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Stressed solid

It was shown earlier that the NabaiTO-Hemirg model of creep in solids involved the migration of vacancies out of the stressed solid accompanied by counter-migration of atoms to reduce dre length of the solid in the direction of the applied stress. This property could clearly contribute to densification under an external pressure, given sufficient time of application of the stress... [Pg.208]

K. Kassner, C. Misbah. Nonlinear evolution of a uniaxially stressed solid a route to fracture Europhys Lett 28 145, 1994. [Pg.919]

Fig-1 Stable equilibrium state (left) given by molecules vibrating about their mean position in a free energy well in an unstressed solid. Metastable equilibrium state (right) given by molecules vibrating in an elevated free energy well in a stressed solid (above the stable minimum for an unstressed solid). [Pg.325]

The concept of metastable solubility values is recognized by scientists familiar with processed (stressed) solids, but it is not well known to scientists accustomed to highly crystalline materials. Because of the relative sensitivity of... [Pg.326]

TABLE 6 Direct Infusion FTMS Results on a Stressed Solid Dosage Formulation... [Pg.542]

Gibbs [J.W. Gibbs (1878)] showed that a non-hydrostatically stressed solid surrounded (Fig. 8-7) by a fluid (in which it is soluble) is entirely determined by the nature and state of the solid through the relation... [Pg.198]

Solid electrolytes may have the requisite properties of a Gibbs fluid [W. Durham, H. Schmalzried (1987)] if 1) their conducting ion corresponds to an atomic component of the solid under stress and 2) they exhibit significant mechanical strength. Topical stress energy densities correspond to electrical potentials in the millivolt range. In order to establish them, only a small fraction of a surface monolayer of the electrolyte needs to dissolve during its equilibration with the stressed solid and... [Pg.198]

In order to derive the relation between EMF and the chemical potential difference probed at different surfaces of the stressed solid, we formulate the reversible work and its electrical equivalent. If zAF-dnA electric charges are transported across the electrolyte between the two surfaces labeled 1 and 2 in Figure 8-8, the electrical work is... [Pg.199]

Figure 8-8. Galvanic cell (schematic) for the determination of the chemical potential difference between surfaces 1 and 2 of non-hydrostatically stressed solids. Cross hatched solid electrolyte ... Figure 8-8. Galvanic cell (schematic) for the determination of the chemical potential difference between surfaces 1 and 2 of non-hydrostatically stressed solids. Cross hatched solid electrolyte ...
A defining characteristic of a solid is the ability to resist shear. Therefore, stress is an additional feature which has to be taken into account when the physical chemistry of solids is at issue. Gibbs treated the thermodynamics of stressed solids a century ago in his classic work Equilibrium of Heterogeneous Substances under the title The Conditions of Internal and External Equilibrium for Solids in Contact with Fluids with Regard to all Possible States of Strain of the Solid . We have already mentioned in the introduction that stress is an unavoidable result of chemical processes in solids. Let us therefore briefly discuss the basic concepts of the thermodynamics of stressed solids. [Pg.332]

To this end, we consider the thermodynamic functions of a homogeneously stressed solid, e.g., [L.D. Landau, E.M. Lifshitz (1989) W. W. Mullins, R. Sekerka (1985)]. In contrast to the unstressed solid, the internal energy of which is U(S, K ,), the internal energy of a stressed solid is given as U(S, VuJk,nj). For the total differential of the internal energy one has1... [Pg.332]

Thermodynamics of Stressed Solids with Only Immobile Components... [Pg.335]

Let us consider a homogeneously, but not hydrostatically, stressed solid which is deformed in the elastic regime and whose structure elements are altogether immobile. If we now isothermally and reversibly add lattice molecules to its different surfaces (with no shear stresses) from the same reservoir, the energy changes are different. This means that the chemical potential of the solid is not single valued, or, in other words, a non-hydrostatically stressed solid with only immobile components does not have a unique measurable chemical potential [J. W. Gibbs (1878)]. [Pg.335]

