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In the continuous case, \(f\) would vary continuously on \(S\) and we might have a differential equation specifying how \(f\) varies.
The material properties vary continuously through the layers thickness.
The material properties are assumed to vary continuously through the thickness direction.
Thus, both Young's modulus and Poisson's ratio vary continuously in coatings across the radius.
Material properties of the beam vary continuously in thickness direction according to a power-law form.
The material properties vary continuously in the thickness direction based on a simple power law distribution.
The main objelasticof the propertiesofsthey the influence of material nonhomogeneity on the buckling resistaree of the grassumedyer for various crack positoons, coating thicknesses and different orthotropic FGMs.
The properties of the FGPM layers vary continuously along the thickness.
The material properties of FG truncated conical shells vary continuously in the thickness direction.
The material properties of FGMs are assumed to vary continuously through the thickness of the shell.
The material properties are assumed to vary continuously according to a simple power law.
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