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Ionic conductivity, Arrhenius activation energy

At temperatures above or near the eutectic temperature of the polymer phase, CSEi values are typically in the range of 0.1-2 pFcm-2 [5], However, for stiff CPEs or below this temperature, CSEI can be as low as 0.001 pFcm 2 (Fig. 16). When a CPE is cooled from 100 °C to 50 °C, the CSE1 falls by a factor of 2-3, and on reheating to 100 °C it returns to its previous value. This is an indication of void formation at the Li/CPE interface. As a result, the apparent energy of activation for ionic conduction in the SEI cannot be calculated from Arrhenius plots of 1// sei but rather from Arrhenius plots of 7SE)... [Pg.447]

The activation energy for conduction, is the major factor controlling the ionic mobility, u. The Arrhenius expression for conductivity is either... [Pg.18]

Fig. 4.1 Arrhenius plots for ionic conductivity, (a) General behaviour for ionically conducting glasses. At room temperature, the most conductive (Li or Ag ) have the lowest activation energy. For the less conductive glasses (Cs or mixed alkali glasses) the activation energy is around 1 eV. (b) Experimental data for Li conducting glasses (Souquet and Kone, 1986). Fig. 4.1 Arrhenius plots for ionic conductivity, (a) General behaviour for ionically conducting glasses. At room temperature, the most conductive (Li or Ag ) have the lowest activation energy. For the less conductive glasses (Cs or mixed alkali glasses) the activation energy is around 1 eV. (b) Experimental data for Li conducting glasses (Souquet and Kone, 1986).
The temperature dependence of the conductivity can be described by the classical Arrhenius equation a = a"cxp(-E7RT), where E is the activation energy for the conduction process. According to the Arrhenius equation the lna versus 1/T plot should be linear. However, in numerous ionic liquids a non-linearity of the Arrhenius plot has been reported in such a case the temperature dependence of the conductivity can be expressed by the Vogel-Tammann-Fuller (VTF) relationship a = a°cxp -B/(T-T0), ... [Pg.100]

Figure 6.5 Arrhenius plots of ln( Figure 6.5 Arrhenius plots of ln(<r/ ) versus l/T for ionic conductivity in a crystal (a) straight-line plot used to obtain the activation energy of migration (b) experimental results for the pyrochlore phases Lu2Ti207, Lu2o Tij 904O6952, and Lu2.286TiL71406.857. [Data adapted from A. V. Shlyakhtina, J. C. C. Abrantes, A. V. Levchenko, A. V. Knot ko, O. K. Karyagina, and L. G. Shcherbakova, Solid State Ionics, 177, 1149-1155 (2006).]...
Such a chemical approach which links ionic conductivity with thermodynamic characteristics of the dissociating species was initially proposed by Ravaine and Souquet (1977). Since it simply extends to glasses the theory of electrolytic dissociation proposed a century ago by Arrhenius for liquid ionic solutions, this approach is currently called the weak electrolyte theory. The weak electrolyte approach allows, for a glass in which the ionic conductivity is mainly dominated by an MY salt, a simple relationship between the cationic conductivity a+, the electrical mobility u+ of the charge carrier, the dissociation constant and the thermodynamic activity of the salt with a partial molar free energy AG y with respect to an arbitrary reference state ... [Pg.85]

Arrhenius plot This plot provides direct information about ionic activation energy, phase transition, and electrical stability of nonelectronic conductors. Biomaterials are polymeric in nature and exhibit a certain Arrhenius nature. Hence, a review of the Arrhenius mechanism is needed. The plot of log a vs. 1/T provides a straight line for ionic conduction and from the slope of the curve the sum of the activation energies. The Arrhenius behaviour of amorphous gum Arabica specimen was measured with a.c. at frequency 1 KHz between room temperature, 20°C-80°C, which is a thermally stable temperature range for gum Arabica biopolymer (as indicated by TGA study). The... [Pg.335]

The standard microwave frequency used for synthesis is 2450 MHz. At this frequency, molecular rotation occurs as molecular dipoles or ions try to align with the alternating electric field of the microwave by processes called dipole rotation or ionic conduction [24, 25). On the basis of the Arrhenius equation, (k = g-Ka/j r j the reaction rate constant depends on two factors, the frequency of collisions between molecules that have the correct geometry for a reaction to occur, A, and the fraction of those molecules that have the minimum energy required to overcome the activation energy barrier,... [Pg.905]

Table 6.4. Values of activation energy graphically determined using the Arrhenius diagram confrontation ofthe activation energy of the ionic conduction process end the evolution slope a of parameter I cKcording to temperature... Table 6.4. Values of activation energy graphically determined using the Arrhenius diagram confrontation ofthe activation energy of the ionic conduction process end the evolution slope a of parameter I cKcording to temperature...
Arrhenius plots of conductivity at various Ph2o values are depicted in Fig. 26. By fitting the data of Fig. 26 by Eq. (3) we can obtain the apparent activation energy Ea and the preexponential factor A which is directly related to the charge ionic capacity of the electrolyte ... [Pg.346]

Effect of nano particles of Al Oj on conventional SPE films have been examined by FTIR, DSC and B-G spectroscopy. The dispersal of Al O nano particles to the SPEs shows dechnation in the glass transition and melting temperature as established from DSC analysis. The FUR spectra show possible interactions between Al O nano particles and host SPE films. The optimum room temperature ionic conductivity of the order of 7 x 10 S/cm having minimum activation energy (E 0.22eV) is observed for NCPE films. This shows one order increment in the conductivity over the conventional SPE films. The temperature dependent conductivity shows Arrhenius type thermally activated behavior before as well as after glass transition temperature. Maximum value of ion transference number is found to be 0.96 which is indicative of predominant ionic (protonic) transport in the SPE and NCPE thin films. It has been observed that dielectric constant for SPE and NCPEs increases with temperature while it decreases with frequency. [Pg.80]


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