modelPartialElectric

Information

Base class for model of an electric chiller, based on the DOE-2.1 chiller model and the CoolTools chiller model that are implemented in EnergyPlus as the models Chiller:Electric:EIR and Chiller:Electric:ReformulatedEIR.

The model takes as an input the set point for the leaving chilled water temperature, which is met if the chiller has sufficient capacity. Thus, the model has a built-in, ideal temperature control. The model has three tests on the part load ratio and the cycling ratio:

1. The test

     PLR1 =min(QEva_flow_set/QEva_flow_ava, PLRMax)
   

   ensures that the chiller capacity does not exceed the chiller capacity specified by the parameter PLRMax.
2. The test

     CR = min(PLR1/per.PRLMin, 1.0)
   

   computes a cycling ratio. This ratio expresses the fraction of time that a chiller would run if it were to cycle because its load is smaller than the minimal load at which it can operature. Notice that this model does continuously operature even if the part load ratio is below the minimum part load ratio. Its leaving evaporator and condenser temperature can therefore be considered as an average temperature between the modes where the compressor is off and on.
3. The test

     PLR2 = max(PLRMinUnl, PLR1)
   

   computes the part load ratio of the compressor. The assumption is that for a part load ratio below PLRMinUnl, the chiller uses hot gas bypass to reduce the capacity, while the compressor power draw does not change.

The electric power only contains the power for the compressor, but not any power for pumps or fans.

Optionally, the model can be configured to represent heat recovery chillers with a switchover option by setting the parameter have_switchover to true. In that case an additional Boolean input connector coo is used. The chiller is tracking a chilled water supply temperature setpoint at the outlet of the evaporator barrel if coo is true. Otherwise, if coo is false, the chiller is tracking a hot water supply temperature setpoint at the outlet of the condenser barrel. See Buildings.Fluid.Chillers.Examples.ElectricEIR_HeatRecovery for an example with a chiller operating in heating mode.

Implementation

This implementation computes the chiller capacity and power consumption the same way as documented in EnergyPlus v22.1.0 Engineering Reference section 14.3.9.2. Especially see equations 14.234 and 14.240 in the referenced document.

The available chiller capacity QEva_flow_ava is adjusted from its nominal capacity QEva_flow_nominal by factor capFunT as

  QEva_flow_ava = QEva_flow_nominal*capFunT

and the compressor power consumption is computed as

  P = -QEva_flow_ava*(1/COP_nominal)*EIRFunT*EIRFunPLR*CR.

The models that extend from this base class implement the functions used above in ways that are shown in the table below.

where TConEnt is the condenser entering temperature, TEvaLvg is the evaporator leaving temperature, TConLvg is the condenser leaving temperatore, and PLR is the part load ratio.

References

• EnergyPlus v22.1.0 Engineering Reference

Parameters

Components

Revisions

• June 4, 2024, by Antoine Gautier:
  Added load limit in heating mode.
  This is for #3815.
• January 11, 2023, by Antoine Gautier:
  Added optional switchover mode for heat recovery chillers.
  This is for #3211.
• November 19, 2021, by David Blum:
  Add humidity to entering condenser state calculation.
  This is for issue 2770.
• June 28, 2019, by Michael Wetter:
  Removed start values and removed nominal=1 for performance curves.
  This is for issue 1465.
• March 12, 2015, by Michael Wetter:
  Refactored model to make it once continuously differentiable. This is for issue 373.
• Jan. 10, 2011, by Michael Wetter:
  Added input signal to switch chiller off, and changed base class to use a dynamic model. The change of the base class was required to improve the robustness of the model when the control is switched on again.
• Sep. 8, 2010, by Michael Wetter:
  Revised model and included it in the Buildings library.
• October 13, 2008, by Brandon Hencey:
  First implementation.