Download or read book Chemical Addition and Superconducting Phase Formation in Magnesium Diboride written by Fang Wan (Ph. D. in materials science) and published by . This book was released on 2020 with total page 177 pages. Available in PDF, EPUB and Kindle. Book excerpt: The low-cost, ease-of-fabrication, and intermediate critical temperature (Tc) of 39 K are key factors enabling magnesium diboride (MgB2) conductors be promising for application. However, the most important parameter for evaluating the electrical performance of MgB2 conductors is the critical current density (Jc). For MgB2 strands, the Jc can be discussed in terms of layer Jc, non-barrier Jc, and engineering Je. The aim of this dissertation is to explore effective routes to enhance the Jcs and Jes of MgB2 conductors, which requires a solid understanding of how superconducting properties are related with microstructure, band scattering, and phase formation in MgB2. Previous studies have shown that the Jcs of MgB2 bulks and layer Jcs of MgB2 strands, which are determined by intrinsic properties of MgB2, can be improved through increases of Bc2/Birr and the density (grain connectivity) of the MgB2 phase. On the other hand, the Jes of MgB2 strands can be further improved by increasing the area fraction of MgB2 relative to the whole strand because Je = layer Jc × A(MgB2)/A(strand) , where A(MgB2) and A(strand) are the transverse cross-sectional area of MgB2 and the transverse cross-sectional area of whole strand, respectively. While the non-barrier Jcs and layer Jcs are identical for powder-in-tube (PIT) in-situ MgB2 strands, the non-barrier Jcs of advanced-internal-magnesium-infiltration (AIMI) MgB2 strands can also be improved by increasing layer Jcs and the MgB2 area fractions within chemical barrier because non-barrier Jc=layer Jc × A(MgB2)/Anb, where Anb is the area within chemical barrier. Chapter 2 summarizes the sample preparation and experimental testing utilized in this dissertation were summarized. Chapter 3 focuses on chemical addition methods including both pure C doping as well as C/Dy2O3 co-addition to improve the non-barrier Jcs (layer Jcs) of PIT in-situ MgB2 strands via increased Bc2/Birr and decreased Bc2 anisotropy. Here C doping was accomplished using pre-C-doped B powders. The doping effects of two types of B powders, SMI B and PVZ B, were compared in terms of the 4.2 K non-barrier Jcs of multifilamentary PIT in-situ strands. By adding 0 ~ 6 wt% Dy2O3 into the 2 mol% C-doped MgB2 strand, non-barrier Jcs with acceptable values were achieved over a wide temperature range of 4.2 to 25 K. The relationship between Bc2 enhancement and band scatterings was investigated. In Chapter 4, a vapor-solid reaction route was established with the aim of increases the area fraction of MgB2 layer in AIMI strands. Moreover, the vapor-solid reaction was also demonstrated to generate MgB2 layers with high levels of uniformity in 18-filamentary AIMI strands. Consequently, high Jes and n-values were achieved by the vapor-solid reacted strands. In Chapter 5, the micron-sized B powders were used to synthesize large-size MgB2 tubes for passive shielding applications The Jcm of 108 A/cm2 was achieved by the best tube at 4.2 K, 1 T. The DC/AC external fields of 0.67 T/1.75 T were completely shielded by the tube at 4.2 K. Long-distance Mg infiltration into B compact and well-connected MgB2 phases were simultaneously obtained using a heat-treatment of 900 oC/36 h.