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Journal of the Optical Society of America

Journal of the Optical Society of America

  • Vol. 4, Iss. 5 — Sep. 1, 1920
  • pp: 340–365

THE ABSORPTION OF HEAT IN GLASS

A. Q. TOOL and C. G. EICHLIN.

JOSA, Vol. 4, Issue 5, pp. 340-365 (1920)
http://dx.doi.org/10.1364/JOSA.4.000340


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Citation
A. Q. TOOL and C. G. EICHLIN., "THE ABSORPTION OF HEAT IN GLASS," J. Opt. Soc. Am. 4, 340-365 (1920)
http://www.opticsinfobase.org/josa/abstract.cfm?URI=josa-4-5-340


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References

  1. A. Q. Tool and J. Valasek, B. S. Sci. Paper No. 358, Jan., 1920.
  2. M. So, Proc, Tokyo Math. and Phys. Soc. (2), 9, p. 426, 1918.
  3. W. Rosenhain, Glass Manufacture, p. 2, 1919.
  4. C. G. Peters, Meeting Opt. Soc, Baltimore, 1918. C. G. Peters and C. H. Cragoe, Jour. Opt. Soc, 4, p. 105, May, 1920.
  5. W. P. White, Am. J. Sci. (4), 47, P. 44, 1919.
  6. J. O. Reed, Wied. Ann. d. Phys. u. Chem., 65, p. 707, 1898.
  7. Loc. cit.
  8. Loc. cit.
  9. Jackson, J. Roy. Soc. of Arts, 68, p. 134, 1920.
  10. A. L. Day and R. B. Sosman, Am. J. Sci. (4), 3I, p. 341, 1911.
  11. A discussion of a very similar condition in the devitrification of glass was recently given by N. L. Bowen, J. Am. Cer. Soc., 2, p. 261, 1919.
  12. Relaxation time may be defined as the time required for the viscous or plastic deformation to reach a value equal to the initial elastic deformation, when the viscous or plastic body is being subjected to a constant stress. This ignores the possibility that the rate of deformation immediately after the force has been applied is greater for plastic bodies than at any later time.
  13. R. Reiger, Verh. d. D. Physik. Ges.; 21, p. 421, 1919.
  14. L. Marchis, “Les Modifications Permanentes du Verre et le Deplacetnent du Zero des Thermometres,” 1898.
  15. Lord Rayleigh, Phil. Mag. (6), 1, p. 169, 1901.
  16. A. de la Bastie: Ann. d. Chim. et Phys. (5), 23, p. 286, 1881; Brux. Bll. Pht., 14, pp. 118 and 139, 1875.
  17. F. Siemens: Dtsche Ind. Ztg., 26, p. 236; Chem. C. B. (3), 16, p. 670; Nature, 31, p. 413, 1885.

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