The irreversibility field, H*, has been measured for a variety of mono-and multifilamentary ͑Bi,Pb͒ 2 Sr 2 Ca 2 Cu 3 O x ͑2223͒ tapes using two different transport current techniques. It is common to characterize the quality of 2223 tapes by their zero-field, 77 K critical current density ͓J c (0 T, 77 K͔͒, even though this ignores the fact that significant self-fields depress J c (0 T, 77 K) and the possibility that the in-field J c (B) characteristics may be optimized independently of the J c (0 T, 77 K) value. To provide more useful information, we propose a second characterization, that of the irreversibility field, H*. Having both H* and J c (0 T, 77 K) information helps in separating the two independent contributions that better connectivity and stronger flux pinning can make to the J c of a tape. We illustrate this point with results from a variety of mono-and multifilamentary Bi-2223/Ag tapes in damaged and undamaged conditions, which show that H* ͑77 K͒ can vary from ϳ100 to ϳ200 mT and not directly correlate with J c (0 T, 77 K). The two proposed protocols for H* measurement are robust and compatible with common transport measurement procedures. © 1997 American Institute of Physics. ͓S0003-6951͑97͒00352-5͔Both the zero-field, J c (0), and the in-field, J c (B), critical current densities of ͑Bi,Pb͒ 2 Sr 2 Ca 2 Cu 3 O x ͑2223͒ tapes must be improved to make applications economically feasible. J c is defined experimentally as J c ϭI c /A where I c is the critical current and A is the area of the whole ceramic cross section. However, this averaged, overall J c is most certainly an understatement of the maximum local J c because the current percolates through only a fraction of the cross-sectional area, A active . J c (0) contains significant contributions from current paths that include weakly linked grain boundaries, which are decoupled by small magnetic fields, and it is thus at least partially limited by self-fields generated by the transport current. However, J c (B) is strongly influenced by the strength of the flux pinning. At high fields, either intragranular 1-6 or intergranular 7,8 flux pinning becomes the main J c -limiting mechanism. Because different mechanisms determine J c (0) and J c (B), this leads us to believe that J c (B) may be optimized independently of J c (0). The irreversibility field, H*, is an increasingly common parameter used to measure flux pinning because it is strongly influenced by flux pinning. H* can be measured by several magnetization and transport current techniques. Previous work [8][9][10] has shown that individual composites often show a direct correlation between H* and J c (0). However, as we have accumulated a larger database of H* and J c (0) characterizations, we have found that there is no universal correlation and we, therefore, conclude that it is vital to characterize both the flux pinning and zero-field properties, if the highest performance is to be developed in BSCCO-2223 tapes.When H* is measured by magnetization, the magnetization signal is averaged ov...