modelFixedApproach

Cooling tower with constant approach temperature

Extends from Buildings.Fluid.HeatExchangers.CoolingTowers.BaseClasses.CoolingTower (Base class for cooling towers).

Information

Model for a steady-state or dynamic cooling tower with constant approach temperature. The approach temperature is the difference between the leaving water temperature and the entering air temperature. The entering air temperature is used from the signal TAir. If connected to the a dry-bulb temperature, then a dry cooling tower is modeled. If connected to a wet-bulb temperature, then a wet cooling tower is modeled.

By connecting a signal that contains either the dry-bulb or the wet-bulb temperature, this model can be used to estimate the water return temperature from a cooling tower. For a more detailed model, use for example the YorkCalc model.

Parameters

TypeNameDefaultDescription
BooleanhomotopyInitialization (from TwoPortHeatMassExchanger)true= true, use homotopy method
Modelica.Units.SI.TemperatureDifferenceTApp2Approach temperature difference
Assumptions
BooleanallowFlowReversal (from PartialTwoPort)true= false to simplify equations, assuming, but not enforcing, no flow reversal
Nominal condition
Modelica.Units.SI.MassFlowRatem_flow_nominal (from PartialTwoPortInterface)Nominal mass flow rate
Modelica.Units.SI.PressureDifferencedp_nominal (from TwoPortFlowResistanceParameters)Pressure difference
Advanced
Modelica.Units.SI.MassFlowRatem_flow_small (from PartialTwoPortInterface)1E-4*abs(m_flow_nominal)Small mass flow rate for regularization of zero flow
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)
Realn (from TwoPortFlowResistanceParameters)2Flow exponent, n=1 for laminar, n=2 for turbulent
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.Units.SI.Timetau (from TwoPortHeatMassExchanger)30Time constant at nominal flow (if energyDynamics <> SteadyState)
Dynamics › Conservation equations
Modelica.Fluid.Types.DynamicsenergyDynamics (from TwoPortHeatMassExchanger)Modelica.Fluid.Types.Dynamics.DynamicFreeInitialType of energy 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.RealOutputTLvg (from CoolingTower)Leaving water temperature
Modelica.Blocks.Interfaces.RealInputTAirEntering air dry or wet bulb temperature

Components

TypeNameDefaultDescription
Modelica.Units.SI.MassFlowRatem_flow (from PartialTwoPortInterface)port_a.m_flowMass flow rate from port_a to port_b (m_flow > 0 is design flow direction)
Modelica.Units.SI.PressureDifferencedp (from PartialTwoPortInterface)port_a.p - port_b.pPressure difference between port_a and port_b
Medium.ThermodynamicStatesta_a (from PartialTwoPortInterface)if allowFlowReversal then Medium.setState_phX(port_a.p, noEvent(actualStream(port_a.h_outflow)), noEvent(actualStream(port_a.Xi_outflow))) else Medium.setState_phX(port_a.p, noEvent(inStream(port_a.h_outflow)), noEvent(inStream(port_a.Xi_outflow)))Medium properties in port_a
Medium.ThermodynamicStatesta_b (from PartialTwoPortInterface)if allowFlowReversal then Medium.setState_phX(port_b.p, noEvent(actualStream(port_b.h_outflow)), noEvent(actualStream(port_b.Xi_outflow))) else Medium.setState_phX(port_b.p, noEvent(port_b.h_outflow), noEvent(port_b.Xi_outflow))Medium properties in port_b
Buildings.Fluid.MixingVolumes.MixingVolumevol (from TwoPortHeatMassExchanger)
Buildings.Fluid.FixedResistances.PressureDroppreDro (from TwoPortHeatMassExchanger)Flow resistance
Modelica.Units.SI.HeatFlowRateQ_flow (from CoolingTower)preHea.Q_flowHeat input into water circuit

Revisions

  • January 16, 2020, by Michael Wetter:
    Refactored model to avoid mixing textual equations and connect statements.
  • July 12, 2011, by Michael Wetter:
    Introduced common base class for Buildings.Fluid.HeatExchangers.CoolingTowers.YorkCalc and Buildings.Fluid.HeatExchangers.CoolingTowers.FixedApproach so that they can be used as replaceable models.
  • May 12, 2011, by Michael Wetter:
    Added binding equations for Q_flow and mXi_flow.
  • March 8, 2011, by Michael Wetter:
    Removed base class and unused variables.
  • April 7, 2009, by Michael Wetter:
    Changed interface to new Modelica.Fluid stream concept.
  • May 14, 2008, by Michael Wetter:
    First implementation.