2003
DOI: 10.1103/physreve.67.046404
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Gibbs-Bogolyubov inequality and transport properties for strongly coupled Yukawa fluids

Abstract: The Gibbs-Bogolyubov inequality is used to establish a mapping between the Yukawa system and both the hard-sphere and the one-component reference systems. The transport coefficients of self-diffusion, shear viscosity, and thermal conductivity are computed for the Yukawa fluid using known properties of the reference systems. Comparisons are made with simulation results. For sufficiently strong screening, the hard-sphere reference system yields a lower upper bound of the Yukawa Helmholtz free energy and a better… Show more

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Cited by 75 publications
(83 citation statements)
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“…It is observed, that the results of λ 0 are within the range of ~7-50% for EMD, 10-16% for NEMD, and ~10-40% for HPMD. Moreover, Figure 3(a) shows, that obtained thermal conductivity at F ext = 0.005 for N = 864 is in good agreement with HPMD simulation of Shahzad and He [1], but it is noted, that our results are slightly greater than EMD of Salin and Caillol [19], NEMD of Donko and Hartmann [20], and VP of Faussurier and Murillo [21] at lower values of Γ. Deviation of the present data from EMD, HPMD, and inhomogeneous that diferences between the simulation data calculated by diferent authors are large at some state points and diferences with their own present data sets are much smaller. Plasma's thermal conductivity is generally overpredicted within ~3-17% (~8-15%), ~5-30% (~5-38%), and ~5-40% (~3-17%) relative to the data of EMD by Salin and Caillol [19], inhomogeneous NEMD by Donko and Hartman [20], and HPMD by Shahzad and He [1], respectively, for N = 500 (864).…”
Section: Normalized Thermal Conductivitysupporting
confidence: 71%
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“…It is observed, that the results of λ 0 are within the range of ~7-50% for EMD, 10-16% for NEMD, and ~10-40% for HPMD. Moreover, Figure 3(a) shows, that obtained thermal conductivity at F ext = 0.005 for N = 864 is in good agreement with HPMD simulation of Shahzad and He [1], but it is noted, that our results are slightly greater than EMD of Salin and Caillol [19], NEMD of Donko and Hartmann [20], and VP of Faussurier and Murillo [21] at lower values of Γ. Deviation of the present data from EMD, HPMD, and inhomogeneous that diferences between the simulation data calculated by diferent authors are large at some state points and diferences with their own present data sets are much smaller. Plasma's thermal conductivity is generally overpredicted within ~3-17% (~8-15%), ~5-30% (~5-38%), and ~5-40% (~3-17%) relative to the data of EMD by Salin and Caillol [19], inhomogeneous NEMD by Donko and Hartman [20], and HPMD by Shahzad and He [1], respectively, for N = 500 (864).…”
Section: Normalized Thermal Conductivitysupporting
confidence: 71%
“…HNEMD simulation is used to compute the thermal conductivity normalized by plasma frequency (ω p ) as λ 0 = λ/nk B ω p a ws , or by Einstein frequency (ω E ) as λ * = λ/√3nk B ω E a ws of YDPLs, at the normalized external ield strength. These normalizations of transport properties, including λ 0 , were widely used in earlier studies of one-component complex plasma (OCCP) [18] and NICDPs [1][2][3][19][20][21]. HNEMD method is employed to investigate λ 0 of 3D NICDPs at reduced external force ield F ext = 0.005 over suitable domain of plasma parameters of coupling (1 ≤ Γ ≤ 300) and screening (1 ≤ κ ≤ 4).…”
Section: Normalized Thermal Conductivitymentioning
confidence: 99%
“…The total contribution of the specific heats is then C v = 3/2 + C ex v and C p = 5/2 + C ex p . The formulas for the transport coefficient and the excess energy can also be generalised for a screened Yukawa liquid [34,38].…”
Section: P-6mentioning
confidence: 99%
“…C p is the specific heat at constant pressure and C v the specific heat at constant volume. The transport properties of the ionic fluid can be estimated from fits for one component plasmas, i.e., by assuming the ions are immersed in a rigid neutralising background of negative charges [33,34] …”
Section: P-6mentioning
confidence: 99%
“…One important challenge in using micro and nanotechnologies is the lack of knowledge regarding their thermal conductivity. A novel homogenous nonequilibrium molecular simulation (HNEMS) approach is to be needed to compute the thermal conductivity of complex (nonideal) systems of much of the thermophysical property research in the fields of science and technology [9][10][11].…”
Section: Introductionmentioning
confidence: 99%