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Frequency values

Frequency Phase 3 Use Branch Point Estimates to Develop a Ere-quency Estimate for the Accident Scenarios. The analysis team may choose to assign frequency values for initiating events and probability values for the branch points of the event trees without drawing fault tree models. These estimates are based on discussions with operating personnel, review of industrial equipment failure databases, and review of human reliability studies. This allows the team to provide initial estimates of scenario frequency and avoids the effort of the detailed analysis (Frequency Phase 4). In many cases, characterizing a few dominant accident scenarios in a layer of protection analysis will provide adequate frequency information. [Pg.40]

Fig. 8. Summary of real and imaginary e2(tu) parts of the dielectric function for Cgo vacuum-sublimed solid films at room temperature over a wide frequency range, using a variety of experimental techniques. The arrow at the left axis points to i = 4.4, the observed low frequency value of ei obtained from optical data [81]. Fig. 8. Summary of real and imaginary e2(tu) parts of the dielectric function for Cgo vacuum-sublimed solid films at room temperature over a wide frequency range, using a variety of experimental techniques. The arrow at the left axis points to i = 4.4, the observed low frequency value of ei obtained from optical data [81].
Cumulati ve frequencies Accumulated sums of frequency values in a frequency distribution. [Pg.1426]

In the inset of Fig. 9 we show the mean field frequency 0 = 0// as a function of density for T = 1. At this temperature the system undergoes a phase transition from a paramagnetic to a ferromagnetic fluid at a density whose mean field value is p mf = 0-4- For densities below this value we obtain 0 = cjq, which agrees with the frequency value of the low-order virial expansion (see Eq. (34)). For p > Pc,mF) increases with the density due to increase of the magnetization. [Pg.104]

Raw frequency values computed at the Hartree-Fock level contain known systematic errors due to the neglect of electron correlation, resulting in overestimates of about 10%-12%. Therefore, it is usual to scale frequencies predicted at the Hartree-Fock level by an empirical factor of 0.8929. Use of this factor has been demonstrated to produce very good agreement with experiment for a wide range of systems. Our values must be expected to deviate even a bit more from experiment because of our choice of a medium-sized basis set (by around 15% in all). [Pg.63]

If applicable, the program notes that there is an imaginary frequency present just prior to the frequency and normal modes output, and the first frequency value is less than zero. Log files may be searched for this line as a quick check for imaginary frequencies. [Pg.70]

All in all, B3LYP performs best on this problem of all of the model chemistries we have considered. It provides good structural and qualitative frequency predictions, although its computed frequency values are only fair. ... [Pg.135]

Frequenz, /. frequency crowd attendance traffic, -messer, m. frequency meter, wave-meter, ondometer. -wert, m. frequency value, frequency. [Pg.164]

Figures 5.29a and 5.29b show the Bode and Nyquist plot for a resistor, Ro, connected in series with a resistor, Rt, and capacitor, Ci, connected in parallel. This is the simplest model which can be used for a metal-solid electrolyte interface. Note in figure 5.29b how the first intersect of the semicircle with the real axis gives Ro and how the second intersect gives Ro+Rj. Also note how the capacitance, Ct, can be computed from the frequency value, fm, at the top of the semicircle (summit frequency), via C l JifmR . Figures 5.29a and 5.29b show the Bode and Nyquist plot for a resistor, Ro, connected in series with a resistor, Rt, and capacitor, Ci, connected in parallel. This is the simplest model which can be used for a metal-solid electrolyte interface. Note in figure 5.29b how the first intersect of the semicircle with the real axis gives Ro and how the second intersect gives Ro+Rj. Also note how the capacitance, Ct, can be computed from the frequency value, fm, at the top of the semicircle (summit frequency), via C l JifmR .
Normal coordinate analysis of the radical has been carried out and excellent agreement of experimental and calculated frequency values was obtained for the trans structure of HOCO. [Pg.37]

Divide G(v) by H(v) at corresponding frequency values (aecording to the rules for the division of two complex numbers), which gives F(v)... [Pg.554]

Regardless of the force field chosen, the calculation of vibrational frequencies by the method outlined above is based on the harmonic approximation. Tabulated values of force constants can be used to calculate vibrational frequencies, for example, of molecules whose vibrational spectra have not been observed. However, as anharmonicities have been neglected in the above analysis, the resulting frequency values are often no better than 5% with respect to those observed. [Pg.123]

