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Mechanism and conductance

Fig. 6.7 Average shear (mechanical) and conductivity (electric modules) relaxation times, T, and for ionically conductive materials, (a) For glassy materials r, r, above 7 and t T, below Tf. (b) For polymer electrolytes ((PP0),3 NaCF3S03) shown), x, > t, for T> T.. Fig. 6.7 Average shear (mechanical) and conductivity (electric modules) relaxation times, T, and for ionically conductive materials, (a) For glassy materials r, r, above 7 and t T, below Tf. (b) For polymer electrolytes ((PP0),3 NaCF3S03) shown), x, > t, for T> T..
Choi, P. Jalani, N.H. Datta, R. Thermodynamics and proton transport in Nafion II. Proton diffusion mechanisms and conductivity. J. Electrochem. Soc. 2005, 152 (3), E123-E130. [Pg.2528]

The final Teflon percentage is of 70% and provides suitable mechanic and conducting characteristics to the composite material. [Pg.162]

Nanotube theoretical and experimental research has developed very rapidly over the last seven years, following the bulk production of C(jo and structural identification of carbon nanotubes in soot deposits formed during plasma arc experiments. This review summarises achievements in nanotube technology, in particular various routes to carbon nanotubes and their remarkable mechanical and conducting properties. The creation of novel nanotubules, nanowires and nanorods containing other elements such as B, N, Si, O, Mo, S and W is also reviewed. These advances are paving the way to nanoscale technology and promise to provide a wide spectrum of applications. [Pg.189]

B.K. Kuila and A.K. Nandi, Physical, mechanical and conductivity properties of poly(3-hexylthiophene)-montmorillonite clay nanocomposites produced by the solvent casting method. Macromolecules, 37, 8577-8584 (2004). [Pg.370]

D.M. Bigg, Mechanical and conductive properties of metal fibre-filled polymer composites. Composites 10 (2) (1979) 95—100. [Pg.691]

Metals share excellent mechanical and conductivity (electrical and thermal) properties ideal for high stress apphcations such as heart valves. Titanium—nickel alloys have become the most common material for metaUic cardiovascular applications (stents and valves) due to unique properties shape memory effect, super-elasticity, high degree of biocompatibility moreover, they are almost completely inert and nonmagnetic. [Pg.64]

Where A is the area of contact and h is the transfer coefficient. Both these terms can be analyzed in greater detail by relying on basic impact mechanics and conductance of charge. A detailed analysis of h and A has been given by Soo based on work by Timoshenko (1951) and Hertz (1881). The highlight of this development will be considered here, as well as caJculations of these coefficients for some specific conditions. The charge-transfer coefficient is given as... [Pg.134]

The purposes of the grid are to hold the active material mechanically and conduct electricity between the active material and the ceU terminals. The mechanical support can be provided by nonmetallic materials (polymer, ceramic, rabber, etc.) inside the plate, but these are not electrically conductive. Additional mechanical support is sometimes gained by the construction method or by various wrappings on the outside of the plate. Metals other than lead alloys have been investigated to provide electrieal conductivity, and some (copper, aluminum, silver) are more conductive than lead. These alternate conductors are not corrosion-resistant in the sulfuric acid electrolyte and are often more expensive than lead alloys. Titanium has been evaluated as a grid material it is not corroded after special surface treatments but is very expensive. Copper grids are used in the negatives of some submarine batteries. [Pg.607]

The synthesis, thermal, mechanical, and conduction properties of blends of a cationic polyelectrolyte, poly-(diallyldimethylammonium-dihydrogenphosphate), PAMA H3PO4" , and phosphoric acid are reported [115]. Blends of PAMA -HjPO -xHjPO with 0.5 < x < 2.0 can be cast into amorphous films, which are stable up to 150°C. DSC results show that the softening temperatures of the blends decrease from 126°C for x = 0.5 to -23°C for x = 2.0. Furthermore, the dc conductivity increases with x and reaches 10 S cm" at ambient temperature... [Pg.267]

H. Hakkinen, R.N. Barnett, A.G. Scherbakov, U. Landman, Nanowire gold chains formation mechanisms and conductance. J. Phys. Chem. B 104(39), 9063-9066 (2000)... [Pg.146]

In the case of dielectric materials, the dielectric permitlivily formalism cannot explain the relaxation process completely because of the significant contribution of dc conductivity in the low frequency region. Therefore modulus formalism has been considered as a useful tool to explain the electrical transport mechanism and conductivity relaxation process. The electrical modulus can be expressed as. [Pg.107]

The aim of this contribution is to establish a base for further studies, rationalize and comment on the processes used to prepare those compounds, and finally to illustrate some properties of these materials such as thermal, mechanical, and conductivity and to caU the attention of clay scientists and engineers to the numerous opportunities that this type of new materials offer. [Pg.144]

This study showed that thin films (-0.015 cm) of IPNs could be prepared by a simple process, and have good mechanical and conductive properties, which are two of the essential requirements of a SPE. The ease of preparation and handling of these films would be vital if the IPNs fulfilled their commercial potential, if the large-scale mixing of different materials to form solutions of the IPNs would not cause the chemical engineer too many problems, and if the casting of the films would also be quite simple on a large scale. [Pg.10]


See other pages where Mechanism and conductance is mentioned: [Pg.161]    [Pg.189]    [Pg.212]    [Pg.357]    [Pg.1163]    [Pg.134]    [Pg.144]    [Pg.425]    [Pg.137]    [Pg.139]    [Pg.59]    [Pg.81]    [Pg.152]    [Pg.86]    [Pg.186]    [Pg.266]    [Pg.146]    [Pg.272]   
See also in sourсe #XX -- [ Pg.49 , Pg.50 , Pg.51 ]




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