Bk. Choudhary et al., Creep deformation and fracture behaviour of forged thick section 9Cr-1Mo ferritic steel in the temperature range 773-873 K, T I INST ME, 53(3), 2000, pp. 203-215
Creep tests have been performed to examine the creep deformation and ruptur
e behaviour of forged thick section 9Cr-1Mo ferritic steel in quenched and
tempered (Q+T), simulated post weld heat treatment (SPWHT) and thermally ag
ed (TA) conditions in a wide range of stresses (50-300 MPa) and temperature
s (773-873 K). Applied stress dependence of steady state creep rate obeyed
Norton's power law and exhibited two slope behaviour with stress exponents
of similar to 5-6 at low stresses and 10.2 at high stresses. This is also r
eflected in two apparent activation energy values of 266 and 468 kJ mol(-1)
in the low and high stress regimes, respectively. Invoking the concept of
resisting stress into Dorn type creep relationship, a single slope behaviou
r with a true stress exponent of similar to 4 and a true activation energy
of 250 kJ mol(-1) have been obtained. These observations suggest that the c
reep deformation in both the stress regimes is climb controlled. Stress dep
endence of rupture life exhibited two slope behaviour. This is also reflect
ed in the two constants in the Monkman-Grant and modified Monkman-Grant rel
ationships and two creep damage tolerance factors in the two stress regimes
. The high creep ductility of the alloy increased with increase in temperat
ure. The failure mode remained transgranular. At 793 K, no significant diff
erence in the creep-rupture properties was noticed between Q+T, SPWHT and T
A conditions, while at 873 K, SPWHT specimens exhibited inferior creep-rupt
ure strength than that of Q+T specimens. The extensive tertiary creep obser
ved in the alloy has been attributed to microstructural degradation associa
ted with precipitates and dislocation substructure. The creep-rupture stren
gth of the forging has been found to be lower than that of thin section bar
s and tubes.