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For low strain rates, the simplifying assumption that failure is governed by the largest flaw may be justified.
Variations in flaw size increase the scatter in the strength more for low strain rate loadings and less clustered microstructures.
In fact, when exposed to various increasing temperature levels, the material endurance tends to decreases for low strain range (correspond to high number of cycle).
However, there was a significant difference in the strength of the texture for different orientations that was absent for low strain rate deformed samples at high strain rate.
It has previously shown experimentally and numerically that for low strain rates larger particles can cool the flames more efficiently compared to smaller particles.
For low strain amplitudes (γpl<3×10−4), cyclic saturation occurred after an initial cyclic hardening stage, but for high strain amplitudes (γpl≥6.0×10−4) saturation could not be reached until fatigue failure.
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It can be noted that structure undergoes small strains and thus piezoelectric based harvester is not suitable for low strains.
A flame stability map based on the flame oscillation modes is also provided for low-strain-rate flames.
It is deduced that in the loading conditions used to determine the self-heating curves, the dissipative mechanisms imply recoverable strains (anelasticity) for low stress magnitudes and unrecoverable strains (inelasticity) for higher stress magnitudes.
This revealed that electrical properties resulting from localized nanoparticle nucleation have higher strain dependence as compared to bulk stretchable conductors, allowing for utilization as a strain sensor for relatively low strain conditions (ε < 50%).
For the nonpremixed counterflow, results show that a secondary S-curve is developed on the lower branch of the conventional, primary S-curve for sufficiently low strain rates and/or sufficiently high pressures, with its own distinct ignition extinction turning points.
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