Abstract
GRIFFITH1 extrapolated from his experiments the strength of glass to the order of 1,000 kp./mm.2, which is many times larger than the strength of the best steel. Orowan2 calculated from mechanical principles a value of the same order. More recent measurements, however, gave a much higher value for several silica-glass fibres, namely, 2,460 kp./mm.2 (ref. 3) ; therefore a calculation based on the atomic structure of glass seems to be important.
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References
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Orowan, E., Inst. Eng. Shipbuild. Scotland, 89, 165 (1945–46).
Anderegg, F. O., Indust. Eng. Chem., 31, 290 (1939).
Náray-Szabó, I., Acta Phys. Hung., 8, 37 (1957).
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Kossel, W., Ann. Phys., 4, 49, 330 (1916). See also Ketelaar, J. A. A., “Chemical Constitution”, second ed. (Elsevier, Amsterdam, 1958).
Herzberg, G., “Molecular Spectra and Molecular Structure I. Spectra of Diatomic Molecules”, 101 (van Nostrand Co., Toronto, New York, London, 1958).
Herzberg, G., “Molecular Spectra and Molecular Structure I. Spectra of Diatomic Molecules”, 100 (van Nostrand Co., Toronto, New York, London, 1958).
Herzberg, G., “Molecular Spectra and Molecular Structure I. Spectra of Diatomic Molecules”, 570 (van Nostrand Co., Toronto, New York, London, 1958).
Zukowski, R., and Gaze, R., Nature, 183, 35 (1959).
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NÁRAY-SZABÓ, I., LADIK, J. Strength of Silica Glass. Nature 188, 226–227 (1960). https://doi.org/10.1038/188226a0
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DOI: https://doi.org/10.1038/188226a0
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