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 ...
Chapter 5 Table 5.1. Discussion Page 5.5 Table 5.1: Number Concentration
Chapter 5 Discussion Page 5.6 The number
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Chapter 5<br />
Table 5.1.<br />
Discussi<strong>on</strong> Page 5.5<br />
Table 5.1: Number C<strong>on</strong>centrati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> Large Particles in Viscous Sub-layer<br />
Test % Large No. Particles<br />
Particles per m 2<br />
KW 22 163<br />
K 20 20 296<br />
.<br />
RFlO 4 24<br />
RF 20 5 36<br />
RF 30 6 57<br />
S 10 47 336<br />
S 20 55 463<br />
S 30 62 540<br />
From Table 5.1 it can be seen that <str<strong>on</strong>g>the</str<strong>on</strong>g> highest number <str<strong>on</strong>g>of</str<strong>on</strong>g><str<strong>on</strong>g>particle</str<strong>on</strong>g>s per square meter was 540.<br />
This indicates that if <str<strong>on</strong>g>the</str<strong>on</strong>g> <str<strong>on</strong>g>particle</str<strong>on</strong>g>s were evenly spaced that approximately <strong>on</strong>e large <str<strong>on</strong>g>particle</str<strong>on</strong>g><br />
would be found every 5cm. This is fairly low for <strong>on</strong>e would expect for a <str<strong>on</strong>g>particle</str<strong>on</strong>g> roughness<br />
<str<strong>on</strong>g>effect</str<strong>on</strong>g> for <str<strong>on</strong>g>the</str<strong>on</strong>g>re to be at least <strong>on</strong>e large <str<strong>on</strong>g>particle</str<strong>on</strong>g> per millimetre (Slatter, 1996) and yet even<br />
with a low number c<strong>on</strong>centrati<strong>on</strong> <str<strong>on</strong>g>the</str<strong>on</strong>g>re is evidence <str<strong>on</strong>g>of</str<strong>on</strong>g> a <str<strong>on</strong>g>particle</str<strong>on</strong>g> roughness <str<strong>on</strong>g>effect</str<strong>on</strong>g>. In fact,<br />
Slatter (1994) detected a <str<strong>on</strong>g>particle</str<strong>on</strong>g> roughness <str<strong>on</strong>g>effect</str<strong>on</strong>g> even when testing slurries with a<br />
volumetric c<strong>on</strong>centrati<strong>on</strong> as low as 2 %. It would <str<strong>on</strong>g>the</str<strong>on</strong>g>refore appear from tests c<strong>on</strong>ducted by<br />
Slatter (1994) and test c<strong>on</strong>ducted for this <str<strong>on</strong>g>the</str<strong>on</strong>g>sis tllat <str<strong>on</strong>g>the</str<strong>on</strong>g> large <str<strong>on</strong>g>particle</str<strong>on</strong>g>s have a dominant <str<strong>on</strong>g>effect</str<strong>on</strong>g><br />
<strong>on</strong> tUrbulence even when <str<strong>on</strong>g>the</str<strong>on</strong>g> number c<strong>on</strong>centrati<strong>on</strong> is extremely. This would indicate that<br />
:he Particle roughness <str<strong>on</strong>g>effect</str<strong>on</strong>g> is due to <str<strong>on</strong>g>the</str<strong>on</strong>g> mere fact that <str<strong>on</strong>g>particle</str<strong>on</strong>g>s are present in <str<strong>on</strong>g>the</str<strong>on</strong>g> slurry per<br />
,e but it is strange that a small number produce <str<strong>on</strong>g>the</str<strong>on</strong>g> same <str<strong>on</strong>g>effect</str<strong>on</strong>g> as a large number.