Miniature Joule-Thomson Cryocooling 2012
DOI: 10.1007/978-1-4419-8285-8_2
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The Joule-Thomson Effect, Its Inversion and Other Expansions

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Cited by 5 publications
(3 citation statements)
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“…At room temperature (300 K), the real gases except hydrogen, helium and neon cool during expansion according to the Joule-Thomson (J-T) effect. 20,21 Therefore, when the compressed air is discharged from a container or flows through a pressure regulator, the air temperature drops. In the APE, the inside cylinder of the APE is a typical location where the air gets cold because the compressed air expands in it.…”
Section: Locations Of the Temperature Dropmentioning
confidence: 99%
“…At room temperature (300 K), the real gases except hydrogen, helium and neon cool during expansion according to the Joule-Thomson (J-T) effect. 20,21 Therefore, when the compressed air is discharged from a container or flows through a pressure regulator, the air temperature drops. In the APE, the inside cylinder of the APE is a typical location where the air gets cold because the compressed air expands in it.…”
Section: Locations Of the Temperature Dropmentioning
confidence: 99%
“…The Joule-Thomson effect contribution to the total cooling of the mixture can be evaluated by the integral isenthalpic Joule-Thomson effect (Gustafsson, 1970;Maytal and Pfotenhauer, 2013), which can be defined as the temperature drop when the mixture is subject to a given decompression:…”
Section: Introductionmentioning
confidence: 99%
“…A clue to the route by which heat is transmitted through the corona to the solar wind is provided by the predominance of H and He in the Sun's composition. These are two of the three gases (the third is neon) with such a low inversion temperature that is above ambient temperature and under isoenthalpic conditions, their response to the Joule-Thomson effect is heating rather than cooling [22]. In the absence of experimental data for coronal temperatures we must rely on extrapolation of inversion curves [23], but to advance the discussion we note that at very high temperatures the Joule-Thomson coefficient μJT may be represented by -b/Cp [24], where b is of course one of the two constants that distinguish the van der Waals equation from the Real Gas Law and that vary according to the gas at issue, and Cp is the heat capacity.…”
mentioning
confidence: 99%