This application is a national phase application of International Application No. PCT/CN2020/104867, filed on Jul. 27, 2020, which claims the priority to the Chinese patent application No. 202010281385.9, entitled “DISPLACEMENT DETECTION CIRCUIT OF MAGLEV ROTOR SYSTEM AND DISPLACEMENT SELF-SENSING SYSTEM THEREOF,” filed on Apr. 10, 2020, to the China National Intellectual Property Administration, the entire contents of each of which are incorporated herein by reference.
The present disclosure relates to the technical field of maglev bearings, and more particularly to a displacement detection circuit of a maglev rotor system and a displacement self-sensing system thereof.
A maglev bearing has the characteristics of non-contact friction, high rotating speed, no lubrication and the like, and a maglev rotor system itself may realize active vibration control without additional hardware equipment, such that the maglev rotor system has been widely used in earth observation satellite, space telescope, and other aspects. To realize the high-precision control of a maglev rotor, it is necessary to accurately obtain a position of the rotor relative to a stator in the maglev bearing.
With the development of various high-resolution satellites, higher requirements are put forward for the stability and vibration of a maglev control system. Due to the non-contact characteristic of the maglev system, it is necessary to use a non-contact sensor to determine a displacement of the rotor relative to the stator in the maglev rotor system. A traditional displacement sensor needs to select a detection surface separately, which not only increases an axial size of the rotor, but also makes the detection and control of the displacement non-coplanar, thus resulting in an error in the detection of the displacement. Moreover, the traditional displacement sensor has a high cost and poor reliability. In addition, a traditional displacement self-sensing magnetic bearing estimates the position of the rotor only by extracting a component in a current ripple. In order to ensure an estimation precision of the component, it is necessary to design a complex extracting circuit, such that a traditional displacement detection method limits the improvement of the vibration performance of the maglev system.
The technical problem to be solved by the present disclosure is that the existing displacement sensor needs to select a detection surface separately, which increases an axial size of a rotor, and makes the detection and control of a displacement non-coplanar, thus resulting in an error in the detection of the displacement.
In order to solve the technical problem above, an embodiment of the present disclosure provides a displacement detection circuit of a maglev rotor system, which comprises:
Optionally, the current sampling circuit comprises:
Optionally, an amplification factor of the first amplifying circuit satisfies the following formula:
a=2μ0N(4A2h1+2A1h2),
Optionally, the Hall signal processing circuit comprises:
Optionally, the displacement signal resolving circuit comprises:
Optionally, the square rooting circuit comprises:
Optionally, the offset adjustment value corresponding to the offset adjustment circuit satisfies the following formula:
b=(2A2h1+A1h2)2,
Optionally, amplification factor control resistors in the current sampling circuit and the Hall signal processing circuit, an amplification factor control resistor in the offset adjustment circuit, and an introduction resistor of the reference signal are all sliding rheostats.
Optionally, a width of a primary air gap corresponding to the displacement of the rotor satisfies the following calculation formula:
In a second aspect, an embodiment of the present disclosure further provides a maglev rotor displacement self-sensing system, which comprises a maglev rotor system and the displacement detection circuit of the maglev rotor system in a first aspect, wherein the maglev rotor system is connected to the displacement detection circuit, and the maglev rotor system comprises a permanent magnet offset maglev rotor system with an auxiliary air gap.
Compared with the prior art, the technical solutions provided by the embodiments of the present disclosure have the following advantages.
The displacement detection circuit provided by the embodiment of the present disclosure comprises the current sampling circuit, the Hall sensors, the Hall signal processing circuit and the displacement signal resolving circuit, wherein the current sampling circuit is configured to collect the current flowing through the corresponding coil, and the coil comprises the coils distributed in series in the maglev rotor system; the Hall sensors are arranged in the upper auxiliary air gap and the lower auxiliary air gap of the maglev rotor system, and the sensing surfaces of the Hall sensors are perpendicular to the magnetic field directions in the corresponding auxiliary air gaps; the Hall signal processing circuit is configured to perform differential processing on the Hall sensing signal corresponding to the upper auxiliary air gap and the Hall sensing signal corresponding to the lower auxiliary air gap; and the displacement signal resolving circuit is configured to acquire the displacement of the rotor in the maglev rotor system according to the current and the result of the differential processing. The embodiment of the present disclose is suitable for detecting the position of the rotor in the permanent magnet offset maglev rotor system with the auxiliary air gap. Only the current value of the coil is needed. The detection by the Hall sensors and the control by the maglev rotor system are coplanar, all functions of a traditional position sensor and a traditional position self-sensing detection method are realized, and meanwhile, there are advantages that the axial size of the rotor is reduced, the detection and the control are coplanar, and high precision and simple design are realized, thus providing conditions for high-precision control by the maglev system.
