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Arrhenius plot of electrical

Figure 3. Arrhenius plot of electrical conductivity of HC104 5.5H20 and of the halfwidth of the 2H-NMR signal. Figure 3. Arrhenius plot of electrical conductivity of HC104 5.5H20 and of the halfwidth of the 2H-NMR signal.
In general, Zn(acac)2 precursors are applied for production of ZnO films and nanocrys-taUine particles. Low-temperature conductive ZnO films with a minimum resistivity of 2.44 cm have been obtained at 550 °C by CVD in oxygen atmosphere, as reported by Natsume and coworkers ". Arrhenius plots of electrical conductivity exhibited linearity. [Pg.996]

Fig. 4.9 Arrhenius plot of electrical conductivities of the LaGaOs-based oxides doped with some transition metal cations for Ga sites... Fig. 4.9 Arrhenius plot of electrical conductivities of the LaGaOs-based oxides doped with some transition metal cations for Ga sites...
Figure 4.23 shows an Arrhenius plot of electrical conductivities for LaGaOs doped with various transition metal cations on the Ga site. The conductivity increased by doping with Co, Ni and Fe, and decreases by doping with Cu and Mn. n-Type conduction is greatly enhanced by doping with Mn and Ni, and p-type conduction is increased by doping with Cu. Kharton et al. [88] also found... [Pg.104]

Figure 4.23 Arrhenius plots of electrical conductivity of the LaGaOs-hased oxide doped with some... Figure 4.23 Arrhenius plots of electrical conductivity of the LaGaOs-hased oxide doped with some...
Figure 51. Arrhenius plot of ln 1/(3 [ Q t)ldt2]) from data corresponding to Fig. 54. The conformational energy consumed per mole of polymeric segments in the absence of any external electric field (AH) can be obtained from the slope. (Reprinted from T. F. Otero and H.-J. Grande, Reversible 2D to 3D electrode transition in polypyrrole films. Colloid Surf. A. 134, 85, 1998, Figs. 4-9. Copyright 1998. Reproduced with kind permission of Elsevier Science-NL, Sara Burgerhartstraat 25, 1055 Amsterdam, The Netherlands.)... Figure 51. Arrhenius plot of ln 1/(3 [ Q t)ldt2]) from data corresponding to Fig. 54. The conformational energy consumed per mole of polymeric segments in the absence of any external electric field (AH) can be obtained from the slope. (Reprinted from T. F. Otero and H.-J. Grande, Reversible 2D to 3D electrode transition in polypyrrole films. Colloid Surf. A. 134, 85, 1998, Figs. 4-9. Copyright 1998. Reproduced with kind permission of Elsevier Science-NL, Sara Burgerhartstraat 25, 1055 Amsterdam, The Netherlands.)...
Arrhenius plots of conductivity for the four components of the elementary cell are shown in Fig. 34. They indicate that electrolyte and interconnection materials are responsible of the main part of ohmic losses. Furthermore, both must be gas tight. Therefore, it is necessary to use them as thin and dense layers with a minimum of microcracks. It has to be said that in the literature not much attention has been paid to electrode overpotentials in evaluating polarization losses. These parameters greatly depend on composition, porosity and current density. Their study must be developed in parallel with the physical properties such as electrical conductivity, thermal expansion coefficient, density, atomic diffusion, etc. [Pg.120]

Figure 9.4. Arrhenius plot of the optical relaxation time of RbBr Ag+. 60 and 90° transitions are measured for electric directions [100] and [110], respectively. (From Kapphan and Luty [1983].)... Figure 9.4. Arrhenius plot of the optical relaxation time of RbBr Ag+. 60 and 90° transitions are measured for electric directions [100] and [110], respectively. (From Kapphan and Luty [1983].)...
Fig. 22. Arrhenius plots of the electrical conductivities of several rare-earth fluoride stabilized zirconias measured under an oxygen partial pressure of 1.33 x 10 1 Pa. Fig. 22. Arrhenius plots of the electrical conductivities of several rare-earth fluoride stabilized zirconias measured under an oxygen partial pressure of 1.33 x 10 1 Pa.
Figure 4.14 Arrhenius plots ofthe electrical conductivities of BaF2-CaF2 heterostructured thin films (, 0), and thin films of BaF2 ), CaF2 (A) and their mixture Bao5Cao5F2 (-F). Figure 4.14 Arrhenius plots ofthe electrical conductivities of BaF2-CaF2 heterostructured thin films (, 0), and thin films of BaF2 ), CaF2 (A) and their mixture Bao5Cao5F2 (-F).
In order to investigate the influence of the tungsten addition onto the electrical properties of tin oxide as host material, we performed conductance measurements as a function of temperature in wet air (40% relative humidity). Fig. 6a shows the Arrhenius plots of pure and... [Pg.293]

Fig. 23. (a) Measured capacitance and conductance at four ac frequencies versus temperature taken under 4 V reverse bias for an n-type doped a-Si H Schottky-barrier sample in a cleaved chip configuration, (b) Semilog Arrhenius plot of the ac measurement frequency versus 1000/r, where T denotes the temperature of the conductance peak at each frequency as determined from (a). The slope of the straight line drawn through these points indicates an activation energy of 0.147 eV for the electrical conductivity of this sample. [From Cohen ef a/. (1983b).]... [Pg.42]

