Buildings.UsersGuide.ReleaseNotes
Release notes
Information
This section summarizes the changes that have been performed on the Buildings library.
- Version 4.0.0 (March 29, 2017)
- Version 3.0.0 (March 29, 2016)
- Version 2.1.0 (July 13, 2015)
- Version 2.0.0 (May 4, 2015)
- Version 1.6 build1 (June 19, 2014)
- Version 1.5 build3 (February 12, 2014)
- Version 1.5 build2 (December 13, 2013)
- Version 1.5 build1 (October 24, 2013)
- Version 1.4 build1 (May 15, 2013)
- Version 1.3 build1 (January 8, 2013)
- Version 1.2 build1 (July 26, 2012)
- Version 1.1 build1 (February 29, 2012)
- Version 1.0 build2 (December 8, 2011)
- Version 1.0 build1 (November 4, 2011)
- Version 0.12.0 (May 6, 2011)
- Version 0.11.0 (March 17, 2011)
- Version 0.10.0 (July 30, 2010)
- Version 0.9.1 (June 24, 2010)
- Version 0.9.0 (June 11, 2010)
- Version 0.8.0 (February 6, 2010)
- Version 0.7.0 (September 29, 2009)
- Version 0.6.0 (May 15, 2009)
- Version 0.5.0 (February 19, 2009)
- Version 0.4.0 (October 31, 2008)
- Version 0.3.0 (September 30, 2008)
- Version 0.2.0 (June 17, 2008)
- Version 0.1.0 (May 27, 2008)
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Package Content
Name | Description |
---|---|
Version_4_0_0 | Version 4.0.0 |
Version_3_0_0 | Version 3.0.0 |
Version_2_1_0 | Version 2.1.0 |
Version_2_0_0 | Version 2.0.0 |
Version_1_6_build1 | Version 1.6 build 1 |
Version_1_5_build3 | Version 1.5 build 3 |
Version_1_5_build2 | Version 1.5 build 2 |
Version_1_5_build1 | Version 1.5 build 1 |
Version_1_4_build1 | Version 1.4 build 1 |
Version_1_3_build1 | Version 1.3 build 1 |
Version_1_2_build1 | Version 1.2 build 1 |
Version_1_1_build1 | Version 1.1 build 1 |
Version_1_0_build2 | Version 1.0 build 2 |
Version_1_0_build1 | Version 1.0 build 1 |
Version_0_12_0 | Version 0.12.0 |
Version_0_11_0 | Version 0.11.0 |
Version_0_10_0 | Version 0.10.0 |
Version_0_9_1 | Version 0.9.1 |
Version_0_9_0 | Version 0.9.0 |
Version_0_8_0 | Version 0.8.0 |
Version_0_7_0 | Version 0.7.0 |
Version_0_6_0 | Version 0.6.0 |
Version_0_5_0 | Version 0.5.0 |
Version_0_4_0 | Version 0.4.0 |
Version_0_3_0 | Version 0.3.0 |
Version_0_2_0 | Version 0.2.0 |
Version_0_1_0 | Version 0.1.0 |
Buildings.UsersGuide.ReleaseNotes.Version_4_0_0
Version 4.0.0
Information
Version 4.0.0 is a major new release. It is the first release that is based on the Modelica IBPSA Library (https://github.com/ibpsa/modelica). All models simulate with Dymola 2017 FD01 and with JModelica, and the results of these simulators have been cross-compared and are equal within the expected tolerance.
The following major changes have been done:
-
It no longer uses the
Modelica_StateGraph2
library. Instead, it usesModelica.StateGraph
which is part of the Modelica Standard Library. -
The models in
Buildings.Fluid.Movers
have been refactored to increase the numerical robustness at very low speed when the fans or pumps are switched on or off. -
The following new packages have been added:
-
Buildings.Experimental.DistrictHeatingCooling
with models for district heating and cooling with bi-directional flow in the distribution pipes. -
Buildings.Fluid.FMI.Adaptors
andBuildings.Fluid.FMI.ExportContainers
, which allow export of HVAC systems and of thermal zones as Functional Mockup Units. -
Buildings.Fluid.HeatExchangers.ActiveBeams
, with active beams for cooling and heating. -
Buildings.Fluid.HeatExchangers.DXCoils.WaterCooled
, with water-cooled direct expansion cooling coils. -
Buildings.ThermalZones.ReducedOrder
, with reduced order models of thermal zones based on VDI 6007 that are suitable for district energy simulation.
-
-
The package
Buildings.Rooms
has been renamed toBuildings.ThermalZones.Detailed
. This was done because of the introduction ofBuildings.ThermalZones.ReducedOrder
, which is from theAnnex60
library, in order for thermal zones to be in the same top-level package.
For Dymola, the conversion script will update models that use any model of the packageBuildings.Rooms
. -
The model
Buildings.Fluid.FixedResistances.FixedResistanceDpM
has been refactored. Now, if the hydraulic diameter is not yet known, one can use the simpler modelBuildings.Fluid.FixedResistances.PressureDrop
, otherwise the modelBuildings.Fluid.FixedResistances.HydraulicDiameter
may be used. With this refactoring, also the modelBuildings.Fluid.FixedResistances.SplitterFixedResistanceDpM
has been renamed toBuildings.Fluid.FixedResistances.Junction
and parameters that use the hydraulic diameter have been removed. -
The models
Buildings.HeatTransfer.Conduction.SingleLayer
,Buildings.HeatTransfer.Conduction.MultiLayer
, andBuildings.HeatTransfer.Windows.Window
have been refactored to add the option to place a state at the surface of a construction. This leads in many examples that use the room model to a smaller number of non-linear system of equations and a 20% to 40% faster simulation. -
The models
Buildings.Fluid.HeatPumps.ReciprocatingWaterToWater
andBuildings.Fluid.HeatPumps.ScrollWaterToWater
have been added. Parameters to these models rely on calibration with tabulated heat pump performance data. Python scripts for the calibration of the heat pump models are inBuildings/Resources/src/fluid/heatpumps/calibration
. This is for issue 587.
The following new libraries have been added:
Buildings.Experimental.DistrictHeatingCooling | Package with models for district heating and cooling with bi-directional flow in the distribution pipes. |
Buildings.Fluid.FMI.Adaptors Buildings.Fluid.FMI.ExportContainers |
Library with adaptors to export HVAC systems and thermal zones
as a Functional Mockup Unit for Model Exchange. This is for Buildings, #506. |
Buildings.Fluid.HeatExchangers.ActiveBeams | Package with models of active beams for space cooling and heating. |
Buildings.Fluid.HeatExchangers.DXCoils.WaterCooled | Package with models of water-cooled direct expansion cooling coils with single speed, variable speed or multi-stage compressor. |
Buildings.Fluid.HeatPumps.Compressors | Package with models of compressors for heat pumps. |
Buildings.ThermalZones.ReducedOrder | Package with reduced order models of thermal zones based on VDI 6007. |
The following new components have been added to existing libraries:
Buildings.Fluid.Sensors | |
Buildings.Fluid.Sensors.Velocity | Sensor for the flow velocity. |
Buildings.Fluid.HeatExchangers | |
Buildings.Fluid.HeatExchangers.EvaporatorCondenser | Model for evaporator/condenser with refrigerant experiencing constant temperature phase change. |
Buildings.Fluid.HeatPumps | |
Buildings.Fluid.HeatPumps.ReciprocatingWaterToWater | Model for water to water heat pump with a reciprocating compressor. |
Buildings.Fluid.HeatPumps.ScrollWaterToWater | Model for water to water heat pump with a scroll compressor. |
Buildings.HeatTransfer.Windows.BaseClasses | |
Buildings.HeatTransfer.Windows.BaseClasses.HeatCapacity | Model for adding a state on the room-facing surface of a window. This closes issue 565. |
Buildings.Media | |
Buildings.Media.Refrigerants.R410A | Model for thermodynamic properties of refrigerant R410A. |
Buildings.Media.Specialized.Water.ConstantProperties_pT | Model for liquid water with constant properties at user-selected temperature. This closes IBPSA, #511. |
Buildings.Utilities.Math | |
Buildings.Utilities.Math.IntegratorWithReset | Integrator with optional input that allows
resetting the state if the input changes from false
to true .This closes IBPSA, #494. |
Buildings.Utilities.Time | |
Buildings.Utilities.Time.CalendarTime | Block that outputs the calendar time, time of the week, hour of the day etc. This closes IBPSA, #501. |
The following existing components have been improved in a backward compatible way:
Buildings.BoundaryConditions | |
Buildings.BoundaryConditions.WeatherData.BaseClasses.Examples.GetHeaderElement Buildings.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath Buildings.BoundaryConditions.WeatherData.BaseClasses.getHeaderElementTMY3 Buildings.BoundaryConditions.WeatherData.ReaderTMY3 Buildings.BoundaryConditions.SolarGeometry.ProjectedShadowLength |
Refactored the use of Modelica.Utilities.Files.loadResource
to make the model work in JModelica.
This closes
issue 506.
Removed the use of Modelica.Utilities.Files.fullPathName
in Buildings.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath
which is implicitly done in Modelica.Utilities.Files.loadResource.
Removed in Buildings.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath
the addition of file:// to file names which do not start
with file:// , or modelica:// .
This is not required when using
Modelica.Utilities.Files.loadResource .
This closes
issue 539.
|
Buildings.BoundaryConditions.WeatherData.ReaderTMY3 | Shifted the computation of the infrared irradiation such that
the results in Buildings.BoundaryConditions.SkyTemperature.Examples.BlackBody
are consistent for both option of the black-body sky temperature calculation.
This closes
IBPSA, #648.
|
Buildings.BoundaryConditions.SolarIrradiation.BaseClasses.SkyClearness | Reduced tolerance for regularization if the sky clearness is near one or eight. This closes IBPSA, #521. |
Buildings.Controls | |
Buildings.Controls.Continuous.LimPID Buildings.Controls.Continuous.PIDHysteresis Buildings.Controls.Continuous.PIDHysteresisTimer |
Added option to reset the control output when an optional boolean input signal
changes from false to true .This closes IBPSA, #494. |
Buildings.Electrical | |
Buildings.Electrical.DC.Storage.Examples.Battery | Replaced Modelica_StateGraph2 with
Modelica.StateGraph .
This closes
issue 504.
|
Buildings.Examples | |
Buildings.Examples.DualFanDualDuct.ClosedLoop Buildings.Examples.VAVReheat.ClosedLoop |
Added hysteresis to the economizer control to avoid many events.
This change was done in
Buildings.Examples.VAVReheat.Controls.EconomizerTemperatureControl .
This closes
issue 502.
|
Buildings.Examples.DualFanDualDuct.ClosedLoop | Set filteredSpeed=false in fan models to avoid a large
increase in computing time when simulated between t=1.60E7
and t=1.66E7.
|
Buildings.Examples.VAVReheat.ClosedLoop | Changed chilled water supply temperature to 6ˆC. This closes issue 509. |
Buildings.Examples.ChillerPlant.BaseClasses.Controls.BatteryControl Buildings.Examples.ChillerPlant.BaseClasses.Controls.WSEControl Buildings.Examples.HydronicHeating.TwoRoomsWithStorage Buildings.Examples.Tutorial.Boiler.System7 |
Replaced Modelica_StateGraph2 with
Modelica.StateGraph .
This closes
issue 504.
|
Buildings.HeatTransfer | |
Buildings.HeatTransfer.Conduction.SingleLayer | Added option to place a state at the surface of a construction. This closes issue 565. |
Buildings.HeatTransfer.Conduction.MultiLayer | Added option to place a state at the surface of a construction. This closes issue 565. |
Buildings.HeatTransfer.Windows.Window | Added option to place a state at the surface of a construction. This closes issue 565. |
Buildings.HeatTransfer.Windows.BeamDepthInRoom | Refactored the use of Modelica.Utilities.Files.loadResource .
This closes
issue 506.
|
Buildings.ThermalZones | |
Buildings.ThermalZones.Detailed.CFD Buildings.ThermalZones.Detailed.BaseClasses.CFDExchange |
Refactored the use of Modelica.Utilities.Files.loadResource .
This closes
issue 506.
|
Buildings.ThermalZones.Detailed.MixedAir Buildings.ThermalZones.Detailed.CFD |
Refactored the distribution of the diffuse solar irradiation. Previously, the model assumed that all diffuse irradiation first hits the floor before it is diffusely reflected to all other surfaces. Now, the incoming diffuse solar irradiation is distributed to all surfaces, proportional to their emissivity plus transmissivity times area. This closes issue 451. |
The following existing components have been improved in a non-backward compatible way:
Buildings.BoundaryConditions | |
Buildings.BoundaryConditions.WeatherData.BaseClasses.getHeaderElementTMY3 | This function is used to read location coordinates
from the TMY3 weather data file. The call to
Buildings.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath
has been removed as it calls the function
Modelica.Utilities.Files.loadResource, whose return value needs
to be known at compilation time to store the weather data in the FMU.
This is not supported by JModelica.
Most models should still work as this call has been added at a higher level
of the model hierarchy. If models don't work, add a call to loadResource
at the top-level.
This closes
Buildings, #506.
|
Buildings.Controls | |
Buildings.Controls.Continuous.PIDHysteresis | Set zer(final k=0) and made
swi , zer and
zer1 protected, as they are for
Buildings.Controls.Continuous.PIDHysteresis.
Only models that access these instances, which typically is not the case,
are affected by this change.
|
Buildings.Controls.Continuous.LimPID Buildings.Controls.Continuous.PIDHysteresis Buildings.Controls.Continuous.PIDHysteresisTimer |
Removed the parameter limitsAtInit as
it is not used.For Dymola, the conversion script will update models that set this parameter. |
Buildings.Controls.SetPoints.Table | Changed protected final parameter nCol to nRow .For Dymola, the conversion script will update models that access this parameter. This is for issue 555. |
Buildings.Fluid.Actuators | |
Buildings.Fluid.Actuators.Dampers.Exponential Buildings.Fluid.Actuators.Dampers.MixingBox Buildings.Fluid.Actuators.Dampers.MixingBoxMinimumFlow Buildings.Fluid.Actuators.Dampers.VAVBoxExponential Buildings.Fluid.Actuators.Dampers.MixingBoxMinimumFlow Buildings.Fluid.Actuators.Valves.ThreeWayEqualPercentageLinear Buildings.Fluid.Actuators.Valves.ThreeWayLinear Buildings.Fluid.Actuators.Valves.TwoWayEqualPercentage Buildings.Fluid.Actuators.Valves.TwoWayLinear Buildings.Fluid.Actuators.Valves.TwoWayPressureIndependent Buildings.Fluid.Actuators.Valves.TwoWayQuickOpening Buildings.Fluid.Actuators.Valves.TwoWayTable |
Renamed the parameter
filteredOpening to
use_inputFilter .For Dymola, the conversion script will update models that access this parameter. This is for IBPSA, #665 |
Buildings.Fluid.Actuators.Dampers.Exponential Buildings.Fluid.Actuators.Dampers.MixingBox Buildings.Fluid.Actuators.Dampers.MixingBoxMinimumFlow Buildings.Fluid.Actuators.Dampers.VAVBoxExponential Buildings.Fluid.Actuators.Dampers.MixingBoxMinimumFlow |
Renamed the parameters
use_v_nominal and all area related parameters,
because m_flow_nominal and v_nominal
are used to compute the area.For Dymola, the conversion script will update models that access this parameter. This is for IBPSA, #544 |
Buildings.Fluid.Chillers | |
Buildings.Fluid.Chillers.Carnot_TEva Buildings.Fluid.Chillers.Carnot_y |
Removed the parameters
effInpEva and
effInpCon .
Now, always the leaving water temperatures are used to compute the coefficient
of performance (COP). Previously, the
entering water temperature could be used, but this can give COPs that are higher than
the Carnot efficiency if the temperature lift is small.
For Dymola, the conversion script will update models.This is for IBPSA, #497 |
Buildings.Fluid.FixedResistances | |
Buildings.Fluid.FixedResistances.FixedResistanceDpM | Renamed
Buildings.Fluid.FixedResistances.FixedResistanceDpM to
Buildings.Fluid.FixedResistances.PressureDrop
and removed the parameters use_dh , dh and ReC .
For Dymola, the conversion script will update models.
If a model needs to be used that allows specifying dh and ReC ,
then the new model
Buildings.Fluid.FixedResistances.HydraulicDiameter can be used.
|
Buildings.Fluid.FixedResistances.SplitterFixedResistanceDpM | Renamed
Buildings.Fluid.FixedResistances.SplitterFixedResistanceDpM to
Buildings.Fluid.FixedResistances.Junction
and removed the parameters use_dh , dh and ReC .
For Dymola, the conversion script will update models.
If a model needs to be used that allows specifying dh and ReC ,
then use Buildings.Fluid.FixedResistances.Junction with
dp_nominal = 0 (which removes the pressure drop) and use
Buildings.Fluid.FixedResistances.HydraulicDiameter at each fluid port.
|
Buildings.Fluid.FMI | |
Buildings.Fluid.FMI.InletAdaptor Buildings.Fluid.FMI.OutletAdaptor Buildings.Fluid.FMI.TwoPort Buildings.Fluid.FMI.TwoPortComponent |
Renamed
Buildings.Fluid.FMI.InletAdaptor to
Buildings.Fluid.FMI.Adaptors.Inlet ,renamed Buildings.Fluid.FMI.OutletAdaptor to
Buildings.Fluid.FMI.Adaptors.Outlet ,renamed Buildings.Fluid.FMI.TwoPort to
Buildings.Fluid.FMI.ExportContainers.PartialTwoPort ,renamed Buildings.Fluid.FMI.TwoPortComponent to
Buildings.Fluid.FMI.ExportContainers.ReplaceableTwoPort .
This was due to the restructuring of the Buildings.Fluid.FMI
package for
Buildings, #506.For Dymola, the conversion script updates these models. |
Buildings.Fluid.HeatExchangers | |
Buildings.Fluid.HeatExchangers.DXCoils.SingleSpeed Buildings.Fluid.HeatExchangers.DXCoils.VariableSpeed Buildings.Fluid.HeatExchangers.DXCoils.MultiStage Buildings.Fluid.HeatExchangers.DXCoils.Data |
Renamed
Buildings.Fluid.HeatExchangers.DXCoils.SingleSpeed toBuildings.Fluid.HeatExchangers.DXCoils.AirCooled.SingleSpeed ,Buildings.Fluid.HeatExchangers.DXCoils.VariableSpeed toBuildings.Fluid.HeatExchangers.DXCoils.AirCooled.VariableSpeed ,Buildings.Fluid.HeatExchangers.DXCoils.MultiStage toBuildings.Fluid.HeatExchangers.DXCoils.AirCooled.MultiStage andBuildings.Fluid.HeatExchangers.DXCoils.Data toBuildings.Fluid.HeatExchangers.DXCoils.AirCooled.Data .This was due to the addition of the new package Buildings.Fluid.HeatExchangers.DXCoils.WaterCooled .
This is for
Buildings, #635.For Dymola, the conversion script updates these models. |
Buildings.Fluid.HeatPumps | |
Buildings.Fluid.HeatPumps.Carnot_TEva Buildings.Fluid.HeatPumps.Carnot_y |
Removed the parameters
effInpEva and
effInpCon .
