From the technological point of view, the difficulty of brittle mechanical properties and the low critical current density of c~b~per oxide superconductors must be overcome. To improve the mechanical properties, doping with silver has been found to give the most satisfactory results [1]. Improvement of critical current density can be achieved in several ways: by pinning the magnetic flux Well by creating defects [2], or by adding fine particles [3]; or by orienting the high-Jc directions of the microcrystals in the bulk sample in the direction of current flow by zone-melt processing [4], shock compaction [5]. Cold pressing [6] or vibrational alignment [7]. In the present work a series of studies were carried out to determine the optimal silver content in the composite AgxBi~.TPb0.3Sr2Ca2Cu3010, which does not decrease Tc too much but can improve the Jc and ductility of the bulk sample. The silver-ceramic composite was compressed in thez-direction while allowing it to expand freely in the xand y-directions. Both T~ and J~ were increased by adding silver and by compression. Pellets of composition BiL7Pbo3Sr2Ca2Cu3Olo, which was reported as the optimum composition for obtaining pure high-Tc phase in the B i P b S r C a C u O system [8], were prepared by thoroughly mixing Bi203, PbO, SrCO 3, CaCO 3 and CuO, calcining and sintering with intermediate regrinding several times as described previously [8]. The 110 K (onset) and 90-100 K (zero resistance) of the pellets as determined by four-point resistance measurements showed that they consisted of two phases, which is also consistent with the x-ray powder diffraction patterns and with the magnetization data obtained with a superconducting quantum induction device (SQUID). The Bil.TPb0.3Sr2Ca2Cu3010 pellets were ground to a fine powder and mixed with different stoichiometric amounts of Ag20 pressed at 50 MPa into 0.4 g pellets and heated for 30 min at 550 °C to convert all the Ag20 to metallic silver. The resultant pellets of composition Ag~Bil.7Pb0.3Sr2Ca2Cu3010 (x = 0, 4, 8, 12 and 16) were cut into narrow rectangular slices. Each selected small rectangular slice was compressed between the stainless surfaces of a large die at 1.5 GPa for 5 min. Then the irregular edge area was cut off and the slice was compressed again at 4 GPa for 5 min. The compressed as well as the uncompressed samples were annealed at 850 °C for 20 h in air to improve the coupling at the grain boundaries. The temperature dependence of resistance, R(T)/R(280), for a series of uncompressed and compressed samples of AgxBil.7Pb0.3Sr2Ca2Cu3010 ( x = 0 , 8 and 16; x = 4 and 12 not shown) is illustrated in Fig. la and b, respectively• It was found that increasing the silver content from x = 0 to x = 16 decreased the T c of the uncompressed
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