modelPlateHeatExchangerEffectivenessNTU

Plate heat exchanger with effectiveness - NTU relation and no moisture condensation

Extends from Buildings.Fluid.HeatExchangers.BaseClasses.PartialEffectivenessNTU (Partial model for heat exchanger with effectiveness - NTU relation and no moisture condensation).

Information

Model of a plate heat exchanger without humidity condensation. This model transfers heat in the amount of

Q̇ = Q̇max ε
ε = f(NTU, Z, flowRegime),

where max is the maximum heat that can be transferred, ε is the heat transfer effectiveness, NTU is the Number of Transfer Units, Z is the ratio of minimum to maximum capacity flow rate and flowRegime is the heat exchanger flow regime. such as parallel flow, cross flow or counter flow.

The flow regimes depend on the heat exchanger configuration. All configurations defined in Buildings.Fluid.Types.HeatExchangerConfiguration are supported.

Convective heat transfer coefficients

The convective heat transfer coefficients scale proportional to (ṁ/ṁ0)nCon, where is the mass flow rate and 0 is the nominal mass flow rate. By default, the exponents are nCon=0.8 for both streams. The convective heat transfer coefficients are computed based on the UA-value, neglecting the thermal conductance of the heat exchanger material. The ratio of the convection coefficients at design conditions can be adjusted using the parameter r0=(hA)0,1 ⁄ (hA)0,2 where (hA)0,1 and (hA)0,2 are the respective products of the heat transfer coefficient times surface area. By default, the ratio r0 is computed based on the similarity law for turbulent flow, which states that the convective heat transfer coefficient h follows the proportionality law

h ∝ k (ρ v x / η)nCon1 Pr1/3,

where k is the heat conductivity of the fluid, ρ is the density, v is the flow velocity, x is the characteristic length, η is the dynamic viscosity and Pr is the Prandtl number. Under the assumption that both sides of the heat exchanger are identical, and considering that the velocity is proportional to the mass flow rate divided by the density, the ratio r0 is

r0 = (k1 (ṁ0,1 / η0,1)nCon1 Pr0,11/3) ⁄ (k2 (ṁ0,2 / η0,2)nCon2 Pr0,21/3).

This is the default setting for the parameter r_nominal. Thus, if both sides of the heat exchanger have the same temperature difference, and the same medium, then r0=1. However, if medium 1 is air and medium 2 is water, and the heat exchanger is designed to have the same temperature drop for both media, then r0=0.5.

Related model

For a heat and moisture exchanger, use Buildings.Fluid.MassExchangers.ConstantEffectiveness.

