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Tellurite And Fluorotellurite Glasses For Active And Passive

Tellurite And Fluorotellurite Glasses For Active And Passive

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2. Literature review; MDO 17<br />

conductivity. However, it cannot explain all phenomena, such as property effects thought<br />

to be due to short range ordering, and the glass formation in some novel systems also<br />

contradict the criteria of this theory. The kinetic theory of glass formation provides a<br />

more satisfactory explanation of glass formation of known systems, but the structural<br />

theories are still valid and widely used [2].<br />

2.2.2.4. Dietzel and field strength<br />

By extending Goldschmidt’s original consideration of glass formation to radius and<br />

charge of the constituent atoms / ions, Dietzel classified elements according to their field<br />

strength, Fs. This considers the forces (attraction / repulsion) between cations and anions<br />

in the glass [2].<br />

F<br />

s<br />

τ c<br />

=<br />

( ra<br />

+ rc<br />

2<br />

)<br />

(2.1)<br />

where τc is the valence of the cation, r the ionic radius of the cation (c) or anion (a).<br />

Using Zachariasen’s classification, ions can be catagorised into three field strength<br />

groups, Fs = 0.1 to 0.4 (network modifiers), Fs = 0.5 to 1 (intermediates), and Fs = 1.4 to<br />

2 (network formers) [2].<br />

On cooling a binary melt with cations of approximately the same field strength, phase<br />

separation or crystallisation of the pure oxide phases is normally seen (e.g. SiO2-P2O5,<br />

SiO2-B2O3, B2O3-P2O5). To form a single stable crystalline compound normally requires<br />

∆Fs > 0.3. As ∆Fs increases, so does the number of possible stable compounds, and the

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