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 ...
5.1 INTRODUCTION CHAPTERS DISCUSSION This chapter deals with discussing
Chapter 5 Discussion Page 5.2 Fur
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Chapter 5 Discussi<strong>on</strong> Page 5.2<br />
Fur<str<strong>on</strong>g>the</str<strong>on</strong>g>r investigati<strong>on</strong> needs to be c<strong>on</strong>ducted and a large data base established to determine<br />
whe<str<strong>on</strong>g>the</str<strong>on</strong>g>r <str<strong>on</strong>g>the</str<strong>on</strong>g> roughness <str<strong>on</strong>g>effect</str<strong>on</strong>g> will:<br />
• follow <str<strong>on</strong>g>the</str<strong>on</strong>g> Nikuradse trend;<br />
• c<strong>on</strong>tinue increasing, following more closely <str<strong>on</strong>g>the</str<strong>on</strong>g> oblique asymptote;<br />
• or if it does follow <str<strong>on</strong>g>the</str<strong>on</strong>g> horiz<strong>on</strong>tal asymptote as proposed by Slatter.<br />
5.3 ROUGHNESS FUNCTION CORRELATION USING OPTIMUM PARTICLE<br />
SIZES<br />
If, however, <str<strong>on</strong>g>the</str<strong>on</strong>g> optimum <str<strong>on</strong>g>particle</str<strong>on</strong>g> <str<strong>on</strong>g>size</str<strong>on</strong>g>s are used to plot <str<strong>on</strong>g>the</str<strong>on</strong>g> roughness functi<strong>on</strong> correlati<strong>on</strong><br />
as shown in Figure 4.11 <str<strong>on</strong>g>the</str<strong>on</strong>g> data points for mixture 2 tend to lie just above <str<strong>on</strong>g>the</str<strong>on</strong>g> horiz<strong>on</strong>tal<br />
asymptote. On <str<strong>on</strong>g>the</str<strong>on</strong>g> whole <str<strong>on</strong>g>the</str<strong>on</strong>g> data points tend to follow more closely <str<strong>on</strong>g>the</str<strong>on</strong>g> assumpti<strong>on</strong>s <strong>on</strong><br />
which <str<strong>on</strong>g>the</str<strong>on</strong>g> Slatter model is based. What this does bring into questi<strong>on</strong> is that <str<strong>on</strong>g>the</str<strong>on</strong>g> d S5 <str<strong>on</strong>g>size</str<strong>on</strong>g> does<br />
not necessarily give <str<strong>on</strong>g>the</str<strong>on</strong>g> best representative <str<strong>on</strong>g>particle</str<strong>on</strong>g> <str<strong>on</strong>g>size</str<strong>on</strong>g>. These optimum <str<strong>on</strong>g>particle</str<strong>on</strong>g> <str<strong>on</strong>g>size</str<strong>on</strong>g>s<br />
indicate that <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> will vary depending <strong>on</strong> <str<strong>on</strong>g>the</str<strong>on</strong>g> PSD <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> slurry<br />
being transported. In fact it would seem from Table 4.1, looking at <str<strong>on</strong>g>the</str<strong>on</strong>g> optimum <str<strong>on</strong>g>size</str<strong>on</strong>g>s for<br />
kaolin clay and mixture 2, that a slurry with a steep PSD for <str<strong>on</strong>g>the</str<strong>on</strong>g> smaller <str<strong>on</strong>g>particle</str<strong>on</strong>g>s (eg. kaolin<br />
clay test sets) would have a higher representative <str<strong>on</strong>g>particle</str<strong>on</strong>g> <str<strong>on</strong>g>size</str<strong>on</strong>g> than a slurry which has a PSD<br />
shape that is less steep from small to large <str<strong>on</strong>g>particle</str<strong>on</strong>g>s. In Table 4.1 <str<strong>on</strong>g>the</str<strong>on</strong>g> kaolin clay test sets<br />
have an average <str<strong>on</strong>g>particle</str<strong>on</strong>g> <str<strong>on</strong>g>size</str<strong>on</strong>g> <str<strong>on</strong>g>of</str<strong>on</strong>g> d x =d 91 as opposed to mixture 2 tests sets which have an<br />
average representative <str<strong>on</strong>g>particle</str<strong>on</strong>g> <str<strong>on</strong>g>size</str<strong>on</strong>g> <str<strong>on</strong>g>of</str<strong>on</strong>g> d. =d 71 • Therefore <str<strong>on</strong>g>the</str<strong>on</strong>g> higher fracti<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> larger<br />
Particles present in <str<strong>on</strong>g>the</str<strong>on</strong>g> slurry <str<strong>on</strong>g>the</str<strong>on</strong>g> lower <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>, as <str<strong>on</strong>g>the</str<strong>on</strong>g> best<br />
representati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> roughness <str<strong>on</strong>g>effect</str<strong>on</strong>g> is reached at a lower d x value.<br />
5.4 SLURRY TEMPERATURE<br />
As reported in secti<strong>on</strong> 4.2.7 an increase in temperature <str<strong>on</strong>g>of</str<strong>on</strong>g> between goC to 10°C made no<br />
significant difference and no temperature <str<strong>on</strong>g>effect</str<strong>on</strong>g>s were found. It is surprising to see this trend<br />
since this would cause a decrease in <str<strong>on</strong>g>the</str<strong>on</strong>g> viscosity for water <str<strong>on</strong>g>of</str<strong>on</strong>g> approximately 20%. This<br />
Could influence <str<strong>on</strong>g>the</str<strong>on</strong>g> rheology <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> slurry and might lead <strong>on</strong>e to questi<strong>on</strong> <str<strong>on</strong>g>the</str<strong>on</strong>g> method <str<strong>on</strong>g>of</str<strong>on</strong>g>