3 research outputs found
Viscosities and Densities of Binary Mixtures of Hexadecane with Dissolved Methane or Carbon Dioxide at Temperatures from (298 to 473) K and at Pressures up to 120 MPa
We report measurements
of the viscosity and density of two binary
mixtures comprising hexadecane with dissolved carbon dioxide or methane
over the temperature range from (298.15 to 473.15) K and at pressures
up to 120 MPa. The measurements were conducted at various mole fractions <i>x</i> of the light component as follows: <i>x</i> =
(0, 0.0690, 0.5877, and 0.7270) for <i>x</i>CO<sub>2</sub> + (1 – <i>x</i>)C<sub>16</sub>H<sub>34</sub> and <i>x</i> = (0, 0.1013, 0.2021, 0.2976, and 0.3979) for <i>x</i>CH<sub>4</sub> + (1 – <i>x</i>)C<sub>16</sub>H<sub>34</sub>. The viscosity and density measurements were carried
out simultaneously using a bespoke vibrating-wire apparatus with a
suspended sinker. With respect to the first mixture, the apparatus
was operated in a relative mode and was calibrated in octane whereas,
for the second mixture, the apparatus was operated in an absolute
mode. To facilitate this mode of operation, the diameter of the centerless-ground
tungsten wire was measured with a laser micrometer, and the mass and
volume of the sinker were measured independently by hydrostatic weighing.
In either mode of operation, the expanded relative uncertainties at
95% confidence were 2% for viscosity and 0.3% for density. The results
were correlated using simple relations that express both density and
viscosity as functions of temperature and pressure. For both pure
hexadecane and each individual mixture, the results have been correlated
using the modified Tait equation for density, and the Tait–Andrade
equation for viscosity; both correlations described our data almost
to within their estimated uncertainties. In an attempt to model the
viscosity of the binary mixtures as a function of temperature, density,
and composition, we have applied the extended-hard-sphere model using
several mixing rules for the characteristic molar core volume. The
most favorable mixing rule was found to be one based on a mole-fraction-weighted
sum of the pure component molar core volumes raised to a power γ
which was treated as an adjustable parameter. In this case, deviations
of the experimental viscosities from the model were within ±25%
Densities of Aqueous MgCl<sub>2</sub>(aq), CaCl<sub>2</sub>(aq), KI(aq), NaCl(aq), KCl(aq), AlCl<sub>3</sub>(aq), and (0.964 NaCl + 0.136 KCl)(aq) at Temperatures Between (283 and 472) K, Pressures up to 68.5 MPa, and Molalities up to 6 mol·kg<sup>–1</sup>
We report the densities of MgCl<sub>2</sub>(aq), CaCl<sub>2</sub>(aq), KI(aq), NaCl(aq), KCl(aq), AlCl<sub>3</sub>(aq), and
the mixed
salt system [(1 – <i>x</i>)NaCl + <i>x</i>KCl](aq), where <i>x</i> denotes the mole fraction of KCl,
at temperatures between (283 and 472) K and pressures up to 68.5 MPa.
The molalities at which the solutions were studied were (1.00, 3.00,
and 5.00) mol·kg<sup>–1</sup> for MgCl<sub>2</sub>(aq),
(1.00, 3.00, and 6.00) mol·kg<sup>–1</sup> for CaCl<sub>2</sub>(aq), (0.67, 0.90, and 1.06) mol·kg<sup>–1</sup> for KI(aq), (1.06, 3.16, and 6.00) mol·kg<sup>–1</sup> for NaCl(aq), (1.06, 3.15, and 4.49) mol·kg<sup>–1</sup> for KCl(aq), (1.00 and 2.00) mol·kg<sup>–1</sup> for
AlCl<sub>3</sub>(aq), and (1.05, 1.98, 3.15, and 4.95) mol·kg<sup>–1</sup> for [(1 – <i>x</i>)NaCl + <i>x</i>KCl](aq), with <i>x</i> = 0.136. The measurements
were performed with a vibrating-tube densimeter calibrated under vacuum
and with pure water over the full ranges of pressure and temperature
investigated. An analysis of uncertainties shows that the relative
uncertainty of density varies from 0.03 % to 0.05 % depending upon
the salt and the molality of the solution. An empirical correlation
is reported that represents the density for each brine system as a
function of temperature, pressure, and molality with absolute average
relative deviations of approximately 0.02 %. Comparing the model with
a large database of results from the literature, we find absolute
average relative deviations of 0.03 %, 0.06 %, 0.04 %, 0.02 %, and
0.02 % for the systems MgCl<sub>2</sub>(aq), CaCl<sub>2</sub>(aq),
KI(aq), NaCl(aq), and KCl(aq), respectively. The model can be used
to calculate density, apparent molar volume, and isothermal compressibility
over the full ranges of temperature, pressure, and molality studied
in this work. An ideal mixing rule for the density of a mixed electrolyte
solution was tested against our mixed salt data and was found to offer
good predictions at all conditions studied with an absolute average
relative deviation of 0.05 %
Composition Analysis and Viscosity Prediction of Complex Fuel Mixtures Using a Molecular-Based Approach
The automobile industry currently faces the challenge
of developing
a new generation of diesel motor engines that satisfy both increasingly
stringent emission regulations and reduces specific fuel consumption.
The performance of diesel engines, seen in terms of emissions and
specific fuel consumption, generally improves with increasing fuel-injection
pressure. The design of the next generation of diesel fuel injection
systems requires the knowledge of the thermophysical properties, in
particular viscosity, of a wide-type of diesel fuels at pressures
up to 300 MPa or more. The objective of the present work is to demonstrate
that it is possible to predict the viscosity of any petroleum-based
diesel fuel, using, exclusively, its molar fraction distribution as
provided by multidimensional gas chromatography techniques. The precise
knowledge of the fuel chemical constituents allows the understanding
of the influence of the different hydrocarbon families on the fluid
viscosity by means of molecular dynamics simulations. The accuracy
of the Anisotropic United Atom force-field was tested and was found
to be in agreement with experimental viscosities obtained with a new
vibrating wire device at different temperatures and pressures up to
300 MPa. Finally, the experimental and simulated viscosities have
been compared with improved group contribution method that has been
coupled with gas chromatography experimental measurements for a viscosity
prediction that was estimated to be of less than 18% of mean absolute
deviation