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Marginal regime

Fig.22. Evolution of the critical shear rate y at the onset of the marginal regime as a function of the surface density in the grafted surface layer, o, for mP=970 kg mol-1, and mN= 96 kg mol-1. For 0.003 Fig.22. Evolution of the critical shear rate y at the onset of the marginal regime as a function of the surface density in the grafted surface layer, o, for mP=970 kg mol-1, and mN= 96 kg mol-1. For 0.003<a<0.01, y increases linearly with o, indicating an additive effect of the surface chains to the friction, i.e. surface chains contributing to the surface friction independently of each other. Above a surface density of 0.01, a collective behavior of the surface chains shows up...
In terms of shear stresses, the onset of the marginal regime corresponds to the stress... [Pg.351]

In the concentrated and marginal regimes of fig 5,3 a mean-field description, which neglects any spatial fluctuations, is appropriate. In these regimes, the solution is homogeneous and there is no chain-length dependence. Neither does the persistence p of the chains play a role since the Floiy-Huggins expressions do not contain the chain flexibility. This is so because the flexibility is assumed to be the same in the solution and in the reference state, so that p cancels in the entropy difference between the two states. [Pg.621]

For tp > 5 " the strong density fluctuations in the semidilute regime disappear, and in the marginal regime the solution may again be described by a mean-fleld theory, as discussed in 5.2c. [Pg.623]

Actually, we have used the term semidilute in a loose sense here (hence the quotation marks) it denotes neither dilute, nor concentrated. Polymer scientists distinguish a semidilute and a marginal regime. Scaling... [Pg.189]

It should be noted carefully that Pearson s analysis still contains the assumption that instability sets in only by a stationary marginal state, which of course excludes the actual possibility of an oscillatory marginal regime. [Pg.102]

Notation cp = volume fraction, = correlation length, p= C./6, v= excluded volume parameter, 1 - 2x, N= number of bonds per chain, x= Flory-Huggins polymer-solvent interaction parameter, Vc = cross-over from swollen to ideal. Subscripts cr = critical, / = ideal, d = dilute, s = semi-dilute, m = marginal regime, c = concentrated regime, ov= cross-over from dilute to semi-dilute, cp = cross-over from concentrated to phase separated, sm = cross-over from semi-dilute to marginal, me = cross-over from marginal to concentrated. [Pg.151]

Structural analysis of the solid rocket case-grain system using experimentally determined propellant response properties may permit a complete description of the combined stresses and resultant deformations, but a statement expressing the ability of the propellant to withstand these stresses is also required. Such a statement, which relates the physical state at which failure occurs to some material parameters, is called a failure criterion. The criterion for failure permits a prediction of safety margins expected under motor operation and handling and defines the loading regimes where abnormal operations will occur with intolerable frequency. [Pg.227]

As tariffs in the secondary market are market clearing, the owners also collect the full scarcity payments. Hence, the investment incentives should be better than under a marginal cost-pricing regime. The owners rights are pursued, as they are given priority when capacity is scarce, nor are they being inadequately compensated by low tariffs. [Pg.340]


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See also in sourсe #XX -- [ Pg.351 , Pg.354 ]




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