Fractal analysis of the role of the rough interface between Bi2Sr2CaCu2Ox filaments and the Ag matrix in the mechanical behavior of composite round wires

Multifilamentary round wires (RWs) of Bi2Sr2CaCu2Ox (Bi2212) superconductor in a Ag/AgMg matrix have complex microstructures that strongly influence their electrical and mechanical behavior. The Bi2212/Ag interfaces, which in some locations are characterized by Bi2212 growths into the Ag matrix that result in rough, jagged interfaces, and in other locations are characterized by Bi2212 growths that bridge and connect to neighboring Bi2212 filaments, are believed to be amongst the most important microstructural features; yet their role is not well understood. In this work, a fractal-based framework is created in an effort to understand the role of the structure of individual filaments and the Bi2212/Ag interfaces in determining the macroscopic electromechanical behavior of Bi2212 RW. Scanning electron micrographs of an individual Bi2212 filament extracted from a Bi2212 RW are used to analyze the rough Bi2212/Ag interface and develop a fractal model using the Weierstrass–Mandelbrot (W–M) fractal function. The W–M fractal function is then used to generate simulated Bi2212/Ag microstructures. Finally, the mechanical behavior of the microstructures is investigated. It is found that the interfilamentary bridges which play a significant role in Bi2212 transport are not likely to be the cause of electromechanical degradation and failure. Instead, large stress concentrations are identified at the concave tips that occur along the jagged Bi2212/Ag interface. In particular, locations where the concave tips are within the Bi2212 filament are the likely initiation points of failure in Bi2212 RWs.

[1]  J. Schwartz,et al.  Effect of Solidification Conditions on Partial Melt Processed Bi2212/Ag Round Wire , 2011, IEEE Transactions on Applied Superconductivity.

[2]  A. Majumdar,et al.  Fractal characterization and simulation of rough surfaces , 1990 .

[3]  D. Larbalestier,et al.  Filament to filament bridging and its influence on developing high critical current density in multifilamentary Bi2Sr2CaCu2Ox round wires , 2010 .

[4]  M. Rikel,et al.  Development of 2201 intergrowths during melt processing Bi2212/Ag conductors , 2001 .

[5]  M. Meinesz,et al.  Development of round multifilament Bi-2212/Ag wires for high field magnet applications , 2005, IEEE Transactions on Applied Superconductivity.

[6]  Kyriakos Komvopoulos,et al.  A Fractal Theory of the Interfacial Temperature Distribution in the Slow Sliding Regime: Part II—Multiple Domains, Elastoplastic Contacts and Applications , 1994 .

[7]  M. Berry,et al.  On the Weierstrass-Mandelbrot fractal function , 1980, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[8]  J. Zaanen,et al.  High-temperature superconductivity: The benefit of fractal dirt , 2010, Nature.

[9]  J. Schwartz,et al.  Effect of processing defects on stress-strain-I/sub c/ for AgMg sheathed Bi-2212 tapes , 2003 .

[10]  K. Komvopoulos,et al.  A Fractal Analysis of Stiction in Microelectromechanical Systems , 1997 .

[11]  J. Schwartz,et al.  Statistical analysis of the electromechanical behavior of AgMg sheathed Bi2Sr2CaCu2O8+x superconducting tapes using Weibull distributions , 2007 .

[12]  K. Komvopoulos,et al.  Contact analysis of elastic-plastic fractal surfaces , 1998 .

[13]  G. Aeppli,et al.  Optimum inhomogeneity of local lattice distortions in La2CuO4+y , 2012, Proceedings of the National Academy of Sciences.

[14]  Hanping Miao,et al.  Progress in$rm Bi$-2212 Wires for High Magnetic Field Applications , 2006, IEEE Transactions on Applied Superconductivity.

[15]  J. Schwartz,et al.  Proof-of-principle experiments for react–wind–sinter manufacturing of Bi2Sr2CaCu2Ox magnets , 2007 .

