The Kachanov and Rabotnov (K-R) creep damage model was interpreted and appl
ied to type 316LN and HT-9 stainless steels. Seven creep constants of the m
odel, A, B, k, m, lambda, r, and q were determined for type 316LN stainless
steel. In order to quantify a damage parameter, the cavity was interrupted
ly traced during creep for measuring cavity area to be reflected into the d
amage equation, For type 316LN stainless steel, lambda=epsilon (R)/epsilon*
and lambda (f)=epsilon/epsilon (R) were 3.1 and increased with creep strai
n. The creep curve with lambda =3.1 depicted well the experimental data to
the full lifetime and its damage curve showed a good agreement when r=24. H
owever for the HT-9 stainless steel, the values of lambda and lambda (f) we
re different as lambda =6.2 and lambda (f) = 8.5, and their K-R creep curve
s did not agree with the experimental data. This mismatch in the HT-9 steel
was due to the ductile fracture by softening of materials rather than the
brittle fracture by cavity growth. The differences of the values in the abo
ve steels were attributed to creep ductilities at the secondary and the ter
tiary creep stages.