This application relates to superconducting electrodynamic magnetic levitation (maglev), and more specifically to a fault detection device and method for a superconducting electrodynamic maglev track.
In a superconducting electrodynamic magnetic levitation (maglev) system, the figure-8-shaped coil is installed outside the propulsion coil, and is thus directly exposed to outdoor environmental factors, such as sunshine, wind and sand, rain and fog, and ice and snow. Therefore, the coil is prone to insulation deterioration or damage, and even open-circuit fault. However, the figure-8-shaped coil is responsible for levitation and guidance in the superconducting electrodynamic maglev system, and plays an important role in ensuring the stable operation of the maglev train. Therefore, it is necessary to perform fault diagnosis for the figure-8-shaped coil before the actual operation of the maglev train. In the existing technology, the geometric regularity detection and the magnetic field uniformity detection of the sidewall discrete figure-8-shaped coil track cannot be achieved. Therefore, it is urgent to develop a fault detection device for a superconducting electrodynamic maglev track to simultaneously detect the geometric regularity and magnetic field uniformity of the sidewall discrete figure-8-shaped coil track.
An objective of the present disclosure is to provide a fault detection device and method for a superconducting electrodynamic maglev track to solve the above technical problems. The technical solutions of the present disclosure are described as follows.
In a first aspect, this application provides a fault detection device for a superconducting electric maglev track, comprising:
In a second aspect, this application provides a fault detection method for a superconducting electric maglev track, comprising:
The beneficial effects of the present disclosure are described as follows.
Regarding the fault detection device provided herein, the magnetic field generated by the permanent magnet array is applied to the discrete figure-8-shaped coil track, and the coil at the periphery of the permanent magnet array is used as a receiving coil to capture the induced magnetic field generated by the induced current of the discrete figure-8-shaped coil. In addition, the receiving coil is connected to a series of signal processing devices, such as a filtering circuit, an amplifying circuit and an oscilloscope, for extracting and displaying the received electrical signals, thus realizing the non-contact detection of geometrical regularity and magnetic field uniformity of the discrete figure-8-shaped coil track.
Other features and advantages of the present disclosure will be set forth below, parts of which will be apparent from the specification or understood by implementing embodiments of the present disclosure. The objects and other advantages of the present disclosure may be realized and obtained from the specification, the claims and the particularly-indicated structure in the drawings.
To more clearly illustrate the technical solutions of the embodiments of the present application, the accompanying drawings needed in the description of embodiments will be briefly introduced below. It should be understood that the following accompanying drawings merely show some embodiments of the present application, and therefore should not be construed as limitation to the scope of the present disclosure. Other related drawings can be obtained by one of ordinary skill in the art based on the accompanying drawings without making any creative effort.
In the drawings, 1, frame system; 11, vehicle body; 12, bogie; 13, wheel; 14, alternating-current (AC) generator; 131, hub motor; 21, lifting device; 22, clamping device; 23, permanent magnet array; 24, receiving coil; 211, mounting plate; 212, electric push rod; 221, first connection portion; 222, second connection portion; 231, first main magnetic pole; 232, second main magnetic pole; 2211, mounting substrate; 2222, slot; 3, sidewall discrete figure-8-shaped coil track.
To make the purpose, technical solutions and advantages of the embodiments of the present application clearer, the technical solutions in the embodiments of the present application will be described clearly and completely below with reference to the accompanying drawings. Obviously, described herein are merely some embodiments of the present application, rather than all embodiments. The components of embodiments of the present application generally described and illustrated in the accompanying drawings herein may be arranged and designed in a variety of different configurations. Accordingly, the following detailed description is not intended to limit the scope of the present application, but rather represents selected embodiments of the present application. Based on the embodiments of the present application, all other embodiments obtained by one of ordinary skill in the art without making creative effort shall fall within the scope of the present application.
It should be noted that similar symbols and letters denote similar items in the following drawings. Therefore, once an item has been defined in one drawing, there is no need to further define or explain such item in the subsequent drawings. Furthermore, the terms “first”, “second”, and “third” are merely for distinguishment, and should not be understood as indicating or implying relative importance.
Provided herein is a fault detection device for a superconducting electrodynamic maglev track.
As shown in
The frame system 1 is provided between two sidewall discrete figure-8-shaped coil tracks 3, and a signal processing device is provided on a top of the frame system 1.
Two sides of the frame system 1 are each provided with the detection system. The detection system includes a lifting device 21 and a clamping device 22. The lifting device 21 is configured to adjust a vertical height of the clamping device 22, and the clamping device 22 is provided at an outer side of the lifting device 21.
