Abstract
The non-linear distribution of lattice straine310vs sin2Ω observed on the surface of a polished steel specimen can be interpreted by tri-axial stress state with surface components of stress tensorσ11(0)=σ22(0) and gradientsg11=∂σ11/∂T, g33=∂σ33/∂T. The distribution of experimental values\(\bar \varepsilon _\psi \) is duscussed from the viewpoint of various ways of calculatingσ11.
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