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Relaxation equations parameters

In order to compute absolute rate constant values from photostationary parameters such as yp, yg, and [M]i/2, it is necessary to obtain independent measurements of the over-all decay constants l/rf and 1/rp of the emitting species (cf. Eqs. 4 and 12). In the absence of photoassociation ([M] [M] ) the appropriate relaxation equation for the 2-state system... [Pg.178]

One can assume that the anisotropy of the relaxation process can be neglected. This means that, in relaxation equation (9.49), we equate to zero the parameter [3, but retain the parameter k, so that the set of constitutive equations can be rewritten as follows... [Pg.191]

Brace et al. [92] investigated polymer/water interactions using SAW devices coated with either polyimide or cellulose acetate butyrate (CAB). In this study thermodynamic parameters were evaluated from the absorption isotherms, and transient responses to step changes in concentration were monitored. The transient responses observed were not consistent with Fickian diffusion, but could be described using a generalized relaxation equation containing two additive terms. Results under various conditions indicated that relaxation in the polymer system is much slower than diffusion of water. [Pg.175]

Tabulated below, and listed in BPA-PC-Rel. TXT in the accompanying CD, are the results of stress relaxation measurements made on bis-phenol A polycarbonate. Construct the master curve and calculate C, and C2, the WLF equation parameters, for a reference temperature of 150.8 °C. [Pg.126]

The new ideas exposed in these studies (and in a few others like them) inspired great activity in the modification of the RK equation parameters a and b were treated as functions of temperature various constraints on the equation were relaxed new ones were added and many extensions to mixture behavior were proposed. This period (1967-1977) may be well remembered as the Redlich-Kwong Decade. In the midst of all this, Soave (13) published a RK variant which appeared to be a great improvement over other versions. Not surprisingly, the idea behind the new variation was a twist on an older one—the one exploited by Wilson in 1964. [Pg.71]

Table 14.13. Physical aging in polymer blends, studied by Stress relaxation, Mijovic equation parameters ... Table 14.13. Physical aging in polymer blends, studied by Stress relaxation, Mijovic equation parameters ...
Both of these forms of the equation can be put into the complex plane notation and analysed to give both an indication of the mean relaxation frequency and the distribution parameters a and p. In both cases in the limit i.e a 0 and p—>1 the equation equals that of the ideal Debye relaxation, equation (ll). [Pg.107]

The inclusion of PY by yCD is characterized by spectral changes and T variations consistent with equilibria analogous to (3) and (4), and a relaxation equation analogous to eqn (5). The derived parameters for both the PB/yCD and PY/yCD appear in Table 1 together with parameters from related systems. [Pg.60]

One special relaxation process is worthy of note this is the glass to rubber transition. Because the movement of the backbone segments depends on the availability of free volume, the temperature dependence is controlled not solely by the activation energy (as was shown in Chapter 4). As a consequence, the Arrhenius plots are curved and the processes are described by a relaxation equation where the parameter a is not unity. [Pg.142]

The methods previously discussed in this chapter can be used to determine the differential equations, solutions and parameters for a number of mechanical models using a variety of combinations of springs and damper elements. Table 5.1 is a tabulation of the differential equation, parameter inequalities, creep compliances and relaxation moduli for frequently discussed basic models. Note that the equations are given in terms of the pj and qj coefficients of the appropriate differential equation in standard format. The reader is encouraged to verify the validity of the equations given and is also referred to Flugge (1974) for a more complete tabulation. [Pg.177]

In these equations parameters Q, and t, are called relaxation amplitudes and relaxation times, respectively. These parameters are obtained via fitting procedures. An efficient deconvolution of the experimental data in a fitting program described by Porschke and Jung allows one to obtain relaxation times with good quality time resolution. [Pg.294]

Of the adjustable parameters in the Eyring viscosity equation, kj is the most important. In Sec. 2.4 we discussed the desirability of having some sort of natural rate compared to which rates of shear could be described as large or small. This natural standard is provided by kj. The parameter kj entered our theory as the factor which described the frequency with which molecules passed from one equilibrium position to another in a flowing liquid. At this point we will find it more convenient to talk in terms of the period of this vibration rather than its frequency. We shall use r to symbolize this period and define it as the reciprocal of kj. In addition, we shall refer to this characteristic period as the relaxation time for the polymer. As its name implies, r measures the time over which the system relieves the applied stress by the relative slippage of the molecules past one another. In summary. [Pg.98]

Various theoretical and empirical models have been derived expressing either charge density or charging current in terms of flow characteristics such as pipe diameter d (m) and flow velocity v (m/s). Liquid dielectric and physical properties appear in more complex models. The application of theoretical models is often limited by the nonavailability or inaccuracy of parameters needed to solve the equations. Empirical models are adequate in most cases. For turbulent flow of nonconductive liquid through a given pipe under conditions where the residence time is long compared with the relaxation time, it is found that the volumetric charge density Qy attains a steady-state value which is directly proportional to flow velocity... [Pg.107]

DNA duplex of 400 bp, L is 40 (assuming 10 bp per turn in B-DNA). The linking number for relaxed DNA is usually taken as the reference parameter and is written as Lq. L can be equated to the twist (T) and writhe (W) of the duplex, where twist is the number of helical turns and writhe is the number of supercoils ... [Pg.376]


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