This model distributes the incoming short wave radtion onto different
areas of the room according to the approach in the ASHREA Standard,
Annex B7 "Detailed calculation of solar fractions". The ASHREA makes
some assumptions to estimate the sight factors of each element. For
more details on the assumptions, we refer to the ASHREA standard. In
order to ease the usage of this model, we made additional
assumptions.
Assumptions by ASHREA
- First bounce: All shortwave radiation initially hits the floor
- Second bounce: Not absorbed radiation is diffusivly reflected by
floor and distributed over all surfaces according to the view factors
of each surface
- Third bounce: Remaining radiation is distributed over each
surface in proportion to it's area-absorptance product
- Remaining bounces: Based on calculations from third bounce
Additional Assumptions
In order to ease the usage of this model, we added the following
assumptions. You can read more about the reasons of these assumptions
in the corresponding issue 918.
- In constrast to the ASHREA, we allow for different solar
absorptance factors
- All floors act as one joined area. However, the heat flows are
seperated based on areas etc. at the end according to ASHRAE
- All walls have the same heigh + ceiling and floor have (joined
together) the same area. This is necessary in order to use the
approximations of sight factors from the standard. This is checked
via asserts
- We only calculate one view/sight factor, and that is from floor
to ceiling. This assumes floor and ceiling are two parallel areas
with the same total area
- All remaining radiation of the second bounce is distributed
proportional to the areas of the surfaces:
sight_factor_floor_win = A_win / (A_win + A_walls) * (1 -
sight_factor_floor_ceil)
sight_factor_floor_walls = A_walls / (A_win + A_walls) * (1 -
sight_factor_floor_ceil)
sight_factor_floor_wall_i = A_wall_i / A_walls *
sight_factor_floor_walls
sight_factor_floor_win_i = A_win_i / A_win *
sight_factor_floor_walls
Note that the last assumption would be valid for a quadratic room
with no windows. Only for extremly long rooms this assumptions could
be dangerous. However, a floor typically reflects only 10
% of the incoming radiation. Approx. 50 % of
that go to the ceiling, the rest to the walls. Therefor, effects like
correct window placement etc. on the temperatures of the walls will
be of a small magnitude.
Parameterization
You have to connect the bus connector ShortRadSurf of each
surface (floor, wall, ceiling) of type wall to the
corresponding port. As the current implementation of type
window only supports one directional short wave radiation, the
port win_out may be ignored. However, you can check how much
radiation is lost to the ambient.
If you model a room with multiple floor elements, you have to specify
the parameters floor_length and floor_height. These scales are
required to calculate the view factors in the second bounce.
Known Limitations
- Although we implemented the exact same equations as in the ASHREA
(besides out approach for the third bounce), the results of the model
do NOT match the results provided in the tables of the Appendix in
the ASHREA. This is due to the high fiew factor from floor to ceiling
in the second bounce. We could not quantify how the results in the
Appendix are obtained, as their solar fraction for the ceiling is too
low. In order to use the ASHREA values from the tables instead of the
dynamic calculation, you may use the option table_based_calc.
- In the ASHREA, all surfaces shall have the same absorbtance. Our
modelling approach enable differing values.
- This model works best for nearly quadratic rooms
- Windows in the floors or ceilings are not regarded
Sources
- ANSI/ASHREA Standard 140-2017
- Principles of Heat Transfer - Chapter 9.4
[Link]
-
June, 18, 2020 by Fabian Wuellhorst:
#918:
Implemented.
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