Tellurite And Fluorotellurite Glasses For Active And Passive
Tellurite And Fluorotellurite Glasses For Active And Passive Tellurite And Fluorotellurite Glasses For Active And Passive
2. Literature review; MDO 9 2. Literature review In this chapter, the main points relating to the glasses studied here (tellurite and flurotellurite) will be outlined. It will begin with a brief outline of the glass transition, then the general theories, structural and kinetic, of glass formation will be summarised. Important results from early studies on tellurite glasses will subsequently be reviewed, followed by the structure of tellurite glasses. Finally, the impact of fibre optics will be presented, concluding with research in that area on tellurite and fluorotellurite glasses. 2.1. The nature of glass 2.1.1. Behaviour of ‘typical’ glass-forming materials on melt-cooling Many inorganic elements and compounds (e.g. Zn, LiCl, Fe, CdBr2 and Na) melt to form liquids with a viscosity of the order of magnitude as water (≈ 10 -4 to 10 -3 Pa.s) [1]. When these types of liquids are cooled, rapid crystallisation occurs at the melting point. Even when the cooling is fast, in general, crystallisation cannot be avoided. In some cases, small droplets of these types of materials may be supercooled far below the freezing point, but cooling cannot be carried out indefinitely without crystallisation occurring, although theoretically any liquid can be cooled to form a glass if quenching is rapid enough. However, a number of materials exist which melt to form very viscous liquids, of the order of ≈ 10 4 to 10 6 Pa.s (e.g. SiO2, BeF2, B2O3, As2O3, P2O5, and GeO2) [1]. If
2. Literature review; MDO 10 one of these liquids is held at a temperature just below the freezing point, it will slowly crystallise, as the crystalline form is thermodynamically more stable than the liquid state. However, if the liquid is continuously cooled from above the freezing point, crystallisation may, or may not occur, depending on the rate of cooling 1 . If the rate of cooling is slow, the material will more than likely crystallise to some extent, but at high cooling rates, it is possible to avoid crystallisation altogether. During this cooling process, the viscosity of the liquid increases to such a degree that atomic rearrangement becomes difficult and the material has become a solid without long-range periodic order, but with a structure closer to the liquid state. This metastable solid is called a glass. This phenomena is not limited to inorganic materials, there are many examples of organic glasses, and glasses do not necessarily have to be formed from rapid melt cooling; sol-gel glasses are prepared using organic-precursors and heat treated at conditions close to ambient. The relatively recent achievement of cooling rates of the order of 10 6 K.sec. -1 and greater has resulted in the formation of low volume wires or ribbons of glasses formed from very fluid metal melts, i.e. metallic glasses [2]. A better appreciation of the relationship between the liquid, crystalline and glassy forms of a material from melt-cooling can be gained by considering the volume- temperature relationship of a glass-forming substance as shown in fig. (2.1) [1]. 1 It is possible to form glass relatively easily from some systems, such as fluorozirconates (e.g. ZBLAN), which have viscosities of the order of water (≈ 10 -2 Pa.s) at their melting points; this phenomenon will be addressed in section 2.2.3, on the kinetic theory of glass formation.
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2. Literature review; MDO 10<br />
one of these liquids is held at a temperature just below the freezing point, it will slowly<br />
crystallise, as the crystalline form is thermodynamically more stable than the liquid state.<br />
However, if the liquid is continuously cooled from above the freezing point,<br />
crystallisation may, or may not occur, depending on the rate of cooling 1 . If the rate of<br />
cooling is slow, the material will more than likely crystallise to some extent, but at high<br />
cooling rates, it is possible to avoid crystallisation altogether. During this cooling<br />
process, the viscosity of the liquid increases to such a degree that atomic rearrangement<br />
becomes difficult and the material has become a solid without long-range periodic order,<br />
but with a structure closer to the liquid state. This metastable solid is called a glass. This<br />
phenomena is not limited to inorganic materials, there are many examples of organic<br />
glasses, and glasses do not necessarily have to be formed from rapid melt cooling; sol-gel<br />
glasses are prepared using organic-precursors and heat treated at conditions close to<br />
ambient. The relatively recent achievement of cooling rates of the order of 10 6 K.sec. -1<br />
and greater has resulted in the formation of low volume wires or ribbons of glasses<br />
formed from very fluid metal melts, i.e. metallic glasses [2].<br />
A better appreciation of the relationship between the liquid, crystalline and glassy<br />
forms of a material from melt-cooling can be gained by considering the volume-<br />
temperature relationship of a glass-forming substance as shown in fig. (2.1) [1].<br />
1 It is possible to form glass relatively easily from some systems, such as fluorozirconates (e.g. ZBLAN),<br />
which have viscosities of the order of water (≈ 10 -2 Pa.s) at their melting points; this phenomenon will be<br />
addressed in section 2.2.3, on the kinetic theory of glass formation.