modelTableData2DLoadDep_AirCooled
Extends from Modelica.Icons.Example (Icon for runnable examples), Buildings.Fluid.Chillers.Examples.BaseClasses.PartialElectric_AirCooled (Base class for test model of chiller electric EIR with air-cooled condenser).
Information
This model validates Buildings.Fluid.Chillers.ModularReversible.TableData2DLoadDep against the polynomial chiller model Buildings.Fluid.Chillers.ElectricEIR for air-cooled 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 time interval where the PLR value exceeds 1.
In this interval the polynomial model computes a significantly higher
cooling heat flow rate (in negative value) and a slightly higher power.
This discrepancy occurs because the polynomial model calculates the
heat flow rate at PLR ≤ 1 while calculating power at
PLR ≤ per.PLRMax.
Consequently, when PLR increases between 1 and per.PLRMax,
input power increases according to the polynomial EIRFunPLR,
but the heat flow rate only varies due to the effect of the increasing
leaving temperature as the setpoint is no longer met.
This appears as a deficiency in the polynomial model that is resolved
in the data table model.
Parameters
| Type | Name | Default | Description |
|---|---|---|---|
| Modelica.Units.SI.Power | P_nominal (from PartialElectric_AirCooled) | Nominal compressor power (at y=1) | |
| Modelica.Units.SI.TemperatureDifference | dTEva_nominal (from PartialElectric_AirCooled) | 10 | Temperature difference evaporator inlet-outlet |
| Modelica.Units.SI.TemperatureDifference | dTCon_nominal (from PartialElectric_AirCooled) | 10 | Temperature difference condenser outlet-inlet |
| Real | COPc_nominal (from PartialElectric_AirCooled) | 3 | Chiller COP |
| Modelica.Units.SI.MassFlowRate | mEva_flow_nominal (from PartialElectric_AirCooled) | Nominal mass flow rate at evaporator | |
| Modelica.Units.SI.MassFlowRate | mCon_flow_nominal (from PartialElectric_AirCooled) | Nominal mass flow rate at condenser | |
| ModularReversible.Data.TableData2DLoadDep.Generic | datCoo | Chiller performance data | |
| Buildings.Fluid.Chillers.Data.ElectricEIR.ElectricEIRChiller_York_YCAL0033EE_101kW_3_1COP_AirCooled | per | Chiller performance data |
Components
Revisions
-
March 21, 2025, by Antoine Gautier:
First implementation.