Parameters

TypeNameDefaultDescription
BooleanprescribedHeatFlowRate1 (from StaticFourPortHeatMassExchanger)falseSet to true if the heat flow rate into fluid 1 is not a function of the component temperature
BooleanprescribedHeatFlowRate2 (from StaticFourPortHeatMassExchanger)falseSet to true if the heat flow rate into fluid 2 is not a function of the component temperature
BooleanhomotopyInitialization (from StaticFourPortHeatMassExchanger)true= true, use homotopy method
BooleansensibleOnly1 (from StaticFourPortHeatMassExchanger)Set to true if sensible exchange only for medium 1
BooleansensibleOnly2 (from StaticFourPortHeatMassExchanger)Set to true if sensible exchange only for medium 2
Buildings.Fluid.Types.HeatExchangerConfigurationconfiguration (from PartialEffectivenessNTU)Heat exchanger configuration
Booleanuse_dynamicFlowRegime (from PartialEffectivenessNTU)falseIf true, flow regime is determined using actual flow rates
Modelica.Units.SI.ThermalConductanceUA_nominal (from PartialEffectivenessNTU)Nominal UA value
RealNTU_nominal (from PartialEffectivenessNTU)Nominal number of transfer units
Modelica.Units.SI.ThermalConductancehA1_nominal(1 + r_nominal)*UA_nominalNominal convective heat transfer coefficient for medium 1
Modelica.Units.SI.ThermalConductancehA2_nominalhA1_nominal/r_nominalNominal convective heat transfer coefficient for medium 2
Medium1.DynamicViscosityeta1_defaultMedium1.dynamicViscosity(sta1_default)Dynamic viscosity
Medium1.ThermalConductivityk1_defaultMedium1.thermalConductivity(sta1_default)Thermal conductivity
Medium1.PrandtlNumberPr1_defaultMedium1.prandtlNumber(sta1_default)Prandtl number
Medium2.DynamicViscosityeta2_defaultMedium2.dynamicViscosity(sta2_default)Dynamic viscosity
Medium2.ThermalConductivityk2_defaultMedium2.thermalConductivity(sta2_default)Thermal conductivity
Medium2.PrandtlNumberPr2_defaultMedium2.prandtlNumber(sta2_default)Prandtl number
Assumptions
BooleanallowFlowReversal1 (from PartialFourPort)true= false to simplify equations, assuming, but not enforcing, no flow reversal for medium 1
BooleanallowFlowReversal2 (from PartialFourPort)true= false to simplify equations, assuming, but not enforcing, no flow reversal for medium 2
Nominal condition
Modelica.Units.SI.MassFlowRatem1_flow_nominal (from PartialFourPortInterface)Nominal mass flow rate
Modelica.Units.SI.MassFlowRatem2_flow_nominal (from PartialFourPortInterface)Nominal mass flow rate
Modelica.Units.SI.PressureDifferencedp1_nominal (from FourPortFlowResistanceParameters)Pressure difference
Modelica.Units.SI.PressureDifferencedp2_nominal (from FourPortFlowResistanceParameters)Pressure difference
Advanced
Medium1.MassFlowRatem1_flow_small (from PartialFourPortInterface)1E-4*abs(m1_flow_nominal)Small mass flow rate for regularization of zero flow
Medium2.MassFlowRatem2_flow_small (from PartialFourPortInterface)1E-4*abs(m2_flow_nominal)Small mass flow rate for regularization of zero flow
Advanced › Diagnostics
Booleanshow_T (from PartialFourPortInterface)false= true, if actual temperature at port is computed
Flow resistance › Medium 1
BooleancomputeFlowResistance1 (from FourPortFlowResistanceParameters)true=true, compute flow resistance. Set to false to assume no friction
Booleanfrom_dp1 (from FourPortFlowResistanceParameters)false= true, use m_flow = f(dp) else dp = f(m_flow)
Realn1 (from FourPortFlowResistanceParameters)2Flow exponent for side 1, n=1 for laminar, n=2 for turbulent
BooleanlinearizeFlowResistance1 (from FourPortFlowResistanceParameters)false= true, use linear relation between m_flow and dp for any flow rate
RealdeltaM1 (from FourPortFlowResistanceParameters)0.1Fraction of nominal flow rate where flow transitions to laminar
Flow resistance › Medium 2
BooleancomputeFlowResistance2 (from FourPortFlowResistanceParameters)true=true, compute flow resistance. Set to false to assume no friction
Booleanfrom_dp2 (from FourPortFlowResistanceParameters)false= true, use m_flow = f(dp) else dp = f(m_flow)
Realn2 (from FourPortFlowResistanceParameters)2Flow exponent for side 2, n=1 for laminar, n=2 for turbulent
BooleanlinearizeFlowResistance2 (from FourPortFlowResistanceParameters)false= true, use linear relation between m_flow and dp for any flow rate
RealdeltaM2 (from FourPortFlowResistanceParameters)0.1Fraction of nominal flow rate where flow transitions to laminar
Nominal thermal performance
Booleanuse_Q_flow_nominal (from PartialEffectivenessNTU)trueSet to true to specify Q_flow_nominal and temperatures, or to false to specify effectiveness
Modelica.Units.SI.HeatFlowRateQ_flow_nominal (from PartialEffectivenessNTU)Nominal heat flow rate (positive for heat transfer from 1 to 2)
Modelica.Units.SI.TemperatureT_a1_nominal (from PartialEffectivenessNTU)Nominal temperature at port a1
Modelica.Units.SI.TemperatureT_a2_nominal (from PartialEffectivenessNTU)Nominal temperature at port a2
Realeps_nominal (from PartialEffectivenessNTU)Nominal heat transfer effectiveness
Advanced › Heat transfer coefficients
Realr_nominal(k1_default*(m1_flow_nominal/eta1_default)^nCon1*Pr1_default^(1/3))/(k2_default*(m2_flow_nominal/eta2_default)^nCon2*Pr2_default^(1/3))Ratio between convective heat transfer coefficients at nominal conditions, r_nominal = hA1_nominal/hA2_nominal
RealnCon10.8Exponent for convective heat transfer coefficient, h1~m1_flow^n1
RealnCon2nCon1Exponent for convective heat transfer coefficient, h2~m2_flow^n2

Connectors

TypeNameDefaultDescription
Modelica.Fluid.Interfaces.FluidPort_aport_a1 (from PartialFourPort)Fluid connector a1 (positive design flow direction is from port_a1 to port_b1)
Modelica.Fluid.Interfaces.FluidPort_bport_b1 (from PartialFourPort)Fluid connector b1 (positive design flow direction is from port_a1 to port_b1)
Modelica.Fluid.Interfaces.FluidPort_aport_a2 (from PartialFourPort)Fluid connector a2 (positive design flow direction is from port_a2 to port_b2)
Modelica.Fluid.Interfaces.FluidPort_bport_b2 (from PartialFourPort)Fluid connector b2 (positive design flow direction is from port_a2 to port_b2)