It is to be understood that the foregoing general description and the following detailed description are exemplary and explanatory only, and cannot limit the present disclosure
The drawings herein are incorporated into the specification and constitute a part of the specification, show the embodiments consistent with the present disclosure, and serve to explain the principles of the present disclosure together with the specification.
In order to illustrate the technical solutions in the embodiments of the present disclosure or the prior art more clearly, the drawings to be used in the description of the embodiments or the prior art will be briefly described below. Obviously, those of ordinary skills in the art can also obtain other drawings based on these drawings without going through any creative work.
To make the objects, technical solutions, and advantages of the embodiments of the present disclosure clearer, the technical solutions in the embodiments of the present disclosure will be described clearly and completely below. Apparently, the described embodiments are merely some but not all of the embodiments of the present disclosure. Based on the embodiments of the present disclosure, all other embodiments obtained by those of ordinary skills in the art without going through any creative work shall fall within the scope of protection of the present disclosure.
Specifically, with reference to
The Hall sensors 20 are arranged in an upper auxiliary air gap and a lower auxiliary air gap of the maglev rotor system. The sensing surfaces of the Hall sensors are perpendicular to magnetic field directions in the corresponding auxiliary air gaps 8. As illustrated in
The displacement signal resolving circuit 40 is connected to the current sampling circuit 10 and the Hall signal processing circuit 30, respectively. The displacement signal resolving circuit 40 is configured to acquire a displacement of a rotor in the maglev rotor system according to the current and a result of the differential processing, which means that the displacement signal resolving circuit 40 can directly obtain a width of the primary air gap corresponding to the displacement of the rotor to be acquired in the maglev rotor system according to the current flowing through the corresponding coil 4 collected by the current sampling circuit 10 and the result of the differential processing of the Hall sensing signal corresponding to the upper auxiliary air gap and the Hall sensing signal corresponding to the lower auxiliary air gap by the Hall signal processing circuit 30, thus acquiring a position of the rotor in the maglev rotor system. Therefore, all functions of a traditional position sensor and a traditional position self-sensing detection method are realized, and meanwhile, there are advantages that an axial size of the rotor is reduced, the detection and the control are coplanar, and high precision and simple design are realized, thus providing conditions for high-precision control by the maglev system.
Specifically, it is only necessary to sample the current flowing through one coil 4 in the same direction, which means that only one sampling resistor R is needed in the same direction. One end of the sampling resistor R may be connected to one external terminal A of the four coils 4, and the other end of the sampling resistor R may be connected to the other external terminals B of the four coils 4. Currents flowing through the four coils 4 may be obtained by collecting the current flowing through the sampling resistor R. Illustratively, the sampling resistor R may be connected in series with a power amplifier 50 to preliminarily amplify the current collected by the current sampling circuit 10, thus improving a current detection precision.
The first amplifying circuit U2B is configured to amplify the current flowing through the sampling resistor R, and the current sampling circuit 10 may calculate an output current of the corresponding coil 4 by detecting voltages at the positive and negative ends of the sampling resistor R. Illustratively, as shown in
Optionally, referring to
Specifically, the above formula may be derived as follows.
When the rotor in the maglev rotor system is located in the balanced position, the width of the primary air gap is set as h1 and the surface area of the primary air gap is set as A1. The width of the auxiliary air gap is set as h2 and the surface area of the auxiliary air gap is set as A2. The width of the primary air gap corresponding to the displacement of the rotor to be acquired is set as h.
According to the Ampere's circuital law:
Φ×(2R1+R2)=2NI,
R2 satisfies the following formula:
A magnetic induction intensity Bc1 generated by an electromagnetic flux in the upper auxiliary air gap is:
A magnetic induction intensity Bc2 generated by an electromagnetic flux in the lower auxiliary air gap is:
A magnetic field in the auxiliary air gap is formed by superposing an electromagnetic field with a part of a permanent magnetic field, and considering an influence of a permanent magnetic flux BY, a magnetic induction intensity B1 generated by a magnetic field in the upper auxiliary air gap satisfies the following calculation formula:
A magnetic induction intensity B2 generated by a magnetic field in the lower auxiliary air gap satisfies the following formula:
In order to eliminate a common-mode interference, the magnetic induction intensity B1 generated by the magnetic field in the upper auxiliary air gap and the magnetic induction intensity B2 generated by the magnetic field in the lower auxiliary air gap are differentiated to obtained that:
According to an inverse solution, the width h of the primary air gap corresponding to the displacement of the rotor to be acquired satisfies the following calculation formula:
The displacement of the rotor in the maglev rotor system is equal to a position of a stator in the maglev rotor system, which is namely a sum of a position of a bearing and the width h of the primary air gap corresponding to the displacement of the rotor, thus acquiring the displacement of the rotor in the maglev rotor system.