[16]  J. Schwartz,et al.  Development of High Superconductor Fraction Wire for MRI , 2008 .

[17]  Loren F. Goodrich,et al.  Reversible effect of strain on transport critical current in Bi2Sr2CaCu2O8 + x superconducting wires: a modified descriptive strain model , 2011 .

[18]  M. Di Michiel,et al.  Bubble formation within filaments of melt-processed Bi2212 wires and its strongly negative effect on the critical current density , 2011 .

[19]  Francisco Guinea,et al.  The Fractal Nature of Fracture , 1987 .

[20]  E. Hellstrom,et al.  Microstructurally optimized heat treatment for melt-processed, Ag clad Bi2Sr2CaCu2Oy tape step-solidification melt processing , 1995 .

[21]  K. Komvopoulos,et al.  A Fractal Theory of the Interfacial Temperature Distribution in the Slow Sliding Regime: Part I—Elastic Contact and Heat Transfer Analysis , 1994 .

[22]  Jia Du,et al.  CONNECTIVITY AND LIMITATION OF CRITICAL CURRENT IN BI-PB-SR-CA-CU/AG TAPES , 1999 .

[23]  Xia Sun,et al.  Fractal processing of AFM images of rough ZnO films , 2002 .

[24]  J. Schwartz,et al.  Strain effects in high temperature superconductors investigated with magneto-optical imaging , 2003 .

[25]  A. Barabasi,et al.  Fractal concepts in surface growth , 1995 .

[26]  A. Volokitin,et al.  On the nature of surface roughness with application to contact mechanics, sealing, rubber friction and adhesion. , 2005, Journal of physics. Condensed matter : an Institute of Physics journal.

[27]  James H Brown,et al.  The fractal nature of nature: power laws, ecological complexity and biodiversity. , 2002, Philosophical transactions of the Royal Society of London. Series B, Biological sciences.

[28]  D. Sanderson,et al.  Fractal effects of crack propagation on dynamic stress intensity factors and crack velocities , 1996 .

[29]  S. Awaji,et al.  Quantitative strain measurement in Nb3Sn wire and cable conductors using high-energy x-ray and neutron beams , 2013 .

[30]  A. Bianconi,et al.  Fractal Structure Favoring Superconductivity at High Temperatures in a Stack of Membranes Near a Strain Quantum Critical Point , 2011 .

[31]  Xiaotao Liu,et al.  Influencing factors on the electrical transport properties of split-melt processed Bi2Sr2CaCu2Ox round wires , 2012 .

[32]  A. Bianconi,et al.  Spatial inhomogeneity and planar symmetry breaking of the lattice incommensurate supermodulation in the high-temperature superconductor Bi2Sr2CaCu2O8+y , 2011, 1108.2140.

[33]  Xiaotao Liu,et al.  High Field Superconducting Solenoids Via High Temperature Superconductors , 2008, IEEE Transactions on Applied Superconductivity.

[34]  Jasmine Schwartz,et al.  Weibull analysis of the electromechanical behavior of AgMg sheathed Bi2Sr2CaCu2O8 + x round wires and YBa2Cu3O7 − δ coated conductors , 2010 .

[35]  G. Aeppli,et al.  Scale-free structural organization of oxygen interstitials in La2CuO4+y , 2010, Nature.

[36]  T. Hasegawa,et al.  Bi-2212 phase formation process in multifilamentary Bi-2212/Ag wires and tapes , 2005, IEEE Transactions on Applied Superconductivity.

[37]  A. Barabasi,et al.  Fractal Concepts in Surface Growth: Frontmatter , 1995 .

[38]  J. Schwartz,et al.  The Effect of Filament Diameter on ${\rm J}_{\rm e}$ in High Filament Count Bi2212/Ag Round Wire , 2009, IEEE Transactions on Applied Superconductivity.

[39]  Justin Schwartz,et al.  A two‐dimensional ordinary, state‐based peridynamic model for linearly elastic solids , 2014 .