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Charge coefficient

Using these results, we can calculate the electric charge coefficients from Eqs. (50) to (53),... [Pg.263]

Finally, with the data of Eq. (59a) to (59c), the following electric charge coefficient was obtained... [Pg.265]

Figure 13 Charging coefficient As( i) as a function of incident electron energy for (a) a 10-ML film of glassy w-hexane nHg (b) a 13-ML film of crystalline w-hexane nHc (c) 0.1 ML CH3CI on a 5-ML nHg surface (d) the peak near zero energy in (c) shown on an extended scale (e) 0.1 ML CH3CI on a 10-ML Kr surface (f) 0.1 ML CH3CI on 13 ML nHg surface. (From Ref. 232.)... Figure 13 Charging coefficient As( i) as a function of incident electron energy for (a) a 10-ML film of glassy w-hexane nHg (b) a 13-ML film of crystalline w-hexane nHc (c) 0.1 ML CH3CI on a 5-ML nHg surface (d) the peak near zero energy in (c) shown on an extended scale (e) 0.1 ML CH3CI on a 10-ML Kr surface (f) 0.1 ML CH3CI on 13 ML nHg surface. (From Ref. 232.)...
The parameter b is the charge coefficient. It measures the rate of change of electronegativity with charge. Mathematically, h is the second derivative of energy (first derivative of electronegativity) with respect to charge ... [Pg.105]

Fig. 7.6 Crysial structures correlated with atomic charge (slope of lines) for IA-VHA (I—17), IIA-V1A (2- 6). anJ IIIA-VA (13-15) compounds. The abscissa is the difference in electronegativity. ( Fig. 7.6 Crysial structures correlated with atomic charge (slope of lines) for IA-VHA (I—17), IIA-V1A (2- 6). anJ IIIA-VA (13-15) compounds. The abscissa is the difference in electronegativity. (<iA — h). and the ordinate is (he sum of charge coefficients (tj = 16). Note that the charge. 6 (<iA — n)/(6A + / B). is approximately twice the rcriprucal of the slopes as plotted here. [Modified from Shankjr. S.. Parr. R. G. Proc. Nall. Acad. Sci. U. S 4. (985, 62. 264-266. Reproduced with permission. ...
The piezoelectric effect entails a linear coupling between electrical and mechanical energies. Numerous piezoelectric coefficients are in use, depending on the electrical and mechanical boundary conditions imposed on the part under test. Each of the piezoelectric d, e, g, and h coefficients can be defined in terms of a direct and a converse effect the two sets of coefficients are related by thermodynamics. For example, the piezoelectric charge coefficient, dkjk, can be defined via [1] ... [Pg.39]

Because of the very large differences in mechanical compliance between the two phases, the hydrostatic pressures experienced by the polymer phase transfer forces to the rods magnifying the stress in them in the poled direction. This magnified stress increases the charge induced on to the electrode tending to compensate for the inactive polymer. As a result, in typical practical cases, the piezoelectric charge coefficient fi/13) is not very sensitive to volume fraction of PZT . [Pg.376]

Table E-3. Atomic polarizability values 1. Kang-Jhon atomic hybrid polarizabilities aA(ahp) 2. Miller-Savchik average atomic polarizabilities aX(ahc) 3. No-Cho-Jhon-Sheraga atomic polarizabilities a,, o and linear charge coefficient a,y. Table E-3. Atomic polarizability values 1. Kang-Jhon atomic hybrid polarizabilities aA(ahp) 2. Miller-Savchik average atomic polarizabilities aX(ahc) 3. No-Cho-Jhon-Sheraga atomic polarizabilities a,, o and linear charge coefficient a,y.
The piezoelectric charge coefficient is improved, and the materials is more difficult to depole. A typical composition is Pbo,94 Sro.oeCZro.sa Tio.47)03.o. [Pg.525]


See other pages where Charge coefficient is mentioned: [Pg.261]    [Pg.630]    [Pg.211]    [Pg.230]    [Pg.230]    [Pg.232]    [Pg.249]    [Pg.249]    [Pg.105]    [Pg.110]    [Pg.110]    [Pg.127]    [Pg.84]    [Pg.105]    [Pg.110]    [Pg.220]    [Pg.525]    [Pg.526]    [Pg.105]    [Pg.110]    [Pg.110]    [Pg.385]    [Pg.297]    [Pg.186]    [Pg.196]    [Pg.196]    [Pg.49]    [Pg.217]    [Pg.236]    [Pg.236]    [Pg.255]    [Pg.255]   
See also in sourсe #XX -- [ Pg.169 , Pg.174 , Pg.182 ]




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