By ed. by M. J. Assael
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F. J. Hurly, J. Chem. Thermodynamics, 2008, 40, 193. J. Hurly and M. R. Moldover, private communication. J. Hurly, Int. J. , 2004, 25, 625. 5 compares literature data14,15 for the zero-density limit of viscosity of hydrogen with measurements made with the Greenspan viscometer. The agreement is excellent throughout the temperature range 225 K to 400 K. 3 Thermal Conductivity In principle, the thermal conductivity of dilute gases can be deduced from the widths of the radially-symmetric acoustic modes of a spherical or nearly spherical (‘‘quasi-spherical’’), gas-filled cavity of known radius a.
The total root-mean-square amplitude of the surface roughness integrated over all wavelengths is typically between (1 and 100) nm. In an SLS experiment, the dynamics of surface fluctuations are studied as a function of frequency and damping. For the temporal decay of surface fluctuations, two cases may be distinguished. For the case of relatively low viscosity and relatively large surface tension, the amplitude of the surface fluctuation decays in the form of a damped oscillation, while in the case of a relatively large viscosity and relatively small surface tension, the amplitude is damped exponentially.
Thoen and C. W. Garland, Phys. Rev. A, 1974, 10, 1311. 23/06/2014 08:00:55. 1 Introduction to Optical Methods ¨ BA AND STEFAN WILL ANDREAS PAUL FRO This chapter is devoted to the measurement of transport properties by optical methods, in particular by light scattering methods that are either newly developed or have significantly progressed with respect to a reduction of uncertainty or application. All these methods are based on the analysis of light scattering caused by equilibrium, non-equilibrium or induced fluctuations.
Advances in transport properties of fluids by ed. by M. J. Assael