1. Non-contact methods for determining critical currents in HTS tapes of the 2nd generation
- Subjects
кÑиÑиÑеÑкий Ñок ,critical temperature ,ÑвеÑÑ Ð¿ÑоводÑÑее ÑоÑÑоÑние ,намагниÑенноÑÑÑ ,Meissner effect ,ÐСТРленÑÑ ,magnetic fields ,magnetization ,ÑвеÑÑ Ð¿Ñоводники II Ñода ,high temperature superconductors ,ÑÑÑÐµÐºÑ ÐейÑÑнеÑа ,HTS-tape ,type-II superconductor ,кÑиÑиÑеÑÐºÐ°Ñ ÑемпеÑаÑÑÑа ,вÑÑокоÑемпеÑаÑÑÑнÑе ÑвеÑÑ Ð¿Ñоводники ,magnetic flux capture ,superconducting state ,Ð·Ð°Ñ Ð²Ð°Ñ Ð¼Ð°Ð³Ð½Ð¸Ñного поÑока ,critical current ,магниÑнÑе Ð¿Ð¾Ð»Ñ - Abstract
РабоÑа поÑвÑÑена измеÑÐµÐ½Ð¸Ñ ÐºÑиÑиÑеÑÐºÐ¸Ñ Ð¿Ð°ÑамеÑÑов (кÑиÑиÑеÑкой ÑемпеÑаÑÑÑÑ Ð¸ кÑиÑиÑеÑкого Ñока) ÐТСРленÑÑ 2-го Ð¿Ð¾ÐºÐ¾Ð»ÐµÐ½Ð¸Ñ Ð±ÐµÑконÑакÑнÑми магниÑнÑми меÑодами и обÑÑÐ¶Ð´ÐµÐ½Ð¸Ñ Ð´Ð¾ÑÑоинÑÑв ÑÑÐ¸Ñ Ð¼ÐµÑодов по ÑÑÐ°Ð²Ð½ÐµÐ½Ð¸Ñ Ñ ÑÑадиÑионнÑм ÑезиÑÑивнÑм меÑодом.ЦелÑÑ ÑабоÑÑ ÑвлÑеÑÑÑ Ð¸Ð·Ð¼ÐµÑение велиÑÐ¸Ð½Ñ ÐºÑиÑиÑеÑкого Ñока ÐТСРленÑÑ Ð¿Ñи ÑемпеÑаÑÑÑе жидкого азоÑа 2-Ð¼Ñ Ð±ÐµÑконÑакÑнÑми меÑодами: меÑодом измеÑÐµÐ½Ð¸Ñ Ð½Ð°Ð¼Ð°Ð³Ð½Ð¸ÑенноÑÑи и меÑодом Ð·Ð°Ñ Ð²Ð°Ñенного поÑока в колÑÑе.ÐеÑвÑй меÑод иÑполÑзÑÐµÑ Ð¸Ð·Ð¼ÐµÑение намагниÑенноÑÑи РпÑи помоÑи ÑÑвÑÑвиÑелÑного вибÑаÑионного магниÑомеÑÑа. ÐпÑеделÑлаÑÑ ÑемпеÑаÑÑÑа пеÑÐµÑ Ð¾Ð´Ð° ленÑÑ Ð¢Ñ Ð¸Ð· завиÑимоÑÑей Ð(Т), а из завиÑимоÑÑей Ð(Ð) Ð½Ð°Ñ Ð¾Ð´Ð¸Ð»Ð¸ ÑиÑÐ¸Ð½Ñ Ð¿ÐµÑли гиÑÑеÑезиÑа в нÑлевом поле и Ñ Ð¿Ð¾Ð¼Ð¾ÑÑÑ ÑоÑмÑл Ð½Ð°Ñ Ð¾Ð´Ð¸Ð»Ð¸ кÑиÑиÑеÑкий Ñок.ÐÐ»Ñ Ð²ÑоÑого меÑода (иÑполÑÐ·Ð¾Ð²Ð°Ð½Ð¸Ñ ÐºÐ¾Ð»ÐµÑ) измеÑÐµÐ½Ð¸Ñ Ð±Ñли вÑÐ¿Ð¾Ð»Ð½ÐµÐ½Ñ Ð¿Ð¾ ÑамоÑÑоÑÑелÑно ÑобÑанной ÑÑ ÐµÐ¼Ðµ. Ðз ÐТСРленÑÑ Ð²ÑÑезалоÑÑ ÐºÐ¾Ð»ÑÑо, в ÑенÑÑ ÑÑÑанавливалÑÑ Ð´Ð°ÑÑик Холла, ÑбоÑка Ñ ÐºÐ¾Ð»ÑÑом и даÑÑиком помеÑалаÑÑ Ð² жидкий азоÑ, пÑи помоÑи ÑилÑного поÑÑоÑнного магниÑа в колÑÑе наводилÑÑ ÑкÑаниÑÑÑÑий Ñок и пÑи Ñдалении магниÑа в колÑÑе Ð·Ð°Ñ Ð²Ð°ÑÑвалÑÑ Ð¼Ð°Ð³Ð½Ð¸ÑнÑй поÑок. Ðз измеÑенного даÑÑиком Холла магниÑного Ð¿Ð¾Ð»Ñ Ð² ÑенÑÑе колÑÑа вÑÑиÑлÑлÑÑ ÐºÑиÑиÑеÑкий Ñок.ÐнаÑÐµÐ½Ð¸Ñ ÐºÑиÑиÑеÑкого Ñока, полÑÑеннÑе 2-Ð¼Ñ ÑазнÑми ÑпоÑобами, Ñ Ð¾ÑоÑо ÑоглаÑÑÑÑÑÑ Ð¿Ð¾ велиÑине Ð¼ÐµÐ¶Ð´Ñ Ñобой и знаÑением, пÑиводимÑм пÑоизводиÑелем ленÑÑ.