The quasi-static flux tubes library is based on the transient library Magnetic.FluxTubes. The main principles of confined flux and flux tubes apply, too. The quasi-static flux tubes library contains components for modelling of electromagnetic devices with lumped magnetic networks based on quasi-static theory. Models based on this library are suited for quasi-static simulation of transformers at component and system level.
The quasi-static components of this library do not consider saturation since linearity is strictly assumed. In case that the permeability of a saturated circuit needs to be considered, a transient permeability estimation sensor is provided do determine the effective permeability from a transient simulation.
A general introduction into quasi-static (quasi-static) phasor can be found in Modelica.Electrical.QuasiStatic.
This user's guide gives a short introduction to the underlying concept of quasi-static magnetic flux tubes, summarizes basic relationships and equations.
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Name | Description |
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FluxTubeConcept | Flux tube concept |
Literature | Literature |
ReleaseNotes | Release Notes |
Contact | Contact |
Following below, the concept of magnetic flux tubes is outlined in short. For a detailed description of flux tube elements, please have a look at the listed literature. Magnetic flux tubes enable the modeling of magnetic fields with lumped equivalent circuit networks.
Since quasi-static conditions are assumed, each field quantity can be represented by a complex phasor -- which is indicated by underlining the respective variable:
The figure below and the following equations illustrate the relationships between
A flux tube confines the magnetic flux. Flied lines, and flux tubes, respectively are always closed. So there is no flux entering or leaving a flux tube. The total flux of a configuration can be represented by parallel flux tubes, representing different flux paths. This is considered by connecting the elements of a lumped circuit model, such that the sum of all fluxes of a connection is equivalent to zero.
For a section of a flux tube with length the magnetic potential difference is determined by the length integral over the magnetic field strength:
The magnetic flux entering, and leaving a flux tube, respectively, is determined by the surface integral of the normal component of the magnetic field strength:
The magnetic potential difference and the magnetic flux have the same angle, so the reluctance a real (non complex) quantity:
For a generic flux tube reluctance with constant area of cross section, , and length, , the magnetic reluctance is:
The parameter and variable names are chosen as close as possible to the transient FluxTubes library, to avoid additional effort when converting transient into quasi-static flux tubes models.
A similar approach on quasi-static flux tube models is published in [Raabe2012].
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[Raabe2012] | N. Raabe, " An approach for modelling quasi-static magnetic circuits," Modelica Conference, pp. 167-172, 2012. |
Additional reference on magnetic flux tubes are listed in Modelica.Magnetic.FluxTubes.
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Dr. Christian Kral
Electric Machines, Drives and Systems
A-1060 Vienna, Austria
email: dr.christian.kral@gmail.com
Anton Haumer
Technical Consulting & Electrical Engineering
D-93049 Regensburg, Germany
email: a.haumer@haumer.at
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Automatically generated Thu Oct 1 16:07:50 2020.