All types of waves, whether longitudinal or transverse, can be accurately described by their wavelength and frequency values (see Fig. 6), which are mathematically related to each other by the expression vX = c, where the Greek letter X (lambda) is the wavelength, the Greek letter v (nu) is the frequency of the wave, and c is the velocity of the wave. [Pg.41]

The cross-peak coordinates represent two frequency values, va and vp, where va + vp=2v, and v is the proton frequency. When plotted in the coordinates v2a and v2p, the contour lineshape is transformed into a straight line segment. An extrapolation of this straight line permits the determination of the hyperfine tensors. A curve obtained by choosing some frequencies in the range will intersect the line defined by the squares of the values v2a and v2p in two points. The values where the curve intersects the experimental data are (val, vpi) and (va2, vp2), where va=A/2 + v, and vp= Vj-A/2. This gives two values of the anisotropic coupling tensor, Ar... [Pg.174]

With the addition of a pseudopotential interaction between electrons and metal ions, the density-functional approach has been used82 to calculate the effect of the solvent of the electrolyte phase on the potential difference across the surface of a liquid metal. The solvent is modeled as a repulsive barrier or as a region of dielectric constant greater than unity or both. Assuming no specific adsorption, the metal is supposed to be in contact with a monolayer of water, modeled as a region of 3-A thickness (diameter of a water molecule) in which the dielectric constant is 6 (high-frequency value, appropriate for nonorientable dipoles). Beyond this monolayer, the dielectric constant is assumed to take on the bulk liquid value of 78, although the calculations showed that the dielectric constant outside of the monolayer had only a small effect on the electronic profile. [Pg.60]

We have seen in Chapter 2 that the frequency of an EPR spectrum is not a choice for the operator (once the spectrometer has been built or bought) as it is determined by the combined fixed dimensions of the resonator, the dewar cooling system, and the sample. Even if standardized sample tubes are used and all the samples have the same dielectric constant (e.g., frozen dilute aqueous solutions of metalloproteins), the frequency will still slightly vary over time over a series of consecutive measurements, due to thermal instabilities of the setup. By consequence, two spectra generally do not have the same frequency value, which means that we have to renormalize before we can compare them. This also applies to difference spectra and to spectra... [Pg.103]

Since the average reorientation frequency w is far less than the cyclic frequency of valence vibrations ah, expression (A2.8), with measured frequency values at close to coo, can approximately be rewritten as ... [Pg.162]

Table 11-3 Typical Frequency Values Assigned to Initiating Events1 ... Table 11-3 Typical Frequency Values Assigned to Initiating Events1 ...
None of the expected frequency values should be less than 5.0. [Pg.913]

Electrophoresis remained for several decades the most powerful method for demonstrating polymorphism in human proteins. The striking biochemical individuality of human proteins emerged slowly. Harris (1966) demonstrated the existence of many polymorphisms in 3 of 10 enzymes studied in detail. He found an average heterozygosity (in his case the mean fraction of electrophoretically visible allele differences) of 10% in a sample of ethnic Europeans. Later on he extended the set of enzymes and confirmed the range of frequency values. [Pg.410]

If in a DNA or protein sequence a single position is variant, this may be called a polymorphism or mutation. The difference is set by convention a mutation is rare, and a polymorphism is common. By implication, a mutation may be deleterious, or in rare cases it may be advantageous for the reproductive fitness of its carriers. A widespread polymorphism, on the other hand, is unlikely to affect the fitness to such an extent. A frequency value of 1 % of the polymorphic allele is usually taken as a threshold between mutation and polymorphism (Ki-mura, 1983 Li, 1997). A polymorphic site is called biallelic if two variants segregate in the population, and multiallelic if there are more than two variants, which is a rare event in human sequences. [Pg.412]

Then the sum of the magnitudes of the off-diagonal elements in a given row of the Q matrix is calculated at one value of frequency and a circle is drawn with this radius. This is done for several frequency values and for each diagonal... [Pg.580]


See other pages where Frequency values is mentioned: [Pg.298]    [Pg.381]    [Pg.2]    [Pg.194]    [Pg.135]    [Pg.436]    [Pg.461]    [Pg.4]    [Pg.11]    [Pg.13]    [Pg.14]    [Pg.18]    [Pg.28]    [Pg.33]    [Pg.56]    [Pg.238]    [Pg.547]    [Pg.312]    [Pg.68]    [Pg.78]    [Pg.79]    [Pg.80]    [Pg.122]    [Pg.195]    [Pg.492]    [Pg.43]    [Pg.283]    [Pg.90]   
See also in sourсe #XX -- [ Pg.51 ]




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