2015
DOI: 10.1021/ie5038903
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Thermodynamic Properties of Dichloromethane, Bromochloromethane, and Dibromomethane under Elevated Pressure: Experimental Results and SAFT-VR Mie Predictions

Abstract: The speeds of sound in dibromomethane, bromochloromethane, and dichloromethane have been measured in the temperature range from 293.15 to 313.15 K and at pressures up to 100 MPa. Densities and isobaric heat capacities at atmospheric pressure have been also determined. Experimental results were used to calculate the densities and isobaric heat capacities as the function of temperature and pressure by means of a numerical integration technique. Moreover, experimental data at atmospheric pressure were then used t… Show more

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Cited by 13 publications
(8 citation statements)
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“…1 shows intervals, where the crossing occurs, for the series of α, ωdibromoalkanes. They are quite close to the ones found experimentally [17,18] although we use only the data measured at the normal conditions as referent ones.…”
Section: The Crossing Of Expansivity Isotherms and Molecular Packingsupporting
confidence: 86%
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“…1 shows intervals, where the crossing occurs, for the series of α, ωdibromoalkanes. They are quite close to the ones found experimentally [17,18] although we use only the data measured at the normal conditions as referent ones.…”
Section: The Crossing Of Expansivity Isotherms and Molecular Packingsupporting
confidence: 86%
“…The present model was tested using experimental data concerning the density, the speed of sound and the thermal expansivity of α, ω-dibromoalkanes (1,3-dibromopropane to 1,6-dibromohexane [17], dibromomethane [18], and the results of recent new measurements for 1,2-dibromoethane [19], which complete this series), a polar non-associated liquid in which important electrostatic intermolecular interactions occur due to the permanent dipole moments of the molecules. In addition, these compounds are characterized by the socalled intramolecular proximity effect [20], according to which a change in the distance between two halogen atoms in the molecule causes a change in the molecular properties.…”
Section: The Crossing Of Expansivity Isotherms and Molecular Packingmentioning
confidence: 99%
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“…QM/MM simulations and calculations of Franck–Condon factors and electronic-interaction matrix elements were performed as described, , using the restricted Hartree–Fock (RHF) programs ENZYQ and INDIP for photochemical charge separation in HPQ, and their unrestricted Hartree–Fock (UHF) versions (ENZYQ-uhf and INDIP-uhf) for the reactions of the BIP–BQO and BIP–NAP radicals. Each system included an all-atom bath of iso-octane, dichloromethane, or 2-methyltetrahydrofuran composed of the number of solvent molecules required to fill a sphere with a radius of 23.0 Å to the proper density at atmospheric pressure and 296 K. The volume of the sphere was adjusted as necessary to give the measured densities of the solvents at other temperatures. The atomic charges, polarizabilities, dipole moments, and MM parameters for the solvents were the same as used previously. ,, The atomic charges of 2-methyltetrahydrofuran were from Tan et al Fields from the induced dipoles of solvent atoms were evaluated at each step, and interactions with these fields contributed to the energies of the subsystem that was treated quantum mechanically.…”
Section: Methodsmentioning
confidence: 99%
“…This study continues a series of investigations implementing an acoustic method for determining various thermodynamic properties of α,ω-dihaloalkanes in the temperature range from 293.15 to 313.15 K and at pressures up to 100 MPa. Previously, the data on 1,3-dibromopropane and 1,5-dibromopentane; 1,4-dibromobutane and 1,6-dibromohexane; and dichloromethane, bromochloromethane, and dibromomethane have been reported. Yet 1,2-dichloroethane and 1,2-dibromoethane are considered.…”
Section: Introductionmentioning
confidence: 99%