The Path of a Growing Crack – A Simulation of the Fracture Process C. Bjerkén 1 and P. Ståhle 1,2 1 Div. Materials Science, Malmö University, Sweden, christina.bjerken@ts.mah.se 2 Div. Solid Mechanics, Lund University, Sweden, per.stahle@ts.mah.se ABSTRACT. The growth of a crack subjected to corrosion fatigue is studied using adaptive finite elements. The crack is the image of a deep corrosion pit, and the growth is the result of a repeated cycle of dissolution of the material, formation of a protective oxide film and break-down of the oxide film. The break-down of the film is governed by the strain at the surface and the dissolution rate is assumed to be proportional to this stretching. A threshold strain is assumed to exist below which the oxide film remains intact. With this model, no criterion is needed, neither for crack growth, nor for prediction of the growth direction. The reason is that both are immediate results of the evolution of the body shape. The growth of a semi-infinite crack lying in an infinite strip subjected to different degrees of mixed-mode loading is studied and the results are compared to crack path criteria for sharp cracks. Additionally, the path of a corrosion fatigue crack starting at the surface of an elastic layer attached to a stiff substrate is simulated. The result showed some agreement with experimental results found in the literature. INTRODUCTION During stress corrosion, loss of atoms to the environment leads to crack growth. This is a dissolution process that starts if bare metal is exposed to aggressive environments. Fortunately, an impermeable film of mainly metal oxides or hydroxides is formed by dissolved metal. Even though the thickness of this film is typically not more than 10 nm, it reduces the rate of dissolution by several orders of magnitude, cf. [1]. An intact protective film increases the life of the structure tremendously. However, repeated changes of the electrochemical conditions or cyclic mechanical load damage the film, which leads to additional material loss. Several experimental reports show that active loading in terms of either monotonically increasing or fatigue load is an essential prerequisite for development of corrosion cracks, cf. [2]. The passivating film is as being an oxide or hydroxide compound believed to have ceramic material properties. As such it is presumably brittle. Here it is supposed to fracture when stretched more than a threshold strain, ε f . For strains smaller than ε f , the film remains intact. If the threshold strain is exceeded, the film breaks and leave gaps where bare metal is exposed to the environment, see Fig. 1. The area extent of these gaps is assumed to be proportional to the strain exceeding the threshold strain. The broken film leaves gaps