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Transport properties of helium near the liquid-vapor critical point. IV. The shear viscosity of3He and4He
Authors:Charles C Agosta  Suwen Wang  L H Cohen  H Meyer
Affiliation:(1) Department of Physics, Duke University, Durham, North Carolina;(2) Present address: Department of Physics, Harvard University, Cambridge, Massachusetts;(3) Present address: Bell Laboratories of AT&T, Middletown, New Jersey
Abstract:Shear viscosity measurements with a precision of 0.05% are reported for3He and4He along near-critical isochores 0.85<rgr/rgr c <1.12, where rgr c is the critical density. The temperature range was –10–4<epsi<1, where epsi=(T – T c)/T c is the reduced temperature. The experiments were carried out with a torsional oscillator operating at 158 Hz, driven at resonance in a phase-locked loop. The absolute value of the viscosity was obtained by calibration at the superfluid transition of4He, based on published values and from direct calculations using the free decay time constant of the oscillations. The data are analyzed in terms of a model using the recent mode-coupling (MC) expressions by Olchowy and Sengers, and where account is taken of the earth's gravity effects. The theory could be fitted very well to the experiment with a single free parameter, the cutoff wave numberq D, which was found to be 3.0×106 and 7.0×106 cm–1 for3He and4He, respectively. We have used for the critical exponent the MC predicted value of zeegr=0.054, which permits a fit superior to that using zeegr=0.064 predicted by dynamic renormalization group (DRG) theories. Detailed comparisons are made between the model calculations and data for various isochores and isotherms and good agreement is obtained. The effects of gravity are described in some detail. The predicted frequency effect in viscosity measurements is calculated for3He and is shown to be obscured by gravity effects. Using the Olchowy-Sengers formulas, we have also fitted the MC theory to the critical thermal conductivity data of3He, again withq D as the only free parameter. This fit gaveq D=6 × 107 cm–1, which in the ideal situation should have been the same asq D from viscosity. We also discuss a representation of the3He viscosity data along the critical isochore by a power law and first correction-to-scaling erm. Using the viscosity and the critical conductivity data for3He, we have calculated the dynamic amplitude ratio and obtained Rscr=1.05±0.10, in agreement with predictions from MC and DRG theories. Also, Rscr agrees with data of classical fluids. Finally, a comparison is made of recent shear viscosity data for CO2 by Bruschi and Torzo with those on He. The CO2 data are also analyzed in terms of the MC theory, and the discrepancies are discussed. In the Appendices, we present the results of new compressibility measurements on3He along the critical isochore, as used in the MC analysis. We also present a brief analysis of the fluid hydrodynamics in the torsional oscillator leading to relations for the viscosity as a function of the measured quantities. Finally, we give a short outline of the vertical density profile calculations from the earth's gravity field for the calculations of the viscosity nearT c.
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