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paraffin wax deposition and fouling

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— A36 —<br />

A74<br />

Velocity Distribution if I’luid Properties are Constant<br />

Doissler used velocity distribution data for flow without heat<br />

transfer to evaluate the constants K <strong>and</strong> n.<br />

Assuming T<br />

= Tw <strong>and</strong> constant physical properties, a substitution<br />

for cu/rw in equation A73.5 gives:<br />

(1) Away from wall<br />

+<br />

+ y +<br />

u = in —- - u1<br />

.....(A7.4.i)<br />

where y is the lowest<br />

of y for which the equation applies <strong>and</strong> u<br />

is the value o u at y1. From experimental data Deissier found K = 0.3<br />

u<br />

—<br />

(2) Close to wall<br />

y ÷<br />

dy<br />

+<br />

(4<br />

2 + + 2 + +<br />

l+n u y 1-exp(—n u y)<br />

J<br />

From experimental data Deissler found n = 0.124. At small y (< 5) the<br />

equation reduces to<br />

+ +<br />

u = y .....(A7.4.3<br />

Equations A7.4.1 <strong>and</strong> A7.4.3 are the same as in the Universal<br />

Velocity Profile.<br />

Deissler found his data to Lit very well with these equations if<br />

ttaay from the wall” was considered when y26, at which point u = 12.82.<br />

A75<br />

ueratur Distribution if Fluid ProDorties are Constant<br />

Assuming q = q,,, <strong>and</strong> = 1 in the dimensionless form of the heat<br />

flux equation A7.3.6, results in the following equation:<br />

A<br />

dT’<br />

l=ç.+<br />

__)<br />

sucsti;ution for the dimensionless eddy diffusivity gives:

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