Bk. Choudhary et al., Steady state creep deformation behaviour of 9Cr-1Mo ferritic steel forgingin quenched and tempered condition, T I INST ME, 52(5), 1999, pp. 327-336
Constant load isothermal creep tests have been carried out to assess the in
fluence of stress (60-300 MPa) and temperature (773-873 K) on the steady st
ate creep deformation behaviour of 1000 mm diameter and 300 mm thick 9Cr-1M
o ferritic steel forging in quenched and tempered condition. Applied stress
dependence of steady state creep rate obeyed Norton's power law and exhibi
ted two slope behaviour with stress exponents of about 5-6 at low stresses
and 10.2 at high stresses at all temperatures. The two slope behaviour is a
lso reflected in two apparent activation energy values of 266 and 468 kJ mo
l(-1) in the low and high stress regimes, respectively. Invoking the concep
t of resisting stress, the two stress exponents and two apparent activation
energy values in the two stress regimes have been rationalized using modif
ied Dorn equation. Following Lagneborg and Bergman, the resisting stress ha
s been determined from the creep data. The Variation of resisting stress wi
th applied stress and temperature indicated that at low stresses resisting
stress is insensitive to test temperature and increases linearly with appli
ed stress with proportionality constant of 0.77. On the other hand, at high
stresses the resisting stress remains constant equal to threshold stress a
nd decreases with increasing test temperature. Incorporating resisting stre
ss in both low and high stress regimes into modified Dorn equation, a singl
e slope behaviour with stress exponent of about 4 and a true activation ene
rgy of about 250 kJ mol(-1) have been obtained.. These observations suggest
that the steady stare creep deformation in both the stress regimes is clim
b controlled.