Encyclopedia of Glass Science, Technology, History, and Culture. Группа авторов
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3.2 Quantification of Heavy Minerals
One finds approximately 150 × 106 grains of quartz in 1 kg of fine sand [4]. In such a population it is obvious that one cannot detect one grain of chromite or other impurity by routine chemical analysis. To detect these minerals at the part‐per‐billion (ppb) level, one rather takes advantage of the fact that they are denser, or even much denser than quartz (e.g. corundum: ~4 g/cm3; chromite: ~5 g/cm3). One can thus concentrate them by immersing the test powder in a liquid with a density slightly higher than that of quartz, which will then float while heavier minerals will sink, allowing the harmful ones to be identified and quantified with standard methods such as optical microscopy, Raman spectroscopy, or electron microscopy [8]. For this purpose, the most frequently used liquids have long been bromoform (CHBr3) and diiodomethane [CH2I2, also called methylene iodide], whose room‐temperature densities of 2.9 and 3.3 g/cm3, respectively, can be slightly lowered through mixing with lighter ethanol [C2H6O]. Because strict precautions must be observed to handle these toxic liquids, however, sodium polytungstate [SPT, 3 Na2WO4·9 WO3·H2O] has become an efficient alternative [9], thanks to the fact that this salt can readily dissolve in distilled water to yield liquids with a maximum density of 3.1 g/cm3.
Proper sampling of raw materials [4] thus is needed to guarantee their conformity with regard to possible geological heterogeneity and product variability at the quarry level. It relies on suitable quartering techniques to obtain a true fingerprint of the mineralogy of all raw materials from which incorporation of harmful species may be ruled out or at least minimized. In other words, heavy‐mineral content is an overwhelming and crucial specification concerning the physical and chemical properties that must be guaranteed by a producer of raw materials, especially when fabrication of a new glass has to be tested. Not complying with these specifications can generate long‐lasting yield drops and large financial losses for the glassmaker. Since glassmakers constantly need to diversify and secure their supplies of raw materials, heavy‐mineral characterization must routinely be operated by well‐equipped internal or academic laboratories.
Of course, the bulk chemistry must also be determined on a daily basis at the plant by XRF, ICP‐MS, or wet chemistry (cf. Chapter 5.1) to monitor the variability of moisture and oxide content, especially for multielement raw materials, and thus to allow batch adjustments needed to keep the glass recipe constant to be calculated (cf. Chapter 1.3). As indicated above, the PSD, LOI, and COD parameters must in addition be included in the almost daily control of raw materials at the plant. In this way it is possible to anticipate possible drifts away from the targeted specifications of the raw‐material feed. As for the overall meltability, energy demand, and expected quality, they may be tested less routinely through differential scanning calorimetry (DSC) measurements, while it should be compulsory to test the actual batch incrementally, first in the laboratory (few kg), then in a pilot furnace (~1 ton), and finally at the industrial scale (<1000 tons).
3.3 Impurity‐related and Other Melting Defects
Melting quality first and foremost depends on appropriate digestion rates. Batch stones can, for instance, readily occur when market requirements push glassmakers to increase pull rates and, consequently, to reduce the average residence time of the raw materials in the furnace. They also form in case of errors in batch calculation or of scale malfunction. The problem is illustrated with the overall texture and microstructure of the silica batch stone shown in Figure 3. Noteworthy are former quartz grains, whose shape have been preserved although they have been totally replaced by cristobalite (as a pseudomorph) from which newly formed tridymite lath‐shaped crystals have grown radially in a groundmass of silica glass [10]. These textural features are typical of an insufficiently dispersed quartz sand within the batch. Regardless of the actual pull rate, the overall moisture content and distribution can provoke the formation of lumps when grains stick together at the batch plant and quickly sinter at the dog‐house level, preventing natural convection within the melter from properly stirring the melt under formation. Moisture is of special concern in regions facing very wet or very cold (ice) seasons. Preheating or protecting the raw materials yard can then be an effective, but somewhat costly solution.
Figure 3 Silica batch stone in a soda‐lime silica glass, resulting from incomplete digestion of a lump of quartz grains as viewed under an optical microscope (a) and as observed in a thin section under transmitted light (b), where rounded grains of cristobalite formed as quartz pseudomorph are sluggishly digested while generating radially growing tridymite laths in a vitreous groundmass showing an overall open‐porosity.
Quartz batch stones can also result from an inadequate overall PSD when other raw materials contain up to several weight % of free silica as impurities, whose size distribution differs from that of quartz sand. Limestone, dolomite, and feldspars are typical examples, the two carbonates having a dmax for quartz as high as 2 mm or more (Figure 2). Given the aforementioned digestion rates of quartz, such large grains will end up as unmolten stones in the production process.
Figure 4 Undissolved chromite crystal in a soda‐lime silica glass as seen under a binocular microscope (a) and in a polished thin section photo under reflected light (b). The chromite grain shows a preserved FeCr2O4 core, exsolution lamellae, and radially growing eskolaite Cr2O3 laths in the outer shell.
Refractory minerals, of course, raise special difficulties as illustrated in Figure 4 by an incompletely dissolved chromite inclusion. Its core is preserved as FeCr2O4, but it is surrounded by newly formed laths of eskolaite [Cr2O3] radially growing from it according to the decomposition reaction:
(1)
Although Fe2+ then diffuses in the melt, the highly refractory eskolaite crystals (melting at 2435 °C) passivate the chromite core, which will thus remain throughout the production process.
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