Active magnetic compensation control system and method based on magnetic field multi-source disturbance suppression
By using the TD-Smith advance estimater and the enhanced model-assisted expansion state observer in the active magnetic compensation control system, the impact of multi-source magnetic field disturbance on cardiocerebral magneto-magnetic measurement is solved, effective suppression of multi-source disturbances is achieved, and measurement accuracy and system stability are improved.
Patent Information
- Application Number
- CN202411801136.2
- Authority / Receiving Office
- CN · China
- Patent Type
- Applications(China)
- Current Assignee / Owner
- Filing Date
- 2024-12-09
- Publication Date
- 2025-03-18
- Estimated Expiration
- 2044-12-09
AI Technical Summary
When facing multi-source magnetic field disturbances, existing active magnetic compensation control systems are difficult to effectively suppress time delays, external magnetic field disturbances, industrial frequency interference, 1/f noise and model mismatch, affecting the accuracy of cardiocerebral magnetism measurement.
The active magnetic compensation control system based on the TD-Smith advance estimator and the enhanced model assisted expansion state observer (AMESO) is adopted to advance the magnetic field sensor output signal through the TD-Smith advance estimator, and the external magnetic field disturbance is estimated using AMESO, combined with the filter equivalent tuning method to suppress multi-source disturbance.
It effectively suppresses the disturbance of multi-source magnetic field in the magnetic shielding device, improves the accuracy of cardio-brain magnetism measurement, provides an extremely weak magnetic field environment for cardio-brain magnetism measurement, and enhances the stability and robustness of the system.
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Figure CN119644860A_ABST
Abstract
Description
Technical Field
[0001] The present invention relates to the technical field of active magnetic field compensation systems, and in particular to an active magnetic compensation control system and method based on magnetic field multi-source disturbance suppression. Background Art
[0002] Magnetic fields are widely used in life. The precise measurement of magnetic fields is becoming increasingly important in the fields of geophysics, materials, and bioinformatics research. The measurement and research of cardiac and brain magnetic signals are becoming more and more in-depth. The intensity of cardiac and brain magnetic signals is about tens of fT to tens of pT, while the magnetic field intensity in the geomagnetic field environment is about 50,000 nT, which is much larger than that of cardiac and brain magnetic signals. In addition, environmental interference, such as the operation of elevators, the operation of CT equipment, the passage of subways and high-speed railways, etc., generates magnetic fields in the order of nT or even uT. Therefore, a magnetic shielding device is needed to shield the geomagnetic field and external interference, and an active magnetic compensation control system is designed to further suppress the influence of magnetic field interference on the magnetic field inside the magnetic shielding device.
[0003] Due to the needs of cardio-cerebral magnetic measurement, the magnetic field strength in the magnetic shielding device must reach the pT or even fT level, so high-precision magnetic field sensors are required for control and measurement, and OPM magnetic field sensors are generally used. The structure and principle of the OPM magnetic field sensor cause time lag in its output signal, which will affect the stability and control effect of the active magnetic compensation control system. The traditional Smith predictor is very easy to become unstable due to model mismatch, and the time lag will also significantly weaken the interference observation ability of the extended state observer. In addition, the circuit noise, 1 / f noise and sensor measurement noise of the control system are inevitable, and the power frequency interference caused by the power supply mode is also inevitable. When the control gain is large, these interferences will enter the system along the control channel and affect the measurement. Therefore, an active magnetic compensation control system and method based on magnetic field multi-source disturbance suppression are of great significance to suppress multi-source disturbances and provide an extremely weak magnetic measurement environment for cardio-cerebral magnetic measurement. Summary of the invention
[0004] In order to solve the above technical problems, the present invention provides an active magnetic compensation control system and method based on multi-source magnetic field disturbance suppression, which can effectively suppress multi-source magnetic field disturbances in the magnetic shielding device and provide an extremely weak magnetic field environment for cardio-cerebral magnetic measurement.
[0005] The present invention provides an active magnetic compensation control system based on magnetic field multi-source disturbance suppression, the system comprising: an ADC acquisition unit, a DAC output unit, a controller, a high-precision current source, a magnetic compensation coil, a magnetic field sensor, a TD-Smith lead predictor, and an enhanced model assisted extended state observer AMESO.
