Abstract:Total-pressure vapor-liquid equilibrium (VLE) data are reported at approximately 298, 348, and 398 K for each of three nitromethane binaries with ethyl acetate, acetonitrile, and acetone as the other components. The experimental PTx data were reduced to y¡, ;, and GE values by both the Mlxon-Gumowskl-Carpenter and the Barker methods, but only the Mixon et al. results are reported In their entirety. Seven GE correlations were tested In the Barker data reduction with the five-constant Redllch-KIster equation giv… Show more
“…Below the normal boiling temperature (354 K), the majority of the results are within 1% of our work, but results obtained by Hall and Baldt 19 are lower by up to almost 7%, while those obtained by Owens et al are too high by about 3%. Near room temperature, Francesconi et al lies above our equation by almost 6% (to give a total span of more than 12% in the literature data) but is lower by between 1 and 4% above 350 K. Mousa also lies 4% below our work near the critical state but by 6% at 440 K. …”
The vapor pressures of acetonitrile have been measured over the temperature and pressure range of
278 K and 4.3 kPa to 540 K and 4455 kPa. The upper limit exceeds the temperature at which decomposition
of acetonitrile begins (about 536 K) so we were able to assess the effect of pyrolysis on the vapor pressures.
Acetonitrile is strongly hygroscopic, and a comparison of results obtained with “wet” and “dry” samples
allowed us to investigate in a similar way the effect of water as an impurity. The results have been
correlated using generalized Wagner equations, a key feature of which is the use of the reversed reduced
temperature τ = 1 − T/T
c where T
c is the critical temperature. The standard form with terms in τ, τ
1.5,
τ
2.5, and τ
5 produced unacceptable systematic deviations; but the equation ln(p/p
c) = (T
c/T)(c
1τ + c
1.5τ1.5
+ c
2τ2 + c
2.5τ2.5 + c
5.5τ5.5), where p
c is the critical pressure, fits our results from 291 K to 535 K with a
standard deviation of 63 × 10-6 in ln p and significantly extends the range of correlation, toward both
the triple and critical points, compared with work already in the literature. By extrapolation to T
c =
545.46 K, we obtain 4835 kPa for the critical pressure p
c and 167 Pa for the triple-point pressure at
T
s+l+g = 229.35 K. An Antoine equation that describes the results below a pressure of 125 kPa with a
standard deviation of 1.5 mK in the condensation temperature has also been obtained.
“…Below the normal boiling temperature (354 K), the majority of the results are within 1% of our work, but results obtained by Hall and Baldt 19 are lower by up to almost 7%, while those obtained by Owens et al are too high by about 3%. Near room temperature, Francesconi et al lies above our equation by almost 6% (to give a total span of more than 12% in the literature data) but is lower by between 1 and 4% above 350 K. Mousa also lies 4% below our work near the critical state but by 6% at 440 K. …”
The vapor pressures of acetonitrile have been measured over the temperature and pressure range of
278 K and 4.3 kPa to 540 K and 4455 kPa. The upper limit exceeds the temperature at which decomposition
of acetonitrile begins (about 536 K) so we were able to assess the effect of pyrolysis on the vapor pressures.
Acetonitrile is strongly hygroscopic, and a comparison of results obtained with “wet” and “dry” samples
allowed us to investigate in a similar way the effect of water as an impurity. The results have been
correlated using generalized Wagner equations, a key feature of which is the use of the reversed reduced
temperature τ = 1 − T/T
c where T
c is the critical temperature. The standard form with terms in τ, τ
1.5,
τ
2.5, and τ
5 produced unacceptable systematic deviations; but the equation ln(p/p
c) = (T
c/T)(c
1τ + c
1.5τ1.5
+ c
2τ2 + c
2.5τ2.5 + c
5.5τ5.5), where p
c is the critical pressure, fits our results from 291 K to 535 K with a
standard deviation of 63 × 10-6 in ln p and significantly extends the range of correlation, toward both
the triple and critical points, compared with work already in the literature. By extrapolation to T
c =
545.46 K, we obtain 4835 kPa for the critical pressure p
c and 167 Pa for the triple-point pressure at
T
s+l+g = 229.35 K. An Antoine equation that describes the results below a pressure of 125 kPa with a
standard deviation of 1.5 mK in the condensation temperature has also been obtained.
