THERMAL CYCLE AROUND THE CRITICAL-POINT OF CARBON-DIOXIDE UNDER REDUCED GRAVITY

Citation
P. Guenoun et al., THERMAL CYCLE AROUND THE CRITICAL-POINT OF CARBON-DIOXIDE UNDER REDUCED GRAVITY, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics, 47(3), 1993, pp. 1531-1540
Citations number
28
ISSN journal
1063651X
Volume
47
Issue
3
Year of publication
1993
Pages
1531 - 1540
Database
ISI
SICI code
1063-651X(1993)47:3<1531:TCATCO>2.0.ZU;2-M
Abstract
In order to investigate the different aspects of the transport of heat in the absence of gravity, we performed a thermal cycle close to and around the critical point of CO2 at critical density. Reduced gravity was provided during a 6-min flight of a sounding rocket. A cell has be en designed which allows surface and bulk phenomena to be distinguishe d. Special optical devices are used to observe the sample and measure locally temperature and density. We also present experiments under Ear th's gravity at a few mK from the critical temperature (T(c)). Convect ion patterns are observed which correspond to Grashof numbers as large as a few 10(4). The thermal cycle of the experiment in weightlessness starts at T(c) +2.5 mK, where we study the relaxation of the perturba tions caused by liftoff: fluid flows, density and temperature gradient s. We then investigate the effect of a quench from T(c) + 2.3 to T(c) + 1.3 mK, and the expected mechanism of heat transport by the ''Piston effect'' (PE) is experimentally evidenced. In particular, we observe homogeneous thermalization, with a time of thermalization less than a few seconds. We compare this time with a number of theoretical estimat ions. During thermalization, density and temperature gradients are not affected by the PE and are seen to relax diffusively. We perform then a quench at T(c) - 0.8 mK. We observe the onset of phase separation, making a clear visualization of the PE. Thereafter, spinodal decomposi tion occurs, followed by the growth of a bicontinuous pattern of gas a nd liquid domains. After a last quench back to T(c) + 2.0 mK, we still observe the PE in spite of the presence of density gradients. These g radients are seen to relax by diffusion.