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Constitutive functional

Another generalization uses referential (material) symmetric Piola-Kirchhoff stress and Green strain tensors in place of the stress and strain tensors used in the small deformation theory. These tensors have components relative to a fixed reference configuration, and the theory of Section 5.2 carries over intact when small deformation quantities are replaced by their referential counterparts. The referential formulation has the advantage that tensor components do not change with relative rotation between the coordinate frame and the material, and it is relatively easy to construct specific constitutive functions for specific materials, even when they are anisotropic. [Pg.119]

The referential formulation is translated into an equivalent current spatial description in terms of the Cauchy stress tensor and Almansi strain tensor, which have components relative to the current spatial configuration. The spatial constitutive equations take a form similar to the referential equations, but the moduli and elastic limit functions depend on the deformation, showing effects that have misleadingly been called strain-induced hardening and anisotropy. Since the components of spatial tensors change with relative rigid rotation between the coordinate frame and the material, it is relatively difficult to construct specific constitutive functions to represent particular materials. [Pg.119]

As with any constitutive theory, the particular forms of the constitutive functions must be constructed, and their parameters (material properties) must be evaluated for the particular materials whose response is to be predicted. In principle, they are to be evaluated from experimental data. Even when experimental data are available, it is often difficult to determine the functional forms of the constitutive functions, because data may be sparse or unavailable in important portions of the parameter space of interest. Micromechanical models of material deformation may be helpful in suggesting functional forms. Internal state variables are particularly useful in this regard, since they may often be connected directly to averages of micromechanical quantities. Often, forms of the constitutive functions are chosen for their mathematical or computational simplicity. When deformations are large, extrapolation of functions borrowed from small deformation theories can produce surprising and sometimes unfortunate results, due to the strong nonlinearities inherent in the kinematics of large deformations. The construction of adequate constitutive functions and their evaluation for particular... [Pg.120]

If a motion is specified with satisfies the continuity condition, the velocity, strain, and density at each material particle are determined at each time t throughout the motion. Given the constitutive functions (e, k), c(e, k), b( , k), and a s,k) with suitable initial conditions, the constitutive equations (5.1), (5.4), and (5.11) may be integrated along the strain history of each material particle to determine its stress history. If the density, velocity, and stress histories are substituted into (5.32), the history of the body force at each particle may be calculated, which is required to sustain the motion. Any such motion is termed an admissible motion, although all admissible motions may not be attainable in practice. [Pg.131]

The remainder of this section will be concerned with a particular case in which normality conditions hold. The constitutive equation for the internal state variables (5.11) involves the constitutive function a, and the normality conditions (5.56) and (5.57) involve an unknown scalar factor y. In some circumstances, a may be eliminated and y may be evaluated by using the consistency condition. These circumstances arise if b is nonsingular so that the normality condition in strain space (5.56j) may be solved for k... [Pg.139]

It is the dependence of the spatial constitutive functions on the changing current configuration through F that renders the spatial constitutive equations objective. It is also this dependence that makes their construction relatively more difficult than that of their referential counterparts. If this dependence is omitted, then the spatial moduli and elastic limit functions must be isotropic to satisfy objectivity, and the spatial constitutive equations reduce to those of hypoinelasticity. Of course, there are other possible formulations for the spatial constitutive functions which are objective without requiring isotropy. One of these will be considered in the next section. [Pg.163]

Originally discovered as DNA-binding proteins that mediate interferon signaling, recent data demonstrated that STAT1 can also exert constitutive functions in the nucleus, which do not require STAT activation with tyrosine phosphorylation. Cells lacking STAT1 are... [Pg.668]

For reasons that are not yet clear, skeletal muscle transverse (T)-tubule membranes contain 50-100-fold more high affinity DHP receptors than any other source yet identified [43,45]. Transverse tubule membranes contain 30-70 pmol/mg protein of DHP receptors that bind [ H]PN 200-100 with a of 0.1-0.2nM. The strategy utilized for the purification of L-type channels was similar to that used for the purification of other high affinity ligand binding proteins, and its success was predicted from the prior use of such an approach for the purification of other ion channels [54,55]. Thus the L-type channels were purified as high affinity DHP receptors, with the anticipation that the purified component(s) would constitute functional Ca channels. [Pg.320]

ADMET Predictor Constitutional, functional group counts, topological, E-state, Moriguchi descriptors, Meylan flags, molecular patterns, electronic properties, 3D descriptors, hydrogen bonding, acid-base ionization, empirical estimates of quantum descriptors 297... [Pg.35]

