Abstract
ONE of the most striking and least-understood aspects of refractory corrosion by molten glass is the relatively high rate of solution at the refractory-glass-gas interface, compared with that which occurs below the glass-level1,2. Any attempts to explain this phenomenon, or even measure it, are made exceedingly difficult by the complex nature of the materials involved3,4. This difficulty has been partially overcome by the use of single crystals of corundum as the refractory materials5,6, thus eliminating factors such as porosity, pore size, pore shape, texture, etc.
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