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Solution regularity

Denote next by Rs x ) the ball of the radius 5 centred at the point x. The following assertion holds. [Pg.100]

Theorem 2.12. Let the above hypotheses be fulfilled. Then the inclusions take place for 5 small enough. [Pg.100]

Choose a smooth function such that = 1 in Rs x ), = Q [Pg.100]

Let us notice the following. Assuming that a function p 0 on F, n O(x ), it is easy to check that with the above function ip the relation [Pg.100]

Bearing in mind this fact the vector t = w, w, Wr) is easily proved to satisfy the restriction (2.111) that is, [Pg.101]


In this chapter we analyse a wide class of equilibrium problems with cracks. It is well known that the classical approach to the crack problem is characterized by the equality type boundary conditions considered at the crack faces, in particular, the crack faces are considered to be stress-free (Cherepanov, 1979, 1983 Kachanov, 1974 Morozov, 1984). This means that displacements found as solutions of these boundary value problems do not satisfy nonpenetration conditions. There are practical examples showing that interpenetration of crack faces may occur in these cases. An essential feature of our consideration is that restrictions of Signorini type are considered at the crack faces which do not allow the opposite crack faces to penetrate each other. The restrictions can be written as inequalities for the displacement vector. As a result a complete set of boundary conditions at crack faces is written as a system of equations and inequalities. The presence of inequality type boundary conditions implies the boundary problems to be nonlinear, which requires the investigation of corresponding boundary value problems. In the chapter, plates and shells with cracks are considered. Properties of solutions are established existence of solutions, regularity up to the crack faces, convergence of solutions as parameters of a system are varying and so on. We analyse different constitutive laws elastic, viscoelastic. [Pg.69]

In what follows we prove the solution regularity in a neighbourhood of points belonging to the crack faces and not having contact with the punch. Let a ° G be any fixed point such that w x ) > moreover,... [Pg.102]

The crack shape is defined by the function -ip. This function is assumed to be fixed. It is noteworthy that the problems of choice of the so-called extreme crack shapes were considered in (Khludnev, 1994 Khludnev, Sokolowski, 1997). We also address this problem in Sections 2.4 and 4.9. The solution regularity for biharmonic variational inequalities was analysed in (Frehse, 1973 Caffarelli et ah, 1979 Schild, 1984). The last paper also contains the results on the solution smoothness in the case of thin obstacles. As for general solution properties for the equilibrium problem of the plates having cracks, one may refer to (Morozov, 1984). Referring to this book, the boundary conditions imposed on crack faces have the equality type. In this case there is no interaction between the crack faces. [Pg.110]

The properties of the constructed measures p and 7 depend largely on the solution regularity. We thus prove some statements. [Pg.153]

The arguments given below are concerned with a justification of C °°-regularity of the solution for the crack of zero opening. We shall prove the solution regularity in the neighbourhood of the line x (0,t°), where = (0,0), > 0, i.e. in the vicinity of the crack tip. The solution... [Pg.182]

We prove the existence of the solution and state additional qualitative properties - in particular, a solution regularity near the crack faces and near the external boundary. The results of this section are obtained in (Khludnev, 1997c). [Pg.185]

The above boundary conditions hold provided that the solution rj = (x, ) is sufficiently smooth. We shall use only a part of the conditions (3.69), (3.70) to prove the solution regularity. [Pg.193]

The considered problem is formulated as a variational inequality. In general, the equations (3.140)-(3.142) hold in the sense of distributions. In addition to (3.143), complementary boundary conditions will be fulfilled on F, X (0,T). The exact form of these conditions is given at the end of the section. The assumption as to sufficient solution regularity requires the variational inequality to be a corollary of (3.140)-(3.142), the initial and all boundary conditions. The relationship between these two problem formulations is discussed in Section 3.4.4. We prove an existence of the solution in Section 3.4.2. In Section 3.4.3 the main result of the section concerned with the cracks of minimal opening is established. [Pg.212]

In the book, two- and three-dimensional bodies, plates and shells with cracks are considered. Properties of solutions are established existence of solutions, regularity up to the crack faces, convergence of solutions as parameters of a system are varying and so on. We analyse different constitutive laws elastic, thermoelastic, elastoplastic. The book gives a new outlook on the crack problem, displays new methods of studying the problems and proposes new models for cracks in elastic and nonelastic bodies satisfying physically suitable nonpenetration conditions between crack faces. [Pg.393]

