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Bonjour @Santos. Without knowing the range of "mortar plaster" conductivities you're looking into, I ran the following variations to get an idea of some trends:

1.000 W/m.K (high end)
0.656 W/m.K (current value in the .osm)
0.400 W/m.K (low end)

Results (Tunis, single storey building):

k (W/m.K) Heat (GJ) Cool (GJ) Fans (GJ) peak (kW) hours of safety [heat] 
_________ _________ _________ _________ _________ ______________________
    1.000      3214       313       484       686                   5169
    0.656      3144       322       482       678                   5106           
    0.400      3037       334       478       661                   4590

First, a few observations:

  • order of magnitude difference between annual heating (++++) vs annual cooling (-)
  • facility peak demand occurs in winter - not summer
  • heating likely exaggerated in part due to constant 18°C below slab-on-grade (fix).
  • low annual cooling due to having a single zone with AC (1x PTHP)

Although I did not plot temperature trends for different zones (during different periods), I'm inferring from the hours of safety (heat) that summer temperatures in free-floating zones (i.e. no AC) often remain near or above 30°C. Without taking any deeper dives or commenting on the magnitude of these numbers, these trends are generally consistent with incremental reductions in material thermal conductivity (given the initial model setup):

  • reduced annual heating (and peak demand)
  • slight increase in cooling (20 GJ, i.e. < 1% of annual facility GJ)
  • related decrease in the number of hours of safety during heat events

image description

The slight increase in cooling seems counterintuitive. In line with what's summarized here (and in other UMH posts), there are likely periods where outdoor conditions are cool enough to trigger envelope free cooling (e.g. increased surface convection, improved radiative exchanges with the night sky). An improvement in envelope thermal resistance prevents the structure from free cooling (to a degree), hence the slight increase in cooling. Something similar is likely occurring with the number of hours of safety. For free-floating zones, a revised night cooling (natural ventilation) strategy could easily compensate and in fact reverse these two trends. A suggestion.


Avoiding any deeper dives at this stage, as I believe there are some substantial fixes required here. From the above list of rooms, I'm guessing a single family dwelling. Yet the modelled facility is huge:

  • total floor area exceeds 11 500 m2 (or 125 000 ft2), average size of a US middle school
  • all walls are 17.83 m tall - that's almost 60ft (akin to big box retail)
  • with consequent load calculations (e.g. PTHP is approx. 65 tons of cooling)
  • the "Thermal Celier" has 240 m3/s as ZoneExhaust

I'm not seeing the use of multipliers in your model (e.g. a multi-unit residential building), and so the numbers seem generally out of whack for a single residence (at least an order of magnitude too high). I may be completely wrong, but it looks like the dimensions may have either been entered as if in IP, yet really in SI units (17ft instead of 17m), or something wrong happened during translation. Can only speculate. If these are indeed incorrect dimensions, then you would likely need to rehaul model geometry.


I suggest a QAQC exercise before further investigating material conductivities. I'd start with the basics, especially geometry (!), then setpoint/schedule validation, before moving on to key passive cooling strategies like night ventilation (if most spaces are to remain free-floating, i.e. no AC). Maybe even factoring ceiling fans, all towards minimizing heat stress events. Only then, and after getting rid of most of the warnings in the eplusout.err file, would I have enough confidence in simulation results to investigate changes in material conductivities.

Hoping this helps.

Bonjour @Santos. Without knowing the range of "mortar plaster" conductivities you're looking into, I ran the following variations to get an idea of some trends:

1.000 W/m.K (high end)
0.656 W/m.K (current value in the .osm)
0.400 W/m.K (low end)

Results (Tunis, single storey building):building model you referenced here):

k (W/m.K) Heat (GJ) Cool (GJ) Fans (GJ) peak (kW) hours of safety [heat] 
_________ _________ _________ _________ _________ ______________________
    1.000      3214       313       484       686                   5169
    0.656      3144       322       482       678                   5106           
    0.400      3037       334       478       661                   4590

First, a few observations:

  • order of magnitude difference between annual heating (++++) vs annual cooling (-)
  • facility peak demand occurs in winter - not summer
  • heating likely exaggerated in part due to constant 18°C below slab-on-grade (fix).
  • low annual cooling due to having a single zone with AC (1x PTHP)

Although I did not plot temperature trends for different zones (during different periods), I'm inferring from the hours of safety (heat) that summer temperatures in free-floating zones (i.e. no AC) often remain near or above 30°C. Without taking any deeper dives or commenting on the magnitude of these numbers, these trends are generally consistent with incremental reductions in material thermal conductivity (given the initial model setup):

  • reduced annual heating (and peak demand)
  • slight increase in cooling (20 GJ, i.e. < 1% of annual facility GJ)
  • related decrease in the number of hours of safety during heat events

image description

The slight increase in cooling seems counterintuitive. In line with what's summarized here (and in other UMH posts), there are likely periods where outdoor conditions are cool enough to trigger envelope free cooling (e.g. increased surface convection, improved radiative exchanges with the night sky). An improvement in envelope thermal resistance prevents the structure from free cooling (to a degree), hence the slight increase in cooling. Something similar is likely occurring with the number of hours of safety. For free-floating zones, a revised night cooling (natural ventilation) strategy could easily compensate and in fact reverse these two trends. A suggestion.


Avoiding any deeper dives at this stage, as I believe there are some substantial fixes required here. From the above list of rooms, I'm guessing a single family dwelling. Yet the modelled facility is huge:huge:

  • total floor area exceeds 11 500 m2 (or 125 000 ft2), average size of a US middle school
  • all walls are 17.83 m tall - that's almost 60ft 60 ft (akin to big box retail)
  • with consequent load calculations (e.g. PTHP is offers approx. 65 tons of cooling)
  • the "Thermal Celier" has 240 m3/s as ZoneExhaust

I'm not seeing the use of multipliers in your model (e.g. a multi-unit residential building), and so the numbers seem generally out of whack for a single residence (at least an order of magnitude too high). I may be completely wrong, but it looks like the dimensions may have either been entered as if in IP, yet really in SI units (17ft instead of 17m), or something wrong happened during translation. Can only speculate. If these are indeed incorrect dimensions, then you would likely need to rehaul model geometry.


I suggest a QAQC exercise before further investigating material conductivities. I'd start with the basics, especially geometry (!), then setpoint/schedule validation, before moving on to key passive cooling strategies like night ventilation (if most spaces are to remain free-floating, i.e. no AC). Maybe even factoring ceiling fans, all towards minimizing heat stress events. Only then, and after getting rid of most of the warnings in the eplusout.err file, would I have enough confidence in simulation results to investigate changes in material conductivities.

Hoping this helps.