Larche, F.C. (1988) Thermodynamics of Stressed Solids, Solid State Phenomena, Vol. 3-4, 205... [Pg.353]

J.W. Cahn s early contributions to elastic coherency theory were motivated by his work on spinodal decomposition. His subsequent work with F. Larche created a rigorous thermodynamic foundation for coherency theory and stressed solids in general. A single volume, The Selected Works of John W. Cohn [15], contains papers that provide background and advanced reading for many topics in this textbook. This derivation follows from one in a publication included in that collection [16]. [Pg.446]

Pascal s law states that the pressure in a static fluid is the same in all directions. This condition is different from that for a stressed solid in static equilibrium. In such a solid, the stress on a plane depends upon the orientation of that plane, A liquid m contact with the atmosphere is sometimes called a free surface. A static liquid has a horizontal free surface if gravity is the only type of force acting. [Pg.1367]

As the title suggests, in this chapter we stress solid materials and films. Therefore, special concerns related to fluids or biological specimens are not addressed [9], We cover the most commonly applicable methods that the... [Pg.380]

Steinicke and Linke [17] refer to several microscopic and macroscopic states of mechanically stressed solids. Short time effects can be described by stochastic means or nonequilibrium thermodynamics. Long-lasting effects can be measured by calorimetry. The chemical potential and activity of the stressed solid can be measured depending on the induced defects. These defects include ... [Pg.408]

A. Venkateswaran and D. P. H. Hasselman. Elastic Creep of Stressed Solids due to Time-Dependent Changes in Elastic Properties, J. Mater. Sci., 16, 1627-1632 (1981). [Pg.159]

Figire 17.16. Applied oscillatory, sinusoidal stress (solid), and sample response strain for pure solid (long dash) (A), pure liquid (short dash) (B) and a viscoelastic material (long short dash). The phase angle (< )) is the raw single used to determine G and G". [Pg.391]

Corticotropin- CRH-RI and 41-residue peptide Involved in stress Solid-phase... [Pg.2182]

In the rest of this chapter, we will discuss briefly the theoretical ideas and the models employed for the study of failure of disordered solids, and other dynamical systems. In particular, we give a very brief summary of the percolation theory and the models (both lattice and continuum). The various lattice statistical exponents and the (fractal) dimensions are introduced here. We then give brief introduction to the concept of stress concentration around a sharp edge of a void or impurity cluster in a stressed solid. The concept is then extended to derive the extreme statistics of failure of randomly disordered solids. Here, we also discuss the competition between the percolation and the extreme statistics in determining the breakdown statistics of disordered solids. Finally, we discuss the self-organised criticality and some models showing such critical behaviour. [Pg.4]

As the fracture propagates, the elastic energy released due to the micro-fractures occurring within the sample can be measured. This ultrasonic emission due to micro-fracture aftershock relaxation has recently been measured for various laboratory samples. Petri et al (1994) measured the ultrasonic emission amplitude distribution in a large number of stressed solid samples under different experimental conditions. A power law decay for the cumulative energy release distribution n Er) with the released energy amplitude Er was observed in all cases n Er) E (see Fig. 3.21). This is indeed very similar to the Guttenberg-Richter law for the frequency distribution of earthquakes, as discussed briefly in Chapter 1, and will be discussed in detail in the next chapter. [Pg.126]

The numerical approach presented in this paper allows one to calculate the distribution of hydrogen in stressed solids with limited expenditure of computer resources. Its generalization for the case of stress and strain assisted diffusion is straightforward. [Pg.140]


See other pages where Stressed solid is mentioned: [Pg.59]    [Pg.259]    [Pg.326]    [Pg.326]    [Pg.443]    [Pg.47]    [Pg.332]    [Pg.332]    [Pg.335]    [Pg.336]    [Pg.336]    [Pg.337]    [Pg.339]    [Pg.341]    [Pg.386]    [Pg.84]    [Pg.86]    [Pg.3132]    [Pg.39]    [Pg.2735]   
See also in sourсe #XX -- [ Pg.199 ]




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