Pj. Smits et al., HIGH-PRESSURE PHASE-BEHAVIOR OF (XCHF(3)-X)H2O) AND (X(1)CHF(3)+X(2)NACL+(1-X(1)-X(2))H2O)((1), Journal of Chemical Thermodynamics, 29(12), 1997, pp. 1517-1525
Experimental results of the high-pressure phase behaviour for {xCHF(3)
+ (1 - x)H2O) and {x(1)CHF(3) + x(2)NaCl + (1 - x(1) - x(2))H2O} are
presented. (Gas + gas) equilibria for five compositions with x(CHF3) (
0.0334 +/- 0.0002)< x < (0.1389 +/- 0.0002) as well as for six composi
tions with x(1)(CHF3) (0.0305 +/- 0.0002) < x(1) < (0.1096 +/- 0.0002)
, and mole fractions x(2)(NaCl) (0.0046 +/- 0.0002) < x(2) < (0.0100 /- 0.0002) were measured in a high-pressure autoclave equipped with sa
pphire windows and magnetic stirring. The phase transitions were deter
mined visually. The pressure ranged from 20 MPa to 200 MPa, and the te
mperature from T = 470 K to T = 625 K. The (xCHF(3) + (1 - x)H2O} exhi
bits a type-III fluid phase behaviour without (gas + gas) immiscibilit
y of the first kind. Isopleths for NaCl mass fractions omega = (0.0167
7 and 0.03336) relative to H2O are shifted towards higher temperatures
compared with the binary mixture {xCHF(3) + (1 - x)H2O). In this syst
em the temperature shift is more pronounced than for isopleths in the
system (xCF(4) + (1 - x)H2O} upon NaCl addition. The objective of this
study was to investigate the phase behaviour of model-systems encount
ered in supercritical water oxidation processes. (C) 1997 Academic Pre
ss Limited.