The constitutive equations use a thermodynamic framework, that in fact embodies not only purely mechanical aspects, but also transfers of masses between the phases and diffusion of matter through the extrafibrillar phase. Since focus is on the chemo-mechanical couplings, we use experimental data that display different salinities. The structure of the constitutive functions and the state variables on which they depend are briefly motivated. Calibration of material parameters is defined and simulations of confined compression tests and of tree swelling tests with a varying chemistry are described and compared with available data in [3], The evolution of internal entities entering the model, e.g. the masses and molar fractions of water and ions, during some of these tests is also documented to highlight the main microstructural features of the model. [Pg.168]

A similar result has been proven by Hakim [39] for a cleiss of White-Metzner models (still with e < 1) under suitable assumptions on the constitutive functions A(II) and t (I1). These assumptions are satisfied in particular by the Carreau smd the Gaidos-Darby laws [40]. [Pg.209]

A similar result for White-Metzner models is proven in [25] under the same hypotheses on the constitutive functions as for the local existence result mentioned earlier, plus the hypothesis x) < M, for all x in R+. [Pg.211]

Figure 1. Representative polyoxometalates in polyhedral notation. A. the isopolyanion decatungstate (Wio032 ) (C>4h point group symmetry) and B. the heteropolyanion family, (TM)PWii039 , where TM is a first row divalent transition metal ion, P is the heteroatom (Cs point group symmetry). In the latter class of complexes, which constitute functional oxidatively resistant inorganic metalloporphyrin analogs, P is one of many elements that can function as the heteroatom. The darker octahedron on the surface and the veiy dark internal tetrahedron of B represent the TM ion and the heteroatom, respectively. In polyhedral notation a complementary notation to ball-and-stick or bond representations, the vertices of the polyhedra, principally W06 octahedra, are the nuclei of the oxygen atoms. The metal atoms lie inside each polyhedron. Figure 1. Representative polyoxometalates in polyhedral notation. A. the isopolyanion decatungstate (Wio032 ) (C>4h point group symmetry) and B. the heteropolyanion family, (TM)PWii039 , where TM is a first row divalent transition metal ion, P is the heteroatom (Cs point group symmetry). In the latter class of complexes, which constitute functional oxidatively resistant inorganic metalloporphyrin analogs, P is one of many elements that can function as the heteroatom. The darker octahedron on the surface and the veiy dark internal tetrahedron of B represent the TM ion and the heteroatom, respectively. In polyhedral notation a complementary notation to ball-and-stick or bond representations, the vertices of the polyhedra, principally W06 octahedra, are the nuclei of the oxygen atoms. The metal atoms lie inside each polyhedron.
In (3.118), the concise form of writing of several constitutive equations with the same variables was used, i.e., here T stands for constitutive functions s, u, q, T respectively (overhead symbol differs function from its value rare exclusion, see, e.g., Sect. 3.2). Because the response as well as the independent variables are functions of X and t, we add in (3.118) also explicit dependence on these quantities. In formulation of constitutive equations (3.118) the constitutive principle of equipresence was used in all constitutive equations (3.118) we used the same independent variables. This prevents the unjustified preference of some of such equations it is a rather plausible rule, cf. Rem. 25, Sect. 2.1, which in special cases, e.g. [28, 60], may be left. [Pg.100]

We also note that the vector or tensor responses (3.187), (3.189) depend only on the vector or tensor driving forces respectively. This fact is known in linear irreversible thermodynamics as the Curie principle [36, 80, 88, 89] (cf. discussion in [34, 38]). Present theory shows however, that this property follows from the isotropy of constitutive functions and from the representation theorems of such linear functions, see Appendix A.2, Eqs.(A.ll)-(A.13) and (A.57)-(A.59). But representation theorems for nonlinear isotropic constitutive functions [64, 65] show that the Curie principle is not valid generally. [Pg.121]

We calculate derivatives of constitutive functions (denoted by hat) needed in (A.130)-(A.133)... [Pg.304]

At finite times, the network yields under the presence of a stress, cr. Using a constitutive function with an appropriate memory function [54], Brochard and de Gennes showed that the viscous yield occurred in a finite time of the order of the reptation time of the polymer. The important parameter arising out of this analysis is 1, defined as... [Pg.185]

The main idea that I am challenging is that a regularity theory should try to accommodate functional events as causes. Thus, I myself would not object to Melnyk s account of causation on the grounds that it renders functional events epiphenomena. I would recommend not countenancing functional events — events with constitutive functional properties. Even if quantification is a property-forming operation, there seems to me no good reason to think that it is an event-forming one. [Pg.97]


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See also in sourсe #XX -- [ Pg.17 , Pg.18 ]




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