Now, always the leaving water temperatures are used to compute the coefficient
of performance (COP). Previously, the
entering water temperature could be used, but this can give COPs that are higher than
the Carnot efficiency if the temperature lift is small.
For Dymola, the conversion script will update models.This is for IBPSA, #497 |
Buildings.Fluid.HeatExchangers.Boreholes | Moved the package Buildings.Fluid.HeatExchangers.Boreholes to
Buildings.Fluid.HeatExchangers.Ground.Boreholes .
This is for compatibility with an ongoing model development that will include
a borefield model.For Dymola, the conversion script will update models that use any model of the package Buildings.Fluid.HeatExchangers.Boreholes .
|
Buildings.Fluid.Movers | Removed the function
Buildings.Fluid.Movers.BaseClasses.Characteristics.flowApproximationAtOrigin
and changed the arguments of the function
Buildings.Fluid.Movers.BaseClasses.Characteristics.pressure .This was done due to the refactoring of the fan and pump model for low speed. This is for IBPSA, #458. Users who simply use the existing model in Buildings.Fluid.Movers are not affected by
this change as the function are called by a low-level implementation only.
|
Buildings.Fluid.Movers.
Buildings.Fluid.Movers.FlowControlled_dp Buildings.Fluid.Movers.FlowControlled_m_flow Buildings.Fluid.Movers.SpeedControlled_Nrpm Buildings.Fluid.Movers.SpeedControlled_y |
Renamed the parameter
filteredSpeed to
use_inputFilter .For Dymola, the conversion script will update models that access this parameter. This is for IBPSA, #665 |
Buildings.Fluid.HeatExchangers.CoolingTowers | Changed the name of the function
Buildings.Fluid.HeatExchangers.CoolingTowers.BaseClasses.Characteristics.efficiency
to
Buildings.Fluid.HeatExchangers.CoolingTowers.BaseClasses.Characteristics.normalizedPower .
Changed the name of the record
Buildings.Fluid.HeatExchangers.CoolingTowers.BaseClasses.Characteristics.efficiencyParameters
to
Buildings.Fluid.HeatExchangers.CoolingTowers.BaseClasses.Characteristics.fan ,
and changed the parameter of this record from
eta to r_P .
This change was done as the performance is for the relative power consumption, and not the fan
efficiency, as the old parameter name suggests.
Users who use the default parameters are not affected by this change.
If the default parameters were changed, then for Dymola,
the conversion script will update the model.
|
Buildings.HeatTransfer | |
Buildings.HeatTransfer.BaseClasses.TransmittedRadiation Buildings.HeatTransfer.BaseClasses.WindowRadiation |
Refactored the model to allow separate treatment for the diffuse and direct irradiation, which is needed for issue 451. |
Buildings.HeatTransfer.Conduction.BaseClasses.PartialConstruction | Removed parameter A as it is already declared in
Buildings.HeatTransfer.Conduction.BaseClasses.PartialConductor
which is often used with this class.
|
Buildings.ThermalZones | |
Buildings.ThermalZones.Detailed | Moved package from Buildings.Rooms to Buildings.ThermalZones.Detailed .
This was done because Buildings has a new package
Buildings.ThermalZones.ReducedOrder with reduced order building models.
Hence, the more detailed room models should be in the same top-level package as they
are also for modeling of thermal zones.For Dymola, the conversion script will update models that use any model of the package Buildings.ThermalZones .
|
Buildings.ThermalZones.Detailed.CFD Buildings.ThermalZones.Detailed.MixedAir Buildings.ThermalZones.Detailed.BaseClasses.CFDAirHeatMassBalance Buildings.ThermalZones.Detailed.BaseClasses.MixedAirHeatMassBalance Buildings.ThermalZones.Detailed.BaseClasses.PartialAirHeatMassBalance Buildings.ThermalZones.Detailed.BaseClasses.RoomHeatMassBalance |
Refactored implementation of latent heat gain for
Buildings, #515.
Users who simply use Buildings.MixedAir.Rooms.CFD or
Buildings.MixedAir.Rooms.MixedAir will not be affected by this change,
except if they access variables related to the heat gain.
|
Buildings.ThermalZones.Detailed.BaseClasses.AirHeatMassBalanceMixed Buildings.ThermalZones.Detailed.BaseClasses.MixedAirHeatGain |
Removed models as these are no longer needed due after the refactoring of the room model for Buildings, #515. |
Buildings.ThermalZones.Detailed.BaseClasses.RoomHeatMassBalance Buildings.ThermalZones.Detailed.BaseClasses.SolarRadiationExchange |
Refactored the distribution of the diffuse solar irradiation, which required replacing the
input and output signals.
Previously, the model assumed that all diffuse irradiation first hits the floor before it is
diffusely reflected to all other surfaces. Now, the incoming diffuse solar irradiation is distributed
to all surfaces, proportional to their emissivity plus transmissivity times area. This closes issue 451. |
Buildings.ThermalZones.Detailed.BaseClasses.CFDHeatGain | Renamed model from Buildings.ThermalZones.Detailed.BaseClasses.CFDHeatGain to
Buildings.ThermalZones.Detailed.BaseClasses.HeatGain .This is for Buildings, #515. |
Buildings.ThermalZones.Detailed.BaseClasses.CFDExchange | Removed the parameter uStart as it is not required. As this is in a base
class, users typically won't need to change their models
unless they use this base class directly.This is for Buildings, #579. |
Buildings.Utilities | |
Buildings.Utilities.Psychrometrics.WetBul_pTX | Deleted the model
Buildings.Utilities.Psychrometrics.WetBul_pTX
as the same functionality is provided by
Buildings.Utilities.Psychrometrics.TWetBul_TDryBulXi .
Users who use Buildings.Utilities.Psychrometrics.WetBul_pTX
need to replace the model manually and reconnect the input and output ports.This is for IBPSA, #475. |
The following critical errors have been fixed (i.e., errors that can lead to wrong simulation results):
Buildings.Fluid | |
Buildings.Fluid.HeatExchangers.DXCoils.AirCooled.MultiStage Buildings.Fluid.HeatExchangers.DXCoils.AirCooled.SingleSpeed Buildings.Fluid.HeatExchangers.DXCoils.AirCooled.VariableSpeed Buildings.Fluid.HeatExchangers.DXCoils.AirCooled.BaseClasses.Evaporation |
Corrected the computation of the wet bulb state in the model that computes the reevaporation of water vapor into the air stream when the coil is switched off. The results change slightly. This closes issue 520 and integrates the change of IBPSA, #474. |
Buildings.Fluid.Storage.StratifiedEnhancedInternalHex | Corrected computation of the heat exchanger location which was wrong
if hHex_a < hHex_b , e.g., the port a of the heat exchanger
is below the port b.
This closes
issue 531.
|
Buildings.Examples | |
Buildings.Examples.VAVReheat.ClosedLoop Buildings.Examples.DualFanDualDuct.ClosedLoop Buildings.Examples.VAVReheat.Controls.Economizer |
Corrected the economizer controller which closed the outside air when there was no freeze concern during summer. This closes issue 511. |
The following uncritical errors have been fixed (i.e., errors that do not lead to wrong simulation results, e.g., units are wrong or errors in documentation):
Buildings.Electrical | |
Buildings.Electrical.AC.OnePhase.Sources.Grid Buildings.Electrical.AC.ThreePhasesUnbalanced.Sources.Grid Buildings.Electrical.AC.ThreePhasesUnbalanced.Sources.Grid_N |
Corrected sign error in documentation string of
variable P .
|
Buildings.Fluid | |
Buildings.Fluid.HeatExchanger.WetCoilCounterFlow Buildings.Fluid.HeatExchanger.WetCoilDiscretized |
Redeclared Medium2 to force it to be a subclass
of Modelica.Media.Interfaces.PartialCondensingGases .This is for issue 544. |
Buildings.Fluid.Storage | Removed medium declaration, which is not needed and inconsistent with
the declaration in the base class. This is for issue 544. |
Buildings.ThermalZones.Detailed.Validation.BESTEST | |
Buildings.ThermalZones.Detailed.Validation.BESTEST.Case900 Buildings.ThermalZones.Detailed.Validation.BESTEST.Case900 |
Added missing parameter keyword,
which is required as the variable (for the materials) is assigned to a parameter.
This is for
issue 543.
|
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_3_0_0
Version 3.0.0
Information
Version 3.0.0 is a major new release.
The following major changes have been done:
-
Electrochromic windows have been added. See
Buildings.ThermalZones.Detailed.Examples.ElectroChromicWindow
. -
The models in
Buildings.Fluid.Movers
can now be configured to use three different control input signals: a continuous signal (depending on the model either normalized speed, speed in rpm, prescribed mass flow rate or prescribed head), discrete stages of these quantities, or on/off. The models also have been refactored to make their implementation clearer. -
The new package
Buildings.Fluid.HeatPumps
has been added. This package contains models for idealized heat pumps whose COP changes proportional to the change in COP of a Carnot cycle, with an optional correction for the part load efficiency. -
Various models, in particular in the package
Buildings.Electrical
, have been reformulated to comply with the Modelica Language Definition. All models comply with the pedantic Modelica check of Dymola.
The following new libraries have been added:
Buildings.Fluid.HeatPumps | Library with heat pump models.
This library contains models for idealized heat pumps
whose COP changes proportional to the change in COP of a Carnot cycle.
Optionally, a part load efficiency curve can be specified.
The model Buildings.Fluid.HeatPumps.Carnot_TCon
takes as a control input the leaving
condenser fluid temperature, and the model
Buildings.Fluid.HeatPumps.Carnot_y takes as
a control signal the compressor speed.
|
The following new components have been added to existing libraries:
Buildings.BoundaryConditions.SolarGeometry | |
Buildings.BoundaryConditions.SolarGeometry.ProjectedShadowLength | Block that computes the length of a shadow projected onto a horizontal plane into the direction that is perpendicular to the azimuth of a surface. |
Buildings.Electrical | |
Buildings.Electrical.AC.ThreePhasesUnbalanced.Interfaces.Adapter3to3 Buildings.Electrical.AC.ThreePhasesUnbalanced.Interfaces.Connection3to3Ground_n Buildings.Electrical.AC.ThreePhasesUnbalanced.Interfaces.Connection3to3Ground_p |
Adapters for unbalanced three phase systems which are required because the previous formulation used connect statements that violate the Modelica Language Definition. This change was required to enable pedantic model check and translation in Dymola 2016 FD01. This is for #426. |
Buildings.Fluid.Chillers | |
Buildings.Fluid.Chillers.Carnot_TEva | Chiller model whose efficiency changes with temperatures similarly to a change in Carnot efficiency. The control input signal is the evaporator leaving fluid temperature. This is for IBPSA, #353. |
Buildings.Fluid.Sensors | |
Buildings.Fluid.Sensors.PPM Buildings.Fluid.Sensors.PPMTwoPort |
Sensors that measure trace substances in parts per million. |
Buildings.HeatTransfer.Windows | |
Buildings.HeatTransfer.Windows.BeamDepthInRoom | Block that computes the maximum distance at which a solar beam that enters the window hits the workplane. |
Buildings.Utilities.Math | |
Buildings.Utilities.Math.Functions.smoothInterpolation | Function that interpolates for vectors xSup[] , ySup[]
and independent variable x .
The interpolation is done using a cubic Hermite spline with linear extrapolation.
|
The following existing components have been improved in a backward compatible way:
Buildings.Fluid | |
Buildings.Fluid.Actuators.Valves.ThreeWayEqualPercentageLinear Buildings.Fluid.Actuators.Valves.ThreeWayLinear |
Changed the default value for valve leakage
parameter l from 0 to 0.0001 .
This is the same value as is used for the two-way valves,
and avoids an assertion that would be triggered if l=0 .
|
Buildings.Fluid.HeatExchangers.Ground.Boreholes.UTube | Updated code for 64 bit on Linux and Windows. This closes issue 485. |
Buildings.Fluid.HeatExchangers.DryEffectivenessNTU | Reformulated model to allow translation in OpenModelica. This is for issue #490. |
Buildings.Fluid.Chillers.Carnot | Changed the sign convention for dTEva_nominal .
Now, this quantity needs to be negative.
This change was done to be consistent with other models.
In this version, a warning will be written if the sign
is not updated, but the results will be the same.
In future versions the warning will be
changed to an error.The parameters dTEva_nominal and
dTCon_nominal are now used
to assign default values for the nominal mass flow rates.
|
Buildings.Fluid.MixingVolumes.MixingVolume Buildings.Fluid.MixingVolumes.MixingVolumeMoistAir |
Added the parameter use_C_flow . If set
to true , an input connector will be enabled that can be used
to add a trace substance flow rate, such as CO2, to the volume.
|
Buildings.Fluid.Movers.FlowControlled_dp Buildings.Fluid.Movers.FlowControlled_m_flow Buildings.Fluid.Movers.FlowControlled_Nrpm Buildings.Fluid.Movers.FlowControlled_y |
Added the parameter inputType which allows
to set the input as an continuous input signal,
to set the input as an integer input signal that selects the stage of the mover,
or to remove the input connector and use a parameter
to assign the control signal.
|
Buildings.Fluid.Storage.StratifiedEnhancedInternalHex | Added option to set dynamics of heat exchanger material separately from the dynamics of the fluid inside the heat exchanger. This is for issue #434. |
Buildings.Fluid.Interfaces.FourPortHeatMassExchanger Buildings.Fluid.Interfaces.TwoPortHeatMassExchanger |
Propagated parameter allowFlowReversal
which can cause a simpler energy balance to be used.
|
Buildings.Fluid.Interfaces.PartialTwoPortTransport | Implemented more efficient computation of port_a.Xi_outflow
and port_a.C_outflow when allowFlowReversal=false .
This is for
IBPSA issue 305.
|
Buildings.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp Buildings.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow |
Refactored for a more efficient implementation.
Removed double declaration of smooth(..) and smoothOrder
and changed Inline=true to LateInline=true .
This is for
IBPSA issue 301
and for IBPSA issue 279.
|
Buildings.ThermalZones | |
Buildings.ThermalZones.Detailed.BaseClasses.CFDExchange | Set start and fixed
attributes in
u[nWri](start=_uStart, each fixed=true)
to avoid a warning in Dymola 2016 about unspecified initial conditions.
This closes
issue 422.Set start and fixed
attributes in
firstTrigger(start=false, fixed=true) ,
retVal(start=0, fixed=true) and modTimRea(fixed=false)
to avoid such a warning in the pedantic Modelica check in Dymola 2016.
This closes
issue 459.
|
Buildings.ThermalZones.Detailed.CFD | Updated code for 64 bit on Linux and Windows. This closes issue 485. |
Buildings.Utilities.Math.Functions | Refactored Buildings.Utilities.Math.Functions.inverseXRegularized
to make it more efficient as it is used in many steady-state energy balances.
This closes
IBPSA issue 302.
|
The following existing components have been improved in a non-backward compatible way:
Buildings.BoundaryConditions | |
Buildings.BoundaryConditions.SkyTemperature.BlackBody Buildings.BoundaryConditions.WeatherData.Bus |
Renamed the connector from radHorIR to HHorIR
This is for
IBPSA issue 376.
For Dymola, the conversion script updates these connections.
However, this also results in a renaming of the weather bus variable
weaBus.radHorIR to HHorIR , which may
require a manual update.
|
Buildings.Fluid | |
Buildings.Fluid.Interfaces.StaticTwoPortConservationEquation | Removed the constant sensibleOnly and
introduced instead the parameter use_mWat_flow .
The new parameter, if set to true , will enable an input connector
that can be used to add water to the conservation equation..
For Dymola, the conversion script updates the model for these changes.
|
Buildings.Fluid.Chillers.Carnot | Renamed the model to Buildings.Fluid.Chillers.Carnot_y
due to the addition of the new model Buildings.Fluid.Chillers.Carnot_TEva .
In addition, the following parameter names were changed:
use_eta_Carnot was changed to use_eta_Carnot_nominal , and
etaCar was changed to etaCarnot_nominal .
This is for
IBPSA issue 353.
For Dymola, the conversion script removes these parameters.
|
Buildings.Fluid.Movers.FlowControlled_dp Buildings.Fluid.Movers.FlowControlled_m_flow Buildings.Fluid.Movers.FlowControlled_Nrpm Buildings.Fluid.Movers.FlowControlled_y |
Removed the parameters use_powerCharacteristics
and motorCooledByFluid as these are already
declared in the performance data record per .
This is for issue
#457.
For Dymola, the conversion script removes these parameters.
|
Buildings.Fluid.Movers.FlowControlled_dp Buildings.Fluid.Movers.FlowControlled_m_flow Buildings.Fluid.Movers.FlowControlled_Nrpm Buildings.Fluid.Movers.FlowControlled_y |
Removed the public variable r_N .
This is for
IBPSA issue 417.
For Dymola, the conversion script removes
assignments of r_N(start) .
|
Buildings.Fluid.Movers.FlowControlled_dp Buildings.Fluid.Movers.FlowControlled_m_flow |
Write a warning if no pressure curve is provided because
the efficiency calculation can only be done correctly if a pressure curve
is provided. The warning can be suppressed by providing a pressure curve, or
by setting nominalValuesDefineDefaultPressureCurve=true .
|
Buildings.Fluid.Movers.Data | Replaced the parameters
Buildings.Fluid.Movers.Data.FlowControlled ,
Buildings.Fluid.Movers.Data.SpeedControlled_y , and
Buildings.Fluid.Movers.Data.SpeedControlled_Nrpm by
the parameter
Buildings.Fluid.Movers.Data.Generic
which is used for all four types of movers.
This is for
IBPSA issue 417.
This change allows to correctly compute the fan or pump power also for the models
Buildings.Fluid.Movers.FlowControlled_dp ,
Buildings.Fluid.Movers.FlowControlled_m_flow
for speeds that are different from the nominal speed, provided that the user
specifies the pressure curve.
For Dymola, the conversion script updates this parameter.In the previous record Buildings.Fluid.Movers.Data.SpeedControlled_Nrpm ,
changed the parameter N_nominal to speed_rpm_nominal .
This is for
IBPSA issue 396.
For Dymola, the conversion script updates this parameter.
|
Buildings.Fluid.BaseClasses.PartialThreeWayResistance Buildings.Fluid.Movers.BaseClasses.PartialFlowMachine Buildings.Fluid.Movers.FlowControlled_dp Buildings.Fluid.Movers.FlowControlled_m_flow Buildings.Fluid.Movers.FlowControlled_Nrpm Buildings.Fluid.Movers.FlowControlled_y Buildings.Fluid.Actuators.Valves.ThreeWayEqualPercentageLinear Buildings.Fluid.Actuators.Valves.ThreeWayLinear Buildings.Fluid.Actuators.Valves.TwoWayEqualPercentage |
Removed parameter dynamicBalance that overwrote the setting
of energyDynamics and massDynamics .
This is for
IBPSA, issue 411.
