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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Chapter 2 Literature Review Page 2.36<br />
• Fully developed rough wall <strong>turbulent</strong> flow does exist and <str<strong>on</strong>g>the</str<strong>on</strong>g> partially rough<br />
wall <strong>turbulent</strong> regi<strong>on</strong> is much narrower than for Newt<strong>on</strong>ian fluids.<br />
• Fully developed <strong>turbulent</strong> flow is independent <str<strong>on</strong>g>of</str<strong>on</strong>g><str<strong>on</strong>g>the</str<strong>on</strong>g> viscous characteristics <str<strong>on</strong>g>of</str<strong>on</strong>g><br />
<str<strong>on</strong>g>the</str<strong>on</strong>g> slurry.<br />
• Plug flow does not occur.<br />
In order to determine whe<str<strong>on</strong>g>the</str<strong>on</strong>g>r smooth wall <strong>turbulent</strong> flow or fully developed rough wall<br />
<strong>turbulent</strong> flow exists a roughness Reynolds number was formulated in terms <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> yield<br />
pseudoplastic model.<br />
The roughness Reynolds number is:<br />
(2.72)<br />
Where cl. is <str<strong>on</strong>g>the</str<strong>on</strong>g> representative <str<strong>on</strong>g>particle</str<strong>on</strong>g> <str<strong>on</strong>g>size</str<strong>on</strong>g>. d.=d85 was found to be good representative<br />
<str<strong>on</strong>g>particle</str<strong>on</strong>g> <str<strong>on</strong>g>size</str<strong>on</strong>g> for <str<strong>on</strong>g>the</str<strong>on</strong>g> slurries tested.<br />
If Re, < 3,32 <str<strong>on</strong>g>the</str<strong>on</strong>g>n smooth wall <strong>turbulent</strong> flow exists and <str<strong>on</strong>g>the</str<strong>on</strong>g> mean velocity is given by:<br />
V = 2,5 In [R] -<br />
• dgs<br />
+ 2,5 In Re, + 1,75 .<br />
(2.73)<br />
If Re, > 3,32 <str<strong>on</strong>g>the</str<strong>on</strong>g>n fully developed rough wall <strong>turbulent</strong> flow exists and <str<strong>on</strong>g>the</str<strong>on</strong>g> mean velocity<br />
is given by:<br />
V = 2,5 In [R] -<br />
• d85 Which reduces to<br />
+ 4,75 ,<br />
(2.74)