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Several genes responded to the same stress; for example, TaCBL9, TCIPK7, 15, 24, and 32 were induced by H2O2.
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Experiments on shot peened notched specimens do not exhibit the same stress redistribution even for larger applied stresses.
The difference in local strain between irradiated regions and nonirradiated regions under the same stress is critical for the appearance and disappearance of the invisible patterns.
It also suggests that the transition from Stage I crack growth (short crack) to Stage II for the same stress level occurs at smaller crack lengths for the exfoliated material.
In conclusion, the stress gradient over the plate thickness, the effective plate thickness due to vertical web plates and high notch effects slow down the crack propagation rate if the same stress value being effective for fatigue appears at the weld toe.
The fatigue life was shortened when applying the mean stress for the same strain range, whereas it was increased for the same stress amplitude.
A base for recognising each specific ideal configuration is a fine coincidence between actual interferograms and analogous reference fringe patterns constructed for the same stress state.
Results are compared for the same stress ratio and relevant differences on fatigue crack growth are commented based on crack closure concepts.
The detected creep was pressure sensitive, higher in tension than in compression for the same stress level, following the strength differential effect (SDE) at material yielding.
Small cracks grew faster than large cracks for the same stress intensity range ΔK, as expected from previous research by others.
Moreover, fatigue crack growth rates of small cracks in these alloys were found to be greater than those of large cracks for the same stress intensity factor range.
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