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Pseudoplastic INDEX

This combination of long riser and relatively shallow hole probably favours a polymer with a high pseudoplastic index - high viscosity at the low shear rate in the slow-moving fluid in the riser - and rapid, clean breaking at the well bottom temperature. [Pg.171]

In the specific case of polymer melts these almost invariably are of the pseudoplastic type. In such cases the flow behaviour index n is less than 1 the greater the divergence from Newtonian behaviour the lower its value. [Pg.166]

The non-Newtonian index is plotted against the blend ratio in Fig. 2. There are three distinct stages of the change of value with %NBR in the preblend. First, a decrease of up to 40% of NBR, a rapid rise of up to 60% of NBR, and beyond this ratio a further decrease are observed. Heating of blends shows the only minimum at 50 50 ratio. It is obvious that 60-50% of Hypalon in the NBR-Hypalon blend is an optimum range where maximum extent of interchain crosslinking reaction is expected, and this blend is supposed to be more pseudoplastic. [Pg.612]

Decreases in concentration or increases in temperature usually decrease the consistency indexes K and K but leave the flow-behavior indexes n and n relatively unaltered. The latter appear to be determined primarily by the components of the non-Newtonian fluid and increase only slightly with increases in temperatures or decreases in concentration for pseudoplastic materials. [Pg.111]

Values of the consistency index K and the flow behavior index n for a non-Newtonian fluid can be determined experimentally. For pseudoplastic fluids, n < 1. [Pg.194]

The exponent, n, the power-law-index is n = 1 for Newtonian behaviour, and n < 1 for pseudoplasticity. The apparent viscosity is then given by ... [Pg.96]

For a Newtonian fluid, the power law index n = 1, and k is the fluid viscosity. Also, for shear-thinning (pseudoplastic) fluids, n < 1. [Pg.174]

Power Law Fluid or Emulsion A fluid or emulsion whose rheological behavior is reasonably well-described by the power law equation. Here shear stress is set proportional to the shear rate raised to an exponent n, where n is the power law index. The fluid is pseudoplastic for n < 1, Newtonian for n = 1, and dilatant for n > 1. [Pg.400]

Vemuri S. Flow and consistency index dependence of pseudoplastic guar gum solutions. Drug Dev Ind Pharm 1988 14 905-914. [Pg.317]

One can see that the index n of a power-law fluid substantially affects the velocity profile. With increasing pseudoplasticity the distribution of the velocity becomes more and more homogeneous, approaching a quasisolid distribution with profile V = (V) = const in the limit as n —> 0. On the contrary, dilatancy makes the flow field more and more nonuniform, and as n - oo the velocity profile approaches the triangular shape given by... [Pg.269]


See other pages where Pseudoplastic INDEX is mentioned: [Pg.443]    [Pg.379]    [Pg.75]    [Pg.392]    [Pg.241]    [Pg.241]    [Pg.1339]    [Pg.443]    [Pg.379]    [Pg.75]    [Pg.392]    [Pg.241]    [Pg.241]    [Pg.1339]    [Pg.228]    [Pg.170]    [Pg.99]    [Pg.23]    [Pg.99]    [Pg.104]    [Pg.107]    [Pg.109]    [Pg.109]    [Pg.126]    [Pg.17]    [Pg.67]    [Pg.173]    [Pg.144]    [Pg.213]    [Pg.184]    [Pg.189]    [Pg.202]    [Pg.495]    [Pg.958]    [Pg.228]    [Pg.379]    [Pg.132]    [Pg.164]    [Pg.17]    [Pg.48]    [Pg.389]    [Pg.476]    [Pg.756]   
See also in sourсe #XX -- [ Pg.355 ]




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