For Dymola, the conversion script updates the models.
|
Buildings.Fluid.Interfaces.PartialTwoPort | Renamed the protected parameters
port_a_exposesState , port_b_exposesState and
showDesignFlowDirection .
This is for
IBPSA issue 349
and
IBPSA issue 351.
For Dymola, the conversion script updates models
that extend from Buildings.Fluid.Interfaces.PartialTwoPort .
|
Buildings.Fluid.Interfaces.FourPort | Renamed model to Buildings.Fluid.Interfaces.PartialFourPort and
removed the parameters
h_outflow_a1_start ,
h_outflow_b1_start ,
h_outflow_a2_start and
h_outflow_b2_start
to make the model similar to Buildings.Fluid.Interfaces.PartialTwoPort .
See IBPSA issue 299
for a discussion.
For Dymola, the conversion script updates models
that extend from Buildings.Fluid.Interfaces.FourPort .
|
Buildings.Fluid.Interfaces.StaticTwoPortConservationEquation |
Revised implementation of conservation equations and
added default values for outlet quantities at port_a
if allowFlowReversal=false .
This is for IBPSA issue 281.
Also, revised implementation so that equations are always consistent
and do not lead to division by zero,
also when connecting a prescribedHeatFlowRate
to MixingVolume instances.
Renamed use_safeDivision to prescribedHeatFlowRate .
See IBPSA issue 282
for a discussion.
For users who simply instantiate existing component models, this change is backward
compatible.
However, developers who implement component models that extend from
Buildings.Fluid.Interfaces.StaticTwoPortConservationEquation may need to update
the parameter use_safeDivision and use instead prescribedHeatFlowRate .
See the model documentation.
|
Buildings.ThermalZones | |
Buildings.ThermalZones.Detailed.MixedAir Buildings.ThermalZones.Detailed.CFD |
These models can now be used with electrochromic windows.
This required to change the glass properties
tauSol , rhoSol_a and rhoSol_b
to be arrays. For example, to convert an existing model, use
tauSol={0.6} instead of tauSol=0.6 .
For Dymola, the conversion script will automatically
update existing models.
|
Buildings.Obsolete | |
Buildings.Obsolete.Fluid.Movers Buildings.Obsolete.Media |
Removed these packages which have models from release 2.0.0. |
The following critical errors have been fixed (i.e., errors that can lead to wrong simulation results):
Buildings.Fluid.Chillers | |
Buildings.Fluid.Chillers.Carnot | Corrected wrong computation of state of leaving fluid
staB1 and staB2
for the configuration without flow reversal.
The previous implementation mistakenly used the inStream operator.
This is for
issue 476
|
The following uncritical errors have been fixed (i.e., errors that do not lead to wrong simulation results, e.g., units are wrong or errors in documentation):
Buildings.Electrical | |
Buildings.Electrical.Interfaces.PartialWindTurbine | Reformulated test for equality of Real variables. This closes
issue 493.
|
Buildings.HeatTransfer | |
Buildings.HeatTransfer.Conduction.SingleLayer Buildings.HeatTransfer.Data.BaseClasses |
Reformulated test for equality of Real variables. This closes
issue 493.
|
Buildings.Fluid | |
Buildings.Fluid.FMI.FlowSplitter_u | Corrected wrong assert statement. This closes issue 442. |
Buildings.Fluid.Chillers.Carnot | Corrected wrong assert statement for test on the efficiency function. This closes issue 468. |
Buildings.Media | |
Buildings.Media.Specialized.Water.TemperatureDependentDensity | Removed dublicate entry of smooth and smoothOrder .
This is for
IBPSA issue 303.
|
Buildings.ThermalZones | |
Buildings.ThermalZones.Detailed.BaseClasses.MixedAirHeatGain | Reformulated test for equality of Real variables. This closes
issue 493.
|
Buildings.Utilities.Math | |
Buildings.Utilities.Math.Functions.BaseClasses.der_2_regNonZeroPower Buildings.Utilities.Math.Functions.BaseClasses.der_polynomial Buildings.Utilities.Math.Functions.BaseClasses.der_regNonZeroPower |
Corrected wrong derivative implementation and improved their regression tests. This is for IBPSA issue 303. |
Buildings.Utilities.Psychrometrics | |
Buildings.Utilities.Psychrometrics.Density_pTX | Corrected wrong default component name. |
Buildings.Utilities.Psychrometrics.Functions.saturationPressure | Changed smoothOrder from 5 to 1 as
Buildings.Utilities.Math.Functions.spliceFunction is only once
continuously differentiable.
Inlined the function.
|
Buildings.Utilities.IO.Python27 | |
Buildings.Utilities.IO.Python27.exchange | Updated Python implementation to allow compiling code
on 64 bit Linux. Previously, on Linux a segmentation fault
occurred during run-time if 64 bit code rather than
32 bit code was generated. This is now corrected. Also, Windows 64 bit binaries have been added. This closes issue 287. |
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_2_1_0
Version 2.1.0
Information
Version 2.1.0 is fully compatible with version 2.0.0.
It adds the package Buildings.Fluid.FMI
that provides containers
for exporting thermofluid flow components as FMUs.
It also updates the temperature sensor to optionally simulate heat losses,
and it contains bug fixes for the trace substance sensor if used without flow reversal.
Improvements have been made to various models to reduce the simulation time, and
to Buildings.Examples.Tutorial.Boiler
to simplify the control implementation.
The following new libraries have been added:
Buildings.Fluid.FMI | This package contains blocks that serve as containers for exporting
models from Buildings.Fluid as a Functional Mockup Unit (FMU).This allows using models from Buildings.Fluid , add them
to a block that only has input and output signals, but no acausal connectors,
and then export the model as a Functional Mockup Unit.
Models can be individual models or systems that are composed of various
models.
For more information, see the
User's Guide.
|
The following existing components have been improved in a backward compatible way:
Buildings.Examples | |
Buildings.Examples.Tutorial.Boiler.System5 Buildings.Examples.Tutorial.Boiler.System6 Buildings.Examples.Tutorial.Boiler.System7 |
Changed control input for conPIDBoi and set
reverseAction=true
to address issue
#436.
|
Buildings.Fluid | |
Buildings.Fluid.Chillers.Carnot Buildings.Fluid.HeatExchangers.DXCoils.BaseClasses.PartialDXCoil Buildings.Fluid.HeatExchangers.HeaterCooler_u Buildings.Fluid.MassExchangers.Humidifier_u |
Set parameter prescribedHeatFlowRate=true
which causes a simpler energy balance to be used.
|
Buildings.Fluid.Sensors.TemperatureTwoPort | Added option to simulate thermal loss, which is useful if the sensor is used to measure the fluid temperature in a system with on/off control for the mass flow rate. |
Buildings.Fluid.SolarCollectors.ASHRAE93 Buildings.Fluid.SolarCollectors.EN12975 |
Corrected sign error in computation of heat loss
that prevents the medium to exceed Medium.T_min
or Medium.T_max . With the previous implementation,
an assertion may be generated unnecessarily rather than
the model guiding against the violation of these bounds.
|
Buildings.Fluid.MixingVolumes.BaseClasses.PartialMixingVolume | Added test on allowFlowReversal in criteria
about what energy balance implementation to use.
This causes simpler models, for example when exporting
Buildings.Fluid.HeatExchangers.HeaterCooler_u
as an FMU.
|
The following critical errors have been fixed (i.e., errors that can lead to wrong simulation results):
Buildings.Fluid | |
Buildings.Fluid.Sensors.TraceSubstanceTwoPort | Corrected wrong sensor signal if allowFlowReversal=false .
For this setting, the sensor output was for the wrong flow direction.
This corrects
issue 249.
|
The following uncritical errors have been fixed (i.e., errors that do not lead to wrong simulation results, e.g., units are wrong or errors in documentation):
Buildings.Fluid | |
Buildings.Fluid.Interfaces.ConservationEquation Buildings.Fluid.Interfaces.StaticTwoPortConservationEquation |
Corrected documentation. |
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_2_0_0
Version 2.0.0
Information
Version 2.0.0 is a major release that contains various new packages, models and improvements.
The following major additions have been done in version 2.0:
- A CFD model that is embedded in a thermal zone has been added. This model is implemented in Buildings.ThermalZones.Detailed.CFD. The CFD model is an implementation of the Fast Fluid Dynamics code that allows three-dimensional CFD inside a thermal zone, coupled to building heat transfer, HVAC components and feedback control loops.
- A new package Buildings.Electrical has been added. This package allows studying buildings to electrical grid integration. It includes models for loads, transformers, cables, batteries, PV and wind turbines. Models exist for DC and AC systems with two- or three-phase that can be balanced and unbalanced. The models compute voltage, current, active and reactive power based on the quasi-stationary assumption or using the dynamic phasorial representation.
- The new package Buildings.Controls.DemandResponse contains models for demand response simulation.
- The new package Buildings.Controls.Predictors contains a data-driven model that predicts the electrical load of a building. The prediction can be done either using an average baseline or a linear regression with respect to outside temperature. For both, optionally a day-of adjustment can be made.
The tables below give more detailed information to the revisions of this library compared to the previous release 1.6 build 1.
The following new libraries have been added:
Buildings.Electrical | Library for electrical grid simulation that allows to study building to electrical grid integration. The library contains models of loads, generation and transmission for DC and AC systems. |
Buildings.Controls.DemandResponse | Library with a model for demand response prediction. |
Buildings.Controls.Predictors | Library with a data-driven model that predicts the electrical load of a building. The prediction can be done either using an average baseline or a linear regression with respect to outside temperature. For both, optionally a day-of adjustment can be made. |
The following new components have been added to existing libraries:
Buildings.Fluid | |
Buildings.Fluid.Actuators.Valves.TwoWayPressureIndependent | Model of a pressure-independent two way valve. |
Buildings.Fluid.HeatExchangers.HeaterCooler_T | Model of a heater or cooler that takes as an input the set point for the temperature of the fluid that leaves the component. The set point is tracked exactly if the component has sufficient capacity. Optionally, the component can be configured to compute a dynamic rather than a steady-state response. |
Buildings.Utilities | |
Buildings.Utilities.Psychrometrics.Phi_pTX Buildings.Utilities.Psychrometrics.Functions.phi_pTX |
Block and function that computes the relative humidity for given pressure, temperature and water vapor mass fraction. |
Buildings.ThermalZones | |
Buildings.ThermalZones.Detailed.CFD | Room model that computes the room air flow using computational fluid dynamics (CFD). The CFD simulation is coupled to the thermal simulation of the room and, through the fluid port, to the air conditioning system. Currently, the supported CFD program is the Fast Fluid Dynamics (FFD) program. See Buildings.ThermalZones.Detailed.UsersGuide.CFD for detailed explanations. |
The following existing components have been improved in a backward compatible way:
Buildings.BoundaryConditions | |
Buildings.BoundaryConditions.WeatherData.ReaderTMY3 | Added option to obtain the black body sky temperature
from a parameter or an input signal rather than
computing it in the weather data reader. Removed redundant connection connect(conHorRad.HOut, cheHorRad.HIn); .
|
Buildings.Fluid | |
Buildings.Chillers.ElectricEIR Buildings.Chillers.ElectricReformulatedEIR |
Changed implementation so that the model is continuously differentiable. This is for issue 373. |
Buildings.Fluid.HeatExchangers.DryCoilCounterFlow | Changed assignment of T_m to avoid using the conditionally
enabled model ele[:].mas.T , which is only
valid in a connect statement.
Moved assignments of
Q1_flow , Q2_flow , T1 ,
T2 and T_m outside of equation section
to avoid mixing graphical and textual modeling within the same model.
|
Buildings.Fluid.HeatExchangers.DryCoilDiscretized | Removed parameter m1_flow_nominal , as this parameter is already
declared in its base class
Buildings.Fluid.Interfaces.PartialFourPortInterface.
This change avoids an error in OpenModelica as the two declarations
had a different value for the min attribute, which is not valid
in Modelica.
|
Buildings.Fluid.HeatExchangers.BaseClasses.CoilRegister Buildings.Fluid.HeatExchangers.BaseClasses.DuctManifoldDistributor |
Reformulated the multiple iterators in the sum function
as this language construct is not supported in OpenModelica.
|
Buildings.Fluid.HeatExchangers.RadiantSlabs.SingleCircuitSlab | Set start value for hPip(fluid(T)) to avoid
a warning about conflicting start values.
|
Buildings.Fluid.Movers.SpeedControlled_y Buildings.Fluid.Movers.SpeedControlled_Nrpm Buildings.Fluid.Movers.FlowControlled_dp Buildings.Fluid.Movers.FlowControlled_m_flow |
For the parameter setting use_powerCharacteristic=true ,
changed the computation of the power consumption at
reduced speed to properly account for the
affinity laws. This is in response to
#202.
|
Buildings.Fluid.SolarCollectors.ASHRAE93 Buildings.Fluid.SolarCollectors.EN12975 |
Reformulated the model to avoid a translation error
if glycol is used. Propagated parameters for initialization in base class Buildings.Fluid.SolarCollectors.BaseClasses.PartialSolarCollector
and set prescribedHeatFlowRate=true .
|
Buildings.Fluid.Storage.StratifiedEnhancedInternalHex | Replaced the abs() function in the assignment of the parameter
nSegHexTan as the return value of abs()
is a Real which causes a type error during model check.
|
Buildings.HeatTransfer | |
Buildings.HeatTransfer.Conduction.MultiLayer | Changed the assignment of _T_a_start ,
_T_b_start and RTot to be
in the initial equation section as opposed to
the parameter declaration.
This is needed to avoid an error during model check
and translation in Dymola 2015 FD01 beta1.
|
Buildings.HeatTransfer.Windows.InteriorHeatTransferConvective | Changed model to allow a temperature dependent convective heat transfer on the room side. This is for issue 52. |
Buildings.Media | |
Buildings.Media.Interfaces.PartialSimpleIdealGasMedium Buildings.Media.Interfaces.PartialSimpleMedium |
Set T(start=T_default) and
p(start=p_default) in the
ThermodynamicState record. Setting the start value for
T is required to avoid an error due to
conflicting start values when translating
Buildings.Examples.VAVReheat.ClosedLoop in pedantic mode.
|
Buildings.ThermalZones | |
Buildings.ThermalZones.Detailed.MixedAir | Changed model to allow a temperature dependent convective heat transfer on the room side for windows. This is for issue 52. |
Rooms.BaseClasses.ExteriorBoundaryConditionsWithWindow | Conditionally removed the shade model if no shade is present. This corrects #234. |
The following existing components have been improved in a non-backward compatible way:
Buildings.Airflow | |
Buildings.Airflow.Multizone.ZonalFlow_ACS Buildings.Airflow.Multizone.ZonalFlow_m_flow |
Removed parameter forceErrorControlOnFlow as it was not used.
For Dymola, the conversion script will automatically
update existing models.
|
Buildings.BoundaryConditions | |
Buildings.BoundaryConditions.WeatherData.ReaderTMY3 | Changed the following signals for compatibility with OpenModelica:weaBus.sol.zen to weaBus.solZen .weaBus.sol.dec to weaBus.solDec .weaBus.sol.alt to weaBus.solAlt .weaBus.sol.solHouAng to weaBus.solHouAng .For Dymola, the conversion script will automatically update existing models. |
Buildings.Examples | |
Buildings.Examples.VAVReheat.Controls.IntegerSum | Removed block as it is not used in any model.
Models that require an integer sum can use
Modelica.Blocks.MathInteger.Sum .
|
Buildings.Examples.VAVReheat.Controls.UnoccupiedOn | Removed block as it is not used in any model. |
Buildings.HeatTransfer | |
Buildings.HeatTransfer.Data.GlazingSystems.Generic | Removed parameter nLay as OpenModelica
could not assign it during translation.
For Dymola, the conversion script will automatically
update existing models.
|
Buildings.HeatTransfer.Conduction.BaseClasses.der_temperature_u | Changed the input argument for this function from type
Buildings.HeatTransfer.Data.BaseClasses.Material
to the elements of this type as OpenModelica fails to translate the
model if the input to this function is a record.
|
Buildings.HeatTransfer.Types.Azimuth Buildings.HeatTransfer.Types.Tilt |
Moved these types from Buildings.HeatTransfer
to the top-level package Buildings because
they are used in Buildings.BoundaryConditions ,
Buildings.HeatTransfer and Buildings.ThermalZones.Detailed .For Dymola, the conversion script will automatically update existing models. |
Buildings.Fluid | |
Buildings.Fluid.FixedResistances.Pipe Buildings.Fluid.FixedResistances.BaseClasses.Pipe Buildings.Fluid.HeatExchangers.RadiantSlabs.SingleCircuitSlab |
Renamed pressure drop from res to
preDro to use the same name as in other models.
This corrects
#271.
For Dymola, the conversion script will automatically
update existing models.
|
Buildings.Fluid.HeatExchangers.DryCoilDiscretized Buildings.Fluid.HeatExchangers.WetCoilDiscretized |
Reformulated flow splitter in the model to reduce
the dimension of the coupled linear or nonlinear
system of equations. With this revision, the optional
control volume in the duct inlet has been removed
as it is no longer needed. Therefore, the parameter
dl has also been removed.
Replaced the parameters energyDynamics1
and energyDynamics2 with
energyDynamics .
Removed the parameter ductConnectionDynamics .For Dymola, the conversion script will automatically update existing models. |
Buildings.Fluid.HeatExchangers.HeaterCoolerPrescribed | Renamed the model to HeaterCooler_u due to
the introduction of the new model HeaterCooler_T .For Dymola, the conversion script will automatically update existing models. |
Buildings.Fluid.HeatExchangers.RadiantSlabs.SingleCircuitSlab Buildings.Fluid.HeatExchangers.RadiantSlabs.ParallelCircuitsSlab |
Changed the models to use by default an ε-NTU
approach for the heat transfer between the fluid and the slab
rather than a finite difference scheme along the
flow path.
Optionally, the finite difference scheme can also be used
as this is needed for some control design applications. The new ε-NTU formulation has shown to lead to about five times faster computation on several test cases including the models in Buildings.ThermalZones.Detailed.FLEXLAB.Rooms.Examples. For Dymola, the conversion script will automatically update existing models. |
Buildings.Fluid.HeatExchangers.BaseClasses.DuctManifoldFixedResistance | Reformulated flow splitter in the model to reduce
the dimension of the coupled linear or nonlinear
system of equations. With this revision, the optional
control volume in the duct inlet has been removed
as it is no longer needed. Therefore, the parameters
dl and energyDynamics have
also been removed.For Dymola, the conversion script will automatically update existing models. |
Buildings.Fluid.HeatExchangers.BaseClasses.CoilRegister | Replaced the parameters energyDynamics1
and energyDynamics2 with
the new parameter energyDynamics .
Removed the parameters steadyState_1
and steadyState_2 as this information
is already contained in energyDynamics .For Dymola, the conversion script will automatically update existing models. |
Buildings.Fluid.MassExchangers.HumidifierPrescribed | Renamed the model to Humidifier_u due to
the introduction of the new model HeaterCooler_T
and to use the same naming pattern as HeaterCooler_u .For Dymola, the conversion script will automatically update existing models. |
Buildings.Fluid.Movers | This package has been redesigned.