Optionally, an amplification factor of the first amplifying circuit U2B may be set based on the following formula:
a=2μ0N(4A2h1+2A1h2),
Specifically, one amplifying branch may be connected to the Hall sensor 20 corresponding to the upper auxiliary air gap, and the other amplifying branch may be connected to the Hall sensor 20 corresponding to the lower auxiliary air gap. For example, the amplifying branch comprising the resistor R8 may be connected to the Hall sensor 20 corresponding to the upper auxiliary air gap, and the amplifying branch comprising the resistor R15 may be connected to the Hall sensor 20 corresponding to the lower auxiliary air gap. The Hall sensors 20 transmit sensed signals of the corresponding auxiliary air gaps to the corresponding amplifying branches respectively, and the second amplifying circuits amplify corresponding currents by a set number of times and then output the amplified currents to the differential circuit U4D. Illustratively, a magnetic induction intensity B (a sum of an electromagnetic induction intensity and a permanent magnetic induction intensity) is detected based on a Hall effect. A Hall voltage U H=KHIHB is obtained through the Hall sensors, wherein KH is a Hall sensitivity, which is related to a material property and a geometric dimension of a Hall sheet, and is a constant for a certain Hall probe; and IH is a supply current to the probe, which is unrelated to the current of the coil. Therefore, it is obtained that:
Illustratively, as shown in
Optionally, the displacement signal resolving circuit 40 may comprise a division circuit and a square rooting circuit. The division circuit is connected to the square rooting circuit, the division circuit is configured to divide an output signal of the current sampling circuit 10 and an output signal of the Hall signal processing circuit 30, and the square rooting circuit is configured for performing offset adjustment and square rooting functions on an output signal of the division circuit.
This result is a negative number.
Specifically, the square rooting circuit may further comprise a reference signal generating circuit, which is namely a circuit shown in the upper right of
Optionally, the offset adjustment value corresponding to the offset adjustment circuit satisfies the following calculation formula:
b=(2A2h1+A1h2)2,
(2A2h1+A1h2)2 is superimposed on the calculation result and then the calculation result is inversely outputted. The calculation result passes through the third filter circuit U7D and then is calculated by the negative voltage square-rooting processing circuit, thus obtaining the width h of the primary air gap corresponding to the displacement of the rotor to be acquired.
Optionally, referring to
In the embodiment of the present disclosure, the current of the coil in the sampling resistor may be obtained by the current sampling circuit 10 and is amplified and filtered. The Hall sensors 20 are placed in the auxiliary air gaps of the permanent-magnet offset maglev rotor system, and the sensing surfaces are perpendicular to the magnetic field directions. In this structure, a variable electromagnetic flux and a part of permanent magnetic flux pass through the auxiliary air gaps, and the part of permanent magnetic flux is a fixed value. The Hall sensors 20 sense the magnetic fields in the air gaps to obtain Hall voltages. After amplification and filtration by the Hall signal processing circuit 30, a magnetic induction intensity of a unilateral air gap is obtained, and then magnetic induction intensities of bilateral air gaps are differentiated to eliminate the common-mode interference caused by the permanent magnetic flux in the auxiliary air gaps. The displacement signal resolving circuit 40 composed of a divider and an open circuit divides a filtered magnetic bearing coil current signal and a differentiated magnetic bearing air gap magnetic induction intensity first, and then a square-rooting operation is performed after offset adjustment to obtain a displacement signal. All functions of a traditional position sensor and a traditional position self-sensing detection method are realized, and meanwhile, there are advantages that the axial size of the rotor is reduced, the detection and the control are coplanar, and high precision and simple design are realized, thus providing conditions for high-precision control by the maglev system.
The embodiment of the present disclosure further provides a maglev rotor displacement self-sensing system. As shown in
It should be noted that relational terms herein such as “first” and “second” and the like, are used merely to distinguish one entity or operation from another entity or operation, and do not necessarily require or imply there is any such relationship or order between these entities or operations. Furthermore, the terms “including”, “comprising” or any variations thereof are intended to embrace a non-exclusive inclusion, such that a process, a method, an article, or a device including a series of elements, includes not only those elements but also includes other elements not expressly listed, or also includes elements inherent to such process, method, article, or device. In the absence of further limitation, an element defined by the phrase “including a . . . ” does not exclude the presence of the same element in the process, method, article, or device.
The above are only specific embodiments of the present disclosure, so that those skilled in the art can understand or realize the present disclosure. Many modifications to these embodiments will be obvious to those skilled in the art, and the general principles defined herein can be implemented in other embodiments without departing from the spirit or scope of the present disclosure. Therefore, the present disclosure will not to be limited to these embodiments shown herein but is to be in conformity with the widest scope consistent with the principles and novel features disclosed herein.
