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a Prandtl number  a a%5e%7B1 a%5e3 a%5e2 a
Stagnant fluidNatural ConvectionForced Convection
OEIS sequence A282581
J. DIRKER & J. P. MEYER


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anchorNu0
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{\rm Nu}=3.6568



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{\rm Nu} = \frac{2 \cdot \epsilon({\rm Ra})}{\ln (r_{out}/r_{in})}



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{\rm Nu}= c \cdot \mbox{Re}_D^p \cdot \mbox{Pr}^{0.4}\cdot \left( \frac{\mu}{\mu_w} \right)^{0.14}




wherewhere

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body--uriencoded--\epsilon(%7B\rm Ra%7D)

Natural Convection Heat Transfer Multiplier 

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body--uriencoded--\displaystyle \mbox%7BPr%7D = \frac%7B\nu%7D%7Ba%7D


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body--uriencoded--%7B\rm Ra%7D

Rayleigh number 

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p
body\nu



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bodya

thermal diffusivity


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body--uriencoded--

\zeta = r_%7Bout%7D/r_%7Bin%7D




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bodyp = 1.013 \cdot\exp \left[ -0.067 \cdot

\zeta \right]



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body--uriencoded--\displaystyle c = \frac%7B0.03 \,

\zeta%5e%7B1.86%7D%7D%7B0.063 \,

\zeta%5e3 -0.674 \,

\zeta%5e2 +2.225 \,

\zeta - 1.157 %7D


See also

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Physics / Thermodynamics / Heat Transfer /  Heat Transfer Coefficient (HTC) / Heat Transfer Coefficient (HTC) @model

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