The models have been renamed as follows:Buildings.Fluid.Movers.FlowMachine_dp
is now called
Buildings.Fluid.Movers.FlowControlled_dp .Buildings.Fluid.Movers.FlowMachine_m_flow
is now called
Buildings.Fluid.Movers.FlowControlled_m_flow .Buildings.Fluid.Movers.FlowMachine_Nrpm
is now called
Buildings.Fluid.Movers.SpeedControlled_Nrpm .Buildings.Fluid.Movers.FlowMachine_y
is now called
Buildings.Fluid.Movers.SpeedControlled_y .In addition, the performance data of all movers are now stored in a record. These records are in Buildings.Fluid.Movers.Data. For most existing instances, it should be sufficient to enclose the existing performance data in a record called per .
For example,
becomes
See the User's Guide for more information about these records. For Dymola, the conversion script will update existing models to use the old implementations which are now in the package Buildings.Obsolete.Fluid.Movers .
|
Buildings.Media | |
Buildings.Media |
Renamed all media to simplify the media selection.
For typical building energy simulation,
Buildings.Media.Air and
Buildings.Media.Water
should be used. The following changes were made. Renamed Buildings.Media.GasesPTDecoupled.MoistAirUnsaturated to Buildings.Media.Air .Renamed Buildings.Media.ConstantPropertyLiquidWater to Buildings.Media.Water .Renamed Buildings.Media.PerfectGases.MoistAir to Buildings.Obsolete.Media.PerfectGases.MoistAir .Renamed Buildings.Media.GasesConstantDensity.MoistAirUnsaturated to Buildings.Obsolete.Media.GasesConstantDensity.MoistAirUnsaturated .Renamed Buildings.Media.GasesConstantDensity.MoistAir to Buildings.Obsolete.Media.GasesConstantDensity.MoistAir .Renamed Buildings.Media.GasesConstantDensity.SimpleAir to Buildings.Obsolete.Media.GasesConstantDensity.SimpleAir .Renamed Buildings.Media.IdealGases.SimpleAir to Buildings.Obsolete.Media.IdealGases.SimpleAir .Renamed Buildings.Media.GasesPTDecoupled.MoistAir to Buildings.Obsolete.Media.GasesPTDecoupled.MoistAir .Renamed Buildings.Media.GasesPTDecoupled.SimpleAir to Buildings.Obsolete.Media.GasesPTDecoupled.SimpleAir .For Dymola, the conversion script will update existing models according to the above list. |
Buildings.Media.Water | Removed option to model water as a compressible medium as this option was not useful. |
Buildings.ThermalZones | |
Buildings.ThermalZones.Detailed.BaseClasses.ParameterConstructionWithWindow | Removed the keyword replaceable for the parameters
ove and sidFin .Models that instantiate Buildings.ThermalZones.Detailed.MixedAir are
not affected by this change.
|
Buildings.ThermalZones.Detailed.Examples.BESTEST | Moved the package to Buildings.ThermalZones.Detailed.Validation.BESTEST .
|
Buildings.Utilities | |
Buildings.Utilities.SimulationTime | Moved the block Buildings.Utilities.SimulationTime
to Buildings.Utilities.Time.ModelTime .For Dymola, the conversion script will update existing models according to the above list. |
The following critical errors have been fixed (i.e., errors that can lead to wrong simulation results):
Buildings.BoundaryConditions | |
Buildings.BoundaryConditions.WeatherData.ReaderTMY3 | Corrected error that led the total and opaque sky cover to be ten times too low if its value was obtained from the parameter or the input connector. For the standard configuration in which the sky cover is obtained from the weather data file, the model was correct. This error only affected the other two possible configurations. |
Buildings.Fluid | |
Buildings.Fluid.Data.Pipes | Corrected wrong entries for inner and outer diameter of PEX pipes. |
Buildings.Fluid.HeatExchangers.Ground.Boreholes.BaseClasses.singleUTubeResistances | Corrected error in function that used beta
before it was assigned a value.
|
Buildings.Fluid.Storage.Stratified Buildings.Fluid.Storage.StratifiedEnhanced Buildings.Fluid.Storage.StratifiedEnhancedInternalHex |
Replaced the use of Medium.lambda_const with
Medium.thermalConductivity(sta_default) as
lambda_const is not declared for all media.
This avoids a translation error if certain media are used.
|
Buildings.Fluid.Storage.StratifiedEnhancedInternalHex | Corrected issue #271 which led to a compilation error if the heat exchanger and the tank had different media. |
Buildings.HeatTransfer | |
Buildings.HeatTransfer.Windows.BaseClasses.GlassLayer | Corrected issue #304 that led to an error in the glass temperatures if the glass conductance is very small. |
Buildings.ThermalZones | |
Buildings.ThermalZones.Detailed.MixedAir | Added propagation of the parameter value linearizeRadiation
to the window model. Prior to this change, the radiation
was never linearized for computing the glass long-wave radiation.
|
Buildings.ThermalZones.Detailed.FLEXLAB.Rooms.Examples.TestBedX3WithRadiantFloor Buildings.ThermalZones.Detailed.FLEXLAB.Rooms.Examples.X3AWithRadiantFloor Buildings.ThermalZones.Detailed.FLEXLAB.Rooms.Examples.X3BWithRadiantFloor |
Corrected wrong entries for inner and outer diameter of PEX pipes. |
The following uncritical errors have been fixed (i.e., errors that do not lead to wrong simulation results, e.g., units are wrong or errors in documentation):
Buildings.Fluid | |
Buildings.Fluid.FixedResistances.FixedResistanceDpM | Corrected error in documentation of computation of k .
|
Buildings.HeatTransfer | |
Buildings.HeatTransfer.Windows.BaseClasses.GlassLayer | Changed type of tauIR from
Modelica.SIunits.Emissivity to
Modelica.SIunits.TransmissionCoefficient .
This avoids a type error in OpenModelica.
|
Note:
With version 2.0, we start using semantic versioning as described at http://semver.org/.
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_1_6_build1
Version 1.6 build 1
Information
Version 1.6 build 1 updates the Buildings
library to the
Modelica Standard Library 3.2.1 and to Modelica_StateGraph2
2.0.2.
This is the first version of the Buildings
library
that contains models from the
IEA EBC Annex 60 library,
a Modelica library for building and community energy systems that is
collaboratively developed within the project
"New generation computational tools for building and community energy systems
based on the Modelica and Functional Mockup Interface standards",
a project that is conducted under the
Energy in Buildings and Communities Programme (EBC) of the
International Energy Agency (IEA).
The following new components have been added to existing libraries:
Buildings.Fluid | |
Buildings.Fluid.Actuators.Valves.TwoWayTable | Two way valve for which the opening characteristics is specified by a table. |
Buildings.Utilities.Math | |
Buildings.Utilities.Math.Examples.Average Buildings.Utilities.Math.Examples.InverseXRegularized Buildings.Utilities.Math.Examples.Polynominal Buildings.Utilities.Math.Examples.PowerLinearized Buildings.Utilities.Math.Examples.QuadraticLinear Buildings.Utilities.Math.Examples.RegNonZeroPower Buildings.Utilities.Math.Examples.SmoothExponential Buildings.Utilities.Math.Functions.average Buildings.Utilities.Math.Functions.booleanReplicator Buildings.Utilities.Math.Functions.Examples.IsMonotonic Buildings.Utilities.Math.Functions.Examples.TrapezoidalIntegration Buildings.Utilities.Math.Functions.integerReplicator Buildings.Utilities.Math.InverseXRegularized Buildings.Utilities.Math.Polynominal Buildings.Utilities.Math.PowerLinearized Buildings.Utilities.Math.QuadraticLinear Buildings.Utilities.Math.RegNonZeroPower Buildings.Utilities.Math.SmoothExponential Buildings.Utilities.Math.TrapezoidalIntegration | Various functions and blocks for mathematical operations. |
Buildings.Utilities.Psychrometrics | |
Buildings.Utilities.Psychrometrics.Examples.SaturationPressureLiquid Buildings.Utilities.Psychrometrics.Examples.SaturationPressure Buildings.Utilities.Psychrometrics.Examples.SublimationPressureIce Buildings.Utilities.Psychrometrics.Functions.BaseClasses.der_saturationPressureLiquid Buildings.Utilities.Psychrometrics.Functions.BaseClasses.der_sublimationPressureIce Buildings.Utilities.Psychrometrics.Functions.BaseClasses.Examples.SaturationPressureDerivativeCheck Buildings.Utilities.Psychrometrics.Functions.Examples.SaturationPressure Buildings.Utilities.Psychrometrics.Functions.saturationPressureLiquid Buildings.Utilities.Psychrometrics.Functions.saturationPressure Buildings.Utilities.Psychrometrics.Functions.sublimationPressureIce Buildings.Utilities.Psychrometrics.SaturationPressureLiquid Buildings.Utilities.Psychrometrics.SaturationPressure Buildings.Utilities.Psychrometrics.SublimationPressureIce | Various functions and blocks for psychrometric calculations. |
The following existing components have been improved in a backward compatible way:
Buildings.Fluid | |
Buildings.Fluid.Interfaces.PartialTwoPortInterface Buildings.Fluid.Interfaces.PartialFourPortInterface |
Removed call to homotopy function in the computation of the connector variables as these are conditionally enabled variables and therefore must not be used in any equation. They are only for output reporting. |
Buildings.Fluid.Actuators.Dampers.Exponential | Improved documentation of the flow resistance. |
Buildings.BoundaryConditions | |
Buildings.BoundaryConditions.WeatherData.ReaderTMY3 |
Added the option to use a constant, an input signal or the weather file as the source
for the ceiling height, the total sky cover, the opaque sky cover, the dew point temperature,
and the infrared horizontal radiation HInfHor .
|
The following existing components have been improved in a non-backward compatible way:
Buildings.Fluid | |
Buildings.Fluid.Movers.FlowMachinePolynomial | Moved the model to the package
Buildings.Obsolete ,
as this model is planned to be removed in future versions.
The conversion script should update old instances of
this model automatically in Dymola.
Users should change their models to use a flow machine from
the package Buildings.Fluid.Movers .
|
Buildings.Fluid.Storage.ExpansionVessel | Simplified the model to have a constant pressure.
The following non-backward compatible changes
have been made.
|
Buildings.Fluid.Storage.StratifiedEnhancedInternalHex | Revised the model as the old version required the porta
of the heat exchanger to be located higher than portb.
This makes sense if the heat exchanger is used to heat up the tank,
but not if it is used to cool down a tank, such as in a cooling plant.
The following parameters were changed:
|
The following critical errors have been fixed (i.e., errors that can lead to wrong simulation results):
Buildings.Fluid | |
Buildings.Fluid.HeatExchangers.Ground.Boreholes.UTube | Reimplemented the resistor network inside the borehole
as the old implementation led to too slow a transient
response. This change also led to the removal of the
parameters B0 and B1
as the new implementation does not require them.
|
The following uncritical errors have been fixed (i.e., errors that do not lead to wrong simulation results, e.g., units are wrong or errors in documentation):
Buildings.Fluid | |
Buildings.Fluid.HeatExchangers.Ground.Boreholes.BaseClasses.HexInternalElement | Corrected error in documentation which stated a wrong default value for the pipe spacing. |
Buildings.Fluid.HeatExchangers.BaseClasses.ntu_epsilonZ() | Added dummy argument to function call of Internal.solve
to avoid a warning during model check in Dymola 2015.
|
Buildings.Fluid.HeatExchangers.DryEffectivenessNTU | Changed assert statement to avoid comparing
enumeration with an integer, which triggers a warning
in Dymola 2015.
|
Buildings.ThermalZones.Detailed.Constructions.Examples.ExteriorWall Buildings.ThermalZones.Detailed.Constructions.Examples.ExteriorWallWithWindow Buildings.ThermalZones.Detailed.Constructions.Examples.ExteriorWallTwoWindows |
Corrected wrong assignment of parameter in instance bouConExt(conMod=...)
which was set to an interior instead of an exterior convection model.
|
Buildings.Utilities.Psychrometrics.Functions.TDewPoi_pW() | Added dummy argument to function call of Internal.solve
to avoid a warning during model check in Dymola 2015.
|
The followings issues have been fixed:
Buildings.Fluid | |
#196 | Change capacity location in borehole grout. |
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_1_5_build3
Version 1.5 build 3
Information
Version 1.5 build 3 is a maintenance release that corrects an error in Buildings.Fluid.MassExchangers.HumidifierPrescribed. It is fully compatible with version 1.5 build 2.
The following critical errors have been fixed (i.e., errors that can lead to wrong simulation results):
Buildings.Fluid | |
Buildings.Fluid.MassExchangers.HumidifierPrescribed | Corrected the enthalpy balance, which caused the latent heat flow rate to be added twice to the fluid stream. This closes issue #197. |
The following issues have been fixed:
HumidifierPrescribed accounts twice for latent heat gain | |
#197 | This issue has been addressed by correcting the latent heat added to the fluid stream. |
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_1_5_build2
Version 1.5 build 2
Information
Version 1.5 build 2 is a maintenance release that corrects an error in Buildings.Fluid.HeatExchangers.DryCoilDiscretized and in Buildings.Fluid.HeatExchangers.WetCoilDiscretized. It is fully compatible with version 1.5 build 1.
The following critical errors have been fixed (i.e., errors that can lead to wrong simulation results):
Buildings.Fluid | |
Buildings.Fluid.HeatExchangers.DryCoilDiscretized Buildings.Fluid.HeatExchangers.WetCoilDiscretized |
Corrected wrong connect statements that caused the last register to have no liquid flow. This closes issue #194. |
The following issues have been fixed:
DryCoilDiscretized model not using last register, liquid flow path | |
#194 | This issue has been addressed by correcting the connect statements. |
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_1_5_build1
Version 1.5 build 1
Information
Version 1.5 build 1 is a major release that contains new packages with models for solar collectors and for the Facility for Low Energy Experiments (FLEXLAB) at the Lawrence Berkeley National Laboratory.
This release also contains a major revision of all info sections to correct invalid html syntax.
The package Buildings.HeatTransfer.Radiosity
has been revised to comply
with the Modelica language specification.
The package Buildings.ThermalZones.Detailed
has been revised to aid implementation of
non-uniformly mixed room air models.
This release also contains various corrections that avoid warnings during translation
when used with Modelica 3.2.1.
Various models have been revised to increase compatibility with OpenModelica.
However, currently only a subset of the models work with OpenModelica.
The following new libraries have been added:
Buildings.Fluid.SolarCollectors | Library with solar collectors. |
Buildings.ThermalZones.Detailed.FLEXLAB | Package with models for test cells of LBNL's FLEXLAB (Facility for Low Energy Experiments in Buildings). |
Buildings.Utilities.IO.FLEXLAB | Package that demonstrates two-way data exchange between Modelica and LBNL's FLEXLAB (Facility for Low Energy Experiments in Buildings). |
The following new components have been added to existing libraries:
Buildings.Fluid.Storage | |
Buildings.Fluid.Storage.StratifiedEnhancedInternalHex | Added a model of a tank with built-in heat exchanger. This model may be used together with solar thermal plants. |
Buildings.Resources | |
Buildings.Resources.Include | Added an Include folder and the bcvtb.h
header file to it to fix compilation errors in BCVTB example files.
|
The following existing components have been improved in a backward compatible way:
Buildings.BoundaryConditions | |
Buildings.BoundaryConditions.WeatherData.ReaderTMY3 Buildings.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath |
Improved the algorithm that determines the absolute path of the file.
Now weather files are searched in the path specified, and if not found, the urls
file:// , modelica:// and modelica://Buildings
are added in this order to search for the weather file.
This allows using the data reader without having to specify an absolute path,
as long as the Buildings library
is on the MODELICAPATH .
|
Buildings.Fluid | |
Buildings.Fluid.Interfaces.StaticTwoPortConservationEquation | Reformulated computation of outlet properties to avoid an event at zero mass flow rate. |
Buildings.Fluid.HeatExchangers.CoolingTowers.YorkCalc | Simplified the implementation for the situation if
allowReverseFlow=false .
Avoided the use of the conditionally enabled variables sta_a and
sta_b as this was not proper use of the Modelica syntax.
|
Buildings.Fluid.Interfaces.Examples.ReverseFlowHumidifier | Changed one instance of Modelica.Fluid.Sources.MassFlowSource_T ,
that was connected to the two fluid streams,
to two instances, each having half the mass flow rate.
This is required for the model to work with Modelica 3.2.1 due to the
change introduced in
ticket #739.
|
Buildings.Fluid.Sensors.EnthalpyFlowRate Buildings.Fluid.Sensors.SensibleEnthalpyFlowRate Buildings.Fluid.Sensors.LatentEnthalpyFlowRate Buildings.Fluid.Sensors.VolumeFlowRate |
Removed default value tau=0 as the base class
already sets tau=1 .
This change was made so that all sensors use the same default value.
|
Buildings.Fluid.Sensors.TraceSubstancesTwoPort | Added default value C_start=0 .
|
Buildings.HeatTransfer | |
Buildings.HeatTransfer.Data.OpaqueConstructions.Generic | Changed the annotation of the
instance material from
Evaluate=true to Evaluate=false .
This is required to allow changing the
material properties after compilation.
Note, however, that the number of state variables in
Buildings.HeatTransfer.Data.BaseClasses.Material
are only computed when the model is translated, because
the number of state variables is fixed
at compilation time.
|
Buildings.Utilities | |
Buildings.Utilities.Diagnostics.AssertEquality Buildings.Utilities.Diagnostics.AssertInequality |
Added time in print statement as OpenModelica,
in its error message, does not output the time
when the assert is triggered.
|
The following existing components have been improved in a non-backward compatible way:
Buildings.Airflow | |
Buildings.Airflow.Multizone.Orifice Buildings.Airflow.Multizone.EffectiveAirLeakageArea Buildings.Airflow.Multizone.ZonalFlow_ACS |
Changed the parameter useConstantDensity to
useDefaultProperties to use consistent names
within this package.
A conversion script in Resources/Scripts/Dymola
can be used to update old models that use this parameter.
|
Buildings.Fluid | |
Buildings.Fluid.BaseClasses.IndexWater | Renamed class to
Buildings.Fluid.BaseClasses.IndexMassFraction
as it is applicable for all mass fraction sensors.
|
Buildings.Fluid.HeatExchangers.ConstantEffectiveness Buildings.Fluid.HeatExchangers.DryEffectivenessNTU Buildings.Fluid.Interfaces.ConservationEquation Buildings.Fluid.Interfaces.StaticFourPortHeatMassExchanger Buildings.Fluid.Interfaces.StaticTwoPortConservationEquation Buildings.Fluid.Interfaces.StaticTwoPortHeatMassExchanger Buildings.Fluid.MassExchangers.ConstantEffectiveness Buildings.Fluid.MassExchangers.HumidifierPrescribed Buildings.Fluid.MixingVolumes.BaseClasses.PartialMixingVolumeWaterPort Buildings.Fluid.MixingVolumes.MixingVolume Buildings.Fluid.MixingVolumes.MixingVolumeDryAir Buildings.Fluid.MixingVolumes.MixingVolumeMoistAir Buildings.Fluid.Storage.ExpansionVessel |
Changed the input connector mXi_flow (or mXi1_flow
and mXi2_flow ) to mWat_flow (or mWat1_flow
and mWat2_flow ).
