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Harmonization total

Fig. 1. Total energy (in kj/mol) versus time (in fs) for different integrators for a collinear collision of a classical particle with a harmonic quantum oscillator (for details see [2]). Dashed line Nonsymplectic scheme. Dotted Symplectic integrator of first order. Solid PICKABACK (symplectic, second order). Fig. 1. Total energy (in kj/mol) versus time (in fs) for different integrators for a collinear collision of a classical particle with a harmonic quantum oscillator (for details see [2]). Dashed line Nonsymplectic scheme. Dotted Symplectic integrator of first order. Solid PICKABACK (symplectic, second order).
Three-body and higher terms are sometimes incorporated into solid-state potentials. The Axilrod-Teller term is the most obvious way to achieve this. For systems such as the alkali halides this makes a small contribution to the total energy. Other approaches involve the use of terms equivalent to the harmonic angle-bending terms in valence force fields these have the advantage of simplicity but, as we have already discussed, are only really appropriate for small deviations from the equilibrium bond angle. Nevertheless, it can make a significant difference to the quality of the results in some cases. [Pg.257]

The presentation will focus on the differences and similarities of these systems as well as problems encountered in their practical use. By looking at the analytical process chain characteristics, such as the reliability and traceability of data, documentation standards and total costs of QM are discussed and evaluated. Suggestions for harmonization of QM-Systems and reduction of bureaucracy will be made, resulting in an improvement of the overall practical applicability and cost reduction of QM. [Pg.13]

The greatest effect of ageing is reflected by the variation in its resistive current, which is rich in the third harmonic. Variation in is used in assessing the condition of an arrester. By conducting laboratory tests to determine the characteristics of an arrester, we can establish a ratio between the total leakage current, IZnO and the content of If, to assess the condition of the arrester. If we can monitor this current, we can monitor the condition of the arrester. Below we discuss briefly one such method by which this component can be separated out. [Pg.618]

Table 23.2 Premissible individual and total harmonic voltage distortions - as in G5/3, UK engineering recommendations... Table 23.2 Premissible individual and total harmonic voltage distortions - as in G5/3, UK engineering recommendations...
Nominal system Individual hannonic voltage Total harmonic... [Pg.744]

Refer to Table 23.1, which shows the average cumulative effect of all the harmonics that may be present in a power system. If we can provide a series reactor of 6% of the total kVAr of the capacitor banks connected on the system, most of the harmonics present in the. system can be suppressed. With this reactance, the system would be tuned to below the fifth harmonic (at 204 Hz) for a 50 Hz system as derived below. [Pg.746]

Figure 4 Time step dependence of the average total energy for two models of a partially hydrated dodecamer DNA duplex. Thinner traces show results for virtually harmonic conditions when temperature was lowered to 1 K. The DNA molecule has fixed bond lengths, rigid bases, and fixed valence angles except for the mtra- and extracyclic bond angles m sugars, (a) No modifications of inertia (b) inertia modified as explained m the text. (From Ref. 54.)... Figure 4 Time step dependence of the average total energy for two models of a partially hydrated dodecamer DNA duplex. Thinner traces show results for virtually harmonic conditions when temperature was lowered to 1 K. The DNA molecule has fixed bond lengths, rigid bases, and fixed valence angles except for the mtra- and extracyclic bond angles m sugars, (a) No modifications of inertia (b) inertia modified as explained m the text. (From Ref. 54.)...
The situation simplifies when V Q) is a parabola, since the mean position of the particle now behaves as a classical coordinate. For the parabolic barrier (1.5) the total system consisting of particle and bath is represented by a multidimensional harmonic potential, and all one should do is diagonalize it. On doing so, one finds a single unstable mode with imaginary frequency iA and a spectrum of normal modes orthogonal to this coordinate. The quantity A is the renormalized parabolic barrier frequency which replaces in a. multidimensional theory. In order to calculate... [Pg.79]

