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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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bodyc

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body
--uriencoded--\

displaystyle c = \frac%7B0.03 \, a%5e%7B1.86%7D%7D%7B0.063 \, a%5e3 -0.674 \, a%5e2 +2.225 \, a - 1.157 %7D

mbox%7BPr%7D



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

Rayleigh number 

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bodyp




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bodya

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body--uriencoded--a = r_%7Bout%7D/r_%7Bin%7D








Prandtl number 


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bodyp = 1.013 \cdot\exp \left[ -0.067 \cdot a \right]




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body

a

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body--uriencoded--a = r_%7Bout%7D/r_%7Bin%7D

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body--uriencoded--\mbox%7BPr%7D

Prandtl number 

\displaystyle c = \frac%7B0.03 \, a%5e%7B1.86%7D%7D%7B0.063 \, a%5e3 -0.674 \, a%5e2 +2.225 \, a - 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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