This change has been done as declaring mXi_flow is ambiguous
because it does not specify what other species are added unless a mass flow rate
m_flow is also known. To avoid this confusion, the connector variables
have been renamed.
The equations that were used were, however, correct.
This addresses issue #165.
|
Buildings.Fluid.Storage.BaseClasses.IndirectTankHeatExchanger Buildings.Fluid.BaseClasses.PartialResistance Buildings.Fluid.FixedResistances.BaseClasses.Pipe Buildings.Fluid.FixedResistances.FixedResistanceDpM Buildings.Fluid.FixedResistances.LosslessPipe Buildings.Fluid.HeatExchangers.Ground.Boreholes.BaseClasses.BoreholeSegment Buildings.Fluid.HeatExchangers.Ground.Boreholes.UTube Buildings.Fluid.HeatExchangers.RadiantSlabs.ParallelCircuitsSlab Buildings.Fluid.Interfaces.FourPortHeatMassExchanger Buildings.Fluid.Interfaces.PartialFourPortInterface Buildings.Fluid.Interfaces.PartialTwoPortInterface Buildings.Fluid.Interfaces.StaticFourPortHeatMassExchanger Buildings.Fluid.Interfaces.StaticTwoPortHeatMassExchanger Buildings.Fluid.Interfaces.TwoPortHeatMassExchanger Buildings.Fluid.MixingVolumes.BaseClasses.PartialMixingVolume Buildings.Fluid.Movers.BaseClasses.FlowControlled Buildings.Fluid.Movers.BaseClasses.IdealSource Buildings.Fluid.Movers.BaseClasses.PrescribedFlowMachine |
Removed the computation of V_flow and removed the parameter
show_V_flow .
The reason is that the computation of V_flow required
the use of sta_a (to compute the density),
but sta_a is also a variable that is conditionally
enabled. However, this was not correct Modelica syntax as conditional variables
can only be used in a connect
statement, not in an assignment. Dymola 2014 FD01 beta3 is checking
for this incorrect syntax. Hence, V_flow was removed as its
conditional implementation would require a rather cumbersome implementation
that uses a new connector that carries the state of the medium.
|
Buildings.Fluid.MixingVolumes | Removed Buildings.Fluid.MixingVolumes.MixingVolumeDryAir
as this model is no longer used. The model
Buildings.Fluid.MixingVolumes.MixingVolume
can be used instead of.Removed base class Buildings.Fluid.MixingVolumes.BaseClasses.PartialMixingVolumeWaterPort
as this model is no longer used.
|
Buildings.Fluid.Sensors.Examples.TraceSubstances | Renamed example from ExtraProperty to
TraceSubstances in order to use the same name
as the sensor.
|
Buildings.Fluid.Sources.PrescribedExtraPropertyFlowRate | Renamed model toTraceSubstancesFlowRate to
use the same terminology than the Modelica Standard Library.The conversion script updates existing models that instantiate this model. |
Buildings.Fluid.Sources.Examples.PrescribedExtraPropertyFlow | Renamed example toTraceSubstancesFlowRate
in order to use the same name as the source model.
|
Buildings.Fluid.MixingVolumes.BaseClasses.PartialMixingVolume Buildings.Fluid.FixedResistances.Pipe Buildings.Fluid.HeatExchangers.RadiantSlabs.ParallelCircuitsSlab Buildings.Fluid.HeatExchangers.RadiantSlabs.SingleCircuitSlab Buildings.Fluid.Movers.BaseClasses.FlowControlled |
Renamed X_nominal to X_default
or X_start , where X may be
state , rho , or mu ,
depending on whether the medium default values or the start values
are used in the computation of the state
and derived quantities.
|
Buildings.HeatTransfer Buildings.ThermalZones |
|
Buildings.HeatTransfer.Interfaces.RadiosityInflow Buildings.HeatTransfer.Interfaces.RadiosityOutflow Buildings.HeatTransfer.Radiosity.BaseClasses.ParametersTwoSurfaces Buildings.HeatTransfer.Radiosity.Constant Buildings.HeatTransfer.Radiosity.Examples.OpaqueSurface Buildings.HeatTransfer.Radiosity.Examples.OutdoorRadiosity Buildings.HeatTransfer.Radiosity.IndoorRadiosity Buildings.HeatTransfer.Radiosity.OpaqueSurface Buildings.HeatTransfer.Radiosity.OutdoorRadiosity Buildings.HeatTransfer.Radiosity.RadiositySplitter Buildings.HeatTransfer.Radiosity.package Buildings.HeatTransfer.Windows.BaseClasses.Examples.CenterOfGlass Buildings.HeatTransfer.Windows.BaseClasses.Examples.GlassLayer Buildings.HeatTransfer.Windows.BaseClasses.Examples.Shade Buildings.HeatTransfer.Windows.BaseClasses.GlassLayer Buildings.HeatTransfer.Windows.BaseClasses.Shade Buildings.HeatTransfer.Windows.Examples.BoundaryHeatTransfer Buildings.HeatTransfer.Windows.ExteriorHeatTransfer Buildings.HeatTransfer.Windows.InteriorHeatTransfer Buildings.ThermalZones.Detailed.BaseClasses.InfraredRadiationExchange Buildings.ThermalZones.Detailed.BaseClasses.InfraredRadiationGainDistribution Buildings.ThermalZones.Detailed.BaseClasses.MixedAir Buildings.ThermalZones.Detailed.BaseClasses.Overhang Buildings.ThermalZones.Detailed.BaseClasses.SideFins |
Changed the connectors for the radiosity model.
The previous implemenation declared the radiosity as a
flow variables, but the implementation did not use
a potential variable.Therefore, the radiosity was the only variable in the connector, which is not allowed for flow variables.
This change required a reformulation of models because with the new formulation,
the incoming and outcoming radiosity are both non-negative values.
This addresses issue #158.
|
Buildings.HeatTransfer Buildings.ThermalZones |
|
Buildings.HeatTransfer.Windows.BaseClasses.PartialConvection Buildings.HeatTransfer.Windows.BaseClasses.PartialWindowBoundaryCondition Buildings.HeatTransfer.Windows.BaseClasses.Shade Buildings.HeatTransfer.Windows.BaseClasses.ShadeConvection Buildings.HeatTransfer.Windows.BaseClasses.ShadeRadiation Buildings.HeatTransfer.Windows.InteriorHeatTransfer Buildings.HeatTransfer.Windows.InteriorHeatTransferConvective Buildings.ThermalZones.Detailed.ExteriorBoundaryConditionsWithWindow Buildings.ThermalZones.Detailed.PartialSurfaceInterface Buildings.ThermalZones.Detailed.InfraredRadiationExchange Buildings.ThermalZones.Detailed.AirHeatMassBalanceMixed Buildings.ThermalZones.Detailed.SolarRadiationExchange Buildings.ThermalZones.Detailed.RadiationTemperature Buildings.ThermalZones.Detailed.InfraredRadiationGainDistribution |
Redesigned the implementation of the room model and its base classes. This redesign separates convection from radiation, and it provides one composite model for the convection and the heat and mass balance in the room. This change was done to allow an implementation of the room air heat and mass balance that does not assume uniformly mixed room air. |
Buildings.HeatTransfer | |
Buildings.HeatTransfer.Convection.Functions.HeatFlux.rayleigh | Renamed function from raleigh to rayleigh .
|
The following critical errors have been fixed (i.e., errors that can lead to wrong simulation results):
Buildings.Fluid | |
Buildings.Fluid.Sensors.SpecificEntropyTwoPort | Corrected wrong computation of the dynamics used for the sensor signal. |
Buildings.HeatTransfer | |
Buildings.HeatTransfer.Data.GlazingSystems.DoubleClearAir13Clear | Corrected the glass layer thickness, which was 5.7 mm instead of 3 mm, as the documentation states. |
The following uncritical errors have been fixed (i.e., errors that do not lead to wrong simulation results, e.g., units are wrong or errors in documentation):
Buildings | |
Buildings.BoundaryConditions.SkyTemperature.BlackBody Buildings.BoundaryConditions.WeatherData.BaseClasses.CheckTemperature Buildings.BoundaryConditions.WeatherData.ReaderTMY3 Buildings.Controls.SetPoints.HotWaterTemperatureReset Buildings.Examples.ChillerPlant.BaseClasses.Controls.ChillerSwitch Buildings.Examples.ChillerPlant.BaseClasses.Controls.WSEControl Buildings.Fluid.Boilers.BoilerPolynomial Buildings.Fluid.HeatExchangers.BaseClasses.HexElement Buildings.Fluid.HeatExchangers.BaseClasses.MassExchange Buildings.Fluid.HeatExchangers.BaseClasses.MassExchangeDummy Buildings.Fluid.HeatExchangers.DXCoils.BaseClasses.ApparatusDewPoint Buildings.Fluid.HeatExchangers.DXCoils.BaseClasses.ApparatusDryPoint Buildings.Fluid.HeatExchangers.DXCoils.BaseClasses.CoolingCapacity Buildings.Fluid.HeatExchangers.DXCoils.BaseClasses.DXCooling Buildings.Fluid.HeatExchangers.DXCoils.BaseClasses.DryCoil Buildings.Fluid.HeatExchangers.DXCoils.BaseClasses.DryWetSelector Buildings.Fluid.HeatExchangers.DXCoils.BaseClasses.Evaporation Buildings.Fluid.HeatExchangers.DXCoils.BaseClasses.WetCoil Buildings.Fluid.MixingVolumes.BaseClasses.PartialMixingVolumeWaterPort Buildings.Fluid.Sensors.RelativeTemperature Buildings.Fluid.Sensors.Temperature Buildings.Fluid.Sensors.TemperatureTwoPort Buildings.Fluid.Sensors.TemperatureWetBulbTwoPort Buildings.Fluid.SolarCollectors.BaseClasses.PartialHeatLoss Buildings.Utilities.Comfort.Fanger Buildings.Utilities.IO.BCVTB.From_degC Buildings.Utilities.IO.BCVTB.To_degC Buildings.Utilities.Psychrometrics.TDewPoi_pW Buildings.Utilities.Psychrometrics.TWetBul_TDryBulPhi Buildings.Utilities.Psychrometrics.TWetBul_TDryBulXi Buildings.Utilities.Psychrometrics.WetBul_pTX Buildings.Utilities.Psychrometrics.pW_TDewPoi |
Replaced wrong attribute quantity="Temperature"
with quantity="ThermodynamicTemperature" .
|
Buildings.Fluid | |
Buildings.Fluid.Data.Fuels.Generic | Corrected wrong type for mCO2 .
It was declared as Modelica.SIunits.MassFraction ,
which is incorrect.
|
Buildings.Fluid.HeatExchangers.CoolingTowers.Correlations.BaseClasses.Bounds | Corrected wrong type for FRWat_min , FRWat_max
and liqGasRat_max .
They were declared as Modelica.SIunits.MassFraction ,
which is incorrect as, for example, FRWat_max can be larger than one.
|
Buildings.Fluid.HeatExchangers.ConstantEffectiveness Buildings.Fluid.MassExchangers.ConstantEffectiveness |
Corrected error in the documentation that was not updated when the implementation of zero flow rate was revised. |
Buildings.Fluid.Interfaces.ConservationEquation | Corrected the syntax error
Medium.ExtraProperty C[Medium.nC](each nominal=C_nominal)
to
Medium.ExtraProperty C[Medium.nC](nominal=C_nominal)
because C_nominal is a vector.
This syntax error caused a compilation error in OpenModelica.
|
Buildings.Fluid.Sensors.SensibleEnthalpyFlowRate Buildings.Fluid.Sensors.LatentEnthalpyFlowRate Buildings.Fluid.Sensors.MassFraction Buildings.Fluid.Sensors.MassFractionTwoPort |
Changed medium declaration in the extends statement
to replaceable to avoid a translation error in
OpenModelica.
|
Buildings.Fluid.Sensors.TraceSubstances Buildings.Fluid.Sensors.TraceSubstancesTwoPort |
Corrected syntax errors in setting nominal value for output signal and for state variable. This eliminates a compilation error in OpenModelica. |
Buildings.Fluid.Sources.TraceSubstancesFlowSource | Added missing each in declaration of
C_in_internal .
This eliminates a compilation error in OpenModelica.
|
Buildings.Utilities.Python27 | |
Buildings.Utilities.IO.Python27.Functions.exchange | Corrected error in C code that lead to message
'module' object has no attribute 'argv'
when a python module accessed sys.argv .
|
The following issues have been fixed:
Verify mass and species balance | |
#165 | This issue has been addressed by renaming the connectors to avoid an ambiguity in the model equation. The equations were correct. |
Remove flow attribute from radiosity connectors | |
#158 | This issue has been addressed by reformulating the radiosity models. With the new implementation, incoming and outgoing radiosity are non-negative quantities. |
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_1_4_build1
Version 1.4 build 1
Information
Version 1.4 build 1 contains the new package Buildings.Utilities.IO.Python27 that allows calling Python functions from Modelica. It also contains in the package Buildings.HeatTransfer.Conduction.SingleLayer a new model for heat conduction in phase change material. This model can be used as a layer of the room heat transfer model.
Non-backward compatible changes had to be introduced
in the valve models
Buildings.Fluid.Actuators.Valves to fully comply with the Modelica language specification,
and in the models in the package
Buildings.Utilities.Diagnostics
as they used the cardinality
function which is deprecated in the Modelica
Language Specification.
See below for details.
The following new libraries have been added:
Buildings.Utilities.IO.Python27 | Package that contains blocks and functions that embed Python 2.7 in Modelica. Data can be sent to Python functions and received from Python functions. This allows for example data analysis in Python as part of a Modelica model, or data exchange as part of a hardware-in-the-loop simulation in which Python is used to communicate with hardware. |
The following new components have been added to existing libraries:
Buildings.BoundaryConditions.WeatherData | |
Buildings.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath | This function is used by the weather data reader to set the path to the weather file relative to the root directory of the Buildings library. |
The following existing components have been improved in a backward compatible way:
Buildings.Fluid | |
Buildings.Fluid.MixingVolumes.BaseClasses.PartialMixingVolume | Removed the check of multiple connections to the same element
of a fluid port, as this check required the use of the deprecated
cardinality function.
|
Buildings.HeatTransfer | |
Buildings.HeatTransfer.Conduction.SingleLayer | Added option to model layers with phase change material. |
Buildings.ThermalZones | |
Buildings.ThermalZones.Detailed.BaseClasses.InfraredRadiationExchange | Removed the use of the cardinality function
as this function is deprecated in the Modelica Language Specification.
|
The following existing components have been improved in a non-backward compatible way:
Buildings.Fluid | |
Buildings.Fluid.Actuators.Valves | All valves now require the declaration of dp_nominal
if the parameter assignment is
CvData = Buildings.Fluid.Types.CvTypes.OpPoint .
This change was needed because in the previous version,
dp_nominal had
a default value of 6000 Pascals. However, if
CvData >< Buildings.Fluid.Types.CvTypes.OpPoint , then
dp_nominal is computed in the initial algorithm section and hence
providing a default value is not allowed according to
the Modelica Language Specification.
Hence, it had to be removed.As part of this change, we set dp(nominal=6000) for all valves,
because the earlier formulation uses a value that is not known during compilation,
and hence leads to an error in Dymola 2014.
|
Buildings.Fluid.MixingVolumes.MixingVolumeDryAir Buildings.Fluid.MixingVolumes.MixingVolumeMoistAir |
Removed the use of the deprecated
cardinality function.
Therefore, now all input signals must be connected..
|
Buildings.Utilities | |
Buildings.Utilities.Diagnostics.AssertEquality Buildings.Utilities.Diagnostics.AssertInequality |
Removed the option to not connect input signals, as this
required the use of the cardinality function which
is deprecated in the MSL, and not correctly implemented in OpenModelica.
Therefore, if using these models, both input signals must be connected.
|
Buildings.Utilities.Math.Functions.splineDerivatives | Removed the default value
input Boolean ensureMonotonicity=isMonotonic(y, strict=false)
as the Modelica language specification is not clear whether defaults can be computed
or must be constants.
|
The following critical errors have been fixed (i.e., errors that can lead to wrong simulation results):
Buildings.Controls | |
Buildings.Controls.SetPoints.HotWaterTemperatureReset | Corrected error that led to wrong results if the room air temperature is
different from its nominal value TRoo_nominal .
This fixes issue 74.
|
Buildings.HeatTransfer | |
Buildings.Fluid.HeatExchangers.RadiantSlabs.SingleCircuitSlab Buildings.Fluid.HeatExchangers.RadiantSlabs.ParallelCircuitSlab |
Fixed bug in the assignment of the fictitious thermal resistance by replacing
RFic[nSeg](each G=A/Rx) with
RFic[nSeg](each G=A/nSeg/Rx) .
This fixes issue 79.
|
Buildings.Utilities | |
Buildings.Utilities.Diagnostics.AssertEquality Buildings.Utilities.Diagnostics.AssertInequality |
Replaced when test with if test as
equations within a when section are only evaluated
when the condition becomes true.
This fixes issue 72.
|
The following uncritical errors have been fixed (i.e., errors that do not lead to wrong simulation results, e.g., units are wrong or errors in documentation):
Buildings.Fluid | |
Buildings.Fluid.Actuators.Valves.ThreeWayEqualPercentageLinear Buildings.Fluid.Actuators.Valves.ThreeWayLinear |
The documenation was
Fraction Kv(port_1 → port_2)/Kv(port_3 → port_2) instead of
Fraction Kv(port_3 → port_2)/Kv(port_1 → port_2).
Because the parameter set correctly its attributes
min=0 and max=1 ,
instances of these models used the correct value.
|
Buildings.Fluid.Actuators.BaseClasses.ValveParameters | Removed stray backslash in write statement. |
Buildings.Fluid.Interfaces.ConservationEquation Buildings.Fluid.Interfaces.StaticTwoPortConservationEquation Buildings.Fluid.Interfaces.StaticTwoPortHeatMassExchanger |
Removed wrong unit attribute of COut .
|
Buildings.Fluid.HeatExchangers.BaseClasses.HexElement | Changed the redeclaration of vol2 to be replaceable,
as vol2 is replaced in some models.
|
The following issues have been fixed:
Add explanation of nStaRef. | |
#70 |
Described in
Buildings.HeatTransfer.Data.Solids
how the parameter nStaRef is used
to compute the spatial grid that is used for simulating transient heat conduction.
|
Assert statement does not fire. | |
#72 |
The blocks Buildings.Utilities.Diagnostics.AssertEquality and
Buildings.Utilities.Diagnostics.AssertInequality did not fire because
the test on the time was in a when instead of an if statement.