The present disclosure is suitable for detecting the position of the rotor in the permanent magnet offset maglev rotor system with the auxiliary air gap, only the current value of the coil is needed, and the detection by the Hall sensors and the control by the maglev rotor system are coplanar. All functions of a traditional position sensor and a traditional position self-sensing detection method are realized, and meanwhile, there are advantages that the axial size of the rotor is reduced, the detection and the control are coplanar, and high precision and simple design are realized, thus providing conditions for high-precision control by the maglev system, with a very strong industrial practicability.
Number | Date | Country | Kind |
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202010281385.9 | Apr 2020 | CN | national |
Filing Document | Filing Date | Country | Kind |
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PCT/CN2020/104867 | 7/27/2020 | WO |
Publishing Document | Publishing Date | Country | Kind |
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WO2021/203585 | 10/14/2021 | WO | A |
Number | Name | Date | Kind |
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20080143323 | Akahane | Jun 2008 | A1 |
Number | Date | Country |
---|---|---|
101876556 | Nov 2010 | CN |
101931371 | Dec 2010 | CN |
102075131 | May 2011 | CN |
102175131 | Sep 2011 | CN |
102368657 | Mar 2012 | CN |
102545744 | Jul 2012 | CN |
103174746 | Jun 2013 | CN |
104380582 | Feb 2015 | CN |
204179919 | Feb 2015 | CN |
104795958 | Jul 2015 | CN |
204993133 | Jan 2016 | CN |
101802415 | Aug 2018 | CN |
108646571 | Oct 2018 | CN |
108646571 | Oct 2018 | CN |
109067280 | Dec 2018 | CN |
109780985 | May 2019 | CN |
110231133 | Sep 2019 | CN |
110518724 | Nov 2019 | CN |
H0775303 | Mar 1995 | JP |
20150145407 | Dec 2015 | KR |
20160036210 | Apr 2016 | KR |
20170127648 | Nov 2017 | KR |
Entry |
---|
Wang, Xiaoguang et al., “Study on Radial Measuring Method of Axial Displacement of Magnetic Suspension Rotor” China Sciencepaper, vol. 12, No. 16, Aug. 31, 2007, ISSN: 2095-2783, pp. 1805-1809. |
China National Intellectual Property Administration (ISA/CN), International Search Report for PCT/CN2020/104867, dated Jan. 6, 2021, 3 pages. |
China National Intellectual Property Administration (ISA/CN), Written Opinion of the International Searching Authority for PCT/CN2020/104867, dated Jan. 6, 2021, 6 pages. |
Song, Xinda et al., “A Novel Sensorless Rotor Position Detection Method for High-Speed Surface PM Motors in a Wide Speed Range”, IEEE Transactions on Power Electronics, Sep. 2017, 12 pages. |
Wang, Kun et al., “Analysis and Experiment of Self-Differential Eddy-Current Sensor for High-Speed Magnetic Suspension Electric Machine”, IEEE Transactions on Industry Applications, vol. 55, No. 3, May/Jun. 2019, pp. 2538-2547. |
Wang, Kun et al., “Analysis and Experimental Study of a Novel Self-Differential Eddy Current Sensor for High-Speed Magnetic Electrical Machine”, IEEE Xplore, 2017, 6 pages. |
Pesch, Alexander H. et al., “Condition Monitoring of Active Magnetic Bearings on the Internet of Things”, Actuators 2019, www.mdpi.com/journal/actuators, 13 pages. |
Sun, Maolin et al., “Disturbance Force Self-Sensing and Suppression Method for AMB-Rotor System Based on Disturbance Observer”, IEEE Sensors Journal, vol. 20, No. 16, Aug. 15, 2020, pp. 9245-9252. |
Mystkowski, Arkadiusz et al., “Flux measurement and conditioning system for heteropolar active magnetic bearing using Kapton-foil Hall sensors”, Mechanical Systems and Processing, 2019, pp. 394-404. |
Bangcheng, Han, et al., “Loss estimation, thermal analysis, and measurement of a large-scale turbomolecular bump with active magnetic bearings”, The Institution of Engineering and Technology, IET Electr. Power Appl., 2020, vol. 14 Iss 7, pp. 1283-1290. |
Li, Jinlei, et al., “Synchronous Vibration Suppression of Magnetically Suspended Rotor System Using Improved Adaptive Frequency Estimation”, IEEE Sensor Journal, vol. 20, No. 19, Oct. 1, 2020, pp. 11212-11220. |
Feng, et al. “Design and Implementation of Magnetic Suspended Control Moment Gyroscope High-Speed Rotor Driving System,” China Excellent Master's Dissertation Full-text Database Engineering Science and Technology Series II, Mar. 15, 2016, all pages. |
Zhang, et al. “Design and experimental study of a novel self-inductance displacement sensor for active magnetic bearings,” Journal of Instrumentation, Jan. 31, 2018, pp. 100-109, vol. 39, No. 1. |
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20230117718 A1 | Apr 2023 | US |