modelHeaterCooler_u

Heater or cooler with prescribed heat flow rate

Extends from IBPSA.Fluid.Interfaces.TwoPortHeatMassExchanger (Partial model transporting one fluid stream with storing mass or energy).

Information

Model for an ideal heater or cooler with prescribed heat flow rate to the medium.

This model adds heat in the amount of Q_flow = u Q_flow_nominal to the medium. The input signal u and the nominal heat flow rate Q_flow_nominal can be positive or negative. A positive value of Q_flow means heating, and negative means cooling.

The outlet conditions at port_a are not affected by this model, other than for a possible pressure difference due to flow friction.

Optionally, this model can have a flow resistance. Set dp_nominal = 0 to disable the flow friction calculation.

For a model that uses as an input the fluid temperature leaving at port_b, use IBPSA.Fluid.HeatExchangers.PrescribedOutlet

Limitations

This model does not affect the humidity of the air. Therefore, if used to cool air below the dew point temperature, the water mass fraction will not change.

Validation

The model has been validated against the analytical solution in the example IBPSA.Fluid.HeatExchangers.Validation.HeaterCooler_u.

Parameters

TypeNameDefaultDescription
Modelica.SIunits.HeatFlowRateQ_flow_nominalHeat flow rate at u=1, positive for heating
Assumptions
BooleanallowFlowReversal (from PartialTwoPort)true= false to simplify equations, assuming, but not enforcing, no flow reversal
Nominal condition
Modelica.SIunits.MassFlowRatem_flow_nominal (from PartialTwoPortInterface)Nominal mass flow rate
Modelica.SIunits.PressureDifferencedp_nominal (from TwoPortFlowResistanceParameters)Pressure difference
Advanced
Modelica.SIunits.MassFlowRatem_flow_small (from PartialTwoPortInterface)1E-4*abs(m_flow_nominal)Small mass flow rate for regularization of zero flow
BooleanhomotopyInitialization (from TwoPortHeatMassExchanger)true= true, use homotopy method
Advanced › Diagnostics
Booleanshow_T (from PartialTwoPortInterface)false= true, if actual temperature at port is computed
Flow resistance
BooleancomputeFlowResistance (from TwoPortFlowResistanceParameters)true=true, compute flow resistance. Set to false to assume no friction
Booleanfrom_dp (from TwoPortFlowResistanceParameters)false= true, use m_flow = f(dp) else dp = f(m_flow)
BooleanlinearizeFlowResistance (from TwoPortFlowResistanceParameters)false= true, use linear relation between m_flow and dp for any flow rate
RealdeltaM (from TwoPortFlowResistanceParameters)0.1Fraction of nominal flow rate where flow transitions to laminar
Dynamics › Nominal condition
Modelica.SIunits.Timetau (from TwoPortHeatMassExchanger)30Time constant at nominal flow (if energyDynamics <> SteadyState)
Dynamics › Equations
Modelica.Fluid.Types.DynamicsenergyDynamics (from TwoPortHeatMassExchanger)Modelica.Fluid.Types.Dynamics.DynamicFreeInitialType of energy balance: dynamic (3 initialization options) or steady state
Modelica.Fluid.Types.DynamicsmassDynamics (from TwoPortHeatMassExchanger)energyDynamicsType of mass balance: dynamic (3 initialization options) or steady state
Initialization
Medium.AbsolutePressurep_start (from TwoPortHeatMassExchanger)Medium.p_defaultStart value of pressure
Medium.TemperatureT_start (from TwoPortHeatMassExchanger)Medium.T_defaultStart value of temperature
Medium.MassFraction[Medium.nX]X_start (from TwoPortHeatMassExchanger)Medium.X_defaultStart value of mass fractions m_i/m
Medium.ExtraProperty[Medium.nC]C_start (from TwoPortHeatMassExchanger)fill(0, Medium.nC)Start value of trace substances

Connectors

TypeNameDefaultDescription
Modelica.Fluid.Interfaces.FluidPort_aport_a (from PartialTwoPort)Fluid connector a (positive design flow direction is from port_a to port_b)
Modelica.Fluid.Interfaces.FluidPort_bport_b (from PartialTwoPort)Fluid connector b (positive design flow direction is from port_a to port_b)
Modelica.Blocks.Interfaces.RealInputuControl input
Modelica.Blocks.Interfaces.RealOutputQ_flowHeat added to the fluid

Components

TypeNameDefaultDescription
Modelica.SIunits.MassFlowRatem_flow (from PartialTwoPortInterface)port_a.m_flowMass flow rate from port_a to port_b (m_flow > 0 is design flow direction)
Modelica.SIunits.PressureDifferencedp (from PartialTwoPortInterface)port_a.p - port_b.pPressure difference between port_a and port_b
Medium.ThermodynamicStatesta_a (from PartialTwoPortInterface)Medium.setState_phX(port_a.p, noEvent(actualStream(port_a.h_outflow)), noEvent(actualStream(port_a.Xi_outflow)))Medium properties in port_a
Medium.ThermodynamicStatesta_b (from PartialTwoPortInterface)Medium.setState_phX(port_b.p, noEvent(actualStream(port_b.h_outflow)), noEvent(actualStream(port_b.Xi_outflow)))Medium properties in port_b
IBPSA.Fluid.MixingVolumes.MixingVolumevol (from TwoPortHeatMassExchanger)
IBPSA.Fluid.FixedResistances.PressureDroppreDro (from TwoPortHeatMassExchanger)Flow resistance

Revisions

  • November 3, 2016, by Michael Wetter:
    Set preHea(final alpha=0) as this allows to simplify the system of equations.
    This is for #570.
  • November 19, 2015, by Michael Wetter:
    Removed assignment of parameter showDesignFlowDirection in extends statement. This is for #349.
  • May 6, 2015, by Michael Wetter:
    Set prescribedHeatFlowRate=true. This is for issue #412.
  • May 1, 2015, by Marcus Fuchs:
    Corrected typo in documentation.
  • November 12, 2014, by Michael Wetter:
    Added output signal Q_flow so that it has the same output ports as IBPSA.Fluid.HeatExchangers.Validation.PrescribedOutlet.
  • September 11, 2014, by Christoph Nytsch-Geusen:
    Renaming class to HeaterCooler_u.
  • October 15, 2013, by Michael Wetter:
    Redeclared the control volume to be final so that it does not show anymore in the parameter window.
  • July 11, 2011, by Michael Wetter:
    Redeclared fluid volume as final. This prevents the fluid volume model to appear in the dialog window.
  • May 24, 2011, by Michael Wetter:
    Changed base class to allow using the model as a dynamic or a steady-state model.
  • April 17, 2008, by Michael Wetter:
    First implementation.