1977
DOI: 10.1016/0011-2275(77)90165-5
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Speed of sound in saturated and compressed fluid ethane

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Cited by 16 publications
(8 citation statements)
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“…This condition is detected with an oscilloscope by maximizing the resulting reinforced waveshape as seen by the receiving crystal. This technique, developed by Greenspan and Tschiegg [1]; has been used on hydrogen [2], oxygen [3], fluorine [4], methane [5], and ethane [6] in this laboratory and the apparatus is described in detail in the earlier publications. Uncertainty in the measured sound velocities is estimated to be 0.05 percent Temperatures were measured using a platinum resistance thermometer calibrated by the National Bureau of Standards on the IPTS 1968.…”
Section: Methodsmentioning
confidence: 99%
“…This condition is detected with an oscilloscope by maximizing the resulting reinforced waveshape as seen by the receiving crystal. This technique, developed by Greenspan and Tschiegg [1]; has been used on hydrogen [2], oxygen [3], fluorine [4], methane [5], and ethane [6] in this laboratory and the apparatus is described in detail in the earlier publications. Uncertainty in the measured sound velocities is estimated to be 0.05 percent Temperatures were measured using a platinum resistance thermometer calibrated by the National Bureau of Standards on the IPTS 1968.…”
Section: Methodsmentioning
confidence: 99%
“…Noury [14] measured the speed of sound in the critical region of ethane. Speeds of sound in saturated liquid ethane were measured by Poole and Aziz [15], Vangeel [16], and Tsumura and Straty [2]. Only the data set of Tsumura and Straty [2] covers a large part of the liquid region.…”
Section: Resultsmentioning
confidence: 99%
“…For ethane, the most accurate fundamental equation of state was published by Bücker and Wagner [1]. For the optimization of the equation of state in the liquid phase, only one comprehensive speed-of-sound data set by Tsumura and Straty [2] was available. These data were measured with a sing-around pulse-echo technique, have an uncertainty of 0.05 % and cover the low temperature range between 100 K and 323 K with pressures up to 37 MPa.…”
Section: Introductionmentioning
confidence: 99%
“…Data from Poole and Aziz [64] (continued) Data from Tsumura and Straty [63] These data were adjusted slightly as in [20] …”
Section: Sound Speed In the Saturated Liquid (Ccntinued)mentioning
confidence: 99%
“…Data from Tsumura and Straty [63] Calculation of dP/dp \j : AAD2 = 0.100 BIAS2 = -0.015 RMS 2 = 0.164 MPa* dm 3 •mol -1…”
Section: Sound Speed In the Saturated Liquid (Continued)mentioning
confidence: 99%