Measurements of the liquidliquid coexistence curve for hexamethyldisiloxane, octamethyltrisiloxane or decamethyltetrasiloxanetetradecafluorohexane near the upper critical endpoint and of the upper coexistence temperatures T
UCX
for equivolume mixtures of 21 other mixtures of this kind confirm the basic similarity of the thermodynamics of such mixtures to those of alkaneperfluoroalkane mixtures. The upper critical solution temperatures
T
UCS
increase linearly within the range studied with perfluoroalkane chain length and nearly so with dimethylsiloxane chain length. The coexistence curves have been fitted to Wegner extended-scaling expressions in order to investigate the universality of the shape. The temperaturevolume-fraction (
T−
φ) representation is more symmetrical than that in mole fraction and with a reduced temperature
![[T with combining tilde]](https://www.rsc.org/images/entities/i_char_0054_0303.gif)
=(
T/
T
UCS
), withthe upper critical solution temperature
T
UCS
as the reduction factor, the (
![[T with combining tilde]](https://www.rsc.org/images/entities/i_char_0054_0303.gif)
−
φ) representation is universal for all threemixtures as well as nearly so for the comparison mixture C
6
H
14
C
6
F
14
.
T
UCS
(C
6
H
14
C
6
F
14
)=295.80 K and
T
UCS
(hexamethyldisiloxaneC
6
F
14
)=296.95 K are unsurprisingly close, in view of the near-equal temperature reduction factors of hexamethyldisiloxane and hexane. The effect of this correspondence is extended to the analysis of the
T
UCX
of the other mixtures. The results are discussed in terms of the solubility parameter version of the regular solution theory incorporating the Flory–Huggins entropy of mixing term. With a correction of nearly 10% on the geometric-mean combining rule for the cohesive energy density
T
UCS
is reasonably well predicted. For these mixtures, the critical mole fraction is also surprisingly well predicted from the ratio of component molar volumes.