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Tellurite And Fluorotellurite Glasses For Active And Passive

Tellurite And Fluorotellurite Glasses For Active And Passive

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8. Fibre drawing; MDO 356<br />

confirmed by viscosity data reported by Wang et al. [18], which shows TeO2-Na2O-ZnO<br />

and ZBLAL viscosity of 10 6 Pa.s to occur at 352 and 295°C respectively. From fig. (8.4)<br />

it can be seen the viscosity of 10 6 Pa.s occurs at 296 and 306°C for the 25 and 20 mol. %<br />

ZnF2 glasses respectively, closer in fragility to fluorozirconate glasses, but slightly<br />

stronger. The models predict the fibre drawing viscosity (10 4.5 Pa.s) of the clad glass to<br />

occur around 324°C, 74°C below Tx. Figure (8.6) shows the modelling for the core glass.<br />

As expected, the predicted fibre drawing viscosity occurred at a higher temperature than<br />

the value for the clad glass, at 333°C, 61°C below Tx. Table (8.4) shows the parameters<br />

from the viscosity models for both glasses, and predicted fibre drawing temperatures.<br />

These values indicate successful fibre drawing is possible without devitrification.<br />

The VFT and ML models generated negative Kelvin values for T0 in these models for<br />

the core (MOF005) glass, therefore these models were not used on the plots shown in fig.<br />

(8.5) and (8.6). In the VFT model, T0 is believed to correspond to an ideal glass transition<br />

temperature below Tg, where the free volume of the glass tends to zero [19]. Therefore,<br />

some researchers have suggested this justifies the theoretical basis for an otherwise<br />

empirically derived equation. However, as this equation models the viscosity-temperature<br />

behaviour of strong glass formers, such as silicates, more accurately, it will not be<br />

considered further here. The CG model was also developed by the considering the free<br />

volume of the glass [4], although T0 takes on a different meaning. Here it represents the<br />

transition between high and low temperature behaviour, and below the transition certain<br />

relaxation modes in the glass are no longer active. <strong>For</strong> high (h) and low (l) regions,<br />

different values of T0 exist, with the free volume proportional to T-T0l and T-T0h. At high<br />

temperatures, the CG model approximates VFT behaviour (i.e. when (T-T0) 2 >> 4CT),

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