This was wrong because when sections are only evaluated
when the condition becomes true.
|
HotWaterTemperatureReset computes wrong results if room temperature differs from nominal value.
|
|
#74 | The equation
TSup = TRoo_in_internal + ((TSup_nominal+TRet_nominal)/2-TRoo_in_internal) * qRel^(1/m) + (TSup_nominal-TRet_nominal)/2 * qRel;should be formulated as TSup = TRoo_in_internal + ((TSup_nominal+TRet_nominal)/2-TRoo_nominal) * qRel^(1/m) + (TSup_nominal-TRet_nominal)/2 * qRel; |
Bug in RadiantSlabs.SingleCircuitSlab fictitious resistance RFic.
|
|
#79 | This bug has been fixed in the assignment of the fictitious thermal resistance by replacing
RFic[nSeg](each G=A/Rx) with
RFic[nSeg](each G=A/nSeg/Rx) .
The bug also affected RadiantSlabs.ParallelCircuitSlab .
|
Note:
- This version contains various updates that allow the syntax of the example models to be checked in the pedantic mode in Dymola 2014.
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_1_3_build1
Version 1.3 build 1
Information
In version 1.3 build 1, models for direct evaporative cooling coils with multiple stages or with a variable speed compressor have been added. This version also contains improvements to the fan and pump models to better treat zero mass flow rate. Various other improvements have been made to improve the numerics and to use consistent variable names. A detailed list of changes is shown below.
The following new libraries have been added:
Buildings.Fluid.HeatExchangers.DXCoils | Library with direct evaporative cooling coils. |
The following new components have been added to existing libraries:
Buildings.Examples | |
Buildings.Examples.ChillerPlant.DataCenterContinuousTimeControl | Added chilled water plant model with continuous time control that
replaces the discrete time control in
Buildings.Examples.ChillerPlant.DataCenterDiscreteTimeControl .
|
Buildings.Utilities | |
Buildings.Utilities.Psychrometrics.Functions.X_pSatpphi | Function that computes moisture concentration based on saturation pressure, total pressure and relative humidity. |
Buildings.Utilities.Psychrometrics.TWetBul_TDryBulPhi | Block that computes the wet bulb temperature for given dry bulb temperature, relative humidity and atmospheric pressure. |
Buildings.Utilities.Psychrometrics.WetBul_pTX | Block that computes the temperature and mass fraction at the wet bulb state for given dry bulb temperature, species concentration and atmospheric pressure. |
The following existing components have been improved in a backward compatible way:
Buildings.BoundaryConditions | |
Buildings.BoundaryConditions.WeatherData.ReaderTMY3 | Added computation of the wet bulb temperature.
Computing the wet bulb temperature introduces a nonlinear
equation. As we have not observed an increase in computing time
because of computing the wet bulb temperature, it is computed
by default. By setting the parameter
computeWetBulbTemperature=false , the computation of the
wet bulb temperature can be removed.
|
Buildings.Controls | |
Buildings.Controls.SetPoints.OccupancySchedule | Added pre operator and relaxed tolerance in assert statement.
|
Buildings.Fluid | |
Buildings.Fluid.Movers.FlowControlled_dp Buildings.Fluid.Movers.FlowControlled_m_flow Buildings.Fluid.Movers.SpeedControlled_Nrpm Buildings.Fluid.Movers.SpeedControlled_y |
Reformulated implementation of efficiency model to avoid a division by zero at zero mass flow rate for models in which a user specifies a power instead of an efficiency performance curve. |
Buildings.Utilities | |
Buildings.Utilities.Psychrometrics.TWetBul_TDryBulXi | Added option to approximate the wet bulb temperature using an explicit equation. Reformulated the original model to change the dimension of the nonlinear system of equations from two to one. |
The following existing components have been improved in a non-backward compatible way:
Buildings.BoundaryConditions | |
Buildings.BoundaryConditions.WeatherData.ReaderTMY3 Buildings.BoundaryConditions.Types |
Improved the optional inputs for the radiation data global horizontal, diffuse horizontal and direct normal radiation. If a user specifies two of them, the third will be automatically calculated. |
Buildings.BoundaryConditions.SkyTemperature.BlackBody | Renamed radHor to radHorIR
to indicate that the radiation is in the infrared
spectrum.
|
Buildings.Fluid | |
Buildings.Airflow.Multizone.BaseClasses.DoorDiscretized Buildings.Airflow.Multizone.DoorDiscretizedOpen Buildings.Airflow.Multizone.DoorDiscretizedOperable Buildings.Airflow.Multizone.Orifice Buildings.Airflow.Multizone.ZonalFlow_ACS Buildings.Fluid.Actuators.BaseClasses.PartialDamperExponential Buildings.Fluid.Actuators.Dampers.MixingBox Buildings.Fluid.Actuators.Dampers.VAVBoxExponential Buildings.Fluid.BaseClasses.PartialResistance Buildings.Fluid.Interfaces.TwoPortHeatMassExchanger Buildings.Fluid.Movers.BaseClasses.PowerInterface Buildings.Fluid.Storage.BaseClasses.Buoyancy Buildings.Fluid.HeatExchangers.BaseClasses.MassExchange |
Renamed protected parameters for consistency with the naming conventions.
In previous releases, fluid properties had the suffix 0
or _nominal instead of _default when they
where computed based on the medium default properties.
|
Buildings.Fluid.Sensors.SensibleEnthalpyFlowRate Buildings.Fluid.Sensors.LatentEnthalpyFlowRate |
Moved computation of parameter i_w to new base class
Buildings.Fluid.BaseClasses.IndexWater
The value of this parameter is now assigned dynamically and does not require to be specified
by the user.
|
Buildings.Fluid.Storage.BaseClasses.ThirdOrderStratifier | Removed unused protected parameters sta0 and cp0 .
|
Buildings.Examples | |
Buildings.Examples.ChillerPlant.DataCenterDiscreteTimeControl Buildings.Examples.ChillerPlant.BaseClasses.Controls.TrimAndRespond Buildings.Examples.ChillerPlant.BaseClasses.Controls.ZeroOrderHold |
Re-implemented the controls for setpoint reset.
Revised the model TrimAndRespond and deleted the model ZeroOrderHold .
Improved the documentation.
|
The following critical errors have been fixed (i.e., errors that can lead to wrong simulation results):
Buildings.Examples | |
Buildings.Examples.ChillerPlant.DataCenterDiscreteTimeControl | Fixed error in wet bulb temperature. The previous version used a model to compute the wet bulb temperature that takes as an input the relative humidity, but required mass fraction as an input. |
The following uncritical errors have been fixed (i.e., errors that do not lead to wrong simulation results, e.g., units are wrong or errors in documentation):
Buildings.BoundaryConditions | |
Buildings.BoundaryConditions.WeatherData.ReaderTMY3 Buildings.BoundaryConditions.SkyTemperature.BlackBody |
Renamed radHor to radHorIR .
|
Buildings.Fluid | |
Buildings.Fluid.BaseClasses.FlowModels.Examples.InverseFlowFunction | Fixed error in the documentation. |
Buildings.Fluid.Interfaces.TwoPortHeatMassExchanger | Fixed broken link in the documentation. |
Buildings.Fluid.Movers.BaseClasses.Characteristics.powerParameters | Fixed wrong displayUnit and
max attribute for power.
|
Buildings.Fluid.MixingVolumes | In documentation, removed reference to the parameter
use_HeatTransfer which no longer exists.
|
Buildings.HeatTransfer | |
Buildings.HeatTransfer.Windows.Functions.glassPropertyUncoated | Improved the documentation for implementation and added comments for model limitations. |
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_1_2_build1
Version 1.2 build 1
Information
In version 1.2 build 1, models for radiant slabs and window overhangs and sidefins have been added. This version also contains various improvements to existing models. A detailed list of changes is shown below.
The following new libraries have been added:
Buildings.Fluid.HeatExchangers.RadiantSlabs | Package with models for radiant slabs with pipes or a capillary heat exchanger embedded in the construction. |
Buildings.Fluid.Data.Pipes | Package with records for pipes. |
The following new components have been added to existing libraries:
Buildings.HeatTransfer | |
Buildings.HeatTransfer.Windows.FixedShade Buildings.HeatTransfer.Windows.Overhang Buildings.HeatTransfer.Windows.SideFins |
For windows with either an overhang or side fins, these blocks output the fraction of the area that is sun exposed. |
Buildings.ThermalZones | |
Buildings.ThermalZones.Detailed.Examples.BESTEST | Added BESTEST validation models for case 610, 620, 630, 640, 650FF, 650, 920, 940, 950FF, 950, and 960. |
The following existing components have been improved in a backward compatible way:
Buildings.BoundaryConditions | |
Buildings.BoundaryConditions.WeatherData.ReaderTMY3 | Removed assignment of HGloHor_in in its declaration,
because this gives an overdetermined system if the input connector
is used.Added new sub-bus that contains the solar position. This allows reusing the solar position in various other models. |
Buildings.BoundaryConditions.SolarIrradiation.DiffuseIsotropic Buildings.BoundaryConditions.SolarIrradiation.DiffusePerez Buildings.BoundaryConditions.SolarIrradiation.BaseClasses.DiffuseIsotropic Buildings.BoundaryConditions.SolarIrradiation.BaseClasses.DiffusePerez |
Added optional output of diffuse radiation from the sky and ground. This allows reusing the diffuse radiation in solar thermal collector. |
Buildings.BoundaryConditions.SolarGeometry.BaseClasses.SolarAzimuth | Changed implementation to avoid an event at solar noon. |
Buildings.HeatTransfer | |
Buildings.HeatTransfer.Data.BoreholeFillings |
Renamed class to BoreholeFillings
to be consistent with data records being plural.
|
Buildings.Media | |
Buildings.Media.GasesPTDecoupled.MoistAir Buildings.Media.Air Buildings.Media.PerfectGases.MoistAir Buildings.Media.PerfectGases.MoistAirUnsaturated Buildings.Media.GasesConstantDensity.MoistAir Buildings.Media.GasesConstantDensity.MoistAirUnsaturated |
Added redeclaration of ThermodynamicState
to avoid a warning
during model check and translation.
|
Buildings.ThermalZones | |
Buildings.ThermalZones.Detailed.MixedAir | Added a check that ensures that the number of surfaces
are equal to the length of the parameter that contains
the surface area, and added a check to ensure that no surface area
is equal to zero. These checks help detecting erroneous declarations
of the room model. The changes were done in
Buildings.ThermalZones.Detailed.MixedAir.PartialSurfaceInterface .
|
The following existing components have been improved in a non-backward compatible way:
Buildings.ThermalZones | |
Buildings.ThermalZones.Detailed.MixedAir | Added optional modeling of window overhangs and side fins.
The modeling of window overhangs and side fins required the
introduction of the new parameters
hWin for the window height and
wWin for the window width, in addition to the
parameters ove and sidFin which are used
to declare the geometry of overhangs and side fins.
The parameters hWin and wWin
replace the previously used parameter AWin for the
window area.
Users need to manually replace AWin with hWin
and wWin when updating models
from a previous version of the library.See the information section in Buildings.ThermalZones.Detailed.MixedAir for how to use these models. |
The following critical errors have been fixed (i.e., errors that can lead to wrong simulation results):
Buildings.Controls | |
Buildings.Controls.SetPoints.OccupancySchedule | Fixed a bug that caused an error in the schedule if the simulation start time was negative or equal to the first entry in the schedule. |
Buildings.Fluid | |
Buildings.Fluid.Storage.BaseClass.ThirdOrderStratifier | Revised the implementation to reduce the temperature overshoot. |
Buildings.HeatTransfer | |
Buildings.HeatTransfer.Windows.BaseClasses.GlassLayer | Fixed the bug in the temperature linearization and in the heat flow through the glass layer if the transmissivity of glass in the infrared regime is non-zero. |
Buildings.HeatTransfer.Windows.BaseClasses.CenterOfGlass | Fixed a bug in the parameter assignment of the instance glass .
Previously, the infrared emissivity of surface a was assigned to the surface b.
|
Buildings.Utilities | |
Buildings.Utilities.IO.BCVTB | Added a call to Buildings.Utilities.IO.BCVTB.BaseClasses.exchangeReals
in the initial algorithm section.
This is needed to propagate the initial condition to the server.
It also leads to one more data exchange, which is correct and avoids the
warning message in Ptolemy that says that the simulation reached its stop time
one time step prior to the final time.
|
The following uncritical errors have been fixed (i.e., errors that do not lead to wrong simulation results, e.g., units are wrong or errors in documentation):
Buildings.BoundaryConditions | |
Buildings.BoundaryConditions.WeatherData.ReaderTMY3 | Corrected the documentation of the unit requirement for input files, parameters and connectors. |
Buildings.Fluid | |
Buildings.Fluid.Interfaces.PartialFourPortInterface Buildings.Fluid.Interfaces.PartialTwoPortInterface |
Replaced the erroneous function call Medium.density with
Medium1.density and Medium2.density in
PartialFourPortInterface .
Changed condition to remove sta_a1 and
sta_a2 in PartialFourPortInterface , and
sta_a in PartialTwoPortInterface , to also
compute the state at the inlet port if show_V_flow=true .The previous implementation resulted in a translation error if show_V_flow=true , but worked correctly otherwise
because the erroneous function call is removed if show_V_flow=false .
|
Buildings.Fluid.Chillers.Examples.BaseClasses.PartialElectric | Corrected the nominal mass flow rate used in the mass flow source. |
The following issues have been fixed:
Heat transfer in glass layer | |
#56 | Fixed bug in heat flow through the glass layer if the infrared transmissivity is non-zero. |
#57 | Fixed bug in temperature linearization of window glass. |
Overshooting in enhanced stratified tank | |
#15 | Revised the implementation to reduce the temperature over-shoot. |
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_1_1_build1
Version 1.1 build 1
Information
Version 1.1 build 1 contains improvements to models that address numerical problems. In particular, flow machines and actuators now have an optional filter that converts step changes in the input signal to a smooth change in speed or actuator position. Also, ( Buildings.Examples.Tutorial) has been added to provide step-by-step instruction for how to build system models.
The following new libraries have been added:
Buildings.Examples.Tutorial | Tutorial with step by step instructions for how to build system models. |
The following new components have been added to existing libraries:
Buildings.Fluid | |
Buildings.Fluid.FixedResistances.Pipe | Added a model for a pipe with transport delay and optional heat exchange with the environment. |
Buildings.Fluid.Actuators.UsersGuide | Added a user's guide for actuator models. |
Buildings.Fluid.Interfaces.ConservationEquation Buildings.Fluid.Interfaces.StaticConservationEquation |
These base classes have been added to simplify the implementation of dynamic and steady-state thermofluid models. |
Buildings.Fluid.Data.Fuels | Package with physical properties of fuels that are used by the boiler model. |
The following existing components have been improved in a backward compatible way:
Buildings.Fluid | |
Buildings.Fluid.Actuators.Dampers.Exponential Buildings.Fluid.Actuators.Dampers.VAVBoxExponential Buildings.Fluid.Actuators.Dampers.MixingBox Buildings.Fluid.Actuators.Dampers.MixingBoxMinimumFlow Buildings.Fluid.Actuators.Valves.ThreeWayEqualPercentageLinear Buildings.Fluid.Actuators.Valves.ThreeWayLinear Buildings.Fluid.Actuators.Valves.TwoWayEqualPercentage Buildings.Fluid.Actuators.Valves.TwoWayLinear Buildings.Fluid.Actuators.Valves.TwoWayQuickOpening |
Added an optional 2nd order lowpass filter for the input signal.
The filter approximates the travel time of the actuators.
It also makes the system of equations easier to solve
because a step change in the input signal causes a gradual change in the actuator
position. Note that this filter affects the time response of closed loop control. Therefore, enabling the filter may require retuning of control loops. See the user's guide of the Buildings.Fluid.Actuators package. |
Buildings.Fluid.Boilers.BoilerPolynomial | Added computation of fuel usage and improved the documentation. |
Buildings.Fluid.Movers.SpeedControlled_y Buildings.Fluid.Movers.SpeedControlled_Nrpm Buildings.Fluid.Movers.FlowControlled_dp Buildings.Fluid.Movers.FlowControlled_m_flow |
Added a 2nd order lowpass filter to the input signal.
The filter approximates the startup and shutdown transients of fans or pumps.
It also makes the system of equations easier to solve
because a step change in the input signal causes a gradual change in the
mass flow rate. Note that this filter affects the time response of closed loop control. Therefore, enabling the filter may require retuning of control loops. See the user's guide of the Buildings.Fluid.Movers package. |
Buildings.Fluid.Interfaces.StaticTwoPortHeatMassExchanger | Changed model to use graphical implementation of models for pressure drop and conservation equations. |
Buildings.Fluid.BaseClasses.PartialResistance Buildings.Fluid.FixedResistances.FixedResistanceDpM Buildings.Fluid.Actuators.BaseClasses.PartialTwoWayValve Buildings.Fluid.Actuators.BaseClasses.PartialDamperExponential |
Revised base classes and models to simplify object inheritance tree.
Set m_flow_small to final in Buildings.Fluid.BaseClasses.PartialResistance,
and removed its assignment in the other classes.
|
Buildings.Fluid.FixedResistances.FixedResistanceDpM Buildings.Fluid.FixedResistances.SplitterFixedResistanceDpM |
Improved documentation. |
Buildings.HeatTransfer | |
Buildings.HeatTransfer.Windows.Functions.glassProperty | Added the function glassPropertyUncoated that calculates the property for uncoated glass.
|
Buildings.ThermalZones | |
Buildings.ThermalZones.Detailed.MixedAir | Changed model to use new implementation of Buildings.HeatTransfer.Radiosity.OutdoorRadiosity in its base classes. This change leads to the use of the same equations for the radiative heat transfer between window and ambient as is used for the opaque constructions. |
The following existing components have been improved in a non-backward compatible way:
Buildings.Fluid | |
Buildings.Fluid.Actuators.Valves.ThreeWayEqualPercentageLinear Buildings.Fluid.Actuators.Valves.ThreeWayLinear Buildings.Fluid.Actuators.Valves.TwoWayEqualPercentage Buildings.Fluid.Actuators.Valves.TwoWayLinear Buildings.Fluid.Actuators.Valves.TwoWayQuickOpening |
Changed models to allow modeling of a fixed resistance that is
within the controlled flow leg. This allows in some cases
to avoid a nonlinear equation if a flow resistance is
in series to the valve.
This change required changing the parameter for the valve resistance
dp_nominal to dpValve_nominal ,
and introducing the parameter
dpFixed_nominal , with dpFixed_nominal=0
as its default value.
Previous models that instantiate these components need to change the
assignment of dp_nominal to an assignment of
dpValve_nominal .
See also
Buildings.Fluid.Actuators.UsersGuide.
|
Buildings.HeatTransfer | |
Buildings.HeatTransfer.Radiosity.OutdoorRadiosity Buildings.HeatTransfer.Windows.ExteriorHeatTransfer |
Changed model to use new implementation of Buildings.HeatTransfer.Radiosity.OutdoorRadiosity. This change leads to the use of the same equations for the radiative heat transfer between window and ambient as is used for the opaque constructions. |
Buildings.Controls | |
Buildings.Controls.SetPoints.OccupancySchedule | Changed model to fix a bug that caused the output of the block
to be incorrect when the simulation started
at a time different from zero.
When fixing this bug, the parameter startTime was removed,
and the parameter endTime was renamed to period .
