1984
DOI: 10.1021/j150649a037
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Isothermal compressibility of benzene, deuteriobenzene (C6D6), cyclohexane, and deuteriocyclohexane (c-C6D12), and their mixtures from 0.1 to 35 Mpa at 288, 298, and 313 K

Abstract: The densities of the title compounds and of their solutions (0,25,50,75, and 100 nominal mol %) have been measured between 0.1 and 35 MPa at 15, 25, and 40 OC. The data are reported in terms of the parameters of fit to the Tait equation, and as volumes, compressibilities, K, and reduced compressibilities, KR (KR-I = V/(KRT)), and as excess volumes, excess compressibilities, and excess reduced compressibilities for the solutions. The melting points of C6H12 and C6D12 are reported from 0.1 to 25 MPa. Isotope eff… Show more

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Cited by 27 publications
(16 citation statements)
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“…Table 1 lists the flt.orinated ethers for which volumetric property measurements have been made. Van Hook and co-workers determined liquid densities for a series of fluorinated ethels as a function of temperature and pressure in two ways: The first [ 14] employed a Mettler-Paar vibratingtt, be DMA-05 densimeter for (0.1<p<35MPa) and (298<T<the lesser of 373 K or 0.92 T~,), where T~ is the critical temperature; the second employed the (p, I" m, T) apparatus described by Kooner and Van Hook [ 15. 16] for (0.1 < p < 6 MPa) fi'om room temperature to T~..…”
Section: Assessment Of Datamentioning
confidence: 99%
“…Table 1 lists the flt.orinated ethers for which volumetric property measurements have been made. Van Hook and co-workers determined liquid densities for a series of fluorinated ethels as a function of temperature and pressure in two ways: The first [ 14] employed a Mettler-Paar vibratingtt, be DMA-05 densimeter for (0.1<p<35MPa) and (298<T<the lesser of 373 K or 0.92 T~,), where T~ is the critical temperature; the second employed the (p, I" m, T) apparatus described by Kooner and Van Hook [ 15. 16] for (0.1 < p < 6 MPa) fi'om room temperature to T~..…”
Section: Assessment Of Datamentioning
confidence: 99%
“…In this work, we report extensive data of several thermophysical properties of acetone-d 6 in broad temperature and pressure ranges, which when combined with those of acetone-h 6 , permit us to test the reliability of a simple statistical-mechanics approach for heat capacitiy isotope effects. Unfortunately, in contrast to the situation encountered regarding many other properties, there is not, to date, a well-established theory for molar volume isotope effects [2][3][4][5][6][7][8][9][10][11][12]. The rather murky procedure of establishing links between molecular structure and density combined with the lack of extensive (and accurate) data on the molar density shifts upon isotopic substitution are the responsible factors.…”
Section: Introductionmentioning
confidence: 99%
“…While, generally, one can state that, condensed phase IEs are very well interpreted in the light of the quantum-mechanical statistical theory of IEs as originally formulated by Bigeleisen [7] and further developed by Stern et al [8], volumetric and volumerelated properties IEs are currently the least well understood of all IEs on equilibrium physical properties. Matsuo and Van Hook [9] thoroughly investigated the influence of isotopic substitution on the experimental volumetric properties of benzene, cyclohexane and their mixtures, interpreting it in a semi-quantitative fashion. In the same vein, Kooner and Van Hook [3] discussed the high temperature results obtained for acetone.…”
Section: Introductionmentioning
confidence: 99%
“…For substances which are associated through hydrogen bonds there are additional reasons for the change in the intermolecular distance when the hydrogen atoms forming these bonds are replaced by deuterium. It has been shown [9,10] that this substitution produces an appreciable change in length of hydrogen bond, i.e. O---O distance.…”
Section: Resultsmentioning
confidence: 99%