Deprecated: $wgMWOAuthSharedUserIDs=false is deprecated, set $wgMWOAuthSharedUserIDs=true, $wgMWOAuthSharedUserSource='local' instead [Called from MediaWiki\HookContainer\HookContainer::run in /var/www/html/w/includes/HookContainer/HookContainer.php at line 135] in /var/www/html/w/includes/Debug/MWDebug.php on line 372
The effect of the hydrodynamic interaction on the rheological properties of Hookean dumbbell suspensions in steady state shear flow - MaRDI portal

The effect of the hydrodynamic interaction on the rheological properties of Hookean dumbbell suspensions in steady state shear flow (Q580061)

From MaRDI portal





scientific article; zbMATH DE number 4016411
Language Label Description Also known as
English
The effect of the hydrodynamic interaction on the rheological properties of Hookean dumbbell suspensions in steady state shear flow
scientific article; zbMATH DE number 4016411

    Statements

    The effect of the hydrodynamic interaction on the rheological properties of Hookean dumbbell suspensions in steady state shear flow (English)
    0 references
    1987
    0 references
    The diffusion equation for the configurational distribution function of Hookean dumbbell suspensions with the hydrodynamic interaction (HI) was solved, in terms of Galerkin's method, in steady state shear flow; and viscosity, first and second normal-stress coefficients and molecular stretching were then calculated. The results indicate that the HI included in a microscopic model of molecules gives rise to a significant effect on the macroscopic properties of Hookean dumbbell suspensions. For example, the viscosity and the first normal stress coefficient, decreasing as shear rate increases, are no longer constant, the second normal-stress coefficient, being negative with small absolute value and shear-rate dependent, is no longer zero; and an additional stretching of dumbbells is yielded by the HI. The viscosity function and the first normal-stress coefficient calculated from this method are in agreement with those predicted from the self-consistent average method qualitatively, while the negative second normal-stress coefficient from the former seems to be more reasonable than the positive one from the latter.
    0 references
    theory of polymer solutions
    0 references
    diffusion equation
    0 references
    configurational distribution function
    0 references
    Hookean dumbbell suspensions
    0 references
    hydrodynamic interaction
    0 references
    Galerkin's method
    0 references
    steady state shear flow
    0 references
    second normal- stress coefficients
    0 references
    molecular stretching
    0 references
    0 references

    Identifiers