ÐолÑÑеннÑе даннÑе ÑвидеÑелÑÑÑвÑÑÑ, ÑÑо иÑполÑзованнÑе магниÑнÑе меÑÐ¾Ð´Ñ Ð¿Ð¾Ð·Ð²Ð¾Ð»ÑÑÑ Ð¿ÑоÑÑо и надежно измеÑÑÑÑ ÐºÑиÑиÑеÑкий Ñок ÐТСРленÑÑ. ÐÑи меÑÐ¾Ð´Ñ ÑÐ²Ð¾Ð±Ð¾Ð´Ð½Ñ Ð¾Ñ Ð½ÐµÐ´Ð¾ÑÑаÑков ÑезиÑÑивного меÑода измеÑениÑ. ÐеÑод оÑенки кÑиÑиÑеÑкого Ñока по Ð·Ð°Ñ Ð²Ð°ÑÐµÐ½Ð½Ð¾Ð¼Ñ Ð¿Ð¾ÑÐ¾ÐºÑ Ð² колÑÑе Ð¼Ð¾Ð¶ÐµÑ Ð±ÑÑÑ Ñекомендован пÑоизводиÑÐµÐ»Ñ Ð»ÐµÐ½Ñ Ð´Ð»Ñ ÐºÐ°Ð»Ð¸Ð±Ñовки ÑÐ²Ð¾Ð¸Ñ Ð¸Ð·Ð¼ÐµÑиÑелÑнÑÑ ÑÑÑановок., The work is devoted to measure the critical parameters (critical temperature and critical current) of the 2nd generation HTSC tape by non-contact magnetic methods and discussing the advantages of these methods compared to the traditional resistive method.The purpose of this work is to measure the critical current of an HTSC tape at liquid nitro-gen temperature using two non-contact methods: the method of measuring the magnetization and the method of trapped flux in the ring.The first method uses the measurement of the magnetization M with a sensitive vibrating magnetometer. The ribbon transition temperature Tc was determined from the dependences M(T), and from the dependences M(H) the width of the hysteresis loop in zero field was found and the critical current was found using the formulas.For the second method (using rings), the measurements were made according to a self-assembled scheme. A ring was cut out of the HTSC tape, a Hall sensor was installed in the center, the assembly with the ring and the sensor was placed in liquid nitrogen, a shielding current was induced in the ring using a strong permanent magnet, and when the magnet was removed, the magnetic flux was captured in the ring. From the magnetic field measured by the Hall sensor in the center of the ring, the critical current was calculated.The values of the critical current obtained by 2 different methods are matching in magni-tude with each other and the value given by the tape manufacturer.The data obtained indicates that the magnetic methods used make it possible to simply and reliably measure the critical current of an HTSC tape. These methods are free from the disadvantages of the resistive measurement method. The method of estimating the critical current from the trapped flux in the ring can be recommended to the tape manufacturer for calibrating their measuring setups.
- Published
- 2022
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