In the first category of solutions ( regular solutions ), it is the enthalpic contribution (the heat of mixing) which dominates the non-ideality, i.e. In such solutions, the characteristic intermolecular potentials between unlike species differ significantly from the average of the interactions between Uke species, i.e. [Pg.48]

Figures 4b and 4c show that neither unconstrained nor non-negative maximum likelihood approaches are able to recover a usable image. Deconvolution by unconstrained/constrained maximum likelihood yields noise amplification — in otfier words, the maximum likelihood solution remains iU-conditioned (i.e. a small change in the data due to noise can produce arbitrarily large changes in the solution) regularization is needed. Figures 4b and 4c show that neither unconstrained nor non-negative maximum likelihood approaches are able to recover a usable image. Deconvolution by unconstrained/constrained maximum likelihood yields noise amplification — in otfier words, the maximum likelihood solution remains iU-conditioned (i.e. a small change in the data due to noise can produce arbitrarily large changes in the solution) regularization is needed.
Figure 8. Free enthalpy of mixing G of binary solid solutions (regular) Ca,. (PO ) OH F as a function of x at W/2.303 RT = 1.4. Figure 8. Free enthalpy of mixing G of binary solid solutions (regular) Ca,. (PO ) OH F as a function of x at W/2.303 RT = 1.4.
Non-Ideal Solutions Regular and Non-Regular Solution Models... [Pg.8]

The system of equations (4) has two fundamental solutions. We are interested in the solution regular at r—>0. Boundary values of the correct solution are found from the first terms of the expansion into a Taylor series ... [Pg.288]

The most popular chemical theory postulates stoichiometric chemical species that interact accordingly as a regular solution (regular associated-solution model). The associated-solution model is based usually on the following assumptions ... [Pg.162]

To preserve the contact time r = 10 s, the molar ratio of reagents was varied by changing hydrogen peroxide concentration in the initial aqueous solution. Regularities observed from curves in Figure 7.29 can be explained in the framework of catalase and monooxygenase conjugation ideas (see above). [Pg.271]

A radial wave function is normalized so that (u u) = /0°° u (r)u(r)dr = 1. A solution regular at the origin must have the form... [Pg.40]

Morphine is available for oral, rectal, and parenteral administration. Oral formulations include immediate and controlled release tablets, as well as oral solution regular strength and concentrate. Parenterally, it can be administered subcutaneously, intramuscularly, intravenously, or by continuous infusion. It is a drug of abuse and can be nasally insufflated. [Pg.1742]

The standard curve (calibration graph, analytical curve, calibration curve), relating the absorbance to the analyte concentration, is prepared by applying the colour reaction procedure to a set of standard solutions, regularly spaced over a concentration range that will give a maximum absorbance of 0.8-1.0. The conditions specified in the analytic procedure must be strictly adhered to. The curve is plotted with the scale arranged so that the curve is at about 45° to the abscissa, as shown in Fig. 3.1. [Pg.48]

To obtain a more accurate solution, regular solution theory will now be used to compute the y s... [Pg.449]

Symmetric, siightty non-ideal binary solutions ( Regular )... [Pg.395]

The van Laar argument for heat of solution (regular solutions) makes it possible to arrive at an expression for the heat of mixing of a polymer with solvent in which is a dimensionless parameter relating the difference in energy between solvent molecules when immersed in pure polymer and in pure solvent ... [Pg.50]

A second very important physicochemical property of insulin related to iontophoresis is its solubility. As is seen in Fig. 2, the rate of delivery is directly proportional to the molar concentration of the insulin in solution. Regular insulins that are marketed for the treatment of diabetes are available at a concentration of 100 units/ml, or 4 mg/ml. A higher molar concentration will, in principle (see Fig. 2), result in a higher flux, enabling the iontophoresis system to mn at a lower current. [Pg.337]


See other pages where Solution regularity is mentioned: [Pg.100]    [Pg.107]    [Pg.112]    [Pg.115]    [Pg.153]    [Pg.180]    [Pg.181]    [Pg.189]    [Pg.238]    [Pg.106]    [Pg.112]    [Pg.131]    [Pg.197]    [Pg.631]    [Pg.414]    [Pg.559]    [Pg.1322]    [Pg.197]    [Pg.168]   


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Regular solutions

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