modelTableData2DLoadDep_HeatRecovery
Extends from Modelica.Icons.Example (Icon for runnable examples), Buildings.Fluid.Chillers.Examples.BaseClasses.PartialElectric (Base class for test model of chiller electric EIR).
Information
This model validates Buildings.Fluid.Chillers.ModularReversible.TableData2DLoadDep against the polynomial chiller model Buildings.Fluid.Chillers.ElectricEIR for heat recovery chiller applications.
-
The validation setup is duplicated from
Buildings.Fluid.Chillers.Examples.ElectricEIR_AirCooled
and the component
refreads the reference results obtained from that model. - The chiller model is configured to interpolate capacity and power along the evaporator leaving temperature and the condenser entering temperature.
- The performance data are generated with the same polynomial equations as Buildings.Fluid.Chillers.ElectricEIR, using polynomial coefficients from the same data record as the one used in the reference example model, that is Buildings.Fluid.Chillers.Data.ElectricEIR.ElectricEIRChiller_York_YCAL0033EE_101kW_3_1COP_AirCooled.
Results analysis
There is good agreement with the reference results, except during
the model time interval [7500, 8100] s, where the
polynomial model computes lower power.
During this period, the polynomial model calculates lower power
due to the evaporator leaving temperature exceeding the maximum threshold
upper limit per.TEvaLvgMax.
While the data table model does not extrapolate beyond the temperature
values provided in the performance data file,
the reference model continues using polynomial evaluation of capacity
and power outside of the validity range.
Consequently, the polynomial model computes a higher capacity,
resulting in a lower PLR and reduced power during this interval.
Parameters
| Type | Name | Default | Description |
|---|---|---|---|
| Modelica.Units.SI.Power | P_nominal (from PartialElectric) | Nominal compressor power (at y=1) | |
| Modelica.Units.SI.TemperatureDifference | dTEva_nominal (from PartialElectric) | 10 | Temperature difference evaporator inlet-outlet |
| Modelica.Units.SI.TemperatureDifference | dTCon_nominal (from PartialElectric) | 10 | Temperature difference condenser outlet-inlet |
| Real | COPc_nominal (from PartialElectric) | 3 | Chiller COP |
| Modelica.Units.SI.MassFlowRate | mEva_flow_nominal (from PartialElectric) | Nominal mass flow rate at evaporator | |
| Modelica.Units.SI.MassFlowRate | mCon_flow_nominal (from PartialElectric) | Nominal mass flow rate at condenser | |
| Buildings.Fluid.Chillers.Data.ElectricEIR.ElectricEIRChiller_McQuay_WSC_471kW_5_89COP_Vanes | per | Chiller performance data | |
| ModularReversible.Data.TableData2DLoadDep.Generic | datCoo | Chiller performance data |
Components
Revisions
-
March 23, 2026, by Antoine Gautier:
Refactored with two separate connectors for CHW and HW temperature setpoints.
This is for #4507. -
March 21, 2025, by Antoine Gautier:
First implementation.