Scaling of the pinning force (F_p) with temperature, field and strain for Nb₃Sn wires is widely discussed but important issues are still unresolved, for example whether empirical engineering-oriented scaling functions can be replaced by more microscopic, physics-based models, which take account of the fact that F_p becomes zero at an irreversibility field (H*) less than the upper critical field (H_c2). In the present work we compare earlier extensive measurements of the critical current density (J_c) of an ITER-benchmark bronze wire to new measurements of H* and H_c2. Our study was also made in different strain states. We observe that the Kramer extrapolations, which are based on transport data taken up to 13 T, significantly overestimate the low temperature, high field behaviour and also underestimate the critical temperature (T_c) at zero field. An attempt is made to connect measured H_c2(T, ε) data on this practical conductor to microscopic theory. We also discuss the inevitable differences that occur between fully penetrated J_c data which average over all the A15 layers and small current–density probes of the H_c2 transition which are characteristics of the best part of the layer. We connect in this way the large-scale 'average' characteristics of J_c(H, T, ε) to small current 'best' characteristics of H_c2(T, ε).