Model to distribute short wave radiation transmitted through a window to all areas in the room using shape factors
  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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