Ground
Heat Transfer Calculations using Site:GroundDomain:Slab[LINK]
In order to simulate heat transfer with horizontal building
surfaces in contact with the ground, a general finite
difference ground model has been implemented. The model
simulates heat transfer with the horizontal building surfaces
through the ground domain. The domain can simulate heat
transfer for slab-in-grade or slab-on-grade scenarios. In all
scenarios, the ground domain must interact with the zone
through an OthersideConditionsModel as the horizontal
surface’s outside boundary condition.
This model is generalized to be able to handle a number of
different slab and insulation configurations. It uses an
implicit finite difference formulation to solve for the ground
temperatures. As a result the simulation is stable for all
timesteps and grid sizes, but an iteration loop must be
employed to converge the temperatures in the domain for each
domain timestep.
Multiple horizontal surfaces can be coupled to each ground
domain object. The model determines which surfaces are coupled
to the ground domain and creates a surface of equivalent
surface area within the ground domain as a representation of
the horizontal surfaces coupled to the ground domain. This
surface then interacts with the ground providing updated other
side conditions model temperatures to the coupled surfaces for
use in their surface heat balance calculations.
Boundary Conditions[LINK]
At the interface surface, the average surface conduction
heat flux from all surfaces connected to the ground domain is
imposed as a GroundDomain boundary condition at the
Surface/GroundDomain interface cells. Heat flux to each cell
is weighted as was recommended by Pinel &
Beausoleil-Morrison 2012 which is shown in Equation [eq:Pinel-Beausoleil-Morrison].
\[q_{out,i} = q_{out,\mbox{1-D}}
\frac{T_{zone} - T_{out,i}}{T_{zone} - T_{out,avg}}
\label{eq:Pinel-Beausoleil-Morrison}\]
Far-field temperatures are applied as boundary temperature
at the GroundDomain sides and lower surface. The ground
temperature profile at the domain sides and lower surface are
taken from Kusuda & Achenbach 1965. The correlation
requires annual ground surface temperature data.
Ground surface cells are treated as a heat balance, where
long and short wave radiation, conduction, and convection are
considered. Evapotranspiration is also considered. The
evapotranspiration rate is calculated as a moisture loss by
using the Allen et al. (2005) model, and translated into a
heat loss by multiplication with the density and latent heat
of evaporation of water. The evapotranspiration rate is
dependent on the type of vegetation at the surface; the user
can vary the surface vegetation from anywhere between a
concrete surface and a fairly tall grass (about 7”).
Once the ground model has run, the updated cells with zone
surface boundary conditions will update the
OtherSideConditionsModel temperatures which are the used at
the next timestep in the surface heat balance
calculations.
Simulation
Methodology[LINK]
The ground domain is updated at each zone timestep, or
hourly as specified by the user. For situations when the
ground domain is updated at each timestep, the domain is
simulated by applying the surface heat flux boundary
conditions from the previous timestep and calculating a new
OthersideConditionsModeltemperature. At this point, the
surface heat balance algorithms can then take the new outside
surface temperatures to update their surface heat fluxes. For
situations when the user has elected to have the domain update
on an hourly basis, the surface heat balance for each coupled
surface is aggregated and passed to the domain as an average
surface heat flux from the previous hour, which will then
update the outside surface temperatures for the surface heat
balance’s next iteration.
Both in-grade and on-grade scenarios are simulated with the
GroundDomain object. The key difference being that for
in-grade situations, the slab and horizontal insulation are
simulated by the ground domain, whereas for the on-grade
situations the slab and horizontal insulation must be included
in the floor construction object. All possible insulation/slab
configurations are seen in Table 1.
Possible insulation/slab configurations for
Site:GroundDomain model.
| Situations |
Vert. Ins. |
Horiz Ins. (Full) |
Horiz Ins. (Perim) |
|
| In-Grade |
1 |
X |
|
|
| In-Grade |
2 |
X |
X |
|
| In-Grade |
3 |
X |
|
X |
| In-Grade |
4 |
|
|
|
| In-Grade |
5 |
|
X |
|
| In-Grade |
6 |
|
|
X |
| On-Grade |
7 |
X |
|
|
| On-Grade |
8* |
X |
X |
|
| On-Grade |
9 |
|
|
|
| On-Grade |
10* |
|
X |
|
* Horizontal insulation must be included in the floor
construction
For the slab-in-grade scenarios, a thin surface layer must
be included in the floor construction. This can be a very thin
layer of the slab or other floor covering materials above the
slab. This provides a zone boundary condition for the
GroundDomain while still allowing 3-dimensional heat transfer
effects to occur within the slab.
Allen, R.G., Walter, I.A., Elliott, R.L., Howell, T.A.,
Itenfisu, D., Jensen, M.E., Snyder, R.L. 2005. The ASCE
Standardized Reference Evapotranspiration Equation. Reston,
VA: American Society of Civil Engineers.
