the effect of the particle size distribution on non-newtonian turbulent ...
the effect of the particle size distribution on non-newtonian turbulent ...
the effect of the particle size distribution on non-newtonian turbulent ...
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Preamble<br />
T shear stress Pa<br />
T y yield stress Pa<br />
q, functi<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g><br />
X<br />
rheological parameter<br />
v<strong>on</strong> Kannan c<strong>on</strong>stant<br />
0 velocity functi<strong>on</strong><br />
SUbscripts<br />
o<br />
85<br />
ann<br />
c<br />
calc<br />
m-<br />
max<br />
N<br />
NN<br />
obs<br />
P<br />
plug<br />
r<br />
res<br />
s<br />
shear<br />
v<br />
w<br />
x<br />
at <str<strong>on</strong>g>the</str<strong>on</strong>g> pipe wall<br />
85 th percentile <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> <str<strong>on</strong>g>particle</str<strong>on</strong>g>s passing<br />
refers to <str<strong>on</strong>g>the</str<strong>on</strong>g> annulus<br />
critical<br />
calculated<br />
loss, liquid<br />
mixture (slurry)<br />
maximum<br />
Newt<strong>on</strong>ian<br />
n<strong>on</strong>-Newt<strong>on</strong>ian<br />
observed (experimental)<br />
<str<strong>on</strong>g>particle</str<strong>on</strong>g><br />
<str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> plug<br />
roughness<br />
residual<br />
solids<br />
z<strong>on</strong>e over which shear occurs<br />
volumetric<br />
water<br />
representative <str<strong>on</strong>g>size</str<strong>on</strong>g><br />
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