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Point position

The Champ-Sons model is a most effieient tool allowing quantitative predictions of the field radiated by arbitrary transducers and possibly complex interfaces. It allows one to easily define the complete set of transducer characteristics (shape of the piezoelectric element, planar or focused lens, contact or immersion, single or multi-element), the excitation pulse (possibly an experimentally measured signal), to define the characteristics of the testing configuration (geometry of the piece, transducer position relatively to the piece, characteristics of both the coupling medium and the piece), and finally to define the calculation to run (field-points position, acoustical quantity considered). [Pg.737]

Electrostatic attraction (Section 1 2) Force of attraction be tween oppositely charged particles Electrostatic potential (Section 1 10) The energy of interac tion between a point positive charge and the charge field of a molecule... [Pg.1282]

The dependenee of the nueleation rate on stirrer speed is strongly influeneed by the feed point position and the feed eoneentration. The small influenee of the stirrer speed and lienee the power input on the nueleation rate is observed for the feed point positions in a zone of small turbulenee (od). For the feed point inside the draft tube (id) and a residenee time of 660 s, reaehes a maximum at... [Pg.182]

Hz and decreases at 33.4Hz. By comparing data of different feed point positions, it was found that the nucleation rates for the experiments with the feed point located near the impeller were higher than those for feed points outside the draft tube. [Pg.183]

In Figure 8.6, the results for the referenee eonditions (Rushton turbine, 40-min feed time, feed point position elose to the impeller, total eoneentration 0.008 M) for ealeium oxalate eonfirm this observation. [Pg.225]

Figure 8.7 Mean particle size versus specific energy input for different feed point positions if.p.p.) (CaOx, Rushton turbine, 40 min feed time, total concentration 0.008 M.) After Zauner and Jones, 2000b)... Figure 8.7 Mean particle size versus specific energy input for different feed point positions if.p.p.) (CaOx, Rushton turbine, 40 min feed time, total concentration 0.008 M.) After Zauner and Jones, 2000b)...
Electrostatic Potential. A function describing the energy of interaction of a point positive charge with the nuclei and fixed electron distribution of a molecule. [Pg.281]

It is clear that the one-to-one correspondence assumption readily breaks down, notoriously at the position halfway along the path, the saddle point position. This is considered as the most important point apart from the initial position [20, 21], because conventionally the force has been calculated by averaging its values at initial position and saddle point. Until now only the model-pseudopotential method was used, which... [Pg.470]

Figure 4 The wind valence in A1 along the migration path. The initial and saddle point positions are at the origin and at 0.5 respectively. The lower curve is for Cu, the upper curves are for self-electromigration. The dashed and the dotted curve show the influence of a Cu atom at positions 1 and 2 of Fig. 3 respectively, on the wind force in pure A1 (thick curve). Figure 4 The wind valence in A1 along the migration path. The initial and saddle point positions are at the origin and at 0.5 respectively. The lower curve is for Cu, the upper curves are for self-electromigration. The dashed and the dotted curve show the influence of a Cu atom at positions 1 and 2 of Fig. 3 respectively, on the wind force in pure A1 (thick curve).
Drillstring Failure Prevention. Drillstring failures are mainly due to vibrations, shocks and neutral point positioned too close to the drill pipes. They result in drillstring washouts and twist-offs. [Pg.1020]

Higher-order numerical schemes are also available (Kloeden and Platen 1992), but are generally complicated to apply since they involve derivatives of the coefficients. A simpler alternative is to apply a multi-step approach (Pope 1995 Jenny el al. 2001). For example, the mid-point position,30... [Pg.364]

Shortened version of the standard description structural types Several intermetallic phases are known which have the same (or a similar) stoichiometry and crystallize in the same crystal system and space group with the same occupied point positions. Such compounds are considered as belonging to the same structure type. About 30000 intermetallic phases have been described. These, however, may be grouped in about 2800 types. [Pg.113]

To calculate the space-filling value for a specific compound, one has to know the radii of the atoms and the lattice constant. Neither of these is needed for the construction of a space-filling curve of a crystal structure type it is sufficient to know the point positions of the atoms and the axial ratios. The curve is based on a hard sphere... [Pg.255]

