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Gradient theory

IHP) (the Helmholtz condenser formula is used in connection with it), located at the surface of the layer of Stem adsorbed ions, and an outer Helmholtz plane (OHP), located on the plane of centers of the next layer of ions marking the beginning of the diffuse layer. These planes, marked IHP and OHP in Fig. V-3 are merely planes of average electrical property the actual local potentials, if they could be measured, must vary wildly between locations where there is an adsorbed ion and places where only water resides on the surface. For liquid surfaces, discussed in Section V-7C, the interface will not be smooth due to thermal waves (Section IV-3). Sweeney and co-workers applied gradient theory (see Chapter III) to model the electric double layer and interfacial tension of a hydrocarbon-aqueous electrolyte interface [27]. [Pg.179]

Mundt, E. 1 992. Convection flows in rooms with temperature gradients Theory and measurements. In Roomvent 92 Proceedings of the Third International Conference on Air Distrihii-tion in Rooms, vol. 3. Aalborg, Denmark. [Pg.541]

Righetti, P.G., Immobilized pH Gradients Theory and Methodology, Elsevier, Amsterdam, 1990. [Pg.159]

This salt-gradient theory deserves further attention. It is possible that the concepts may be applicable to vapor explosions in different industries. [Pg.143]

One experiment which does not seem to fit into the network of the salt-gradient theory was that of Wright and Humberstone (1966), who impacted water on molten aluminum and obtained explosions. These results are at variance with those of Anderson and Armstrong, but the latter worked at 1 bar whereas the former used a vacuum environment. It might be possible that, under vacuum, it is much easier to achieve intimate contact between the aluminum and water and, under these conditions, there may be sufficient reaction between the aluminum and water to allow soluble aluminum salts to form. This salt layer could then form the superheated liquid which is heated to the homogeneous nucleation temperature and explodes. [Pg.181]

O Farrel PH (1975) J Biol Chem 250 4007 Dunn MJ, Burghes AHM (1983) Electrophoresis 4 97 4 173 Gorg A, Postel W, Gunther S (1988) Electrophoresis 9 531 Righetti PG (1990) Immobilized pH gradients theory and methodology. Laboratory techniques in biochemistry and molecular biology, vol. 20, Elsevier, Amsterdam... [Pg.45]

Once the free energy of an inhomogeneous system is given, one can calculate by standard methods the properties of the interface—for example, the interfacial tension or the density profile perpendicular the interface [285]. Weiss and Schroer compared the various approximations within square-gradient theory discussed earlier in Section IV.F for studying the interfacial properties for pure DH and FL theory [241, 242], In theories based on local density approximations the interfacial thickness and the interfacial tension were found to differ by up to a factor of four in the various approximations. This contrasts with nonionic fluids, where the density profiles and interfacial... [Pg.46]

We analyze, within a linearized second gradient theory, the static infinitesimal deformations of an annular porous cylinder filled with an inviscid fluid and with the inner and the outer surfaces subjected to uniform external pressures pj xt and iff1 respectively. We assume that surface tractions on the inner and the outer surfaces of the cylinder, in the reference configuration, equal -po and postulate that... [Pg.225]

PG Righetti. Immobilized pH gradients theory and methodology. Lab Tech Bio-chem Mol Biol 20, 1990. [Pg.595]

Rapid chromatographic reactions may be accounted for as in the case of the small gradient theory. This and charge neutrality lead to... [Pg.191]

Cowan and coworkers (4 ) in the theory of neuronal interactions in the brain. These equations have been shown to yield a great variety of self-organizing phenomena and hence such phenomena are certain to arise in the present theory. Finally we note that in the limit of small R the theory reduces to the small gradient theory. In the section°on bioelectric patterning we shall demonstrate some aspects of self-organization in this model. [Pg.192]

Imposed Field Effects. In this section we have set forth a set of equations to describe pattern formation in a multicellular electrophysiological system. A central goal of the theory is to study the effects of applied electric fields. This is done by imposing appropriate boundary conditions on the equations developed here. For example, assume we subject a one dimensional tissue to fixed ionic currents 1. Then if the tissue is in the interval 0 x along the x axis, the boundary conditions for the electro-diffusion model of the small gradient theory, i.e. (6k), are replaced by J = I at x = 0, L. One expects the richness of effects to include hyperpolarizability, induction of new phenomena and imperfect bifurcations to be found in these systems... [Pg.198]

Isoelectric Focusing in Immobilized pH Gradients Theory and Newer Technology... [Pg.255]

A gradient theory that predicts the Frank constants was proposed by Nehring and Saupe (1972), Priest (1973), and Straley (1973). There have been many modifications and... [Pg.459]

Keeler, J. Clowes, R.T. Davis, A.L. Laue, E.D. Pulsed field gradients theory and practice. Methods Enzymol 1994, 239, 145-207. [Pg.3458]

P. G. Righetti, Immobilized pH Gradients Theory and Methodology, Elsevier, New York, 1990. N. Catsimpoolas and J. Drysdale, Biological and Biomedical Applications of Isoelectric Focusing, Plenum Press, New York, 1977. [Pg.225]

Mitlin, V.S., and M.M. Sharma. 1993. A local gradient theory for structural forces in thin fluid films. J. Colloid Interface Sci. 157 447-464. [Pg.49]

First-order electrical properties can conveniently be determined from expressions derived by using gradient theory. The Hamiltonian is augmented with an operator representing the studied property. By calculating the first derivative of the total energy with respect to the strength parameter of the property operator, one obtains an expression for the calculation of the specified first-order property. [Pg.771]

The generalization of the interchange theorem [103] to the correlation problem is what makes CC analytical gradient theory viable, and, indeed, routine today. Also, the introduction of the response and the relaxed density matrices provides the non-variational CC generalizations of density matrix theory that makes it almost as easy to evaluate a property as with a normal expectation value. They are actually more general, since they apply to any energy expression whether or not it derives from a wavefunction This is essential, e.g. for CCSD(T). The difference is that we require a solution for both T and A if we want to use untruncated expressions for properties, as is absolutely necessary to define proper critical points. It is certainly true that... [Pg.1206]


See other pages where Gradient theory is mentioned: [Pg.458]    [Pg.286]    [Pg.263]    [Pg.280]    [Pg.565]    [Pg.180]    [Pg.181]    [Pg.514]    [Pg.26]    [Pg.222]    [Pg.54]    [Pg.187]    [Pg.244]    [Pg.460]    [Pg.133]    [Pg.163]    [Pg.189]    [Pg.676]    [Pg.323]    [Pg.308]    [Pg.1236]   
See also in sourсe #XX -- [ Pg.194 , Pg.197 , Pg.214 ]

See also in sourсe #XX -- [ Pg.38 ]

See also in sourсe #XX -- [ Pg.2 ]




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