If the former relaxation mechanism is dominant, nanocracks are intensively generated and converge giving rise to the brittle behavior of a nanocrystalline specimen.
Conant (1929) gave a detailed account of the feeding behavior of a captive specimen from South Carolina.
A majority of these studies, however, are focused on the component behavior of an RC specimen by imposing a predefined cyclic displacement history on the specimen without considering the interaction of the specimen with the entire structural system.
To evaluate this design criterion, an isothermal squeeze flow model describing the behavior of a cylindrical fluid specimen which includes inertial forces is used to predict the experimental results for a model Newtonian fluid.
We surveyed some papers about measuring the electrochemical behavior of NiS specimen for a non-enzymatic glucose sensor.
The overall behavior of specimens J-A (Fig. 14b), J-CFRP (Fig. 14c), J-SJ1 (Fig. 14e), J-SJ2 (Fig. 14f), and J-SJ3 (Fig. 14g), which were strengthened with head re-bars, CFRPs, and steel jackets, respectively, was similar to that of control specimen J-0.
The charging/discharging behavior of the specimen was analyzed using galvanostatic charge/discharge on a potentiostat/galvanostat (SP-150, BioLogic Science Instruments, Claix, France) with DC's of 10 V, 10 pA ~ 100 mA for ~900 s at room temperature.
The analysis of the thermal amplitude trend with the lock-in thermography evidences a variation in the thermal behavior of the specimens, defining a corresponding damage stress σD.
A systemic compliance technique for estimating fatigue crack growth behavior of CIET specimen has been successfully constructed and experimentally verified.
After finishing the measurement for the electrochemical behavior of NiS specimen in 0.1 M NaOH, we also surveyed many papers for a physiological condition.
