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@wikipedia


Dimensionless quantity characterising the ratio of thermal convection to thermal conduction in fluids across (normal to) the boundary with solids:

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{\rm Nu} = \frac{\rm Convective \ heat  \ transfer}{\rm Conductive \ heat \ 
 transfer} = \frac{U}{\lambda / L} =\frac{U \cdot L}{\lambda } 

where 

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bodyU
 is the convective heat transfer coefficient of the flow, 
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bodyL
 is the characteristic length
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body\lambda
 is the thermal conductivity of the fluid.


Stagnant Fluid



For 
 Stagnant Fluid the Nusselt number is a constant number (OEIS sequence A282581):

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anchorNu0
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{\rm Nu}=3.6568


Natural Convection


In Natural Fluid Convection becomes dependant on Rayleigh number 

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body\rm Ra
 and Prandtl number 
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body\rm Pr
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body--uriencoded--\mbox%7BNu%7D = f (\mbox%7BRa%7D, \mbox%7BPr%7D)
.



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\mbox{Nu}= \left[ 0.825 + \frac{0.387 \, \mbox{Ra}^{1/6}}{ \left[ 1+ (0.492/\mbox{Pr})^{9/16} \right]^{8/27}} \right]^2



Churchill and Chu 



All flow regimes


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\mbox{Nu}= 0.68 + \frac{0.663 \, \mbox{Ra}^{1/4}}{ \left[ 1+ (0.492/\mbox{Pr})^{9/16} \right]^{4/9}}



Churchill and Chu



Laminar flows

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body--uriencoded--\mbox%7BRa%7D \leq 10%5e9


Forced Convection



In Forced Fluid Convection the 
Nusselt number becomes dependant on Reynolds number 

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body\rm Re
 and Prandtl number 
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body\rm Pr
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body--uriencoded--\mbox%7BNu%7D = f (\mbox%7BRe%7D, \mbox%7BPr%7D)
.



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{\rm Nu}=3.66 + \frac{ 0.065 \cdot {\rm Re} \cdot {\rm Pr} \cdot {D/L} }{ 1 + 0.04 \cdot ({\rm Re} \cdot {\rm Pr} \cdot {D/L})^{2/3} }




Laminar flow in pipeline



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anchorNu
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{\rm Nu}=\frac{ (f/8) \, ({\rm Re} - 1000) {\rm Pr}  }{ 1 + 12.7 \, (f/8)^{1/2} \, ({\rm Pr}^{2/3} -1) }


Gnielinski


laminar-turbulent transition and turbulent flow in pipeline the Nusselt number (Nu) becomes also dependant on friction with wall, quantifiable by Darcy friction factor 

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bodyf
, and can be estimated through empirical correlation (Gnielinski


 

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body--uriencoded--0.5\leq \mathrm %7BPr%7D \leq 2000
 
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body--uriencoded--%7B\displaystyle 3000\leq \mathrm %7BRe%7D\leq 5\cdot 10%5e%7B6%7D%7D


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anchorNu
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{\rm Nu}=0.3 + \frac{0.62 \, \mbox{Re}^{1/2} \, \mbox{Pr}^{1/3} }
{\left[ 1+ (0.4/\mbox{Pr})^{2/3} \right]^{1/4}}
\left[ 1 + \left( \frac{\mbox{Re}}{282000} \right)^{5/8}\right]^{4/5}


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body--uriencoded--\mbox %7BRe%7D \cdot \mbox %7BPr%7D \geq 0.2

Accuracy 

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body--uriencoded--\sim 20 \%25


See also


Physics / Thermodynamics / Heat Transfer

Heat Transfer Coefficient (HTC) ] Heat Transfer Coefficient @model ]

Dimensionless Heat Transfer Numbers ]


References





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