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 4 Results and Analysis Page 4.27<br />
• At <str<strong>on</strong>g>the</str<strong>on</strong>g> higher wall shear stress values for mixture 2 <str<strong>on</strong>g>the</str<strong>on</strong>g> viscous sub-layer thickness<br />
is less than <str<strong>on</strong>g>the</str<strong>on</strong>g> diameter <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> larger <str<strong>on</strong>g>particle</str<strong>on</strong>g>s.<br />
• An increase in <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> caused an increase in <str<strong>on</strong>g>the</str<strong>on</strong>g> wall shear<br />
stress in <str<strong>on</strong>g>the</str<strong>on</strong>g> <strong>turbulent</strong> flow regi<strong>on</strong>.<br />
• The Slatter model best predicted <str<strong>on</strong>g>the</str<strong>on</strong>g> test data and becomes more accurate with<br />
increasing <str<strong>on</strong>g>particle</str<strong>on</strong>g> <str<strong>on</strong>g>size</str<strong>on</strong>g>.<br />
• The Maude & Whitmore correlati<strong>on</strong> is unable to accurately predict <strong>turbulent</strong> flow<br />
behaviour.<br />
• The Bowen correlati<strong>on</strong> produces good results but does not provide an explanati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g><br />
<str<strong>on</strong>g>the</str<strong>on</strong>g> behaviour <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> slurry in terms <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> physical properties <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> slurry.<br />
• Slarter's model is unable to predict <str<strong>on</strong>g>the</str<strong>on</strong>g> <strong>turbulent</strong> flow behaviour <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> Sive data for<br />
a n<strong>on</strong>-homogeneous settling slurry.<br />
The results and analysis are discussed in Chapter 5.