A low AH for a cooperative cluster rotation allows excitation of a cluster of atoms from normal to saddle-point positions. Such an excitation may, in turn, lower the energy of the saddle-point sites relative to the normal sites, thus effectively introducing a AHg(T) that collapses in a smooth transition. At temperatures T> T, the mobile ions become disordered over the normal and saddle-point sites. Such a situation appears to be illustrated by stoichiometric LijN and PbFj (Goodenough, 1984). [Pg.56]

Fig. 5 Left Mean-field results for the rescaled averaged polymer paths which end at a certain distance Ze from the wall for (S = I, 10, 100 (from top to bottom), corresponding to stretching values of y = 1.1, 1.9, 5.6 (as defined in Eq. 18). The thick solid line shows the unconstrained mean path obtained by averaging over all end-point positions. Note that the end-point stretching is small but finite for all finite stretching parameters p. Right End-point distributions... Fig. 5 Left Mean-field results for the rescaled averaged polymer paths which end at a certain distance Ze from the wall for (S = I, 10, 100 (from top to bottom), corresponding to stretching values of y = 1.1, 1.9, 5.6 (as defined in Eq. 18). The thick solid line shows the unconstrained mean path obtained by averaging over all end-point positions. Note that the end-point stretching is small but finite for all finite stretching parameters p. Right End-point distributions...
The polarization potential provides the energy due to electronic reorganization of the molecule as a result of its interaction with a point positive charge. The sum of the electrostatic and polarization potentials provides a better account of the energy of interaction of a point positive charge than available from the electrostatic potential alone. It properly orders the proton affinities of trimethylamine, dimethyl ether and fluoromethane. [Pg.74]

Of course, the polarization potential does not account for electron transfer as would occur were a reaf electrophile to replace the point positive charge. [Pg.74]

Polarization Potential. Afimction describing the energy of electronic relaxation of a molecular charge distribution following interaction with a point positive charge. The polarization potential may be added to the Electrostatic Potential to provide a more accurate account of the interaction of a point-positive charge and a molecule. [Pg.766]

Lattice Points positions in a unit cell occupied by atom, molecules, or ions Law of Definite Proportion law that states that different samples of the same compound always contain elemental mass percentages that are constant Law of Mass Action mathematical expression based on the ratio between products and reactants at equilibrium, an equation to determine the equilibrium rate constant Law of Multiple Proportions law that states when two elements combine to form more than one compound that the mass of one element compared to the fixed mass of... [Pg.343]

With ID backward LP (see Fig. 5.26) the range and the number of measured data points used for prediction is again defined by the Last Point used for LP and the First Point used for LP respectively. With LP backward to Point positive, the first measured data points ( LP backward to Point up to First Point used for LP) are replaced by predicted points. With LP backward to Point negative, LP backward to Point data points are added to the beginning of the FID and an equal number of points are discarded from the end of the (zero-filled) FID. [Pg.189]

Figure 11.19. Diagrams showing symmetry elements and general point positions for space groups PI, P2, /42, and /42, (which is not different from A2 except for placement of the origin). Figure 11.19. Diagrams showing symmetry elements and general point positions for space groups PI, P2, /42, and /42, (which is not different from A2 except for placement of the origin).

See other pages where Point position is mentioned: [Pg.690]    [Pg.2315]    [Pg.1296]    [Pg.50]    [Pg.226]    [Pg.226]    [Pg.227]    [Pg.29]    [Pg.30]    [Pg.285]    [Pg.467]    [Pg.102]    [Pg.121]    [Pg.50]    [Pg.62]    [Pg.370]    [Pg.164]    [Pg.169]    [Pg.49]    [Pg.230]    [Pg.191]    [Pg.19]    [Pg.251]    [Pg.193]    [Pg.201]    [Pg.101]   
See also in sourсe #XX -- [ Pg.182 ]




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Eigenvalues and positions of equilibrium points

Inflexion point position

Position of a point on the cross-section

Positive displacement pump operating point

Positive for point/gene mutation

Positive ionizable point

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