functioninternalResistancesOneUTube
Extends from AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.partialInternalResistances (Partial model for borehole resistance calculation).
Information
This model computes the different thermal resistances present in a single-U-tube borehole using the method of Bauer et al. (2011). It also computes the fluid-to-ground thermal resistance Rb and the grout-to-grout thermal resistance Ra as defined by Claesson and Hellstrom (2011) using the multipole method.
References
J. Claesson and G. Hellstrom. Multipole method to calculate borehole thermal resistances in a borehole heat exchanger. HVAC&R Research, 17(6): 895-911, 2011.
D. Bauer, W. Heidemann, H. Müller-Steinhagen, and H.-J. G. Diersch. Thermal resistance and capacity models for borehole heat exchangers. International Journal of Energy Research, 35:312–320, 2011.
Inputs
Outputs
| Type | Name | Default | Description |
|---|---|---|---|
| Real | x (from partialInternalResistances) | Capacity location | |
| Modelica.Units.SI.ThermalResistance | Rgb | Thermal resistance between grout zone and borehole wall | |
| Modelica.Units.SI.ThermalResistance | Rgg | Thermal resistance between the two grout zones | |
| Modelica.Units.SI.ThermalResistance | RCondGro | Thermal resistance between: pipe wall to capacity in grout |
Revisions
-
July 9, 2025, by Jianjun Hu:
Added missing value assignment.
This is for IBPSA, #2030. -
November 22, 2023, by Michael Wetter:
Corrected use ofgetInstanceName()which was called inside a function which is not allowed.
This is for IBPSA, #1814. -
February 7, 2022, by Michael Wetter:
Changed function to bepure.
This is for IBPSA, #1582. -
December 11, 2021, by Michael Wetter:
Addedimpuredeclaration for MSL 4.0.0. -
July 18, 2018 by Massimo Cimmino:
Implemented multipole method. -
February 14, 2014 by Michael Wetter:
Added an assert statement to test for non-physical values. -
February 12, 2014, by Damien Picard:
Remove the flow dependency of the resistances, as this function calculates the conduction resistances only. -
January 24, 2014, by Michael Wetter:
Revised implementation. -
January 23, 2014, by Damien Picard:
First implementation.