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 2.6<br />
However, even though <str<strong>on</strong>g>the</str<strong>on</strong>g> above statements can be taken to be true for Newt<strong>on</strong>ian fluids<br />
<str<strong>on</strong>g>the</str<strong>on</strong>g>re are times when certain fluids deviate from <str<strong>on</strong>g>the</str<strong>on</strong>g> Newt<strong>on</strong>ian behaviour. From <str<strong>on</strong>g>the</str<strong>on</strong>g>oretical<br />
c<strong>on</strong>siderati<strong>on</strong>s as presented by Grunberg & Nissan (1945) it can be c<strong>on</strong>cluded that at high<br />
rates <str<strong>on</strong>g>of</str<strong>on</strong>g> shear <str<strong>on</strong>g>the</str<strong>on</strong>g> viscosity <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g>se fluids (eg. n-pentane) may become a functi<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> shear<br />
rate. O<str<strong>on</strong>g>the</str<strong>on</strong>g>r fluids which behave as Newt<strong>on</strong>ian at lower shear stresses also exhibit n<strong>on</strong><br />
Newt<strong>on</strong>ian behaviour above certain shear stresses. In experiments c<strong>on</strong>ducted by We1tmann<br />
(1948) it was shown that several oils have a n<strong>on</strong>-Newt<strong>on</strong>ian behaviour above a limiting shear<br />
stress <str<strong>on</strong>g>of</str<strong>on</strong>g> approximately 958 Pa. This seems to c<strong>on</strong>tradict <str<strong>on</strong>g>the</str<strong>on</strong>g> fact that normally at high<br />
Reynolds numbers n<strong>on</strong>-Newt<strong>on</strong>ian behaviour decreases (see secti<strong>on</strong> 2.5.3.d).<br />
i Examples <str<strong>on</strong>g>of</str<strong>on</strong>g> Newt<strong>on</strong>ian behaviour include:<br />
• all gases,'<br />
• all liquids or soluti<strong>on</strong>s <str<strong>on</strong>g>of</str<strong>on</strong>g> low molecular weight (Metzner, 1956).<br />
2.5.2 N<strong>on</strong>-Newt<strong>on</strong>ian fluids<br />
Unlike Newt<strong>on</strong>ian fluids, <str<strong>on</strong>g>the</str<strong>on</strong>g> term viscosity has no meaning for a n<strong>on</strong>-Newt<strong>on</strong>ian fluid unless<br />
it is related to a particular shear rate (Holland, 1973). However, an apparent viscosity can<br />
be defiiled as (Holland 1973, Wils<strong>on</strong> 1986):<br />
N<strong>on</strong>-Newt<strong>on</strong>ian fluids are normally divided into <strong>on</strong>e <str<strong>on</strong>g>of</str<strong>on</strong>g> two categories (Metzner, 1956):<br />
(a) Fluids with properties independent <str<strong>on</strong>g>of</str<strong>on</strong>g> tome or <str<strong>on</strong>g>the</str<strong>on</strong>g> durati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> shear.<br />
(2.5)<br />
(b) More complex fluids where <str<strong>on</strong>g>the</str<strong>on</strong>g> relati<strong>on</strong>ship between shear stress and shear<br />
rate depends <strong>on</strong> <str<strong>on</strong>g>the</str<strong>on</strong>g> durati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> shear.<br />
A graphical representati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> several possible relati<strong>on</strong>ships between shear stress and shear<br />
rate for n<strong>on</strong>-Newt<strong>on</strong>ian fluids, called a rheogram, is showlLin Figure 2.2.