Abstract
The yield stress of alloys with complex microstructure is composed of the individual contributions of elementary hardening mechanisms in addition to the friction in the pure matrix lattice. The effects of hard and soft obstacles (zero-, one-, and three-dimensional defects, causing strong or weak curvature of the dislocations) and boundaries have been distinguished. Their contributions are not simply additive for microstructures containing different types of hard obstacles (dislocations, particles) or hard obstacles and boundaries.
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