By ed. by M. J. Assael
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1039/9781782625254-00001 Acoustic Techniques for Measuring Transport Properties of Gases 7 vicinity of the Helmholtz mode is to change the ‘‘background’’ due to the tails of other modes, which is weakly dependent on frequency. Within the chambers, the gas compressibility in the long wavelength limit considered here is isothermal near the walls and adiabatic far from the walls. The acoustic impedance of each chamber calculated from the average compressibility within the chamber is given by the expression10 ZV ¼ rc2 1 qﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃﬃ ; ioVc 1 þ 1ð1 À iÞðg À 1ÞS d =V c t 2 (1:5) c which includes the eﬀect of heat conduction over the chamber’s surface area Sc.
15 K. 9), has to be evaluated for the quantities, oq and tC, which may be done directly by a standard nonlinear fit in which the squared sum of the residuals is minimized. The evaluation of the experimental data for viscosity and surface tension has to be performed on the basis of a full solution View Online 23/06/2014 08:00:55. 1039/9781782625254-00019 30 Chapter 2 of the dispersion relation, where also reference data for the density and viscosity of the vapor phase are used. Far from the critical point, the uncertainties in reference data have a comparatively small influence on the final results for the liquid viscosities, so that for this quantity an overall maximum relative uncertainty of less than Æ 1 % can be achieved.
The results from this cavity at low densities were puzzling because the measured values of the half-widths were smaller than the calculated values. This shows that our model for the cavity containing a honeycomb is not accurate. We believe that the honeycomb concept should be explored further. View Online . 6 Chapter 1 (a) A sectioned view of a cylindrical resonator containing a honeycomb lattice (the resonator’s end plates are not shown). (b) Odd-numbered longitudinal modes have a velocity antinode within the honeycomb; they are more sensitive to Z than corresponding modes without the honeycomb, and their half-widths are plotted as a function of dv/rh, where rh is the hydraulic radius of a honeycomb cell.
Advances in transport properties of fluids by ed. by M. J. Assael