Matches in SemOpenAlex for { <https://semopenalex.org/work/W2120289739> ?p ?o ?g. }
- W2120289739 endingPage "959" @default.
- W2120289739 startingPage "945" @default.
- W2120289739 abstract "In this report, we investigate the physical and dynamical properties of model fluids whose constituent particles have their softness varied in a systematic manner. Molecular dynamics (MD) computer simulation is applied to inverse power or soft-sphere fluids, in which the particles interact through the pair potential, where measures the steepness or stiffness of the potential. We have investigated the properties of model fluids with over a wide density range. Attention is paid to local structural properties, the elastic moduli and the transport coefficients (principally the shear viscosity, and self-diffusion coefficient, ). We note that this is the first time mechanical and transport coefficient data have been reported for It was found that the Batschinski–Hildebrand expressions, in which and are assumed to have a linear dependence on the molar volume, represent the data quite well for all . The density for which, on extrapolation, each of these quantities are zero, increases with the softness of the interaction (or ), suggesting that the effective hard sphere diameter decreases with increasing softness in the small limit. This treatment leads to simple empirical formulas for the effect of density (in an intermediate range) and on the two transport coefficients of these fluids. As decreases so do the relative fluctuations in the pressure and force on a particle. The local coordination number as measured up to the first minimum in the radial distribution function does not increase significantly above up to the co-existence packing fluid, even for the softest of particles ( ). If we assume that the effective hard sphere diameter is approximately the position of the first peak in the radial distribution function, the Stokes–Einstein expression reproduces the simulation data reasonably well, with the boundary condition being typically between the stick and slip limits, and approaching the latter with increasing density. For the softer particles and with increasing packing fraction, the shear viscosity increases more rapidly than the self-diffusion coefficient decreases. For the softer systems, the bulk viscosity is relatively low compared to the shear viscosity, in contrast to the trend for the corresponding infinite frequency moduli. The softer particles are more “rubbery” in their response (relatively high bulk modulus compared to the shear modulus), which leads us to conclude that auxetic behaviour is more likely to arise when the building units are quite hard." @default.
- W2120289739 created "2016-06-24" @default.
- W2120289739 creator A5027973161 @default.
- W2120289739 creator A5036654343 @default.
- W2120289739 date "2005-11-01" @default.
- W2120289739 modified "2023-10-17" @default.
- W2120289739 title "Mechanical, rheological and transport properties of soft particle fluids" @default.
- W2120289739 cites W1820132600 @default.
- W2120289739 cites W1967690208 @default.
- W2120289739 cites W1970464918 @default.
- W2120289739 cites W1970654251 @default.
- W2120289739 cites W1976748252 @default.
- W2120289739 cites W1985035466 @default.
- W2120289739 cites W1993457762 @default.
- W2120289739 cites W1998532422 @default.
- W2120289739 cites W1998710773 @default.
- W2120289739 cites W2000501196 @default.
- W2120289739 cites W2005690151 @default.
- W2120289739 cites W2028339501 @default.
- W2120289739 cites W2032971403 @default.
- W2120289739 cites W2037276037 @default.
- W2120289739 cites W2043793667 @default.
- W2120289739 cites W2044862798 @default.
- W2120289739 cites W2044955719 @default.
- W2120289739 cites W2049286683 @default.
- W2120289739 cites W2056470446 @default.
- W2120289739 cites W2056802580 @default.
- W2120289739 cites W2057981597 @default.
- W2120289739 cites W2065467183 @default.
- W2120289739 cites W2067758333 @default.
- W2120289739 cites W2071762192 @default.
- W2120289739 cites W2073534459 @default.
- W2120289739 cites W2074053232 @default.
- W2120289739 cites W2079150039 @default.
- W2120289739 cites W2084041890 @default.
- W2120289739 cites W2087242668 @default.
- W2120289739 cites W2088498783 @default.
- W2120289739 cites W2088905004 @default.
- W2120289739 cites W2139526932 @default.
- W2120289739 cites W2140394047 @default.
- W2120289739 cites W2146294839 @default.
- W2120289739 cites W2165802023 @default.
- W2120289739 cites W2169704717 @default.
- W2120289739 cites W3022833029 @default.
- W2120289739 cites W4256223194 @default.
- W2120289739 cites W2015311297 @default.
- W2120289739 doi "https://doi.org/10.1080/08927020500378006" @default.
- W2120289739 hasPublicationYear "2005" @default.
- W2120289739 type Work @default.
- W2120289739 sameAs 2120289739 @default.
- W2120289739 citedByCount "9" @default.
- W2120289739 countsByYear W21202897392017 @default.
- W2120289739 countsByYear W21202897392023 @default.
- W2120289739 crossrefType "journal-article" @default.
- W2120289739 hasAuthorship W2120289739A5027973161 @default.
- W2120289739 hasAuthorship W2120289739A5036654343 @default.
- W2120289739 hasConcept C111368507 @default.
- W2120289739 hasConcept C121332964 @default.
- W2120289739 hasConcept C121864883 @default.
- W2120289739 hasConcept C127172972 @default.
- W2120289739 hasConcept C127313418 @default.
- W2120289739 hasConcept C132459708 @default.
- W2120289739 hasConcept C134306372 @default.
- W2120289739 hasConcept C135508586 @default.
- W2120289739 hasConcept C147597530 @default.
- W2120289739 hasConcept C159985019 @default.
- W2120289739 hasConcept C185592680 @default.
- W2120289739 hasConcept C192562407 @default.
- W2120289739 hasConcept C200990466 @default.
- W2120289739 hasConcept C204323151 @default.
- W2120289739 hasConcept C2778517922 @default.
- W2120289739 hasConcept C33923547 @default.
- W2120289739 hasConcept C57879066 @default.
- W2120289739 hasConcept C59593255 @default.
- W2120289739 hasConcept C69357855 @default.
- W2120289739 hasConcept C97355855 @default.
- W2120289739 hasConcept C99987037 @default.
- W2120289739 hasConceptScore W2120289739C111368507 @default.
- W2120289739 hasConceptScore W2120289739C121332964 @default.
- W2120289739 hasConceptScore W2120289739C121864883 @default.
- W2120289739 hasConceptScore W2120289739C127172972 @default.
- W2120289739 hasConceptScore W2120289739C127313418 @default.
- W2120289739 hasConceptScore W2120289739C132459708 @default.
- W2120289739 hasConceptScore W2120289739C134306372 @default.
- W2120289739 hasConceptScore W2120289739C135508586 @default.
- W2120289739 hasConceptScore W2120289739C147597530 @default.
- W2120289739 hasConceptScore W2120289739C159985019 @default.
- W2120289739 hasConceptScore W2120289739C185592680 @default.
- W2120289739 hasConceptScore W2120289739C192562407 @default.
- W2120289739 hasConceptScore W2120289739C200990466 @default.
- W2120289739 hasConceptScore W2120289739C204323151 @default.
- W2120289739 hasConceptScore W2120289739C2778517922 @default.
- W2120289739 hasConceptScore W2120289739C33923547 @default.
- W2120289739 hasConceptScore W2120289739C57879066 @default.
- W2120289739 hasConceptScore W2120289739C59593255 @default.
- W2120289739 hasConceptScore W2120289739C69357855 @default.
- W2120289739 hasConceptScore W2120289739C97355855 @default.
- W2120289739 hasConceptScore W2120289739C99987037 @default.