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Most of the material volume is therefore occupied by polymer.
Here, f(A) denotes a mechanical behavior index, and the material volume is limited by W0.
The material volume is modeled, by a Digital Concrete model which takes into account the microstructure heterogeneities and the "real" aggregate size of concrete.
The largest of these defects in a critical material volume is in the range of tens of micrometres which is on the same size scale as the grain size.
The locations and severities of damages are characterized by using a damage distribution function, and a damaged small material volume is represented by the effective orthotropic elastic stiffnesses, which are derived in terms of damage orientation and size.
At identical iodine flux and iodine dose, the injected contrast material volume is higher, both in total as well as per unit time, for lower concentration media.
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The total volume and the cavity volume, as well as the high conductivity material volume, are fixed, but the geometric lengths and thickness of both X-shaped configurations can vary.
Understanding temperature-dependent deformation behaviour of small material volumes is a key issue in material science, especially the deformation behaviour of bcc metals at elevated temperatures is of particular interest for small-scale structural applications.
The extended version of the Lagrange equations for systems containing non-material volumes is employed to derive the equations of motion, resulting directly in a set of coupled nonlinear ordinary differential equations.
Despite the exceptionally terse and dense presentation, the elementary material in this volume is recommended to those new to the concept of path integrals.
Electric field-induced and excimer laser-induced techniques however are expected to effectively evaporate (etch out) the material, and hence material volume reduction is speculated.
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