[0006] Preferably, the system as a whole is a closed-loop structure, the enhanced model assisted extended state observer AMESO output z1 is used for negative feedback of closed-loop control, the reference value of the controller is 0, and the error between the controller and the feedback z1 of the enhanced model assisted extended state observer AMESO is used to design the control law to obtain the controller output; the disturbance estimation output z1 of the enhanced model assisted extended state observer AMESO is n+1 Feedforward to the controller output to obtain the final control output.
[0007] Preferably, the magnetic compensation coil is the actuator of the system, which is used to convert the control current into a magnetic field; the final control output is converted into an analog voltage signal through a DAC output unit, and current is applied to the magnetic compensation coil through a high-precision current source to compensate for multi-source disturbances in the magnetic field, so that the magnetic field disturbance measured by the magnetic field sensor is close to 0, providing an extremely weak magnetic environment for cardio-cerebral magnetic measurement.
[0008] The present invention also provides an active magnetic compensation control method based on magnetic field multi-source disturbance suppression, the method is applied to any one of the above systems, and comprises the following steps:
[0009] The signal containing time delay output by the magnetic field sensor is collected by the ADC collection unit;
[0010] The signal with time delay output by the magnetic field sensor is estimated by the TD-Smith advance predictor, wherein the TD advance device performs advance correction on the lagging interference signal;
[0011] The model-assisted extended state observer MESO is tuned by using the filter equivalent tuning method to obtain the enhanced model-assisted extended state observer AMESO.
[0012] The external magnetic field disturbance is estimated by the enhanced model-assisted extended state observer AMESO and fed forward to the controller output to obtain the final control output;
[0013] The final control output applies current to the magnetic compensation coil after passing through the DAC output unit and the high-precision current source, thereby suppressing multi-source disturbances of the magnetic field including time lag, external magnetic field disturbance, power frequency interference, 1 / f noise and model mismatch.
[0014] Preferably, the TD advance device includes a TD tracking differentiator and an advance compensation polynomial, and the TD-Smith advance predictor predicts the signal containing time delay output by the magnetic field sensor, including:
[0015] A basic Smith predictor is established based on the nominal time lag τ0 of the magnetic field sensor and the nominal model G0(s) of the system;
[0016] According to the system noise level and the model mismatch degree, the TD advancer order n and the tracking factor r are selected, and the TD tracking differentiator is used to obtain the 1st to nth order differentials of the disturbance signal with time delay.
[0017] The n-order lead compensation polynomial is used to combine 1-n-order differential polynomials to approximate the lead compensation of the time lag; wherein the lead compensation polynomial is in the form of:
[0018]
[0019] Where s is the Laplace operator, k is the indicator variable of the summation function, k! is the factorial of k, k! = k×(k-1)×(k-2)×...×1;
[0020] The disturbance corrected by the TD advancer and the system output estimated by Smith are added and then transmitted to the enhanced model assisted extended state observer AMESO.
[0021] Preferably, the filter equivalent tuning method is used to tune the model-assisted extended state observer MESO to obtain the enhanced model-assisted extended state observer AMESO, which includes:
[0022] According to the n-order nominal model G0(s), an n+1-order model-assisted extended state observer is established;
[0023] Using the bandwidth tuning method, the gain matrix of the n+1-order model-assisted extended state observer is obtained as L0=[β1 β2 …β n β n+1 ] T ;
[0024] According to the design principle of low-pass filter in disturbance observer, Chebyshev type I filter is selected as the frequency domain equivalent filter of model-assisted extended state observer.
[0025] Choose the appropriate maximum passband attenuation value α max The selection principle is that if the high-frequency measurement noise is large, the maximum passband attenuation value α is increased. max If you want to improve the observer performance, reduce the maximum passband attenuation value α max ;
[0026] According to the determined α max Calculate the passband ripple coefficient
[0027] Select the filter order N+1, which is the same as the order of the model-assisted extended state observer, and select the filter cutoff frequency ω b , which is the same as the observation bandwidth of the model-assisted extended state observer;
[0028] Calculate the N+1 order Chebyshev polynomial P(ω)=cos[(N+1)arccos(ω)], |ω|≤1;
[0029] According to the transfer function of the Chebyshev filter, find the equation The solution s1,s2…s in the left half plane N ,s N+1 , and calculate the polynomial f(s) = (s-s1)(s-s2)…(sS N+1 )=s N+1 +a1s N +…+a N s+a N+1 The coefficients are recorded as correction coefficients a1, a2…a N ,a N+1 ;
[0030] The obtained correction coefficient is used to correct the observer gain matrix to be L = [a1β1 a2β2 … a N β n α N+1 β n+1 ] T , the setting is completed.
