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Tellurite And Fluorotellurite Glasses For Active And Passive

Tellurite And Fluorotellurite Glasses For Active And Passive

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7. Surface properties; MDO 321<br />

with Ag + did not occur. The content decreased to 0.7 at. % at 1 µm depth for the 100 µm<br />

layer, and 0.4 at. % at 2 µm depth for the 300 µm layer. Silver ions ‘exchange’ with Na +<br />

ions in the glass due to their similar ionic radii (114 and 113 pm respectively in four-fold<br />

coordination), and both are monovalent, ensuring charge neutrality. At room temperature,<br />

the ion exchange of the silver layer will be kinetically inhibited. However, at elevated<br />

temperatures, the exchange becomes thermodynamically and kinetically more favourable,<br />

and due to the concentration difference at the silver / glass interface, Ag + /Na + ion-<br />

exchange takes place. Equation (7.13) shows Fick’s second law.<br />

2<br />

∂N<br />

∂ N<br />

= D 2<br />

∂t<br />

∂x<br />

(7.13)<br />

where N is the exchanged ion concentration (i.e. silver), t is time, x the depth of exchange<br />

into the material, and D the diffusion coefficient of the ion. Solving this equation results<br />

in a concentration profile shown by equation (7.14). Flux of sodium ions out of the glass<br />

results in a more complex profile, with the silver content levelling off initially, before<br />

decreasing according to an erfc function.<br />

⎡ x ⎤<br />

N ( x,<br />

t)<br />

= N 0 erfc⎢<br />

0.<br />

5 ⎥<br />

(7.14)<br />

⎣2(<br />

Dt)<br />

⎦<br />

where N0 is the surface concentration [1], and erfc is the complementary error function<br />

defined by equation (7.15).

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