By Inderjeet Kaur

This booklet is the 1st complete treatise of 1 of the foremost actual approaches happening in a variety of fabrics at increased temperatures. The publication offers crucial heritage info for fabrics scientists, metallurgists, reliable nation physicists and semiconductor technologists engaging in learn or improvement during this and comparable parts. the 1st and moment variants of the ebook have been released via the college of Stuttgart in 1988 and 1989. within the current 3rd variation the ebook has been up-to-date and basically enlarged to hide all contemporary advancements within the region of grain and interphase boundary diffusion. The reader will locate greater than a hundred new textual content pages, 60 new figures and a hundred new references. This distinctive ebook is strongly suggested as a textbook for college students in addition to a reference e-book for physicists, chemists, metallurgists and engineers.

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**Extra info for Fundamentals of grain and interphase boundary diffusion**

**Example text**

The ﬂuid is assumed to be an incompressible Newtonian ﬂuid of shear viscosity μ f . 2 Viscous flow in a cylindrical pore space where (d P/d x ) e x denotes the pressure gradient. Since the pore pressure is uniform in each section, the pressure gradient is the same at both the microscopic and the macroscopic scale. e. 3) to ﬁnd out if both display a linear relation between the macroscopic ﬁltration velocity and the pressure gradient. Thus, from this comparison, the factor (πa 4 /8S)/μ f appears as the permeability K of this 1-D thought model, which captures the geometrical characteristics of the (no doubt too simplistic) cylindrical morphology of the pore space.

Let vi be the solution for α = e i , so that the solution v(α) is v = αi vi . 36) in the (e i ) base. 31) for α = e j ) are inversely proportional to μ f , tensor K also obeys this inverse proportionality. 32). 2). 41) Scale Effects on Permeability We are interested here in the scale effects on the permeability tensor that can be found from the micromechanics theory. 15) deﬁned in U f of the unit cell U. We now consider the domain U˜ f , which is the image of U f obtained by the homothety ˜ z) and v(˜ ˜ z) be a pressure and a H of center O and ratio λ: H(z) = λz.

106) There are several effects of deformation on the ﬂow through porous media. The ﬁrst possible coupling is due to the displacement of the solid–ﬂuid interface, which a priori inﬂuences the transport properties. The second one is the mechanical effect of the pore pressure on the overall deformation behavior of the porous material. The ﬁrst coupling is examined here with regard to Darcy’s law. The second coupling with the deformation behavior will be studied in Chapter 5, where we will see a consistent derivation of the macroscopic poroelasticity theory from homogenization techniques.