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Correlations Periodicity

Comparison with the highest possible values of a multivariate random correlation (see also Section 6.6.3) shows a correlation period of approximately two weeks and two days. This means that sampling of suspended dust at intervals of two weeks is sufficient for the characterization of the average impact of multielement emissions (for all investigated elements simultaneously) at that particular sampling point. [Pg.252]

Of importance in using this molecular dynamics technique and other molecular dynamics techniques that utilize periodic boundary conditions are issues with artificially-induced correlations due to the finite size of the computational cell. Artificial phase transitions or other dynamics can be observed when the computational cell dimensions are sufficiently small to allow a particle to interact with its (correlated) periodic image. Artificial effects can be circumvented by making the computational cell sufficiently large that periodic atomic images are separated by a distance greater than the atomic correlation length in the material. [Pg.313]

The first sharp diffraction peak (FSDP) in Figure l-l(a), the position of peaks in the RDF(r) curve which correspond to the interatomic distances, andpeak-to-peak distances in the C(r) curve, which correspond to the correlation periodicity or the size of the repeated structinal unit, are important parameters in order to discuss the MRO of the xerogel and glasses. [Pg.690]

The correlation period T for the integration is taken to be very long (i.e., T oo). The correlation time x may be regarded as an arbitrary time interval between the measurement of two dynamic dichroism signals. For a fixed correlation time, X(x) is is determined by a pair of independent wavenumbers Vi and V2, which allows the dimensionality of the analysis to be reduced from three (as in Figure 21.4) to two. [Pg.450]

Different plant operating conditions (steady load, load variations, startups / shutdowns) have been encountered during the monitoring period. Electrical load, steam pressure and steam temperature values vs time have been acquired and stored during the entire period. At the same time, the RMS values of the acoustical background noise were have been continuously checked and stored, thus providing a quick check of proper instrumentation condition and a correlation between variations of plant parameters and the acoustical behaviour of the components. [Pg.78]

Fig.6 Correlator output versus the peak to peak amplitude of the periodic change in the sum of the principal stresses at the measuring point (R5) for an assigned frequency (5Hz). Fig.6 Correlator output versus the peak to peak amplitude of the periodic change in the sum of the principal stresses at the measuring point (R5) for an assigned frequency (5Hz).
This ionic potential is periodic. A translation of r to r + R can be acconnnodated by simply reordering the sunnnation. Since the valence charge density is also periodic, the total potential is periodic as the Hartree and exchange-correlation potentials are fiinctions of the charge density. In this situation, it can be shown that the wavefiinctions for crystalline matter can be written as... [Pg.101]

Figure C 1.5.10. Nonnalized fluorescence intensity correlation function for a single terrylene molecule in p-terjDhenyl at 2 K. The solid line is tire tlieoretical curve. Regions of deviation from tire long-time value of unity due to photon antibunching (the finite lifetime of tire excited singlet state), Rabi oscillations (absorjDtion-stimulated emission cycles driven by tire laser field) and photon bunching (dark periods caused by intersystem crossing to tire triplet state) are indicated. Reproduced witli pennission from Plakhotnik et al [66], adapted from [118]. Figure C 1.5.10. Nonnalized fluorescence intensity correlation function for a single terrylene molecule in p-terjDhenyl at 2 K. The solid line is tire tlieoretical curve. Regions of deviation from tire long-time value of unity due to photon antibunching (the finite lifetime of tire excited singlet state), Rabi oscillations (absorjDtion-stimulated emission cycles driven by tire laser field) and photon bunching (dark periods caused by intersystem crossing to tire triplet state) are indicated. Reproduced witli pennission from Plakhotnik et al [66], adapted from [118].
Luminol chemiluminescence has also been recommended for measuring bacteria populations (304,305). The luminol—hydrogen peroxide reaction is catalyzed by the iron porphyrins contained in bacteria, and the light intensity is proportional to the bacterial concentration. The method is rapid, especially compared to the two-day period required by the microbiological plate-count method, and it correlates weU with the latter when used to determine bacteria... [Pg.275]

The long latent periods involved in development of cancers make correlation of chemical exposures and disease extremely difficult. This can be countered pardy with tests on naturally short-Hved animals. Tests on bacteria, eg, the Ames test, may permit rapid detection of cancer potential, although there is no direct relationship between the results of bacterial tests and the effects of the tested chemicals on humans (56). [Pg.96]


See other pages where Correlations Periodicity is mentioned: [Pg.40]    [Pg.1399]    [Pg.690]    [Pg.692]    [Pg.329]    [Pg.40]    [Pg.1399]    [Pg.690]    [Pg.692]    [Pg.329]    [Pg.3]    [Pg.79]    [Pg.411]    [Pg.246]    [Pg.595]    [Pg.1324]    [Pg.1407]    [Pg.1408]    [Pg.1409]    [Pg.1409]    [Pg.1509]    [Pg.1769]    [Pg.2219]    [Pg.2227]    [Pg.2242]    [Pg.2305]    [Pg.2493]    [Pg.11]    [Pg.298]    [Pg.443]    [Pg.460]    [Pg.408]    [Pg.415]    [Pg.434]    [Pg.379]    [Pg.384]    [Pg.530]    [Pg.101]    [Pg.134]    [Pg.134]    [Pg.413]    [Pg.8]    [Pg.245]    [Pg.221]    [Pg.154]    [Pg.474]   
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