Kusuda, T. & Achenbach, P. 1965. Earth Temperature and
Thermal Diffusivity at Selected Stations in the United States,
ASHRAE Transactions 71(1): 61–75.
Pinel, P & Beausoleil-Morrison, I. 2012. Coupling soil
heat and mass transfer models to foundation models in
whole-building simulation packages. In Proceedings of eSim
2012, Halifax, Canada.
Ground Heat Transfer Calculations using Site:GroundDomain:Slab[LINK]
In order to simulate heat transfer with horizontal building surfaces in contact with the ground, a general finite difference ground model has been implemented. The model simulates heat transfer with the horizontal building surfaces through the ground domain. The domain can simulate heat transfer for slab-in-grade or slab-on-grade scenarios. In all scenarios, the ground domain must interact with the zone through an OthersideConditionsModel as the horizontal surface’s outside boundary condition.
Approach[LINK]
This model is generalized to be able to handle a number of different slab and insulation configurations. It uses an implicit finite difference formulation to solve for the ground temperatures. As a result the simulation is stable for all timesteps and grid sizes, but an iteration loop must be employed to converge the temperatures in the domain for each domain timestep.
Multiple horizontal surfaces can be coupled to each ground domain object. The model determines which surfaces are coupled to the ground domain and creates a surface of equivalent surface area within the ground domain as a representation of the horizontal surfaces coupled to the ground domain. This surface then interacts with the ground providing updated other side conditions model temperatures to the coupled surfaces for use in their surface heat balance calculations.
Boundary Conditions[LINK]
At the interface surface, the average surface conduction heat flux from all surfaces connected to the ground domain is imposed as a GroundDomain boundary condition at the Surface/GroundDomain interface cells. Heat flux to each cell is weighted as was recommended by Pinel & Beausoleil-Morrison 2012 which is shown in Equation [eq:Pinel-Beausoleil-Morrison].
\[q_{out,i} = q_{out,\mbox{1-D}} \frac{T_{zone} - T_{out,i}}{T_{zone} - T_{out,avg}} \label{eq:Pinel-Beausoleil-Morrison}\]
Far-field temperatures are applied as boundary temperature at the GroundDomain sides and lower surface. The ground temperature profile at the domain sides and lower surface are taken from Kusuda & Achenbach 1965. The correlation requires annual ground surface temperature data.
Ground surface cells are treated as a heat balance, where long and short wave radiation, conduction, and convection are considered. Evapotranspiration is also considered. The evapotranspiration rate is calculated as a moisture loss by using the Allen et al. (2005) model, and translated into a heat loss by multiplication with the density and latent heat of evaporation of water. The evapotranspiration rate is dependent on the type of vegetation at the surface; the user can vary the surface vegetation from anywhere between a concrete surface and a fairly tall grass (about 7”).
Once the ground model has run, the updated cells with zone surface boundary conditions will update the OtherSideConditionsModel temperatures which are the used at the next timestep in the surface heat balance calculations.
Simulation Methodology[LINK]
The ground domain is updated at each zone timestep, or hourly as specified by the user. For situations when the ground domain is updated at each timestep, the domain is simulated by applying the surface heat flux boundary conditions from the previous timestep and calculating a new OthersideConditionsModeltemperature. At this point, the surface heat balance algorithms can then take the new outside surface temperatures to update their surface heat fluxes. For situations when the user has elected to have the domain update on an hourly basis, the surface heat balance for each coupled surface is aggregated and passed to the domain as an average surface heat flux from the previous hour, which will then update the outside surface temperatures for the surface heat balance’s next iteration.
Both in-grade and on-grade scenarios are simulated with the GroundDomain object. The key difference being that for in-grade situations, the slab and horizontal insulation are simulated by the ground domain, whereas for the on-grade situations the slab and horizontal insulation must be included in the floor construction object. All possible insulation/slab configurations are seen in Table 1.
* Horizontal insulation must be included in the floor construction
For the slab-in-grade scenarios, a thin surface layer must be included in the floor construction. This can be a very thin layer of the slab or other floor covering materials above the slab. This provides a zone boundary condition for the GroundDomain while still allowing 3-dimensional heat transfer effects to occur within the slab.
References[LINK]
Allen, R.G., Walter, I.A., Elliott, R.L., Howell, T.A., Itenfisu, D., Jensen, M.E., Snyder, R.L. 2005. The ASCE Standardized Reference Evapotranspiration Equation. Reston, VA: American Society of Civil Engineers.
Kusuda, T. & Achenbach, P. 1965. Earth Temperature and Thermal Diffusivity at Selected Stations in the United States, ASHRAE Transactions 71(1): 61–75.
Pinel, P & Beausoleil-Morrison, I. 2012. Coupling soil heat and mass transfer models to foundation models in whole-building simulation packages. In Proceedings of eSim 2012, Halifax, Canada.
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