Primary and secondary phase separation of sodium silicate glasses

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Abstract

The immiscibility curve in the system Na2OSiO2 shows that the amount of Na2O content in the silica rich phase is small at 500°C and hardly changes with temperature up to 800°C but increases sharply in the interval 800–865°C. The silica content of the alkali-rich phase increases continuously with temperature. The curve is thus extremely asymmetric. The electron microscope photographs show that the separate phases (primary phase separation) separate again into two phases during cooling or during a second heating of the glass at a lower temperature. This secondary phase separation does not depend upon the duration of the initial heating of the glass. It is connected with the asymmetry of the immiscibility curve. The alkali-rich phase separates more easily but with the help of a repeated treatment the silica-rich phase can also be caused to phase separate. This secondary phase separation is a general phenomenon and must be given attention when discussing the number of phases in the glass. Certainly the existence of triple-phase glasses cannot be excluded. Phase separation of higher orders can be achieved with the help of heat treatments in several steps.

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