Abstract:A reliable set of cross-section parameters of the variable soft sphere (VSS) molecular model is determined for the Monte Carlo simulation of air species from the transport collision integrals or potential parameters provided by Cubley and Mason [Phys. Fluids 18, 1109 (1975)] over the high-temperature range 300–15 000 K. The VSS cross-section parameters for the inverse-power-law potential are also determined from the viscosity coefficients recommended by Maitland and Smith [J. Chem. Eng. Data 17, 150 (1972)] fo… Show more
“…By multiplying r ith the measured value. In He+H 2 , the rotational relaxation occurs faster than (15) where τ r and τ v are rotational and vibrational relaxation times, respectively. In the present work, the relaxation times of the state-resolved method are determined by the e-folding curve-fit method proposed by Kim et al [7,8].…”
Section: Rvt Energy Transitions and Coupled Chemical Reactions In Dsmcmentioning
confidence: 99%
“…Previously, variable hard-sphere (VHS) [1], variable soft-sphere (VSS) [14,15], general hard-sphere (GHS) [16], and general soft-sphere (GSS) [17,18] models were developed to determine the total cross sections in the DSMC calculations. However, these previous models have limitations to be employed in the state-resolved method.…”
Section: State-specific Total Cross Sectionsmentioning
A method of describing the rovibrational energy transitions and coupled chemical reactions in the direct simulation Monte Carlo (DSMC) calculations is constructed for H( 2 S)+H2(X 1 ∑g) and He( 1 S)+H2(X 1 ∑g). First, the state-specific total cross sections for each rovibrational states are proposed to describe the state-resolved elastic collisions. The state-resolved method is constructed to describe the rotational-vibrational-translational (RVT) energy transitions and coupled chemical reactions by these state-specific total cross sections and the rovibrational state-to-state transition cross sections of bound-bound and bound-free transitions. The RVT energy transitions and coupled chemical reactions are calculated by the state-resolved method in various heat bath conditions without relying on a macroscopic properties and phenomenological models of the DSMC. In nonequilibrium heat bath calculations, the state-resolved method are validated with those of the master equation calculations and the existing shock-tube experimental data. In bound-free transitions, the parameters of the existing chemical reaction models of the DSMC are proposed through the calibrations in the thermochemical nonequilibrium conditions. When the bound-free transition component of the state-resolved method is replaced by the existing chemical reaction models, the same agreement can be obtained except total collision energy model.
“…By multiplying r ith the measured value. In He+H 2 , the rotational relaxation occurs faster than (15) where τ r and τ v are rotational and vibrational relaxation times, respectively. In the present work, the relaxation times of the state-resolved method are determined by the e-folding curve-fit method proposed by Kim et al [7,8].…”
Section: Rvt Energy Transitions and Coupled Chemical Reactions In Dsmcmentioning
confidence: 99%
“…Previously, variable hard-sphere (VHS) [1], variable soft-sphere (VSS) [14,15], general hard-sphere (GHS) [16], and general soft-sphere (GSS) [17,18] models were developed to determine the total cross sections in the DSMC calculations. However, these previous models have limitations to be employed in the state-resolved method.…”
Section: State-specific Total Cross Sectionsmentioning
A method of describing the rovibrational energy transitions and coupled chemical reactions in the direct simulation Monte Carlo (DSMC) calculations is constructed for H( 2 S)+H2(X 1 ∑g) and He( 1 S)+H2(X 1 ∑g). First, the state-specific total cross sections for each rovibrational states are proposed to describe the state-resolved elastic collisions. The state-resolved method is constructed to describe the rotational-vibrational-translational (RVT) energy transitions and coupled chemical reactions by these state-specific total cross sections and the rovibrational state-to-state transition cross sections of bound-bound and bound-free transitions. The RVT energy transitions and coupled chemical reactions are calculated by the state-resolved method in various heat bath conditions without relying on a macroscopic properties and phenomenological models of the DSMC. In nonequilibrium heat bath calculations, the state-resolved method are validated with those of the master equation calculations and the existing shock-tube experimental data. In bound-free transitions, the parameters of the existing chemical reaction models of the DSMC are proposed through the calibrations in the thermochemical nonequilibrium conditions. When the bound-free transition component of the state-resolved method is replaced by the existing chemical reaction models, the same agreement can be obtained except total collision energy model.
“…However, some macroscopic quantities calculated via the HS model, such as viscosity, can at most qualitatively agree with experimental results. The VSS model [14,15] …”
The temperature inside modern hard disk drives (HDDs) can become as high as 100°C during operation. The effects of such high temperatures on the slider's flying attitude and the shear forces on the slider and the disk are investigated in this paper. General formulae for the shear forces are derived, and the generalized Reynolds equation is modified to take into account the temperature effect on the mean free path of air as well as the air viscosity. Numerical results are obtained for two different air bearing surface designs. It is shown that the temperature changes result in non-negligible changes in the slider's flying height and the shear forces. These changes could further induce changes in the deformation and instability of the lubricant layer and thereby affect the reliability of the HDDs.
“…MONACO employs the Variable Soft Sphere (VSS) collision model of Koura et al [15], a variable rotational energy exchange probability model of Boyd [16] and the variable vibrational energy exchange probability model of Vijayakumar et al [17]. The flow conditions here do not involve chemical reactions.…”
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