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The practical advantages of TCD over other methods are its relative simplicity and the fact that it requires only a few mechanical properties, which can be determined from simple tests or available data on the material.
As with models (1) and (2) the local stability of these steady states cannot be determined from simple linearization techniques.
This approach significantly simplifies the analysis of the resulting transients and appears to allow reliable 1° KIEs to be determined from simple (multi exponential fitting of the data.
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It is noted that the parameters B 2 and B 6 in Eq. (3) correspond to the global deformation of the laminate and, therefore, the unknown constants B 2 and B 6 may be determined from the simple first-order shear deformation plate theory (FSDT).
The coefficients that appear in the new criterion can be determined from uniaxial tension and compression, and simple shearing tests.
The hmF2 values can be determined from the ionosonde observations using a simple relation given by Bradley and Dudeney (1973).
Substituting the nondimensional values μ = (g 4 + g 5)/t t and η = 1 + T p,b b/M p,t into Eq. 18, the following equation for shear resistance of the top angle can be obtained: left[ {frac{{V_{t2} }}{{V_{p,t} }}} right]^{4} + 2mu frac{{V_{t2} }}{{V_{p,t} }} - eta = 0, (20)where V t2 can be determined from Eq. 20 by a simple iterative procedure.
Then a simple linear regression was compared with a segmented linear regression where the timepoint of the intersection of the two segments must be determined from the data.
The mechanical properties and the formability parameters of the sheets were determined from the simple tensile tests.
The effect of clogging factor on a multiple-grate inlet located in sag is determined from a simple expression suggested in this study.
The eigenstrain is determined from a simple geometry sample, and applied to the more complex geometry to predict the residual stress after Laser Shock Peening.
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