“…Moreover, the hardening behavior is described by means of the Hollomon power law written for RD as:Y(ε¯p)=Kfalse(ε¯0+ε¯pfalse)n where K is the strength coefficient, n is the hardening exponent (note that in this context, unlike other approaches [1,7,14,16,17], these two coefficients are only defined for RD), and with ε¯0=(σypRDK)1n, σypRD being the yield strength for RD (see Table 1). In addition, the rate of the equivalent plastic strain is ε¯p˙=σm:bold-italicε˙pσ¯, such that εp is the plastic strain tensor whose rate obeys the classical (objective, i.e., frame-indifferent) associated flow rule bold-italicε˙p=trueλ˙∂trueσ¯…”