Components

TypeNameDefaultDescription
Medium1.MassFlowRatem1_flow (from PartialFourPortInterface)port_a1.m_flowMass flow rate from port_a1 to port_b1 (m1_flow > 0 is design flow direction)
Modelica.Units.SI.PressureDifferencedp1 (from PartialFourPortInterface)port_a1.p - port_b1.pPressure difference between port_a1 and port_b1
Medium2.MassFlowRatem2_flow (from PartialFourPortInterface)port_a2.m_flowMass flow rate from port_a2 to port_b2 (m2_flow > 0 is design flow direction)
Modelica.Units.SI.PressureDifferencedp2 (from PartialFourPortInterface)port_a2.p - port_b2.pPressure difference between port_a2 and port_b2
Medium1.ThermodynamicStatesta_a1 (from PartialFourPortInterface)if allowFlowReversal1 then Medium1.setState_phX(port_a1.p, noEvent(actualStream(port_a1.h_outflow)), noEvent(actualStream(port_a1.Xi_outflow))) else Medium1.setState_phX(port_a1.p, inStream(port_a1.h_outflow), inStream(port_a1.Xi_outflow))Medium properties in port_a1
Medium1.ThermodynamicStatesta_b1 (from PartialFourPortInterface)if allowFlowReversal1 then Medium1.setState_phX(port_b1.p, noEvent(actualStream(port_b1.h_outflow)), noEvent(actualStream(port_b1.Xi_outflow))) else Medium1.setState_phX(port_b1.p, port_b1.h_outflow, port_b1.Xi_outflow)Medium properties in port_b1
Medium2.ThermodynamicStatesta_a2 (from PartialFourPortInterface)if allowFlowReversal2 then Medium2.setState_phX(port_a2.p, noEvent(actualStream(port_a2.h_outflow)), noEvent(actualStream(port_a2.Xi_outflow))) else Medium2.setState_phX(port_a2.p, inStream(port_a2.h_outflow), inStream(port_a2.Xi_outflow))Medium properties in port_a2
Medium2.ThermodynamicStatesta_b2 (from PartialFourPortInterface)if allowFlowReversal2 then Medium2.setState_phX(port_b2.p, noEvent(actualStream(port_b2.h_outflow)), noEvent(actualStream(port_b2.Xi_outflow))) else Medium2.setState_phX(port_b2.p, port_b2.h_outflow, port_b2.Xi_outflow)Medium properties in port_b2
Modelica.Units.SI.HeatFlowRateQ1_flow (from StaticFourPortHeatMassExchanger)Heat transferred into the medium 1
Medium1.MassFlowRatemWat1_flow (from StaticFourPortHeatMassExchanger)Moisture mass flow rate added to the medium 1
Modelica.Units.SI.HeatFlowRateQ2_flow (from StaticFourPortHeatMassExchanger)Heat transferred into the medium 2
Medium2.MassFlowRatemWat2_flow (from StaticFourPortHeatMassExchanger)Moisture mass flow rate added to the medium 2
Medium1.TemperatureT_in1 (from PartialEffectiveness)if allowFlowReversal1 then fra_a1*Medium1.temperature(state_a1_inflow) + fra_b1*Medium1.temperature(state_b1_inflow) else Medium1.temperature(state_a1_inflow)Inlet temperature medium 1
Medium2.TemperatureT_in2 (from PartialEffectiveness)if allowFlowReversal2 then fra_a2*Medium2.temperature(state_a2_inflow) + fra_b2*Medium2.temperature(state_b2_inflow) else Medium2.temperature(state_a2_inflow)Inlet temperature medium 2
Modelica.Units.SI.ThermalConductanceC1_flow (from PartialEffectiveness)abs(m1_flow)*(if allowFlowReversal1 then fra_a1*Medium1.specificHeatCapacityCp(state_a1_inflow) + fra_b1*Medium1.specificHeatCapacityCp(state_b1_inflow) else Medium1.specificHeatCapacityCp(state_a1_inflow))Heat capacity flow rate medium 1
Modelica.Units.SI.ThermalConductanceC2_flow (from PartialEffectiveness)abs(m2_flow)*(if allowFlowReversal2 then fra_a2*Medium2.specificHeatCapacityCp(state_a2_inflow) + fra_b2*Medium2.specificHeatCapacityCp(state_b2_inflow) else Medium2.specificHeatCapacityCp(state_a2_inflow))Heat capacity flow rate medium 2
Modelica.Units.SI.ThermalConductanceCMin_flow (from PartialEffectiveness)min(C1_flow, C2_flow)Minimum heat capacity flow rate
Modelica.Units.SI.HeatFlowRateQMax_flow (from PartialEffectiveness)CMin_flow*(T_in2 - T_in1)Maximum heat flow rate into medium 1
Modelica.Units.SI.ThermalConductanceUA (from PartialEffectivenessNTU)UA value
Realeps (from PartialEffectivenessNTU)Heat exchanger effectiveness
Modelica.Units.SI.ThermalConductancehA1Convective heat transfer coefficient for medium 1
Modelica.Units.SI.ThermalConductancehA2Convective heat transfer coefficient for medium 2

Revisions

  • June 19, 2026, by Michael Wetter:
    Renamed exponents for convective heat transfer coefficients from n1 and n2 to nCon1 and nCon2.
    This is for issue 4620.
  • March 15, 2022, by Michael Wetter:
    Introduced parameter r_nominal and exposed exponents of convective heat transfer coefficients.
    This is for issue 2918.
  • September 25, 2018, by Michael Wetter:
    First implementation.