The self-diffusion of Na was studied at temperatures ranging from 300 to 1200C by using a 22Na radiotracer. It was found that the diffusivity depended upon the temperature and the composition and ranged from 10-11 to 10-5cm2/s. The Arrhenius plots were non-linear over the entire temperature range but could be divided into 3 sections (table 124). One section was below the glass transition temperature, one was between the transition temperature and 700C, and the third was situated above 700C. This behavior suggested a change from a pure jump mechanism in the glass to a mechanism which was governed by the free volume of the glass melt. There were also some indications of the occurrence of a mixed alkali effect whose magnitude varied with temperature and composition.

M.Braedt, G.H.Frischat: Physics and Chemistry of Glasses, 1988, 29[5], 214-8

 

 

 

Table 124

Diffusion of Na in xNa2O-(1-x)Rb2O•3SiO2 Glasses

 

x

Temperature (C)

Do (cm2/s)

E (kJ/mol)

0

below 520

17.7

149

0

520 to 700

0.5

126

0

above 700

0.039

105

0.25

below 463

1.0

126

0.25

463 to 700

0.4

122

0.25

above 700

0.032

101

0.5

below 448

3.6

130

0.5

448 to 700

0.8

120

0.5

above 700

0.035

96

0.75

below 441

0.099

103

0.75

441 to 700

1.4

118

0.75

above 700

0.0079

75

1

below 478

0.002

67

1

478 to 700

0.16

93

1

above 700

0.0092

71