“…VLE of binary mixtures of n ‐alkanes, n ‐pentane (○) n ‐hexane (□), n ‐heptane (∆), with low dipolar strength fluids, (a) dichloromethane at T = 298 K, and (b) tetrahydrofuran at P = 0.101 MPa. Polar soft‐SAFT predictions (solid lines), and polar soft‐SAFT calculations with ξ = 0.997 (dashed lines) compared to experimental data of mixtures with dichloromethane 64‐68 and tetrahydrofuran 69‐71 (symbols). See text for details [Color figure can be viewed at wileyonlinelibrary.com]…”
Section: Resultsmentioning
confidence: 99%
“…Conversely, extending polar and nonpolar models of chloroform to binary mixtures with n-alkanes resulted in a different behavior as shown in Figure 3b, contrary to the earlier results with 1-hexene. The predictions from polar soft-SAFT for the VLE of chloroform, modeled as a polar fluid, with n-hexane (T = 318), 60 n-heptane (T = 298 K), 61 and n-decane (T = 298 K) 62 Polar soft-SAFT predictions for modeling binary mixtures of npentane and n-hexane with dichloromethane at 298 K, 64,65 shown in Figure 4a, are highly accurate in representing the experimental VLE behavior, in particular capturing the azeotrope of DCM + n-pentane, even at other conditions [64][65][66][67][68] (see Figure S7 in the Supporting Information). Similarly, as seen in Figure 4b, polar soft-SAFT provides accurate predictions of the VLE experimental behavior of binary mixtures of n-pentane, n-hexane, and n-heptane with tetrahydrofuran at 0.101 MPa, [69][70][71] with a high level of accuracy, slightly underestimating the azeotropic pressure of THF + n-hexane with a relative deviation of 1.9%.…”
Section: Pure Substancesmentioning
confidence: 96%
“…Polar soft-SAFT predictions for modeling binary mixtures of npentane and n-hexane with dichloromethane at 298 K, 64,65 shown in Figure 4a, are highly accurate in representing the experimental VLE behavior, in particular capturing the azeotrope of DCM + n-pentane, even at other conditions [64][65][66][67][68] (see Figure S7 in the Supporting Information). Similarly, as seen in Figure 4b, polar soft-SAFT provides accurate predictions of the VLE experimental behavior of binary mixtures of n-pentane, n-hexane, and n-heptane with tetrahydrofuran at 0.101 MPa, [69][70][71] with a high level of accuracy, slightly underestimating the azeotropic pressure of THF + n-hexane with a relative deviation of 1.9%.…”
Section: Phase Equilibria Of Binary Mixtures Of N-alkanes With Moderate Dipolar Fluids: Dichloromethane Tetrahydrofuran and Acetonementioning
confidence: 99%
“…These excellent results obtained in mixtures of 2-ketones, primarily acetone, with n-alkanes demonstrate the robust framework of polar soft-SAFT considering all the predictions (VLE/LLE of acetone + n-alkanes, and VLE of other 2-ketones + nalkanes) are done using a single binary parameter independent of both temperature and n-alkane, fitted at a single high temperature isotherm from VLE of acetone + n-pentane.F I G U R E 4 VLE of binary mixtures of n-alkanes, n-pentane () n-hexane (□), nheptane (Δ), with low dipolar strength fluids, (a) dichloromethane at T = 298 K, and (b) tetrahydrofuran at P = 0.101 MPa. Polar soft-SAFT predictions (solid lines), and polar soft-SAFT calculations with ξ = 0.997 (dashed lines) compared to experimental data of mixtures with dichloromethane[64][65][66][67][68] and tetrahydrofuran[69][70][71] (symbols). See text for details [Color figure can be viewed at wileyonlinelibrary.com] F I G U R E 5 Phase equilibria of binary mixtures of acetone with n-alkanes, (a) VLE with n-butane at 330 K 72 (◊), npentane at 373 K 73 (), (b) VLE at 313 K 74 with n-hexane (□), n-heptane, and noctane.…”
We present results concerning the phase equilibria and excess properties of binary mixtures of n-alkanes with a range of fluids from low to high dipolar strength, namely 1-hexene, chloroform, dichloromethane, tetrahydrofuran, acetone, dimethylformamide, and N-methyl pyrrolidone modeled by polar soft-statistical associating fluid theory. Polar interactions are considered through the theory of Gubbins and Twu, extended to chainlike fluids by Jog and Chapman, and a priori fixing the polar parameters of the pure fluids, instead of fitting to experimental data. The equation provides accurate predictions for low to moderate dipolar molecules with n-alkanes, while the induced dipoles created by very strong dipolar fluids (μ ≥ 3.5 D), is implicitly considered by the appropriate selection of pure component parameters and a binary parameter which can be transferred to predict other properties. The equation is used to systematically study the effect of asymmetrical energy scales between polar and nonpolar fluids on vapor-liquid equilibria and excess properties.
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