Effects of Parameters of High-Temperature Superconductor Levitation System on the Vertical Force in Zero-Field Cooling when a Permanent Magnet Is Laterally Traversing

2008 ◽  
Vol 22 (4) ◽  
pp. 381-385 ◽  
Author(s):  
Yong Yang
Keyword(s):  
High Temperature ◽  
Permanent Magnet ◽  
High Temperature Superconductor ◽  
Zero Field ◽  
Vertical Force ◽  
Levitation System ◽  
Zero Field Cooling ◽  
Field Cooling

Calculation of the Interaction Forces between Superconductor and Permanent Magnet Using Equivalent Current Loops in Zero Field Cooling

2013 ◽  
Vol 634-638 ◽  
pp. 2436-2441
Author(s):  
Yong Yang ◽  
Xiao Jing Zheng ◽  
Tao Li ◽  
Zhi Qiang Hua
Keyword(s):  
Permanent Magnets ◽  
High Temperature Superconductors ◽  
Magnetic Bearing ◽  
Image Method ◽  
Zero Field ◽  
Vertical Force ◽  
Interaction Forces ◽  
Magnetic Dipoles ◽  
Zero Field Cooling ◽  
Field Cooling

The levitation between high temperature superconductors (HTSs) and permanent magnets (PMs) has been applied to the flywheel energy storage systems and magnetic bearing systems for the last nearly twenty years. The interaction forces acting on the levitating body are calculated by the modified frozen-image method. The magnetic dipoles are equivalent to Amperian current loops. The current intensity in loops changes linearly when the PM moves. Under the zero field cooling condition, the expression of vertical force is obtained when the PM traverses vertically, and when the PM traverses horizontally, the expressions of vertical and horizontal forces are obtained. Those expressions of vertical and horizontal forces are gained by calculating the forces between current loops and using superposition theorem of vector. The calculations agree well with the previous experimental data, which means that the deductions of the expressions are reliable.

Stable Levitation Performance of Bulk High Temperature Superconductor Magnet in Applied Magnetic Fields

2014 ◽  
Vol 787 ◽  
pp. 436-441 ◽  
Author(s):  
Jun Zheng ◽  
Yan Feng Gou ◽  
Da Bo He ◽  
Rui Xue Sun ◽  
Zi Gang Deng
Keyword(s):  
Magnetic Field ◽  
High Temperature ◽  
Permanent Magnet ◽  
High Temperature Superconductor ◽  
Guidance Force ◽  
Barium Copper ◽  
Levitation Performance ◽  
Maglev Transportation System ◽  
Original Field ◽  
Field Cooling

Bulk high temperature superconductor magnet (HTSCM) has been considered to get the better stable levitation in applied magnetic field which is not the original field-cooling magnetization (FCM) field in this paper. The vibration disturbance experiments firstly showed that a permanent magnet (PM) can suspend stably under a bulk Yttrium Barium Copper Oxide (YBCO) HTSCM. This implies that the stable levitation of one single bulk HTSCM is able to realize in the other magnetic field even from one single small PM due to the re-magnetization effect. Secondly, it is found that the HTSCM with more trapped flux produced larger guidance forces and smaller repulsion levitation forces compared with the well-recognized FCM condition of the30mm field-cooling height by the permanent magnet guideway (PMG). Especially, the HTSCM with the 0.349T trapped field achieved a maximum 9.8N guidance force, which is over impressive 7 times than the conventional FCM condition. So, it is feasible to introduce the bulk HTSCM into the HTS Maglev transportation system because this pre-magnetization method of the onboard superconductor bulks is not only helpful to improve the levitation capability and stability, but also enhance the dynamic property above the practical PMG.

Study on Flux Pinned Vertical Force between High-Temperature Superconductor and Permanent Magnet

2012 ◽  
Vol 531-532 ◽  
pp. 755-758
Author(s):  
Ming Liang Zhang ◽  
Yong Lu ◽  
Dong Gao ◽  
Wei Chen
Keyword(s):  
Experimental Data ◽  
Quantum Effect ◽  
Analytical Form ◽  
Zero Field ◽  
Vertical Force ◽  
Magnetic Strength ◽  
Precise Version ◽  
Precise Expression ◽  
Zero Field Cooling ◽  
Field Cooling

The flux pinned force attracts our eyes, where the levitating system is widely investigated for the transportable application. Although plenty of experiments can lead to many significant consequences, the mechanism has been not understood completely since the enormously complicated behavior and quantum effect involve. In this paper, in order to calculate the flux pinned force analytically, the image-dipole model is adopted and improved and the simple and precise expression of magnetic strength is utilized, so the flux pinned vertical force can be calculated in analytical form. In addition, the experimental data in case of zero field-cooling and field-cooling experiment can be collected in our experimental table and the comparison is completed between the precise and simple formula and the experimental data, the precise version of expression fro flux pinned vertical force can correspond to the experimental data well.

scholarly journals Síntesis del superconductor YBa2Cu3O7- δ mediante sinterización por descarga luminiscente anormal

2017 ◽  
Vol 41 (158) ◽  
pp. 36
Author(s):  
Erika Yazmin Soto-Gómez ◽  
Armando Sarmiento-Santos ◽  
Carlos Arturo Parra-Vargas
Keyword(s):  
Zero Field ◽  
Zero Field Cooling ◽  
Field Cooling

En este trabajo se reporta la síntesis del superconductor YBa2Cu3O7-δ mediante el método no convencional de sinterización por plasma en el rango de descarga luminiscente anormal (DLA). Las muestras se sometieron a diferentes temperaturas y tiempos de sinterización. Como referencia se usó una muestra superconductora obtenida por el método convencional (horno resistivo). La caracterización estructural de estas muestras se hizo por difracción de rayos X y refinamiento con el método de Rietveld. El comportamiento superconductor se determinó mediante el análisis de las curvas de magnetización en función de la temperatura según los procedimientos experimentales de enfriado en campo magnético cero (zero field cooling, ZFC) y enfriado con campo magnético aplicado (field cooling, FC). Las muestras sinterizadas por DLA presentaron características estructurales (ortorrómbica Pmmm) y superconductoras con una temperatura crítica de Tc~ 92 K, similares a las obtenidas por el método convencional, pero con una significativa reducción en las temperaturas y tiempos, bajo un ambiente adecuado de presión en el proceso de sinterización. © 2017. Acad. Colomb. Cienc. Ex. Fis. Nat.

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