing option compared to high-purity metal straps for a thermal bus architecture on large cryogenic space telescopes. A novel architecture for the thermal control of optical arrays is proposed utilizing unique configurations of helium pulsating heat pipes that minimize mass, maximize thermal performance, and reduce the risk of mission failure.</p></div>","PeriodicalId":10812,"journal":{"name":"Cryogenics","volume":null,"pages":null},"PeriodicalIF":2.1,"publicationDate":"2024-02-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139954228","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}