Abstract
Fluids at supercritical pressure undergo a continuous phase from a liquid to a gas state if the fluid is heated above the critical pressure. During this phase transition the thermophysical properties of the fluid vary significantly within a narrow temperature range across the pseudo-critical temperature T pc Tpc
(pseudo-critical temperature is defined as the temperature at which the specific heat at constant pressure (c p cp
) attains its peak value). Figure 1 shows the variation of thermophysical properties of CO 2 2
at a thermodynamic supercritical pressure P 0 P0
= 80 bar (P critical =73.773bar Pcritical=73.773bar
) as a function of temperature (Int J Thermophys 24, 1–39 (2003)) [1]. These characteristics make supercritical fluids appealing in many industrial applications, such as: desorption, drying and cleaning in extraction processes; pharmaceutical industry; in power cycles as working fluids (Renew Sustain Energy Rev 14, 3059–3067 (2010)) [2] , (Nucl Technol 154, 283–301 (2006)) [3] and biodiesel production ( Fuel 80, 225–231 (2001)) [4].
Original language | English |
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Title of host publication | Direct and Large-Eddy Simulation X |
Editors | D.G.E. Grigoriadis, B.J. Geurts, H. Kuerten, J. Fröhlich, V. Armenio |
Place of Publication | Cham, Switzerland |
Publisher | Springer |
Pages | 545-551 |
Volume | 24 |
ISBN (Electronic) | 978-3-319-63212-4 |
ISBN (Print) | 978-3-319-63211-7 |
DOIs | |
Publication status | Published - 2015 |
Event | ERCOFTAC WORKSHOP Direct and Large Eddy Simulation 10 - Limassol, Cyprus Duration: 27 May 2015 → 29 May 2015 http://dles10.org/home |
Publication series
Name | ERCOFTAC Series |
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Publisher | Springer |
Volume | 24 (2017) |
Conference
Conference | ERCOFTAC WORKSHOP Direct and Large Eddy Simulation 10 |
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Abbreviated title | DLES-10 |
Country/Territory | Cyprus |
City | Limassol |
Period | 27/05/15 → 29/05/15 |
Internet address |