The steel cool cracking is controlled by repartition of hydrogen in th
e metal too, i.e.. by the possibility of realizing great local concent
rations. The accumulation of hydrogen depends upon the existence of re
versible and irreversible traps, or the possibilities of its diffusion
, for different conditions of thermic gradient, stress level, the conc
entration gradient, or the intensivity of the electric field. A good k
nowledge about these traps is important for the elaboration of materia
ls resistance to fragilization through hydrogen, as well as for the su
bsequent treatment for dehydrogenation.