2D electromagnetic modelling of superconductors

Some issues concerning the numerical analysis of superconductors are discussed and a novel approach to 2D modelling is proposed. Both axial and translational symmetric as well as current driven and voltage driven systems are examined in detail. The E–J power law is chosen instead of the critical state model as a constitutive relation of the material and the need to modify this relation in order to account for the normal state transition at high currents is discussed. A linear space reconstruction of the current density by means of nodal shape functions is used in order to build the finite dimensional model. A method to relax the tangential continuity of the current density, which is inherent to the discretization method used, is discussed. The performance of the proposed approach, both in terms of current distribution and AC loss, is evaluated with reference to some cases of practical interest involving composite materials. The role of the electric field as a natural state variable for superconducting problems is also pointed out. The use of the method as an alternative to the circuit approach or edge elements for modelling the superconductors is finally discussed.

[1]  C. P. Bean,et al.  Magnetization of High-Field Superconductors , 1964 .

[2]  T. A. Coombs,et al.  Numerical solution of critical state in superconductivity by finite element software , 2006 .

[3]  Bertrand Dutoit,et al.  Modelling the E–J relation of high-Tc superconductors in an arbitrary current range , 2004 .

[4]  A. Malozemoff,et al.  Magnetic relaxation in high-temperature superconductors , 1996 .

[5]  C. Navau,et al.  Magnetic properties of finite superconducting cylinders. II. Nonuniform applied field and levitation force , 2001 .

[6]  Antti Stenvall,et al.  Programming finite element method based hysteresis loss computation software using non-linear superconductor resistivity and T − φ formulation , 2010 .

[7]  Antti Stenvall,et al.  An eddy current vector potential formulation for estimating hysteresis losses of superconductors with FEM , 2010 .

[8]  N. Amemiya,et al.  Electromagnetic field analysis of rectangular superconductor with large aspect ratio in arbitrary orientated magnetic fields , 2005, IEEE Transactions on Applied Superconductivity.

[9]  Isaak D. Mayergoyz Nonlinear diffusion and superconducting hysteresis , 1996 .

[10]  A Morandi,et al.  Design of a DC Resistive SFCL for Application to the 20 kV Distribution System , 2010, IEEE Transactions on Applied Superconductivity.

[11]  W. Zamboni,et al.  Three-Dimensional Electromagnetic Analysis of Cable-in-Conduit Conductors for Fusion Applications , 2008, IEEE Transactions on Applied Superconductivity.

[12]  Naoyuki Amemiya,et al.  Numerical modelings of superconducting wires for AC loss calculations , 1998 .

[13]  L. Prigozhin,et al.  Analysis of critical-state problems in type-II superconductivity , 1997, IEEE Transactions on Applied Superconductivity.

[14]  Leonid Prigozhin,et al.  The Bean Model in Superconductivity , 1996 .

[15]  A Morandi,et al.  Experimental Evaluation of AC Losses of a DC Restive SFCL Prototype , 2010, IEEE Transactions on Applied Superconductivity.

[16]  P. Tixador,et al.  Finite-element method modeling of superconductors: from 2-D to 3-D , 2005, IEEE Transactions on Applied Superconductivity.

[17]  A. Morandi,et al.  Experimental and Numerical Investigation of the Levitation Force Between Bulk Permanent Magnet and ${\rm MgB}_{2}$ Disk , 2009, IEEE Transactions on Applied Superconductivity.

[18]  C. P. Bean Magnetization of hard superconductors , 1962 .

[19]  H. R. Kerchner,et al.  Superconducting Properties of High- J c MgB 2 Coatings , 2001 .

[20]  A. Campbell,et al.  A direct method for obtaining the critical state in two and three dimensions , 2009 .

[21]  C. F. Hempstead,et al.  Magnetization and Critical Supercurrents , 1963 .

[22]  A. Campbell,et al.  A new method of determining the critical state in superconductors , 2007 .

[23]  Ernst Helmut Brandt,et al.  SUPERCONDUCTOR DISKS AND CYLINDERS IN AN AXIAL MAGNETIC FIELD. I. FLUX PENETRATION AND MAGNETIZATION CURVES , 1998 .