The period always starts at t=0 seconds.
|
The following critical errors have been fixed (i.e., errors that can lead to wrong simulation results):
Buildings.Controls | |
Buildings.Controls.SetPoints.OccupancySchedule | The output of the block was incorrect when the simulation started at a time different from zero. |
Buildings.Fluid.HeatExchangers | |
Buildings.Fluid.HeatExchangers.DryCoilCounterFlow Buildings.Fluid.HeatExchangers.WetCoilCounterFlow |
Corrected error in assignment of dp2_nominal .
The previous assignment caused a pressure drop in all except one element,
instead of the opposite. This caused too high a flow resistance
of the heat exchanger.
|
The following uncritical errors have been fixed (i.e., errors that do not lead to wrong simulation results, e.g., units are wrong or errors in documentation):
Buildings.BoundaryConditions | |
Buildings.BoundaryConditions.SkyTemperature.BlackBody | Fixed error in BlackBody model that was causing a translation error when calTSky was set to Buildings.BoundaryConditions.Types.SkyTemperatureCalculation.HorizontalRadiation .
|
Buildings.Fluid | |
Buildings.Fluid.Interfaces.TwoPortHeatMassExchanger | Fixed wrong class reference in information section. |
Buildings.Utilities | |
Buildings.Utilities.IO.BCVTB.Examples.MoistAir | Updated fan parameters, which were still for version 0.12 of the Buildings library and hence caused a translation error with version 1.0 or higher. |
The following issues have been fixed:
Exterior longwave radiation exchange in window model | |
#51 | Changed model to use new implementation of Buildings.HeatTransfer.Radiosity.OutdoorRadiosity. This change leads to the use of the same equations for the radiative heat transfer between window and ambient as is used for the opaque constructions. |
#53 | Fixed bug in Buildings.Controls.SetPoints.OccupancySchedule that led to wrong results when the simulation started at a time different from zero. |
Note:
- The use of filters for actuator and flow machine input signals changes the dynamic response of feedback control loops. Therefore, control gains may need to be retuned. See Buildings.Fluid.Actuators.UsersGuide and Buildings.Fluid.Movers.UsersGuide for recommended control gains and further details.
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_1_0_build2
Version 1.0 build 2
Information
Version 1.0 build 2 has been released to correct model errors that were present in version 1.0 build 1. Both versions are compatible. In addition, version 1.0 build 2 contains improved documentation of various example models.
The following existing components have been improved in a backward compatible way:
Buildings.Controls | |
Buildings.Controls.Continuous Buildings.Controls.Discrete Buildings.Controls.SetPoints |
Improved documentation of models and of examples. |
Buildings.Airflow.Multizone | |
Buildings.Airflow.Multizone.DoorDiscretizedOpen Buildings.Airflow.Multizone.DoorDiscretizedOperable |
Changed the computation of the discharge coefficient to use the
nominal density instead of the actual density.
Computing sqrt(2/rho) sometimes causes warnings from the solver,
as it seems to try negative values for the density during iterative solutions.
|
Buildings.Airflow.Multizone.Examples | Improved documentation of examples. |
Buildings.Examples.DualFanDualDuct | |
Buildings.Examples.DualFanDualDuct.Controls.RoomMixingBox | Improved control of minimum air flow rate to avoid overheating. |
The following critical errors have been fixed (i.e., errors that can lead to wrong simulation results):
Buildings.HeatTransfer | |
Buildings.HeatTransfer.Convection.Exterior | Fixed error in assignment of wind-based convection coefficient. The old implementation did not take into account the surface roughness. |
Buildings.ThermalZones | |
Buildings.ThermalZones.Detailed.BaseClasses.SolarRadiationExchange | In the previous version, the radiative properties of the long-wave spectrum instead of the solar spectrum have been used to compute the distribution of the solar radiation among the surfaces inside the room. |
Buildings.ThermalZones.Detailed.BaseClasses.MixedAir | Added missing connect statement between window frame surface and window frame convection model. Prior to this bug fix, no convective heat transfer was computed between window frame and room air. |
Buildings.ThermalZones.Detailed.BaseClasses.HeatGain | Fixed bug that caused convective heat gains to be removed from the room instead of added to the room. |
The following issues have been fixed:
Buildings.Fluid.HeatExchangers.Ground.Boreholes | |
#45 | Dymola 2012 FD01 hangs when simulating a borehole heat exchanger.
This was caused by a wrong release of memory in freeArray.c .
|
Buildings.ThermalZones | |
#46 | The convective internal heat gain has the wrong sign. |
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_1_0_build1
Version 1.0 build 1
Information
Version 1.0 is the first official release of the Buildings
library.
Compared to the last pre-release, which is version 0.12, this version contains
new models as well as significant improvements to the model formulation
that leads to faster and more robust simulation. A detailed list of changes is shown below.
Version 1.0 is not backward compatible to version 0.12, i.e., models developed with versions 0.12 will require some changes in their parameters to work with version 1.0. The conversion script Buildings/Resources/Scripts/Dymola/ConvertBuildings_from_0.12_to_1.0.mos can help in converting old models to this version of the library.
The following new libraries have been added:
Buildings.Fluid.HeatExchangers.Ground.Boreholes | This is a library with a model for a borehole heat exchanger. |
The following new components have been added to existing libraries:
Buildings.Airflow.Multizone | |
Buildings.Airflow.Multizone.BaseClasses.windPressureLowRise | Added a function that computes wind pressure on the facade of low-rise buildings. |
Buildings.Examples | |
Buildings.Examples.ChillerPlant | Added an example for a chilled water plant model. |
Buildings.Fluid.Interfaces | |
Buildings.Fluid.Interfaces.UsersGuide | Added a user's guide that describes the main functionality of all base classes. |
Buildings.Fluid.Sources | |
Buildings.Fluid.Sources.Outside_Cp Buildings.Fluid.Sources.Outside_CpLowRise |
Added models to compute wind pressure on building facades. |
Buildings.HeatTransfer | |
Buildings.HeatTransfer.Conductor | Added a model for heat conduction in circular coordinates. |
Buildings.ThermalZones.Detailed.Examples | |
Buildings.ThermalZones.Detailed.Examples.BESTEST | Added BESTEST validation models. |
Buildings.Utilities.Math | |
Buildings.Utilities.Math.Functions.cubicHermiteLinearExtrapolation Buildings.Utilities.Math.Functions.splineDerivatives. |
Added functions for cubic hermite spline interpolation, with option for monotone increasing (or decreasing) spline. |
The following existing components have been improved in a backward compatible way:
Buildings.Airflow.Multizone | |
Buildings.Airflow.Multizone.BaseClasses.powerLaw | This function has been reimplemented to handle zero flow rate in a more robust and more efficient way. This change improves all components that model flow resistance in the package Buildings.Airflow.Multizone. |
Buildings.BoundaryConditions.WeatherData | |
Buildings.BoundaryConditions.WeatherData.ReaderTMY3 | This model has now the option of using a constant value, using the data from the weather file, or from an input connector for 7 variables, including atmospheric pressure, relative humidity, dry bulb temperature, global horizontal radiation, diffuse horizontal radiation, wind direction and wind speed. |
Buildings.Fluid | |
Buildings.Fluid.Actuators.BaseClasses.PartialActuator Buildings.Fluid.Actuators.BaseClasses.PartialDamperExponential Buildings.Fluid.Actuators.BaseClasses.PartialTwoWayValve Buildings.Fluid.BaseClasses.PartialResistance Buildings.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp Buildings.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow Buildings.Fluid.Interfaces.StaticTwoPortHeatMassExchanger |
The computation of the linearized flow resistance has been moved from
the functions to the model, i.e., into an equation section.
If the linear implementation is in a function body, then a symbolic processor
may not invert the equation. This can lead to systems of coupled equations in
cases where an explicit solution is possible.
In addition, the handling of zero flow rate has been improved for the nonlinear
pressure drop model.
These improvements affect all models in Buildings.Fluid that compute
flow resistance. |
Buildings.Fluid.HeatExchangers | |
Buildings.Fluid.HeatExchangers.HeaterCoolerPrescribed | This model can now be configured as a steady-state or dynamic model. |
Buildings.Fluid.HeatExchangers.DryCoilCounterFlow Buildings.Fluid.HeatExchangers.WetCoilCounterFlow Buildings.Fluid.HeatExchangers.DryCoilDiscretized Buildings.Fluid.HeatExchangers.WetCoilDiscretized |
The implementation for handling zero flow rate, if the models are used as steady-state models, have been improved. |
Buildings.Fluid.HeatExchangers.BaseClasses.ntu_epsilonZ | Changed implementation to use
Modelica.Media.Common.OneNonLinearEquation instead of
Buildings.Utilities.Math.BaseClasses.OneNonLinearEquation ,
which was removed for this version of the library.
|
Buildings.Fluid.HeatExchangers.CoolingTowers | |
Buildings.Fluid.HeatExchangers.CoolingTowers.YorkCalc Buildings.Fluid.HeatExchangers.CoolingTowers.FixedApproach |
These models are now based on a new base class Buildings.Fluid.HeatExchangers.CoolingTowers.BaseClasses.CoolingTower .
This allows using the models as replaceable models without warning when checking the model.
|
Buildings.Fluid.HeatExchangers.CoolingTowers.YorkCalc | Changed implementation of performance curve to avoid division by zero. |
Buildings.Fluid.MassExchangers | |
Buildings.Fluid.MassExchangers.HumidifierPrescribed | This model can now be configured as a steady-state or dynamic model. |
Buildings.Fluid.Sensors | |
Buildings.Fluid.Sensors.*TwoPort | All sensors with two ports, except for the mass flow rate sensor, have been revised to add sensor dynamics. Adding sensor dynamics avoids numerical problems when mass flow rates are close to zero and the sensor is configured to allow flow reversal. See Buildings.Fluid.Sensors.UsersGuide for details. |
Buildings.Fluid.Storage | |
Buildings.Fluid.Storage.Stratified Buildings.Fluid.Storage.StratifiedEnhanced |
Changed the implementation of the model Buoyancy
to make it differentiable in the temperatures. |
Buildings.Media | |
Buildings.Media.Interfaces.PartialSimpleMedium Buildings.Media.Interfaces.PartialSimpleIdealGasMedium |
Moved the assignment of the stateSelect attribute for
the BaseProperties to the model
Buildings.Fluid.MixingVolumes.MixingVolume . This allows
to handle it differently for steady-state and dynamic models. |
Buildings.Utilities.Psychrometrics | |
Buildings.Utilities.Psychrometrics.Functions.TDewPoi_pW | Changed implementation to use
Modelica.Media.Common.OneNonLinearEquation instead of
Buildings.Utilities.Math.BaseClasses.OneNonLinearEquation ,
which was removed for this version of the library.
|
The following existing components have been improved in a non-backward compatible way:
Buildings.Airflow.Multizone | |
Buildings.Airflow.Multizone.MediumColumnDynamic | The implementation has been changed to better handle mass flow rates
near zero flow.
This required the introduction of a new parameter m_flow_nominal
that is used for the regularization near zero mass flow rate. |
Buildings.Fluid | |
Buildings.Fluid.Storage.Examples.Stratified Buildings.Fluid.MixingVolumes |
Removed the parameters use_T_start and h_start ,
as T_start is more convenient to use than h_start
for building simulation.
|
Buildings.Fluid.Boilers | |
Buildings.Fluid.Boilers.BoilerPolynomial | The parameter dT_nominal has been removed
as it can be computed from the parameter m_flow_nominal .
This change was needed to avoid a non-literal value for the nominal
attribute for the mass flow rate in the pressure drop model. |
Buildings.Fluid.MixingVolumes | |
Buildings.Fluid.MixingVolumes.MixingVolume Buildings.Fluid.MixingVolumes.MixingVolumeDryAir Buildings.Fluid.MixingVolumes.MixingVolumeMoistAir |
The implementation has been changed to better handle mass flow rates
near zero flow if the components have exactly two fluid ports connected.
This required the introduction of a new parameter m_flow_nominal
that is used for the regularization near zero mass flow rate. |
Buildings.Fluid.Movers | |
Buildings.Fluid.Movers.SpeedControlled_y Buildings.Fluid.Movers.SpeedControlled_Nrpm Buildings.Fluid.Movers.FlowControlled_dp Buildings.Fluid.Movers.FlowControlled_m_flow |
The performance data are now defined through records and not
through replaceable functions. The performance data now needs to be
declared in the formpressure(V_flow_nominal={0,V_flow_nominal,2*V_flow_nominal}, dp_nominal={2*dp_nominal,dp_nominal,0})where pressure is an instance of a record. A similar declaration is
used for power and efficiency.
The parameter m_flow_nominal has been removed from FlowMachine_y and FlowMachine_Nrpm. The parameter m_flow_max has been replaced by m_flow_nominal in FlowMachine_m_flow. The implementation of the pressure drop computation as a function of speed and volume flow rate has been revised to avoid a singularity near zero volume flow rate and zero speed. The implementation has also been simplified to avoid using two different flow paths if the models are configured for steady-state or dynamic simulation. |
Buildings.Fluid.Interfaces | |
Buildings.Fluid.Interfaces.FourPortHeatMassExchanger Buildings.Fluid.Interfaces.PartialDynamicStaticFourPortHeatMassExchanger Buildings.Fluid.Interfaces.TwoPortHeatMassExchanger Buildings.Fluid.Interfaces.PartialDynamicStaticTwoPortHeatMassExchanger Buildings.Fluid.Interfaces.ConservationEquation |
The implementation has been changed to better handle mass flow rates near zero flow if the components have exactly two fluid ports connected. |
Buildings.Fluid.Sensors | |
Buildings.Fluid.Sensors.TemperatureTwoPortDynamic | This model has been deleted since the sensor Buildings.Fluid.Sensors.TemperatureTwoPort has been revised and can now also be used as a dynamic model of a sensor. |
Buildings.Fluid.Interfaces | |
Buildings.Fluid.Interfaces.PartialStaticTwoPortInterface | Renamed to Buildings.Fluid.Interfaces.PartialTwoPortInterface |
Buildings.Fluid.Interfaces.PartialStaticStaticTwoPortHeatMassExchanger | Renamed to Buildings.Fluid.Interfaces.StaticTwoPortHeatMassExchanger |
Buildings.Fluid.Interfaces.PartialTwoPortHeatMassExchanger | Renamed to Buildings.Fluid.Interfaces.TwoPortHeatMassExchanger |
Buildings.Fluid.Interfaces.PartialFourPort | Renamed to Buildings.Fluid.Interfaces.FourPort |
Buildings.Fluid.Interfaces.PartialStaticStaticFourPortHeatMassExchanger | Renamed to Buildings.Fluid.Interfaces.StaticFourPortHeatMassExchanger |
Buildings.Fluid.Interfaces.PartialStaticFourPortInterface | Renamed to Buildings.Fluid.Interfaces.PartialFourPortInterface |
Buildings.Fluid.Interfaces.PartialFourPortHeatMassExchanger | Renamed to Buildings.Fluid.Interfaces.FourPortHeatMassExchanger |
Buildings.Utilities.Math | |
Buildings.Utilities.Math.BaseClasses.OneNonLinearEquation | This package has been removed, and all functions have been revised to use Modelica.Media.Common.OneNonLinearEquation. |
Buildings.Utilities.Reports | |
Buildings.Utilities.Reports.Printer Buildings.Utilities.Reports.printRealArray |
Changed parameter precision to significantDigits and
minimumWidth to minimumLength
to use the same terminology as the Modelica Standard Library. |
The following critical errors have been fixed (i.e., errors that can lead to wrong simulation results):
Buildings.BoundaryConditions | |
Buildings.BoundaryConditions.SkyTemperature.BlackBody | Fixed error in if-then statement that led to
a selection of the wrong branch to compute the sky temperature. |
Buildings.Media | |
Buildings.Media.PartialSimpleMedium Buildings.Media.GasesConstantDensity.SimpleAir |
Fixed error in assignment of singleState parameter.
This change can lead to different initial conditions if the density of
water is modeled as a function of pressure, or if the
medium model Buildings.Media.GasesConstantDensity.SimpleAir is used. |
Buildings.Media.GasesConstantDensity Buildings.Media.GasesConstantDensity.MoistAir Buildings.Media.GasesConstantDensity.MoistAirUnsaturated Buildings.Media.GasesConstantDensity.SimpleAir |
Fixed error in the function density which returned a non-constant density,
and added a call to ModelicaError(...) in setState_dTX since this
function cannot assign the medium pressure based on the density (as density is a constant
in this model).
|
Buildings.Media.Interfaces.PartialSimpleIdealGasMedium | Updated package with a new copy from the Modelica Standard Library, since the Modelica Standard Library fixed a bug in computing the internal energy of the medium. This bug led to very fast temperature transients at the start of the simulation. |
Buildings.Media.Interfaces.PartialSimpleMedium | Fixed bug in function density, which always returned d_const ,
regardless of the value of constantDensity .
|
Buildings.Media.GasesPTDecoupled | Fixed bug in u=h-R*T , which is only valid for ideal gases.
For this medium, the function is u=h-pStd/dStp .
|
Buildings.Media.GasesConstantDensity | Fixed bug in u=h-R*T , which is only valid for ideal gases.
For this medium, the function is u=h-p/dStp .
|
Buildings.ThermalZones | |
Buildings.ThermalZones.Detailed.MixedAir Buildings.ThermalZones.Detailed.BaseClasses.ExteriorBoundaryConditions |
Fixed bug (issue 35) that leads to the wrong solar heat gain for roofs and for floors. Prior to this bug fix, the outside facing surface of a ceiling received solar irradiation as if it were a floor and vice versa. |
Buildings.ThermalZones.Detailed.MixedAir Buildings.ThermalZones.Detailed.BaseClasses.ExteriorBoundaryConditionsWithWindow |
Fixed bug (issue 36) that leads to too high a surface temperature of the window frame when it receives solar radiation. The previous version did not compute the infrared radiation exchange between the window frame and the sky. |
The following uncritical errors have been fixed (i.e., errors that do not lead to wrong simulation results, but, e.g., units are wrong or errors in documentation):
Buildings.BoundaryConditions | |
Buildings.BoundaryConditions.WeatherData.BaseClasses.ConvertRadiation | Corrected wrong unit label. |
The following issues have been fixed:
Buildings.BoundaryConditions | |
#8 | Add switches for new data. |
#19 | Shift the time for the radiation data 30 min forth and output the local civil time in the data reader. |
#41 | Using when-then sentences to reduce CPU time. |
#43 | Add a ConvertRadiation to convert the unit of radiation from TMY3. |
Buildings.Fluid | |
#28 | Move scripts to Buildings\Resources\Scripts\Dymola. |
Buildings.HeatTransfer | |
#18 | Add a smooth interpolation function to avoid the event. |
Buildings.Media | |
#30 | Removed non-required structurally incomplete annotation. |
Buildings.ThermalZones | |
#35 | Wrong surface tilt for radiation at exterior surfaces of floors and ceilings. |
#36 | High window frame temperatures. |
Note:
-
The version number scheme has been changed. It is now identical to the one used by the Modelica Standard Library.