Table 2.1 provides the value of the total electrical conductivity of various perov-skite-type proton conductors at 900 °C in dry or wet H2 atmospheres. It also lists the activation energies of the electrical conduction in the range 800-950 °C. The Arrhenius plots of the conductivity for some of these perovskite-type ceramics are presented in Figure 2.3. These ceramics become almost pure protonic conductors... [Pg.53]

The columnar phases of metallomesogens have the electrical properties of molecular semiconductors [77-84]. Figure 22 presents the Arrhenius plots of the a.c. conductivity (unaligned samples of copper phthalocyanines (13) determined by Van der Pol et al. [83]. The conductivity increases with increasing temperature. The activation energy is approximately 0.5-0.6 eV at 175 °C for the compounds 13 with R=0C8H 7 and OC12H25. [Pg.1783]

Figure 22. Arrhenius plots of the electrical conductivity (o) of unaligned samples of copper phlhalocy-anines(13). Data points (A) R=H ( ) R=OCHgH,7 ( ) R=OCi2H25. a slight increase in the conductivity is observed for the last compound at the transition from the mesophase to the crystalline phase (indicated by the arrow). (From Van der Pol et al. [83], reproduced by permission of Taylor and Francis Ltd.). Figure 22. Arrhenius plots of the electrical conductivity (o) of unaligned samples of copper phlhalocy-anines(13). Data points (A) R=H ( ) R=OCHgH,7 ( ) R=OCi2H25. a slight increase in the conductivity is observed for the last compound at the transition from the mesophase to the crystalline phase (indicated by the arrow). (From Van der Pol et al. [83], reproduced by permission of Taylor and Francis Ltd.).
Figure 27. Arrhenius plot of the hole mobility (/r) versus the reciprocal of the temperature in the different phases of HHTT. Electric field=2xl0 Vcm. (From Adam et al. [69], reproduced by permission of MacMillan Magazines Ltd.). Figure 27. Arrhenius plot of the hole mobility (/r) versus the reciprocal of the temperature in the different phases of HHTT. Electric field=2xl0 Vcm. (From Adam et al. [69], reproduced by permission of MacMillan Magazines Ltd.).
Figure 19b gives the Arrhenius plot of the electrical conductivity of stabilized zirconia (Zr02 - Y2O3,12 m/ o) as a function of the stoichiometry ratio. [Pg.194]

Fig. 19. (a) Gas circuit, OP oxygen pump, OS oxygen sensor, IMP impedancemeter, (1) reduction process, (2) conductivity measurement (b) Arrhenius plot of the electrical conductivity for various non-stoichiometry ratio x (from Levy et al., 1988). [Pg.194]

Figure 4.17 Arrhenius plots of the electrical conductivity of Ca-doped LnGaOj (Ln = La, Pr, Nd, Sin). Figure 4.17 Arrhenius plots of the electrical conductivity of Ca-doped LnGaOj (Ln = La, Pr, Nd, Sin).
Fig. 5.4 (a) Arrhenius plot of the electrical conductivity of a-MoOs and LLM0O3 and (b) FTIR absorption spectra of a-Mo03 and Lio.3Mo03... [Pg.123]

Figure 12-27. Temperature dependence of the hole mobility in DPOP-PPV at different electric fields Dale for T= 0 have been obtained by extrapolation. The inset shows the intersection of Arrhenius plots at T()=465 K (Ref. 1831). Figure 12-27. Temperature dependence of the hole mobility in DPOP-PPV at different electric fields Dale for T= 0 have been obtained by extrapolation. The inset shows the intersection of Arrhenius plots at T()=465 K (Ref. 1831).
As practiced by the UL, the procedure for selecting an RTI from Arrhenius plots usually involves making comparisons to a control standard material and other such steps to correct for random variations, oven temperature variations, condition of the specimens, and others. The stress-strain and impact and electrical properties frequently do not degrade at the same rate, each having their own separate RTIs. Also, since thicker specimens usually take longer to fail, each thickness will require a separate RTI. [Pg.324]

Evidence on this question may be taken by the behavior of the electrical conductivity CT as a function of temperature. A thermally activated process T dependence on log(CT), Arrhenius plot) is expected if doping takes place, whereas j -i/4 dependence, characteristic of a variable range hopping at the Fermi level is expected for a nondoping situation. [Pg.271]

Fig.4.11. The initial rates v of increase and decrease of electric conductivity of the sensor (/) and adsorbent (2), as functions of the adsorbent temperature ( z), and the Arrhenius plot (b) corresponding to curve (a). The sensor (ZnO) is kept at room temperature. Fig.4.11. The initial rates v of increase and decrease of electric conductivity of the sensor (/) and adsorbent (2), as functions of the adsorbent temperature ( z), and the Arrhenius plot (b) corresponding to curve (a). The sensor (ZnO) is kept at room temperature.

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Arrhenius plot

Arrhenius plot of electrical conductivity

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