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It is also found that the detectability of voids near the surface generally increases with decreasing sample's elastic modulus, and can be further increased by adjusting the striker velocity.
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This assumes that Young's modulus and ν can be engineered independently.
The reason for the temperature-dependent elastic modulus and hardness can be ascribed to the variation in surface rough microstructures.
P-wave velocity is a function of bulk modulus, shear modulus and density can be written as follows: Vp = sqrt {frac{{B + {4 mathord{left/ {vphantom {4 3}} right.
Finally, as will be shown later in the article, the modulus and phase can be established also for the non-integral spectral indexes k, raising the computational effort only negligibly.
The energy dissipation due to the collisions, however insignificant in most situations of practical importance, results in a noticeable decrease in the bulk modulus of elasticity and can therefore cause the break of stability under otherwise identical conditions.
Also Young's modulus, Poisson's ratio, Bulk modulus and Shear modulus can be evaluated using the following equations from the elastic constants.
The values of Young's modulus and shear modulus can be derived from the above values, all of which are listed in Table 1.
With this approach, the cross-sectional area, section modulus and buckling ratio can be quantified.
Finally, temperature effects that cause variations in the Young's modulus and residual stress can be almost completely eliminated easily.
The magneto-induced shear storage modulus and MR effect can be increased by selecting CIP of low carbon content.
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