Bouloukakis Konstantinos, Hunter Mark, Long Nicholas, Dykstra Robin, Parkinson Benjamin
Robinson Research Institute, Victoria University of Wellington, PO Box 33436, Lower Hutt 5046, New Zealand.
Transpower limited Wellington NZ 22 Boulcott Street, Wellington Central, Wellington 6011.
IEEE Trans Appl Supercond. 2021 Aug;31(5). doi: 10.1109/tasc.2021.3059975. Epub 2021 Feb 17.
We have designed and built a small, conduction cooled, 1.5 T high-temperature superconductor (HTS) magnet. The magnet coils have been wet-wound with a novel conductive epoxy resin system to achieve a derivative of the no-insulation coil winding method. The epoxy is filled with copper powder to reliably set the turn-to-turn contact resistivity and diamond powder to accurately space the coil turns apart, as well as match the filled epoxy thermal contraction rate to that of the HTS. The magnet is designed to act as a test bed to measure sudden discharge rates and hence validate models of coil behaviour using the filled epoxy system we have developed. A lumped-element electrical model was used to predict the coil contact resistivity needed to bring the magnetic field of the 1.5 T magnet down to a near-zero level within 0.5 s. The conductive epoxy blend was tuned to give a contact resistivity of 1 × 10 Ω m, based on previous measurements of coil contact resistivity at 77 K. Once the magnet was wound and tested at 40 K, we found the magnet's sudden discharge time constant was 500 ms rather than 69 ms as was predicted from the 77 K measurements. The discrepancy was traced to the temperature dependence of the contact resistivity. With further testing of the individual coils this was accounted for and the model adjusted. The predicted discharge time was 2 s, in good agreement with the measured sudden discharge time of the magnet.
我们设计并制造了一个小型的、传导冷却的1.5T高温超导(HTS)磁体。磁体线圈采用一种新型导电环氧树脂系统进行湿绕,以实现无绝缘线圈绕制方法的一种变体。环氧树脂中填充有铜粉以可靠地设定匝间接触电阻率,填充有金刚石粉以精确隔开线圈匝,同时使填充环氧树脂的热收缩率与高温超导材料的热收缩率相匹配。该磁体被设计用作测试平台,以测量突然放电速率,从而使用我们开发的填充环氧树脂系统验证线圈行为模型。使用集总元件电模型预测将1.5T磁体的磁场在0.5秒内降至接近零水平所需的线圈接触电阻率。基于之前在77K下对线圈接触电阻率的测量,调整导电环氧树脂混合物以使其接触电阻率为1×10Ω·m。一旦磁体绕制完成并在40K下进行测试,我们发现磁体的突然放电时间常数为500ms,而不是根据77K测量结果预测的69ms。差异可追溯到接触电阻率的温度依赖性。通过对单个线圈的进一步测试,对此进行了说明并对模型进行了调整。预测的放电时间为2s,与磁体测量的突然放电时间吻合良好。