Versions are identified with two numbers
x.y
and a build number. The first official release of each version has the build number1
. For each released bug fix, the build number is incremented. See Modelica.UsersGuide.ReleaseNotes.VersionManagement for details. -
To allow adding scripts for multiple simulation environments,
all scripts have been moved to the directory
Buildings/Resources/Scripts/Dymola
and the annotation that generates the entry in theCommand
pull down menu has been changed to__Dymola_Commands(file=...
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_0_12_0
Version 0.12.0
Information
Note: The packages whose name ends with Beta
are still being validated.
The following critical error has been fixed (i.e. error that can lead to wrong simulation results):
Buildings.ThermalZones | |
Buildings.ThermalZones.Detailed.BaseClasses.InfraredRadiationExchange | The model Buildings.ThermalZones.Detailed.BaseClasses.InfraredRadiationExchange
had an error in the view factor approximation.
The error caused too much radiosity to flow from large to small surfaces because the law of reciprocity
for view factors was not satisfied. This led to low surface temperatures if a surface had a large area
compared to other surfaces.
The bug has been fixed by rewriting the view factor calculation.
|
The following improvements and additions have been made:
- Updated library to Modelica 3.2.
-
Added
homotopy
operator. - Restructured package Buildings.HeatTransfer.
-
Rewrote the models in
Buildings.Fluid.Actuators to avoid having the flow coefficient
k
as an algebraic variable. This increases robustness. - Rewrote energy, species and trace substance balance in Buildings.Fluid.Interfaces.StaticTwoPortHeatMassExchanger to better handle zero mass flow rate.
-
Implemented functions
enthalpyOfCondensingGas
andsaturationPressure
in single substance media to allow use of the room model with media that do not contain water vapor. - Revised Buildings.Fluid.Sources.Outside to allow use of the room model with media that do not contain water vapor.
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
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Buildings.UsersGuide.ReleaseNotes.Version_0_11_0
Version 0.11.0
Information
Note: The packages whose name ends with Beta
are still being validated.
- Added the package Buildings.ThermalZones.Detailed to compute heat transfer in rooms and through the building envelope. Multiple instances of these models can be connected to create a multi-zone building model.
- Added the package Buildings.HeatTransfer.Windows to compute heat transfer (solar radiation, infrared radiation, convection and conduction) through glazing systems.
- In package Buildings.Fluid.Chillers, added the chiller models Buildings.Fluid.Chillers.ElectricReformulatedEIR and Buildings.Fluid.Cphillers.ElectricEIR, and added the package Buildings.Fluid.Chillers.Data that contains data sets of chiller performance data.
- Added package Buildings.BoundaryConditions with models to compute boundary conditions, such as solar irradiation and sky temperature.
- Added package Buildings.Utilities.IO.WeatherData with models to read weather data in the TMY3 format.
- Revised the package Buildings.Fluid.Sensors.
- Revised the package Buildings.Fluid.HeatExchangers.CoolingTowers.
-
In
Buildings.Fluid.Interfaces.StaticFourPortHeatMassExchanger
and
Buildings.Fluid.Interfaces.StaticFourPortHeatMassExchanger,
fixed bug in energy and moisture balance that affected results if a component
adds or removes moisture to the air stream.
In the old implementation, the enthalpy and species
outflow at
port_b
was multiplied with the mass flow rate atport_a
. The old implementation led to small errors that were proportional to the amount of moisture change. For example, if the moisture added by the component was0.005 kg/kg
, then the error was0.5%
. Also, the results for forward flow and reverse flow differed by this amount. With the new implementation, the energy and moisture balance is exact. -
In
Buildings.Fluid.Interfaces.ConservationEquation and in
Buildings.Media.Interfaces.PartialSimpleMedium, set
nominal attribute for medium to provide consistent normalization.
Without this change, Dymola 7.4 uses different values for the nominal attribute
based on the value of
Advanced.OutputModelicaCodeWithJacobians=true/false;
in the model Buildings.Examples.HydronicHeating. - Fixed bug in energy balance of Buildings.Fluid.Chillers.Carnot.
- Fixed bug in efficiency curves in package Buildings.Fluid.Movers.BaseClasses.Characteristics.
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_0_10_0
Version 0.10.0
Information
- Added package Buildings.Airflow.Multizone with models for multizone airflow and contaminant transport.
- Added the model Buildings.Utilities.Comfort.Fanger for thermal comfort calculations.
- Rewrote Buildings.Fluid.Storage.BaseClasses.ThirdOrderStratifier, which is used in Buildings.Fluid.Storage.StratifiedEnhanced, to avoid state events when the flow reverses. This leads to faster and more robust simulation.
-
In models of package
Buildings.Fluid.MixingVolumes,
added nominal value for
mC
to avoid wrong trajectory when concentration is around 1E-7. See also https://trac.modelica.org/Modelica/ticket/393. - Fixed bug in fan and pump models that led to too small an enthalpy increase across the flow device.
-
In model
Buildings.Fluid.Movers.FlowControlled_dp,
changed
assert(dp_in ≥ 0, ...)
toassert(dp_in ≥ -0.1, ...)
. The former implementation triggered the assert ifdp_in
was solved for in a nonlinear equation since the solution can be slightly negative while still being within the solver tolerance. - Added model Buildings.Controls.SetPoints.Table that allows the specification of a floating setpoint using a table of values.
- Revised model Buildings.Fluid.HeatExchangers.Radiators.RadiatorEN442_2. The new version has exactly the same nominal power during the simulation as specified by the parameters. This also required a change in the parameters.
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_0_9_1
Version 0.9.1
Information
The following critical error has been fixed (i.e. error that can lead to wrong simulation results):
Buildings.Fluid.Storage. | |
Buildings.Fluid.Storage.StratifiedEnhanced | The model Buildings.Fluid.Storage.BaseClasses.Stratifier
had a sign error that lead to a wrong energy balance.
The model that was affected by this error is
Buildings.Fluid.Storage.StratifiedEnhanced.
The model
Buildings.Fluid.Storage.Stratified was not affected.The bug has been fixed by using the newly introduced model Buildings.Fluid.Storage.BaseClasses.ThirdOrderStratifier. This model uses a third-order upwind scheme to reduce the numerical dissipation instead of the correction term that was used in Buildings.Fluid.Storage.BaseClasses.Stratifier .
The model Buildings.Fluid.Storage.BaseClasses.Stratifier has been removed since it
also led to significant overshoot in temperatures when the stratification was pronounced.
|
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_0_9_0
Version 0.9.0
Information
-
Added the following heat exchanger models
-
Buildings.Fluid.HeatExchangers.DryEffectivenessNTU
for a sensible heat exchanger that uses the
epsilon-NTU
relations to compute the heat transfer. - Buildings.Fluid.HeatExchangers.DryCoilCounterFlow and Buildings.Fluid.HeatExchangers.WetCoilCounterFlow to model a coil without and with water vapor condensation. These models approximate the coil as a counterflow heat exchanger.
-
Buildings.Fluid.HeatExchangers.DryEffectivenessNTU
for a sensible heat exchanger that uses the
- Revised air damper Buildings.Fluid.Actuators.BaseClasses.exponentialDamper. The new implementation avoids warnings and leads to faster convergence since the solver does not attempt anymore to solve for a variable that needs to be strictly positive.
-
Revised package
Buildings.Fluid.Movers
to allow zero flow for some pump or fan models.
If the input to the model is the control signal
y
, then the flow is equal to zero ify=0
. This change required rewriting the package to avoid division by the rotational speed. - Revised package Buildings.HeatTransfer to include a model for a multi-layer construction, and to allow individual material layers to be computed steady-state or transient.
-
In package
Buildings.Fluid, changed models so that
if the parameter
dp_nominal
is set to zero, then the pressure drop equation is removed. This allows, for example, to model a heating and a cooling coil in series, and lump there pressure drops into a single element, thereby reducing the dimension of the nonlinear system of equations. - Added model Buildings.Controls.Continuous.LimPID, which is identical to Modelica.Blocks.Continuous.LimPID, except that it allows reverse control action. This simplifies use of the controller for cooling applications.
- Added model Buildings.Fluid.Actuators.Dampers.MixingBox for an outside air mixing box with air dampers.
- Changed implementation of flow resistance in Buildings.Fluid.Actuators.Dampers.MixingBoxMinimumFlow. Instead of using a fixed resistance and a damper model in series, only one model is used that internally adds these two resistances. This leads to smaller systems of nonlinear equations.
-
Changed
Buildings.Media.PerfectGases.MoistAir.T_phX (and by inheritance all
other moist air medium models) to first compute
T
in closed form assuming no saturation. Then, a check is done to determine whether the state is in the fog region. If the state is in the fog region, thenInternal.solve
is called. This new implementation can lead to significantly shorter computing time in models that frequently callT_phX
. - Added package Buildings.Media.GasesConstantDensity which contains medium models for dry air and moist air. The use of a constant density avoids having pressure as a state variable in mixing volumes. Hence, fast transients introduced by a change in pressure are avoided. The drawback is that the dimensionality of the coupled nonlinear equation system is typically larger for flow networks.
-
In
Buildings.Fluid.Actuators.BaseClasses.PartialDamperExponential,
added default value for parameter
A
to avoid compilation error if the parameter is disabled but not specified. - Simplified the mixing volumes in Buildings.Fluid.MixingVolumes by removing the port velocity, pressure drop and height.
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_0_8_0
Version 0.8.0
Information
-
In
Buildings.Fluid.Interfaces.ConservationEquation,
added to
Medium.BaseProperties
the initializationX(start=X_start[1:Medium.nX])
. Previously, the initialization was only done forXi
but not forX
, which caused the medium to be initialized toreference_X
, ignoring the value ofX_start
. -
Renamed
Buildings.Media.PerfectGases.MoistAirNonSaturated
to Buildings.Media.PerfectGases.MoistAirUnsaturated andBuildings.Media.GasesPTDecoupled.MoistAirNoLiquid
to Buildings.Media.Air, and addedassert
statements if saturation occurs. - Added regularizaation near zero flow to Buildings.Fluid.HeatExchangers.ConstantEffectiveness and Buildings.Fluid.MassExchangers.ConstantEffectiveness.
- Fixed bug regarding temperature offset in Buildings.Media.PerfectGases.MoistAirUnsaturated.T_phX.
- Added implementation of function Buildings.Media.Air.enthalpyOfNonCondensingGas and its derivative.
- In Buildings.Media.PerfectGases.MoistAir, fixed bug in implementation of Buildings.Media.PerfectGases.MoistAir.T_phX. In the previous version, it computed the inverse of its parent class, which gave slightly different results.
- In Buildings.Utilities.IO.BCVTB.BCVTB, added parameter to specify the value to be sent to the BCVTB at the first data exchange, and added parameter that deactivates the interface. Deactivating the interface is sometimes useful during debugging.
-
In
Buildings.Media.GasesPTDecoupled.MoistAir and in
Buildings.Media.PerfectGases.MoistAir, added function
enthalpyOfNonCondensingGas
and its derivative. - In Buildings.Media, fixed bug in implementations of derivatives.
- Added model Buildings.Fluid.Storage.ExpansionVessel.
- Added Wrapper function Buildings.Fluid.Movers.BaseClasses.Characteristics.solve for Modelica.Math.Matrices.solve. This is currently needed since Modelica.Math.Matrices.solve does not specify a derivative.
- Fixed bug in Buildings.Fluid.Storage.Stratified. In the previous version, for computing the heat conduction between the top (or bottom) segment and the outside, the whole thickness of the water volume was used instead of only half the thickness.
- In Buildings.Media.ConstantPropertyLiquidWater, added the option to specify a compressibility. This can help reducing the size of the coupled nonlinear system of equations, at the expense of introducing stiffness. This change required to change the inheritance tree of the medium. Its base class is now Buildings.Media.Interfaces.PartialSimpleMedium, which contains the equation for the compressibility. The default setting will model the flow as incompressible.
-
In
Buildings.Controls.Continuous.Examples.PIDHysteresis
and
Buildings.Controls.Continuous.Examples.PIDHysteresisTimer,
fixed error in default parameter
eOn
. Fixed error by introducing parameterTd
, which used to be hard-wired in the PID controller. - Added more models for fans and pumps to the package Buildings.Fluid.Movers. The models are similar to the ones in Modelica.Fluid.Machines but have been adapted for air-based systems, and to include more characteristic curves in Buildings.Fluid.Movers.BaseClasses.Characteristics. The new models are better suited than the existing fan model Buildings.Fluid.Movers.FlowMachinePolynomial for zero flow rate.
- Added an optional mixing volume to Buildings.Fluid.BaseClasses.PartialThreeWayResistance and hence to the flow splitter and to the three-way valves. This often breaks algebraic loops and provides a state for the temperature if the mass flow rate goes to zero.
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_0_7_0
Version 0.7.0
Information
- Updated library from Modelica_Fluid to Modelica.Fluid 1.0
- Merged sensor and source models from Modelica.Fluid to Buildings.Fluid.
- Added sensor for sensible and latent enthalpy flow rate, Buildings.Fluid.Sensors.SensibleEnthalpyFlowRate and Buildings.Fluid.Sensors.LatentEnthalpyFlowRate. These sensors are needed, for example, to interface air-conditioning systems that are modeled with Modelica with the Building Controls Virtual Test Bed.
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_0_6_0
Version 0.6.0
Information
- Added the package Buildings.Utilities.IO.BCVTB which contains an interface to the Building Controls Virtual Test Bed.
- Updated license to Modelica License 2.
-
Replaced
Buildings.Utilities.Psychrometrics.HumidityRatioPressure.mo
by
Buildings.Utilities.Psychrometrics.HumidityRatio_pWat.mo
and
Buildings.Utilities.Psychrometrics.VaporPressure_X.mo
because the old model used
RealInput
ports, which are obsolete in Modelica 3.0. - Changed the base class Buildings.Fluid.Interfaces.StaticTwoPortHeatMassExchanger to enable computation of pressure drop of mechanical equipment.
- Introduced package Buildings.Fluid.BaseClasses.FlowModels to model pressure drop, and rewrote Buildings.Fluid.BaseClasses.PartialResistance.
- Redesigned package Buildings.Utilities.Math to allow having blocks and functions with the same name. Functions are now in Buildings.Utilities.Math.Functions.
- Fixed sign error in Buildings.Fluid.Storage.BaseClasses.Stratifier which caused a wrong energy balance in Buildings.Fluid.Storage.StratifiedEnhanced.
-
Renamed
Buildings.Fluid.HeatExchangers.HeaterCoolerIdeal
to Buildings.Fluid.HeatExchangers.HeaterCoolerPrescribed to have the same nomenclatures as is used for Buildings.Fluid.MassExchangers.HumidifierPrescribed -
In
Buildings.Fluid/Actuators/BaseClasses/PartialDamperExponential,
added option to compute linearization near zero based on
the fraction of nominal flow instead of the Reynolds number.
This was set as the default, as it leads most reliably to a model
parametrization that leads to a derivative
d m_flow/d p
near the origin that is not too steep for a Newton-based solver. - In damper and VAV box models, added optional parameters to allow specifying the nominal face velocity instead of the area.
-
Set nominal attribute for pressure drop
dp
in Buildings.Fluid.BaseClasses.PartialResistance and in its child classes. - Added models for chiller ( Buildings.Fluid.Chillers.Carnot), for occupancy ( Buildings.Controls.SetPoints.OccupancySchedule) and for blocks that take a vector as an argument ( Buildings.Utilities.Math.Min, Buildings.Utilities.Math.Max, and Buildings.Utilities.Math.Average).
- Changed various variable names to be consistent with naming convention used in Modelica.Fluid 1.0.
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_0_5_0
Version 0.5.0
Information
- Updated library to Modelica.Fluid 1.0.
- Moved most examples from package Buildings.Fluid.Examples to the example directory in the package of the individual model.
- Renamed package Buildings.Utilites.Controls to Buildings.Utilites.Diagnostics.
- Introduced packages Buildings.Controls, Buildings.HeatTransfer (which contains models for heat transfer that generally does not involve modeling of the fluid flow), Buildings.Fluid.Boilers and Buildings.Fluid.HeatExchangers.Radiators.
-
Changed valve models in
Buildings.Fluid.Actuators.Valves so that
Kv
orCv
can be used as the flow coefficient (in [m3/h] or [USG/min]).
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_0_4_0
Version 0.4.0
Information
- Added package Buildings.Fluid.Storage with models for thermal energy storage.
- Added a steady-state model for a heat and moisture exchanger with constant effectiveness. See Buildings.Fluid.MassExchangers.ConstantEffectiveness
- Added package Buildings.Utilities.Reports. The package contains models that facilitate reporting.
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_0_3_0
Version 0.3.0
Information
- Added package Buildings.Fluid.Sources. The package contains models for modeling species that do not affect the medium balance of volumes. This can be used to track for example carbon dioxide or other species that have a small concentration.
- The package Buildings.Fluid.Actuators.Motors has been added. The package contains a motor model for valves and dampers.
-
The package Buildings.Media has been reorganized and
the new medium model
Buildings.Media.GasesPTDecoupled.MoistAir
has been added.
In addition, this package now contains a bug fix that is needed for Modelica 2.2.1 and 2.2.2. The bugs are fixed by using a new base class Buildings.Media.Interfaces.PartialSimpleIdealGasMedium (that fixes the bugs) instead of Modelica.Media.Interfaces.PartialSimpleIdealGasMedium. In the original implementation, initial states of fluid volumes can be far away from the steady-state value because of an inconsistent implementation of the enthalpy and internal energy. When theBuildings
library is upgraded to to Modelica 3.0.0, it should be safe to remove this bug fix. - The package Buildings.Fluid.HeatExchangers has been revised and several models have been renamed. The heat exchanger models have been revised to allow computing the fluid volumes either dynamically, or in steady-state.
-
The damper with exponential opening characteristic has been revised to allow control signals
over the whole range between
0
and1
. This was in earlier versions restricted. In the same model, a bug was fixed that caused the flow to be largest fory=0
, i.e., when the damper is closed. - Additional models for psychrometric equations have been added. The new models contain equations that convert dew point temperature and water vapor pressure, as well as water vapor concentration and water vapor pressure.
- A new mixing volume has been added that allows latent heat exchange with the volume. This model can be used to model a volume of moist air with water vapor condensation inside the volume. The condensate is removed from the volume in its liquid phase.
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_0_2_0
Version 0.2.0
Information
New in this version are models for two and three way valves.
In addition, the Fluids
package has been slightly revised.
The package Fluid.BaseClasses
has been added because in
the previous version, partial models for fixed resistances
where part of the Actuator
package.
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).
Modelica definition
Buildings.UsersGuide.ReleaseNotes.Version_0_1_0
Version 0.1.0
Information
First release of the library.
This version contains basic models for modeling building HVAC systems. It also contains new medium models in the package Buildings.Media. These medium models have simpler property functions than the ones from Modelica.Media. For example, there is medium model with constant heat capacity which is often sufficiently accurate for building HVAC simulation, in contrast to the more detailed models from Modelica.Media that are valid in a larger temperature range, at the expense of introducing non-linearities due to the medium properties.
Extends from Modelica.Icons.ReleaseNotes (Icon for release notes in documentation).