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Logarithmic integral function

FIGURE 15.B.1 Plot of the real part of the logarithm integral function, Re[h(z)] vs. z, from Soldner s constant. [Pg.381]

The inverse hyperbolic functions, sinh" x, etc., are related to the logarithmic functions and are particularly useful in integral calculus. These relationships may be defined for real numbers x and y as... [Pg.33]

The expression given for X as a function of C leaves us in trouble at both ends of the diffusion profile. X appropriately tends towards + oo and - oo when CCe tends asymptotically towards —0.05 and 1.93, respectively, which are nearly the extreme concentrations in the profile. This is what we expect from an infinite system. However, the integrals of the rational fractions are simply natural logarithms which cannot be evaluated for a zero argument and therefore do not converge when evaluated between C0 and Cl. We will therefore restrict the calculation to the interval between extreme concentrations, say C0 = 1.865 and = 0.012. The flux at both ends will not be strictly zero, since for these values,... [Pg.427]

Figure 26. Dimerization of butadiene in the crystalline phase. Lower panel Logarithmic plots of the room-temperature evolution of the integrated absorption of characteristic vinylcyclohexene absorption bands at different pressures. The linear evolution unambiguously demonstrates the first-order kinetics of the reaction. Upper panel Evolution of the natural logarithm of the dimerization rate constant as a function of pressure (full squares, left axis the dotted line is intended as a guide for the eye) and evolution of the intensity ratio between selected polymer and dimer (vinylcyclohexene) bands (empty dots, right axis). Figure 26. Dimerization of butadiene in the crystalline phase. Lower panel Logarithmic plots of the room-temperature evolution of the integrated absorption of characteristic vinylcyclohexene absorption bands at different pressures. The linear evolution unambiguously demonstrates the first-order kinetics of the reaction. Upper panel Evolution of the natural logarithm of the dimerization rate constant as a function of pressure (full squares, left axis the dotted line is intended as a guide for the eye) and evolution of the intensity ratio between selected polymer and dimer (vinylcyclohexene) bands (empty dots, right axis).
Equation (1.15) has been integrated numerically on a logarithmic scale to determine the dummy variable The logarithmic scale weighs more uniformly the relaxation times, which may cover several orders of magnitude. A change of variables, y = n (k = ln(T g/T ), transformed the distribution function given by... [Pg.23]

The actual decrease of the total number of particles of a dispersion coagulating under orthokinetic conditions is described by a logarithmic function obtained from the integration of Equation 5 ... [Pg.113]

The form of the function / is such that the integral diverges logarithmically when the lower limit approaches pmax from above ... [Pg.91]

Fig. 42 Ratio R p/Rgi as a function of the interaction parameter x in a semi-logarithmic scale for the 127-unit alternating and protein-like chains in the corresponding multichain systems. The parameter x is similar to the Flory-Huggins interaction parameter X and characterizes solvent quality in an integral manner. Sufficiently large values of x (X > 1) correspond to a poor solvent. Solvent quality becomes poorer with decreasing temperature or with increasing x. Adapted from [212]... Fig. 42 Ratio R p/Rgi as a function of the interaction parameter x in a semi-logarithmic scale for the 127-unit alternating and protein-like chains in the corresponding multichain systems. The parameter x is similar to the Flory-Huggins interaction parameter X and characterizes solvent quality in an integral manner. Sufficiently large values of x (X > 1) correspond to a poor solvent. Solvent quality becomes poorer with decreasing temperature or with increasing x. Adapted from [212]...
For homogeneous boundary conditions, the logarithmic derivatives f[ /f and fj/f2 are equal at both end-points xo, xi. Hence the integrated term vanishes, and the differential expression L[f] is self-adjoint with these boundary conditions. The weighting function p can be eliminated by converting to u = p - f. Then A[m] = (Pit ) — Qu, where... [Pg.37]

One of the two integrals (4.67) may be evaluated analytically the second one (elliptic) may be calculated numerically by the trapezoidal method with the introduction of a small imaginary part in (4.67) to avoid spurious oscillations due to the finite number of integration points. The resulting density-of-states function is shown in Fig. 4.9. The band is asymmetric because of the equivalent term Vx j it exhibits three van Hove singularity points two discontinuities at the boundaries, and one logarithmic divergence corres-... [Pg.206]


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See also in sourсe #XX -- [ Pg.376 , Pg.380 ]




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