3 research outputs found
Molecular Simulations of the Thermophysical Properties of Polyethylene Glycol Siloxane (PEGS) Solvent for Precombustion CO<sub>2</sub> Capture
The
thermophysical properties for neat polyethylene glycol siloxane
solvent (PEGS) along with CO<sub>2</sub>, H<sub>2</sub>, H<sub>2</sub>O, and H<sub>2</sub>S gas absorption in PEGS at 298ā373 K
were investigated via molecular simulations. The predicted neat PEGS
density, heat capacity, surface tension, and CO<sub>2</sub> and H<sub>2</sub> solubilities in PEGS solvent agree reasonably well with the
experimental data, with typical differences of 0.8ā20%, while
the predicted PEGS solvent viscosity is 1.7ā2.5 times larger
than the experimental data. Gas solubility in PEGS at 298 K decreases
in the following order, H<sub>2</sub>O (31000) > H<sub>2</sub>S
(230)
> CO<sub>2</sub> (33) > H<sub>2</sub> (1), which follows the
same
order as the gasāPEGS interaction. In contrast, gas diffusivity
in PEGS at 298 K decreases in an opposite way, H<sub>2</sub> (1) >
CO<sub>2</sub> (0.22) ā H<sub>2</sub>S (0.12) > H<sub>2</sub>O (0.018). The numbers in parentheses are the corresponding values
relative to H<sub>2</sub>. Compared to the widely studied polyĀ(dimethylsiloxane)
(PDMS) solvent, PEGS is more hydrophilic due to its stronger interaction
with H<sub>2</sub>O and fewer branched āCH<sub>3</sub> groups,
which in turn leads to fewer hydrophobic pockets. The CO<sub>2</sub>/H<sub>2</sub> solubility selectivity in PEGS is larger than that
in PDMS due to a stronger interaction with CO<sub>2</sub> in PEGS.
Finally, it was found that CO<sub>2</sub> absorption in PEGS could
significantly improve the CO<sub>2</sub>āPEGS solution dynamics
by 5ā6 times, resulting in a decrease in solution viscosity
and increase in diffusivity. These CO<sub>2</sub> absorption effects
are due to solution volume expansion upon CO<sub>2</sub> absorption
compared to the neat PEGS solvent volume and the possibility that
CO<sub>2</sub> acts as a ālubricantā to decrease the
solventāsolvent interaction
Viscosity Measurements of Two Potential Deepwater Viscosity Standard Reference Fluids at High Temperature and High Pressure
This paper reports
high-pressure viscosity measurements for Krytox
GPL 102 lot K2391 and trisĀ(2-ethylhexyl) trimellitate (TOTM). These
two viscous liquids have recently been suggested as potential deepwater
viscosity standard (DVS) reference fluids for high temperature, high
pressure viscosity studies associated with oil production from ultradeep
formations beneath the deepwaters of the Gulf of Mexico. The measurements
are performed using a windowed, variable-volume, rolling-ball viscometer
at pressures between 7 and 242 MPa and temperatures between 314 and
527 K with an expanded uncertainty of 3% at a 95% confidence level.
The viscosity results are correlated using an empirical temperature/pressure-dependent
function and a modified VogelāFulcherāTammann (VFT)
Equation. The present viscosity data for TOTM and Krytox GPL 102 lot
K2391 are in good agreement with the available reported data in the
literature at lower temperatures and pressures. The viscosity values
of TOTM and Krytox GPL 102 lot K2391 are 9.5 mPaĀ·s and 25 mPaĀ·s,
respectively, at 473 K and 200 MPa, whereas the desired DVS viscosity
value at this condition is 20 mPaĀ·s. Although the viscosity of
Krytox GPL 102 lot K2391 is closer to the targeted value, a comparison
of the present viscosity results with data obtained for lot K1537
indicates a very large lot-to-lot variation of the viscosity for this
polydisperse perfluoropolyether oil, which represents a significant
deficiency for a DVS
High-Temperature, High-Pressure Volumetric Properties of Propane, Squalane, and Their Mixtures: Measurement and PC-SAFT Modeling
This study reports the high-temperature,
high-pressure density
data for propane, squalane, and their binary mixtures for five compositions
at temperatures to 520 K and pressures to 260 MPa. The density measurements
are obtained with a floating-piston, variable-volume, high-pressure
view cell. From the density data, the isothermal and isobaric excess
molar volumes upon mixing are computed. For the mixture compositions
studied here, the excess volume is mostly negative, showing a minimum
at 0.6550 mole fraction of propane and becomes less negative as the
propane concentration increases. The perturbed-chain statistical associating
fluid theory (PC-SAFT) equation of state (EoS) provides good representation
for the experimental data. A mean absolute percent deviation (Ī“)
of 1.4% is obtained with the PC-SAFT EoS when using propane and squalane
pure component parameters fit to density data at high-temperature,
high-pressure conditions