A term used in PFC is total harmonic distortion. This is defined as... [Pg.224]

We have extended the linear combination of Gaussian-type orbitals local-density functional approach to calculate the total energies and electronic structures of helical chain polymers[35]. This method was originally developed for molecular systems[36-40], and extended to two-dimensionally periodic sys-tems[41,42] and chain polymers[34j. The one-electron wavefunctions here are constructed from a linear combination of Bloch functions c>>, which are in turn constructed from a linear combination of nuclear-centered Gaussian-type orbitals Xylr) (in ihis case, products of Gaussians and the real solid spherical harmonics). The one-electron density matrix is given by... [Pg.42]

K.M. Ho and B.N. Harmon, First-principles total energy calculations applied to displacive transformations. [Pg.332]

The French physicist and mathematician Jean Fourier determined that non-harmonic data functions such as the time-domain vibration profile are the mathematical sum of simple harmonic functions. The dashed-line curves in Figure 43.4 represent discrete harmonic components of the total, or summed, non-harmonic curve represented by the solid line. [Pg.665]

Figure 43.4 Discrete (harmonic) and total (non-harmonic) time-domain vibration curves... Figure 43.4 Discrete (harmonic) and total (non-harmonic) time-domain vibration curves...
The impact energy generated by each piston as it changes direction is clearly visible in the vibration profile. Since all pistons complete a full cycle each time the crankshaft completes one full revolution, the total energy of all pistons is displayed at the fundamental (lx) and second harmonic (2x) locations. [Pg.708]

Equations 22.3-22.14 represent the simplest formulation of filled phantom polymer networks. Clearly, specific features of the fractal filler structures of carbon black, etc., are totally neglected. However, the model uses chain variables R(i) directly. It assumes the chains are Gaussian the cross-links and filler particles are placed in position randomly and instantaneously and are thereafter permanent. Additionally, constraints arising from entanglements and packing effects can be introduced using the mean field approach of harmonic tube constraints [15]. [Pg.611]

FIGURE 30.8 Correction method on total relative torque harmonic content. [Pg.828]

FIGURE 30.10 Modeling the variation of total torque harmonic content (TTHC) with increasing strain. [Pg.830]

According to test protocols described above, RPA-FT test were performed at 100°C, 1 Hz on all samples additional tests at 100°C, 0.5 Hz were performed on IMA TR, IMA FM, and IMA-AG samples. Essentially three types of data will be discussed hereafter The complex modulus G (as derived from the main torque component in the FT torque spectrum), the corrected total torque harmonic component, i.e., cTTHC, and the Q1/Q2 ratio. [Pg.831]

FIGURE 30.15 Ethylene-propylene-diene monomer (EPDM) compounding corrected relative 3rd torque harmonic component and total torque harmonic content (TTHC) versus strain, at 0.5 Hz samples TR, EM, and AG. [Pg.835]

Ethylene-Propylene-Diene Monomer (EPDM) Compounding Rubber Process Analyzer-Fourier Transform (RPA-FT) Results at 100°C Total Torque Harmonic Content (TTHC) versus Strain Fit Parameters of Equation 30.4... [Pg.837]

FIGURE 30.24 Mixing silica-filled compound Total torque harmonic content (TTHC) versus strain amph-tude slope at 200% of TTHC versus y curves varies along the compounding hue. [Pg.846]


See other pages where Harmonization total is mentioned: [Pg.431]    [Pg.110]    [Pg.722]    [Pg.431]    [Pg.110]    [Pg.722]    [Pg.586]    [Pg.250]    [Pg.251]    [Pg.333]    [Pg.35]    [Pg.130]    [Pg.304]    [Pg.7]    [Pg.734]    [Pg.485]    [Pg.513]    [Pg.536]    [Pg.559]    [Pg.14]    [Pg.73]    [Pg.116]    [Pg.234]    [Pg.828]    [Pg.840]   
See also in sourсe #XX -- [ Pg.41 , Pg.137 ]




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