Dear Charles Luanay,
thanks for pointing this out!
I check the coding of this section, and the manual has a
sign error and the drawing is wrong too:
q_comb,s,o = q_c,s,o + q_r,s,o
q_comb,s,o = q_c,s,o - q_r,s,o
q_r,s,o is defined as a loss : q_r,s,o = sigma * epsilon_s,o * (T_s,o^4 – T_fsky^4) P.S.:
What version of TRNSYS are you using? The section numbering of the Type 56
user’s manual looks somwhat strange to me.
Von: LAUNAY Charles 226591 [mailto:charles.launay@cea.fr] Gesendet: Donnerstag, 29. April 2010 10:25 An: trnsys-users@engr.wisc.edu Betreff: [TRNSYS-users] Long wave radiation in the energy balance (Type 56)
Dear
users, I have a question concerning section 2.1.7. of the Type
56 user’s manual : “2. General Mathematical Description of the Thermal Model”
> “2.1.7. The Long-wave radiation”. My question is concerning the formulation of the net
radiative heat transfer with surfaces in view of the outside surface, q_r,s,o.
We can read : q_r,s,o = sigma * epsilon_s,o * (T_s,o^4 –
T_fsky^4) that I understand as the net losses of the outside
surface by long wave radiation. However, q_r,s,o is counted as a gain in the energy
balance (with a plus sign) : q_s,o = q_comb,s,o + S_s,o with q_comb,s,o = q_c,s,o +
q_r,s,o (see figure 3 “Surface heat flux and temperature”,
section 2,1,5. for the nomenclature) How does it happen? How is the heat transfer by long
wave radiation really taken into account in Type 56?
Thanks for your help. Kind regards, Charles LAUNAY CEA
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