Measurements of the velocity of ultrasonic waves in carbon dioxide and ethylene are presented; the velocity was obtained while the gas was allowed to follow a p—v isothermal. For carbon dioxide the pressure range is 5 to 98 atmospheres at temperatures of 28.0°, 30.0°, 31.0°, 32.0°, 33.0°, 35.0° and 38.0°C. For ethylene the pressure range is 35 to 75 atmospheres at temperatures of 9.7°, 18.7° and 23.0°C. For both gases, as pressure increases, the velocity decreases, falls to a sharp minimum, and then rises steeply on the high pressure side of this minimum. The minima have a discontinuity of slope for isothermals below the critical isothermal, which persists for a limited temperature range above the critical temperature. Above this range the curves become continuous in slope through the minimum. The curve log p vs. 1/T for the minima is linear through the critical point and, below the critical point, coincides within experimental error with standard vapor pressure data. Some calculations of ratio of specifi...
[1]
R. S. Alleman.
Dissipative Acoustic Reflection Coefficients in Gases by Ultrasonic Interferometry
,
1939
.
[2]
J. Hubbard.
Acoustic Resonator Interferometer
,
1934
.
[3]
A Fixed Path Acoustic Interferometer for the Study of Matter
,
1939
.
[4]
J. Hubbard,et al.
Ratio of Specific Heats of Air, N2, and CO2 as a Function of Pressure by the Ultrasonic Method
,
1937
.
[5]
F. Fox.
Ultrasonic Interferometry for Liquid Media
,
1937
.
[6]
A. Loomis,et al.
CXXII. The velocity of sound in liquids at high frequencies by the sonic interferometer
,
1928
.
[7]
A. H. Hodge.
An Experimental Determination of Ultrasonic Velocity in Several Gases at Pressures Between One and One Hundred Atmospheres
,
1937
.