As shown in
In the detection device provided herein, the single-sided magnetism of the permanent magnet array 23 is utilized to generate a source magnetic field. When the detection is performed, the source magnetic field is interlinked with a figure-8-shaped coil in the sidewall discrete figure-8-shaped coil track 3 to induce an electric potential within the figure-8-shaped coil. When the figure-8-shaped coil is undamaged, an induced current is generated within the figure-8-shaped coil, which then generates a magnetic field around the figure-8-shaped coil. When the receiving coil 24 is provided at the outer periphery of the permanent magnet array 23, the single-sided magnetism of the permanent magnet array 23 can reduce the influence of the source magnetic field on the receiving coil 24, and the receiving coil 24 induces an electric potential inside by capturing the magnetic field generated by the figure-8-shaped coil. After that, the electric signals within the receiving coil 24 are processed by the signal processing device through filtering, amplifying and displaying to obtain electric signal waveforms reflecting geometrical smoothness and magnetic field uniformity of the figure-8-shaped coil, so as to realize the real-time observation.
In the present disclosure, to ensure the generation of a good source magnetic field, the permanent magnet array 23 includes two Halbach permanent magnets disposed side by side, and each of the two Halbach permanent magnet arrays has at least two different predetermined magnetization acute angles, where a 90° magnetization angle is preset between the at least two different predetermined magnetization acute angles. The Halbach permanent magnet array used herein is an emitter.
The effect of the width of the permanent magnet array 23 on detection results will be clarified with reference to
In the detection device, the predetermined polar distance model is expressed by:
Further, to clarify the setting of the width of a single Halbach permanent magnet in the present device, the first Halbach permanent magnet includes a first boundary magnetic pole, a second boundary magnetic pole and a first main magnetic pole 231. The first main magnetic pole 231 is provided between the first boundary magnetic pole and the second boundary magnetic pole. A width of the first boundary magnetic pole is equal to that of the second boundary magnetic pole, and a width of the first main magnetic pole 231 is larger than that of the first boundary magnetic pole.
The second Halbach permanent magnet includes a third boundary magnetic pole, a fourth boundary magnetic pole and the second main magnetic pole 232. The second main magnetic pole 232 is provided between the third boundary magnetic pole and the fourth boundary magnetic pole. A width of the third boundary magnetic pole is equal to that of the fourth boundary magnetic pole, and a width of the second main magnetic pole 232 is larger than that of the third boundary magnetic pole.
As shown in
As shown in
The second connection portion 222 is a mounting base. The receiving coil 24 is sleevedly provided on an outer wall of the mounting base. The mounting substrate 2211 is arranged at a center of the mounting base 222, and a center of gravity of the mounting substrate 2211 coincides with that of the mounting base 222.
When the mounting substrate 2211 is provided in the center of the mounting base 222, and the center of gravity of the mounting substrate 2211 coincides with the center of gravity of the mounting base 222, the position of the permanent magnet array 23 relative to the receiving coil 24 remains fixed, which can effectively ensure the electromagnetic effects between the permanent magnet array 23, the receiving coil 24 and the figure-8-shaped coil.
As shown in
In the present detection device, the bogie 12 is configured to support and guide the vehicle body 11. When an on-board battery is introduced to provide direct current for the present device, a traction inverter device is required to realize the supply of alternating current, so as to drive the frame system 1.
In the present device, to clarify the specific structure of the signal processing device, the signal processing device includes a filter amplifier and an oscilloscope. The filter amplifier, the oscilloscope and the receiving coil 24 are electrically connected. The signal processing device is configured to filter, amplify and display received electrical signals, so as to realize the electrical signal feedback for the geometrical smoothness and the magnetic field uniformity of the discrete figure-8-shaped coil track.
In the present device, to enable the lifting device 21 to accurately reach a plurality of preset detection heights and to facilitate the adjustment of the preset detection heights, the lifting device 21 includes a mounting plate 211 and an electric push rod 212. One end of the mounting plate 211 is fixedly connected to a side of the frame system 1, and the other end of the mounting plate 211 is fixedly connected to the electric push rod 212. The electric push rod 212 is provided with an output end, and the output end is in transmission connection with the clamping device 22.
Provided herein a fault detection method for a superconducting electric maglev track, which includes the following steps.
A plurality of preset detection heights are set for a clamping device 22 by means of a lifting device 21.
A frame system 1 is operated respectively at the plurality of preset detection heights. A plurality of detection signals respectively corresponding to the plurality of preset detection heights are collected by a signal processing device.
A magnetic field uniformity analysis is performed based on the plurality of detection signals.
A fault point detection analysis is performed on the sidewall discrete figure-8-shaped coil tracks 3 based on the plurality of detection signals.
The magnetic field uniformity analysis is performed based on the plurality of detection signals through the following steps.
When a signal processing device includes a filter amplifier and an oscilloscope, and the filter amplifier, the oscilloscope and a receiving coil 24 are electrically connected, oscilloscope waveforms respectively corresponding to the plurality of detection signals are collected in real time during the traveling of the frame system 1. When the oscilloscope waveform fluctuates up and down at a certain value presenting a periodical change without a sudden change, it means that the figure-8-shaped coil track is geometrically uniformly arranged with a uniform magnetic field.
