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Evolution law

In conclusion, one should temper the vocabulary of the initial MFC paper It is correct to state that the A-transformatiqn leads to an evolution law similar to Ut (in the mathematical sense) W, = AUtA, but not to a physical... [Pg.33]

The Evolution Law of the Potential Drop Across the Double Layer and the Nature of... [Pg.89]

Nonlinear dynamics deals with the evolution of states in systems that are governed by nonlinear evolution laws. Whenever a system s behavior is decisively influenced... [Pg.90]

The properties characteristic for electrochemical nonlinear phenomena are determined by the electrical properties of electrochemical systems, most importantly the potential drop across the electrochemical double layer at the working electrode (WE). Compared to the characteristic length scales of the patterns that develop, the extension of the double layer perpendicular to the electrode can be ignored.2 The potential drop across the double layer can therefore be lumped into one variable, DL, and the temporal evolution law of DL at every position r along the (in general two-dimensional) electrode electrolyte interface is the central equation of any electrochemical model describing pattern formation.3 It results from a local charge bal-... [Pg.95]

When the fibers do not creep, Bf is simply set to zero. The longitudinal stress azz in the fibers and the matrix are denoted oy and am respectively. To accompany Eqns. (13)—(15), evolution laws for the fiber and the matrix stresses are required. These are... [Pg.310]

The fiber and matrix evolution laws for stress are identical to Eqn. (49) with / = 0 and / = 1, respectively. Being isotropic in the plane, this law suffers from the same deficiencies as the 3-D version regarding the orthotropy of the woven mat and any inequality between the warp and the woof. As before, this could be remedied with an anisotropic version of the law. [Pg.316]

If this is equal to a constant r, then the evolution law controlling the growth dynamics is... [Pg.113]

Obviously, in electrochemical experiments, the first condition is almost always fulfilled. However, the requirement of appropriate feedback mechanisms (i.e., appropriate nonlinear evolution laws) seems to constitute a severe restriction on the possible reaction mechanisms that give rise to pattern formation. From this point of view, it is astonishing that nearly all electrochemical systems exhibit dynamic instabilities. [Pg.2]

The inclusion of fluctuations in the description of nonlinear systems is done by two approaches [50]. On the one hand side one adds fluctuating sources in the nonlinear dynamics, transforming thus the differential equations into stochastic differential equations. The second way is the consideration of probability densities for the considered variables and the formulation of their evolution laws. Both concepts are introduced shortly in the next two subsections. [Pg.8]

We underline that the usage of stochastic methods in many particle physics was initiated by Albert Einstein in 1905 working on heavy particles immersed in liquids and which are thus permanently agitated by the molecules of the surrounding liquid. Whereas Einstein formulated an evolution law for the probability P(r, t) to And the particle in a certain position r at time t Paul Langevin formulated a stochastic equation of motion, i.e. a stochastic differential equation for the time dependent position r t) itself. [Pg.8]

Here we reduced to stationary noise sources. Without loss of generality the mean is set to zero. For the later on considered types of noise this formulation is sufficient to obtain general answers for ensembles and their averages of the stochastic excitable system. Thus we can formulate evolution laws for the probability densities and the other moments. We note that the generalization to cases with more than one noise sources is straightforward and crosscorrelations between the noise source have to be defined. [Pg.9]

For the damage evolution law, a standard normal dissipation schema is employed. In the case of time independent dissipation, the damage evolution law is derived from the damage criterion which is a scalar valued function of the themnodynamic force associated to damage variable. We propose here a simple linear function for damage criterion ... [Pg.497]

DAMAGE EVOLUTION LAW OF THE JOINTED ROCK MASS 4.1 Damage evolution equation of Jointed rock mass under compression and shear... [Pg.766]

Fractures at different stress states have different growth model and a damage evolution law is also established for this case based on the arguments described above. Because the more growth of fractures indicates the more degradation of the rock masses, the damage tensor can be expressed as the following... [Pg.767]

The route followed by the system to aperiodic oscillations is through a cascade of period-doubling bifurcations as described by Feigenbaum (1978) in a totally different context. This illustrates again the universality of nonequilibrium dynamic behaviour in nonlinear systems, regardless of the evolution laws governing these systems. [Pg.505]

The second step is to apply the isothermal model to the thermal cycles T(t) predicted from heat flow analysis. Writing the microstructure evolution law (Eq 10.9) in differential form, this may be integrated directly over the cycle, such that Eq 10.9 is replaced by ... [Pg.209]

In the case of a closed crack (transverse compression), the normal stress traction is assumed to be continuous across the crack face. Hence, the degradation factor d2 = 0 and = 0. Zinoviev s and Puck s assumptions are in good correspondence with the following damage evolution law ... [Pg.42]

Jialin Xu et al. 2004. Study on evolution laws and application of rock strata movement bed-separation. Chinese Journal of Geotechnical Engineering 26(5) 632-636. [Pg.318]

The evolution law of energy of ring-down count rate (shown in Fig. 4(b)) is the same as ring-down count rate. [Pg.1294]

Under different conditions of unloading confining pressure, the evolution law of stress and failure mode of numerical experiments are very similar to laboratory experiments of Marble, this phenomenon shows discrete element numerical experiments could displace the laboratory experiments to some extent. [Pg.1295]


See other pages where Evolution law is mentioned: [Pg.7]    [Pg.13]    [Pg.19]    [Pg.33]    [Pg.127]    [Pg.127]    [Pg.406]    [Pg.143]    [Pg.190]    [Pg.310]    [Pg.201]    [Pg.23]    [Pg.114]    [Pg.730]    [Pg.738]    [Pg.499]    [Pg.765]    [Pg.209]    [Pg.40]    [Pg.40]    [Pg.41]    [Pg.1295]    [Pg.185]    [Pg.189]    [Pg.190]   
See also in sourсe #XX -- [ Pg.19 ]




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