|September 28, 2011, 07:57||
Robin BC for T
Join Date: Oct 2010
Posts: 13Rep Power: 6
one equation in my case is
solve ( fvm::ddt(T) + fvm::div(phi,T) - fvm::laplacian(lambda,T) );
T_inf ...const. Far field temperature
alpha ...const. Heat transfer coefficient
T_bc ...Temperature at boundary
Energy conservation yields
q_dot = -lambda (del T)/(del n) = alpha(T_inf - T_bc)
which is my BC.
* Does such a BC exist?
* How should I proceed if I want to implement it?
* I know that it is similar to the BC "mixed" but I think mixed cannot account for non-constant lambda. Are there other BCs that might be useful templates?
Thank you for any comments!
|September 29, 2011, 04:19||
I wrote such a BC few time ago (you find the code here) and it actually is a mixed boundary condition.
The idea is simple, just rewriting the equation you wrote (I also add a general thermal power to handle radiation Q) you end up with:
h/(h+k*deltaCoeff) * T_w + k*deltaCoeff/(h+k*deltaCoeff) * gradT_w = h/(h+k*deltaCoeff) * T_ref + Q*deltaCoeff/(h+k*deltaCoeff)
satisfying both the physical constraint and the form of the mixed boundary condition i.e. VF * T_w + (1-VF) * gradT_w =VF*T_ref + (1-VF) * gradT_ref.
So it just set:
VF = h/(h+k*deltaCoeff)
T_ref = T_ref
gradT_ref = Q*deltaCoeff*VF/(1-VF)/h
in order to make it work you just have to define in your solver a volScalarField kond to store values for the thermal conductivity (optionally you can define it inside the BC if you like).
It was compiled on 1.6.x but I guess you will not have troubles importing it in 1.6-ext or 1.7. Not sure about 2.0, drop me an email if you need a help.
Hope you find this useful.
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