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Fig. 1. A fatigue crack was initiated from porosity in a sand-cast A356- T6 casting. (Image was taken using secondary electron imaging.)


Fig. 2. This fatigue crack was initiated from an (old) oxide film in a sand-cast A356-T6 casting. (Image was taken using secondary electron imaging.)


Fig. 3. Fatigue cracks were initiated from (left) fractured and (right) debonded eutectic particles in a sand-cast A356-T6 casting. (Image was taken using secondary electron imaging.)


various degrees of porosity, oxide levels and microstructural features. When pore and oxide sizes are larger than competing microstructural weak links (such as eutectic silicon particles), crack initiation life can be ignored. However, when the flaw size in the casting approaches the microstructural feature size (~25-50 µm), crack initia- tion life from microstructural con- stituents such as persistent slip bands can dominate the total fatigue life. Fatigue cracks usually initiate from flaws in aluminum castings. In coarse microstructures, the dendrite cell walls act as grain boundaries because they are surrounded by a nearly continuous array of eutectic particles. Te researchers applied MSF models to estimate the fatigue life


2


Procedure At GM, MSF models


have been developed to predict fatigue life of cast aluminum components with


of cast aluminum alloys A356 and 319. Tey used extreme values of the characteristic flaw and microstruc- ture features that were assumed to have nominal value (50% probability) and 99.94% (+3 standard deviations) probability of occurrence. A comparison of the calculated


propagation life based on both long and short crack models with empiri- cally derived constants to actual fatigue life (Nf) was made. Te calculated crack propagation life (Np) was in good agreement with the actual fatigue life. Tis indicated the total fatigue life of cast 319 alloys failing from porosity is mainly comprised of crack propaga- tion and the assumed initiation life near zero is reasonable. Compared to the short crack model, the long crack model is simpler and fits the data over the useful life range of most compo- nents. Given the inherent scatter in fatigue life data, predictions within an order of magnitude of measured


values (dashed lines) are useful. Te researchers compared the pre-


dicted fatigue life based on the long and short crack models using the extreme- value statistics (EVS) estimated maximum pore sizes to the experimen- tal data. As expected, with the upper bound EVS estimate of the maximum pore size, both long crack and short crack models gave a conservative lower bound fatigue life prediction. Tey also performed a comparison


of the calculated fatigue life of samples failed by cracked eutectic particles and debonded eutectic with actual fatigue life. Te samples tested at the stress amplitude of 85 MPa and stress ratio R = -1 had coarse unmodified microstructures and large silicon and iron-rich particles. Te fatigue cracks in all three samples were initiated by cracked silicon and iron-rich particles. Te calculated fatigue life was in good agreement with the actual fatigue life. A comparison of the calculated


May 2013 MODERN CASTING | 39


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