2012
DOI: 10.1063/1.3703507
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Interfacial and coexistence properties of soft spheres with a short-range attractive Yukawa fluid: Molecular dynamics simulations

Abstract: Molecular dynamics simulations have been carried out to obtain the interfacial and coexistence properties of soft-sphere attractive Yukawa (SAY) fluids with short attraction range, κ = 10, 9, 8, 7, 6, and 5. All our simulation results are new. These data are also compared with the recently reported results in the literature of hard-core attractive Yukawa (HAY) fluids. We show that the interfacial and coexistence properties of both potentials are different. For the surveyed systems, here we show that all coexis… Show more

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Cited by 8 publications
(4 citation statements)
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“…Apart from simple spherical models, during the last two decades the interfacial properties of molecular model systems have been investigated using both Monte Carlo and molecular dynamics techniques of a number of systems interacting through different intermolecular potentials, mostly LJ and Mie [2][3][4][5][6][7][8][9][10][11][12][13][14][15] , but also systems that interact via the hard-core Yukawa potential [16][17][18][19][20] , and the square-well (SW) potential 5,9,17,[21][22][23][24][25][26][27][28] . In fact, whereas the computation of interfacial properties of polymer models have been the subject of a number of recent papers, [29][30][31][32][33] results for the well known fully-flexible SW model, in which square-well segments (monomers) of diameter σ and potential range λ are tangentially bonded to form molecular chains are scarce.…”
Section: Introductionmentioning
confidence: 99%
“…Apart from simple spherical models, during the last two decades the interfacial properties of molecular model systems have been investigated using both Monte Carlo and molecular dynamics techniques of a number of systems interacting through different intermolecular potentials, mostly LJ and Mie [2][3][4][5][6][7][8][9][10][11][12][13][14][15] , but also systems that interact via the hard-core Yukawa potential [16][17][18][19][20] , and the square-well (SW) potential 5,9,17,[21][22][23][24][25][26][27][28] . In fact, whereas the computation of interfacial properties of polymer models have been the subject of a number of recent papers, [29][30][31][32][33] results for the well known fully-flexible SW model, in which square-well segments (monomers) of diameter σ and potential range λ are tangentially bonded to form molecular chains are scarce.…”
Section: Introductionmentioning
confidence: 99%
“…This contrasts with the modeling of the core hardness as a power-law, (1/x) n . In this case, even considering extremely large exponents, n > 200, the differences in the coexistence properties between the approximation and the hard-core case do not vanish 32 . A final remarkable issue is that the data series for α = 400 is indistinguishable from the one for α = 800.…”
Section: Resultsmentioning
confidence: 89%
“…It is worth mentioning that the constant-force approximation contrasts previous works where the core hardness is modeled by adding a high-exponent power-law contribution 32,39,40 .…”
Section: Introductionmentioning
confidence: 98%
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