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Additional info for Experimental Thermodynamics Volume IX: Advances in Transport Properties of Fluids
F. Estrada-Alexanders and J. J. Hurly, J. Chem. , 2008, 40, 193. 8. G. Kirchhoﬀ, Ann. Phys. , 1868, 134, 177; English translation in Benchmark Papers in Acoustics: Physical Acoustics, ed. R. B. Lindsay, Dowden, Hutchinson & Ross, Stroudsburg, Pennsylvania, 1974, p. 7. 9. I. B. Crandall, Theory of Vibrating Systems and Sound, Van Nostrand, New York, 1927, 229–241. 10. F. B. Daniels, J. Acoust. Soc. , 1947, 19, 569. 11. J. B. Mehl, J. Acoust. Soc. , 1999, 106, 73. 12. J. J. Hurly and M. R. Moldover, private communication.
J. Hurly and M. R. Moldover, private communication. 13. J. J. Hurly and M. R. Moldover, J. Res. Natl. Inst. Stand. , 2000, 105, 667. 14. J. Kestin and J. Yata, J. Chem. , 1968, 49, 4780. View Online Downloaded on 24/07/2014 09:49:30. 1039/9781782625254-00001 18 Chapter 1 15. E. F. May, R. F. Berg and M. R. Moldover, Int. J. Thermophysics, 2007, 28, 1085. 16. K. A. Gillis, Metrologia, 2012, 49, L21. 17. M. R. Moldover, K. A Gillis, J. J. Hurly, J. B. Mehl and J. Wilhelm, Modern Acoustical Techniques for the Measurement of Mechanical Properties, ed.
For the observation of scattered light within the irradiation plane and View Online 09:49:32. 68 ¨ba and A. Leipertz, Accurate Determination of Reprinted from A. P. Fro Liquid Viscosity and Surface Tension Using Surface Light Scattering (SLS): Toluene under Saturation Conditions between 260 K and 380 K, Int. J. , 2003, 24, 898, Figure 1, Copyright 2003, with kind permission from Springer Science and Business Media. e. kIDkS), the modulus of the scattering vector is given by kS0 j D 2kI sinðYS = 2Þcosðe À YS = 2Þ q ¼ j~ kI0 À ~ ¼ 4pn sinðYS = 2Þcosðe À YS = 2Þ; l0 (2:1) where n is the fluid refractive index and l0 is the laser wavelength in vacuum.