2016 Volume 30 Issue 3 Pages 125-130
Using the apparatus for the measurement of gaseous diffusion coefficients D by the Stefan method described in the first report, the diffusion coefficient of diethyl ether vapor into dry air was measured at 298.15 K (25°C)and at atmospheric pressure. The diffusion path lengths L(≅ 80×10-3 m, 120×10-3 m, 160×10-3 m) and the air flow rates Q (0.8×10-6 m3s-1 -42×10-6 m3s-1 (50 cm3min-1-2500 cm3min-1)) were systematically changed as in the first report. A loose polyester cotton plug was inserted into the horizontal tubing just upstream of the mouth of the evaporation tube to straighten air flow. The present results were compared with those in the first report obtained at 303.15 K (30°C). The air flow rate Q suitable to the measurement (5×10-6 m3s-1 -16×10-6 m3s-1 (300 cm3min-1000 cm3min-1)) was found to be lower than that for 303.15 K. The range of the air flow rate Q suitable to the measurement was narrowed with increasing diffusion path length L. Both the present experimental value (D = 0.091×10-4 m2s-1) and that at 303.15 K in the first report agree well with the extrapolation of our experimental data obtained by the Taylor dispersion method to lower temperature.