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The temperature and strain rate factors of the yield surface can be accurately determined solely by the peak stress of the strength tests.
The new smooth yield surface can be made to approximate the Mohr Coulomb yield function as closely as required by adjusting only two parameters, and is suitable for consistent tangent stiffness formulations.
Although the concept of yield surface has not been explicitly assumed in endochronic theory, it is demonstrated that the cone-cap yield surface can be derived as a special case of the proposed endochronic model.
In this model, the yield surface can be described by Eq. 4 [24]: f_{L - DP} = q - p. tan (beta ) - sigma_{y} = 0 (4)where p is the hydrostatic equivalent stress ((p = - frac{1}{3}(sigma_{1} + sigma_{2} + sigma_{3} ))) and β is the friction angle, a property of the material measured using tensile and compressive tests.
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It is also found that all these "yield" surfaces can be described roughly by a general formula.
Using this model we prescribe offsets of probing plastic strain, so apparent yield surfaces can be determined in a similar way as it is performed in the actual experiments.
A regularly textured surface can be yield with various types of patterns [3, 5, 6] using conventional photolithography.
Falling on this surface can be painful.
The grass surface can be heated to nearly 60 degrees.
Looking beneath the surface can be essential.
A perspective analysis of the correlation between theoretical studies and metal oxide surface modifications is finally offered, discussing their strengths and weaknesses and emphasizing their role as a powerful design tool for a new generation of implantable devices in which metal oxide surfaces can be tuned to yield a specific biological response.
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