[24]  L. Testardi,et al.  Constant E-J relation in the current induced resistive state of YBa/sub 2/Cu/sub 3/O/sub 7-x/ , 1991 .

[25]  Enric Pardo,et al.  Magnetic properties of arrays of superconducting strips in a perpendicular field , 2003 .

[26]  Telschow,et al.  Integral-equation approach for the Bean critical-state model in demagnetizing and nonuniform-field geometries. , 1994, Physical review. B, Condensed matter.

[27]  Macroscopic electrodynamic modelling of superconductors , 2000 .

[28]  G. Rubinacci,et al.  Power-law characteristic for 3-D macroscopic modeling of superconductors via an integral formulation , 2004, IEEE Transactions on Magnetics.

[29]  H. Kitaguchi,et al.  Fabrication and transport properties of MgB2 wire and coil , 2002 .

[30]  Luciano Martini,et al.  Development of an edge-element model for AC loss computation of high-temperature superconductors , 2006 .

[31]  Malcolm McCulloch,et al.  Computer modelling of type II superconductors in applications , 1999 .

[33]  M. Fabbri,et al.  Numerical Analysis and Experimental Measurements of Magnetic Bearings Based on ${\rm MgB}_{2}$ Hollow Cylinders , 2011, IEEE Transactions on Applied Superconductivity.

[34]  T. A. Coombs,et al.  A fast algorithm for calculating the critical state in superconductors , 2001 .

[35]  Carles Navau,et al.  Magnetic properties of finite superconducting cylinders. I. Uniform applied field , 2001 .

[36]  Charles M. Elliott,et al.  3D-modelling of bulk type-II superconductors using unconstrained H-formulation , 2003 .

[37]  A. Bossavit,et al.  Numerical modelling of superconductors in three dimensions: a model and a finite element method , 1994 .

[38]  T. Coombs,et al.  Numerical analysis of high-temperature superconductors with the critical-state model , 2004, IEEE Transactions on Applied Superconductivity.

[39]  R. Albanese,et al.  Finite Element Methods for the Solution of 3D Eddy Current Problems , 1997 .

[40]  Computation of 2-D current distribution in superconductors of arbitrary shapes using a new semi-analytical method , 2007, IEEE Transactions on Applied Superconductivity.

[41]  Brandt,et al.  Superconductors of finite thickness in a perpendicular magnetic field: Strips and slabs. , 1996, Physical review. B, Condensed matter.

[42]  Pascal Tixador,et al.  Different formulations to model superconductors , 2000 .

[43]  Y. Tseng,et al.  Levitation force relaxation in YBCO superconductors , 2004 .

[44]  Leonid Prigozhin Regular ArticleThe Bean Model in Superconductivity: Variational Formulation and Numerical Solution , 1996 .

[45]  H. Hashizume,et al.  Numerical electromagnetic field analysis of Type-II superconductors , 1991 .

[46]  Antonio Morandi,et al.  State of the art of superconducting fault current limiters and their application to the electric power system , 2013 .

[47]  Pascal Tixador,et al.  Comparison of numerical methods for modeling of superconductors , 2002 .

[48]  T. Ogasawara,et al.  Numerical analysis of a.c. losses in superconductors , 1991 .

[49]  Three dimensional finite elements modeling of superconductors , 2000 .

[50]  P. Girdinio,et al.  A computer approach to the nonlinear hysteretic problem of electromagnetic field computation in hard superconductors for loss evaluation , 1982 .

[51]  A. Bossavit,et al.  From Bean's model to the H-M characteristic of a superconductor: some numerical experiments , 1997, IEEE Transactions on Applied Superconductivity.

[52]  M. Fabbri,et al.  Sensitivity of the Field Trapped by Superconducting Bulks on the Parameters of the Magnetization Process , 2006, IEEE Transactions on Applied Superconductivity.

[53]  E. Brandt GEOMETRIC BARRIER AND CURRENT STRING IN TYPE-II SUPERCONDUCTORS OBTAINED FROM CONTINUUM ELECTRODYNAMICS , 1999 .