CRITICAL-CURRENT ANISOTROPY, INTERGRANULAR COUPLING, AND EFFECTIVE PINNING ENERGY IN BI2SR2CACU2O8-CRYSTALS AND AG SHEATHED (BI, PB)(2)SR2CA2CU3O10+DELTA TAPES(DELTA SINGLE)

Bi2Sr2CaCu2O8+delta(Bi-2212) single crystals and Ag sheathed (Bi,Pb)(2 )Sr2Ca2Cu3O10+delta(Bi-2223) tapes have been characterized by magnetom etry and electron microscopy. Dislocations on the (001) planes appear to be the main defect observed in these samples and are considered to be important for flux pinning. Their distribution is more homogeneous in the Bi-2223 tape as a result of thermomechanical processing. In Bi- 2212 single crystals, the measurement of magnetic hysteresis reveals a strong anisotropy in the magnetization critical current density (J(cm )). For the two cases H parallel to c and H perpendicular to c, the me asurable Lorentz forces (F-L) that limit J, are found to be perpendicu lar to the c-axis; one causing vortices to hop in the ab plane and the other to slide along the ab plane. In contrast to this, we have probe d the relative strength ratio of the intrinsic pinning to the extrinsi c pinning in Bi-2223 tapes when we compare the results of H perpendicu lar to c with H parallel to c. No significant difference in J(cm) is o bserved, but for the same average J value, the effective pinning energ y (U-eff) calculated from the time derivative of the magnetization (M) for H perpendicular to c is two orders of magnitude higher than that for H parallel to c. For these two superconductors, their U-eff's foll ow a power-law expression, U-eff(J, T, H)=(U-i/H-n)[1-(T/T-x)(2)](1.5) (J(i)/J)(mu), where U-i is the scale of activation energy, n is of the order of 1, T-x is related to the magnetic irreversibility temperatur e (T-irr), and both J(i) and mu depend on the nux-bundle size and the value of J/J(c). A two-dimensional (2D) flux-line lattice (FLL) is cle arly identified in the Bi-2212 single crystal; however, imperfect text uring in the Bi-2223 tape smears out to some extent the observed J dep endence of U-eff. Consequently, a larger anisotropy in the normalized relaxation rate, S = -d In M/d In t, and much higher S values are obse rved in Bi-2212 than in Bi-2223.