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Appendix B C<strong>on</strong>ference Paper<br />

ABSTRACT<br />

PARTICLE ROUGHNESS<br />

TURBULENCE<br />

PT SLATTER, G S THORVALDSEN & F W PETERSEN<br />

Cape Technik<strong>on</strong>, Cape Town, South Africa<br />

The <strong>turbulent</strong> flow <str<strong>on</strong>g>of</str<strong>on</strong>g>n<strong>on</strong>-Newt<strong>on</strong>ian slurries has remained a problem, despite much<br />

research in this area. The successful resoluti<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g>this problem is vitally imp<strong>on</strong>anr not<br />

<strong>on</strong>ly for hydrotransp<strong>on</strong> applicati<strong>on</strong>s involving fine slurries, but also for mixed regime<br />

slurries, where <str<strong>on</strong>g>the</str<strong>on</strong>g> vehicle comp<strong>on</strong>ent is usually a n<strong>on</strong>-Newt<strong>on</strong>ian slurry. Two major<br />

problem areas are that <str<strong>on</strong>g>the</str<strong>on</strong>g> <strong>turbulent</strong> behaviour <str<strong>on</strong>g>of</str<strong>on</strong>g><str<strong>on</strong>g>the</str<strong>on</strong>g>se slurries appears unrelated to<br />

<str<strong>on</strong>g>the</str<strong>on</strong>g>ir laminar behaviour and yet has been found to be strikingly similar to Newt<strong>on</strong>ian<br />

<strong>turbulent</strong> behaviour, in spite <str<strong>on</strong>g>of</str<strong>on</strong>g><str<strong>on</strong>g>the</str<strong>on</strong>g> obvious difference in rheology.<br />

This paper explores <str<strong>on</strong>g>the</str<strong>on</strong>g>se and o<str<strong>on</strong>g>the</str<strong>on</strong>g>r problem areas in <str<strong>on</strong>g>the</str<strong>on</strong>g> literature and shows how<br />

previous <str<strong>on</strong>g>the</str<strong>on</strong>g>oretical models havefailed to address <str<strong>on</strong>g>the</str<strong>on</strong>g>m adequately. A new approach to<br />

turbulence modelling is reviewed which does address <str<strong>on</strong>g>the</str<strong>on</strong>g>se problem areas. This approach<br />

is based <strong>on</strong> <str<strong>on</strong>g>the</str<strong>on</strong>g> panicle roughness <str<strong>on</strong>g>effect</str<strong>on</strong>g>, but is as yet relatively untested outside <str<strong>on</strong>g>the</str<strong>on</strong>g><br />

range ojslurries and panicle <str<strong>on</strong>g>size</str<strong>on</strong>g>s <strong>on</strong> which it was originally evaluated.<br />

An experimentalprogramme has been initiated to investigate and accumulate a data base<br />

<str<strong>on</strong>g>of</str<strong>on</strong>g><str<strong>on</strong>g>the</str<strong>on</strong>g> behaviour <str<strong>on</strong>g>of</str<strong>on</strong>g>a wider range <str<strong>on</strong>g>of</str<strong>on</strong>g>n<strong>on</strong>-Newt<strong>on</strong>ian slurries. including slurries with a<br />

bimodal panicle <str<strong>on</strong>g>size</str<strong>on</strong>g> <str<strong>on</strong>g>distributi<strong>on</strong></str<strong>on</strong>g>. These new data are analysed and <str<strong>on</strong>g>the</str<strong>on</strong>g> results are<br />

presented and discussed. It is c<strong>on</strong>cluded that <str<strong>on</strong>g>the</str<strong>on</strong>g> new approach to turbulence modelling<br />

using <str<strong>on</strong>g>the</str<strong>on</strong>g> panicle roughness <str<strong>on</strong>g>effect</str<strong>on</strong>g> is valid for <str<strong>on</strong>g>the</str<strong>on</strong>g> slurries tested.<br />

1. INTRODUCTION<br />

The predicti<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g><strong>turbulent</strong> flow or pipe flow energy requirements from <strong>on</strong>ly <str<strong>on</strong>g>the</str<strong>on</strong>g> viscous<br />

properties <str<strong>on</strong>g>of</str<strong>on</strong>g> n<strong>on</strong>-Newt<strong>on</strong>ian suspensi<strong>on</strong>s has over <str<strong>on</strong>g>the</str<strong>on</strong>g> years been questi<strong>on</strong>ed by<br />

researchers. It has been found that <str<strong>on</strong>g>the</str<strong>on</strong>g> flow behaviour and rheology <str<strong>on</strong>g>of</str<strong>on</strong>g><str<strong>on</strong>g>the</str<strong>on</strong>g>se suspensi<strong>on</strong>s<br />

is influenced by such factors as <str<strong>on</strong>g>particle</str<strong>on</strong>g> <str<strong>on</strong>g>size</str<strong>on</strong>g>, shape, weight and <str<strong>on</strong>g>distributi<strong>on</strong></str<strong>on</strong>g> (philipp<str<strong>on</strong>g>of</str<strong>on</strong>g>f<br />

1944, Hedstrom 1952, Orr & Blocker 1955, Zettlemoyer & Lower 1955, Maude &<br />

Whitmore 1956, Thomas 1963, Thomas 1983, Mun 1988, Slatter 1994).<br />

The <strong>turbulent</strong> flow <str<strong>on</strong>g>of</str<strong>on</strong>g> n<strong>on</strong>-Newt<strong>on</strong>ian suspensi<strong>on</strong>s is complex and is <str<strong>on</strong>g>of</str<strong>on</strong>g>ten c<strong>on</strong>sidered<br />

problematic to design. However, in many situati<strong>on</strong>s it has beneficial characteristics,<br />

B.2

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