When the waveform undergoes a sudden change at a certain moment and returns to the previous value after another preset detection moment, it indicates that there is a fault (broken or short circuit) at the figure-8-shaped coil corresponding to the moment where the sudden change of the waveform occurs. The preset detection moment is the electromagnetic induction time of a figure-8-shaped coil and a set of permanent magnet array 23.
The fault point analysis is performed on the sidewall discrete figure-8-shaped coil tracks 3 based on the plurality of detection signals through the following steps.
The judgment basis of the coil fault is obtained by means of finite element simulation. Specifically, in an Ansys software, to establish a three-dimensional (3D) finite element model containing a permanent magnet array 23, a receiving coil 24 and a sidewall discrete figure-8-shaped coil track 3. The simulation type is set as a transient magnetic field. Centers of a permanent magnet array 23, a receiving coil 24 and a sidewall discrete figure-8-shaped coil track 3 are aligned. A motion domain is set for the region where the permanent magnet array 23 and the receiving coil 24 are located, with a move direction along the longitudinal direction of the sidewall discrete figure-8-shaped coil track 3 at a speed of 60 km/h (uniform speed), so that the change curve of the induced current in the receiving coils Winding1 and Winding2 with the running time can be obtained.
To further realize the precise positioning of the fault point of the figure-8-shaped coil for facilitating the overhaul, the current signals in Winding1 and Winding2 are compared. As shown in
Further, an external filtering and amplifying circuit built by Matlab/Simulink may also be used to filter and amplify the electrical signals of the receiving coil to obtain the filtered and amplified signals.
As shown in
As shown in
Described above are merely specific embodiments of the present disclosure, but the scope of the present disclosure is not limited thereto. It should be understood that various changes, modifications or substitutions made by one of ordinary skill in the art without departing from the scope of the present disclosure shall be included in the scope of the present disclosure defined by the appended claims.
This application is a continuation of International Patent Application No. PCT/CN2024/094210, filed on May 20, 2024, which claims the benefit of priority from Chinese Patent Application No. 202310909901.1, filed on Jul. 24, 2023. The content of the aforementioned application, including any intervening amendments thereto, is incorporated herein by reference in its entirety.
Number | Name | Date | Kind |
---|---|---|---|
5511488 | Powell | Apr 1996 | A |
5732636 | Wang et al. | Mar 1998 | A |
6101952 | Thornton | Aug 2000 | A |
6129025 | Minakami | Oct 2000 | A |
6357359 | Davey | Mar 2002 | B1 |
9126487 | Henderson | Sep 2015 | B2 |
9511959 | Bambrogan | Dec 2016 | B2 |
20030005851 | Post | Jan 2003 | A1 |
20070089636 | Guardo | Apr 2007 | A1 |
20100212537 | Borowy | Aug 2010 | A1 |
20130193276 | Hunter | Aug 2013 | A1 |
20180141459 | Henderson | May 2018 | A1 |
20180223481 | Dunham | Aug 2018 | A1 |
20180237996 | Sadeghi | Aug 2018 | A1 |
20180299520 | Piron | Oct 2018 | A1 |
20190100389 | Neubauer | Apr 2019 | A1 |
20190256302 | Neubauer | Aug 2019 | A1 |
20210159091 | Zhou | May 2021 | A1 |
20210347390 | Klim | Nov 2021 | A1 |
20220089196 | Deng | Mar 2022 | A1 |
Number | Date | Country |
---|---|---|
105264389 | Jan 2016 | CN |
105803872 | Jul 2016 | CN |
109270475 | Jan 2019 | CN |
110763491 | Feb 2020 | CN |
111505530 | Aug 2020 | CN |
211689694 | Oct 2020 | CN |
111942165 | Nov 2020 | CN |
113447782 | Sep 2021 | CN |
114643873 | Jun 2022 | CN |
115326440 | Nov 2022 | CN |
116278785 | Jun 2023 | CN |
H03261302 | Nov 1991 | JP |
H04165902 | Jun 1992 | JP |
H05281281 | Oct 1993 | JP |
2005304270 | Oct 2005 | JP |
Entry |
---|
Xu, Xiaozhuo, et al. “Pole optimization and thrust ripple suppression of new Halbach consequent-pole PMLSM for ropeless elevator propulsion.” IEEE Access 8 (2020): 62042-62052. (Year: 2020). |
Gao, Tao, et al. “Design of new energy-efficient permanent magnetic maglev vehicle suspension system.” IEEE Access 7 (2019): 135917-135932. (Year: 2019). |
Luo Cheng et al., “Vertical stability of permanent magnet EDS system with novel Halbach array”, Journal of Traffic and Transportation Engineering, Apr. 15, 2019, vol. 19, No. 2, pp. 101-109. |
Number | Date | Country | |
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Parent | PCT/CN2024/094210 | May 2024 | WO |
Child | 18777170 | US |