Mechanisms of fatigue crack growth have been studied for a range of PM stee
ls at relative densities of 0.90 and 1.0, for which strength, fracture toug
hness, and microstructural information was also available. It is shown that
the Paris exponents for steady state crack growth are between 8 and 18 whe
n rho(r) is similar to 0.9 but when rho(r) is similar to 1.0 the exponents
are between 2.6 and 4.0, i.e in the range typical of wrought steels (2-4).
At both densities, threshold stress intensities are between 5.5 and 10.8 MP
a m(1/2) when R = 0.1. Combinations of these thresholds and yield strengths
are comparable with those for wrought steels. When R = 0.8, reductions in
threshold to between 2.7 and 5 MPa m(1/2) are attributed to crack closure e
ffects. At rho(r) = 0.90, Fe-0.5C fails by progressive rupture of sinter ne
cks. Astaloy A, with 0.2%C and 0.6%C, and Distaloy AB-0.6C have smaller pla
stic zone sizes and the cracks follow more difficult paths through particle
s as well as necks. When rho(r) is similar to 1.0, fracture is partially by
true fatigue modes and partly by cleavage, the bursts of cleavage being mo
re noticeable when K-max is high.