03.07.2013 Views

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 ...

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

Chapter 2 Literature Review Page 2.36<br />

• Fully developed rough wall <strong>turbulent</strong> flow does exist and <str<strong>on</strong>g>the</str<strong>on</strong>g> partially rough<br />

wall <strong>turbulent</strong> regi<strong>on</strong> is much narrower than for Newt<strong>on</strong>ian fluids.<br />

• Fully developed <strong>turbulent</strong> flow is independent <str<strong>on</strong>g>of</str<strong>on</strong>g><str<strong>on</strong>g>the</str<strong>on</strong>g> viscous characteristics <str<strong>on</strong>g>of</str<strong>on</strong>g><br />

<str<strong>on</strong>g>the</str<strong>on</strong>g> slurry.<br />

• Plug flow does not occur.<br />

In order to determine whe<str<strong>on</strong>g>the</str<strong>on</strong>g>r smooth wall <strong>turbulent</strong> flow or fully developed rough wall<br />

<strong>turbulent</strong> flow exists a roughness Reynolds number was formulated in terms <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> yield<br />

pseudoplastic model.<br />

The roughness Reynolds number is:<br />

(2.72)<br />

Where cl. is <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>. d.=d85 was found to be good representative<br />

<str<strong>on</strong>g>particle</str<strong>on</strong>g> <str<strong>on</strong>g>size</str<strong>on</strong>g> for <str<strong>on</strong>g>the</str<strong>on</strong>g> slurries tested.<br />

If Re, < 3,32 <str<strong>on</strong>g>the</str<strong>on</strong>g>n smooth wall <strong>turbulent</strong> flow exists and <str<strong>on</strong>g>the</str<strong>on</strong>g> mean velocity is given by:<br />

V = 2,5 In [R] -<br />

• dgs<br />

+ 2,5 In Re, + 1,75 .<br />

(2.73)<br />

If Re, > 3,32 <str<strong>on</strong>g>the</str<strong>on</strong>g>n fully developed rough wall <strong>turbulent</strong> flow exists and <str<strong>on</strong>g>the</str<strong>on</strong>g> mean velocity<br />

is given by:<br />

V = 2,5 In [R] -<br />

• d85 Which reduces to<br />

+ 4,75 ,<br />

(2.74)

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!