[0031] Compared with the prior art, the present invention has the following beneficial effects:
[0032] 1. The present invention adopts pure time delay to characterize the time lag characteristics of the output signal of the magnetic field sensor, which has higher modeling accuracy for the actual system, and adopts the TD-Smith advance predictor to predict the interference signal containing time lag, thereby improving the poor robustness problem of the traditional Smith prediction method.
[0033] 2. The enhanced model-assisted extended state observer designed in the present invention takes into account the model information and uses the output of the TD-Smith advance predictor for estimation, thereby improving the accuracy and real-time degree of disturbance estimation and effectively improving the magnetic field disturbance compensation capability of the active magnetic compensation system.
[0034] 3. The present invention utilizes the filter equivalent tuning method to obtain an enhanced model-assisted extended state observer, which has better suppression capability for high-frequency interference than the traditional bandwidth tuning method, and can improve the signal-to-noise ratio of the measured signal. At the same time, due to the reduction of multi-source disturbances, especially high-frequency noise, the system bandwidth can be further improved, and the response speed and robustness of the system can be improved.
[0035] 4. The present invention can improve the disturbance suppression capability of the magnetic shielding device, realize real-time estimation and suppression of environmental interference, improve the magnetic field stability inside the magnetic shielding device, and improve the signal-to-noise ratio of the measured cardio-cerebral magnetic signals. BRIEF DESCRIPTION OF THE DRAWINGS
[0036] In order to more clearly illustrate the technical solution of the present invention, the following briefly introduces the drawings required for use in the embodiments. Obviously, the drawings described below are only some embodiments of the present invention. For ordinary technicians in this field, other drawings can be obtained based on these drawings without paying creative labor.
[0037] Figure 1 It is a structural schematic diagram of an active magnetic compensation control system and method based on magnetic field multi-source disturbance suppression for a magnetic shielding device according to an embodiment of the present invention;
[0038] Figure 2 A control block diagram of an active magnetic compensation control system and method based on magnetic field multi-source disturbance suppression for a magnetic shielding device according to an embodiment of the present invention;
[0039] Figure 3 The present invention is a flowchart of a filter equivalent tuning method for an active magnetic compensation control system and method based on magnetic field multi-source disturbance suppression for a magnetic shielding device according to an embodiment of the present invention. DETAILED DESCRIPTION
[0040] The following will be combined with the drawings in the embodiments of the present invention to clearly and completely describe the technical solutions in the embodiments of the present invention. Obviously, the described embodiments are only part of the embodiments of the present invention, not all of the embodiments. Based on the embodiments of the present invention, all other embodiments obtained by ordinary technicians in this field without creative work are within the scope of protection of the present invention.
[0041] It should be noted that, unless otherwise defined, the technical terms or scientific terms used in the embodiments of the present disclosure should be understood by people with ordinary skills in the field to which the present disclosure belongs. The "first", "second" and similar words used in the embodiments of the present disclosure do not indicate any order, quantity or importance, but are only used to distinguish different components. "Including" or "comprising" and similar words mean that the elements or objects appearing before the word cover the elements or objects listed after the word and their equivalents, without excluding other elements or objects. "Connect" or "connected" and similar words are not limited to physical or mechanical connections, but can include electrical connections, whether direct or indirect. "Up", "down", "left", "right" and the like are only used to indicate relative positional relationships. When the absolute position of the described object changes, the relative positional relationship may also change accordingly.
[0042] In order to make the above-mentioned objects, features and advantages of the present invention more obvious and easy to understand, the present invention is further described in detail below with reference to the accompanying drawings and specific embodiments.
[0043] Embodiment 1
[0044] The embodiments of the present invention provide Figure 1 As shown, it is a structural schematic diagram of an active magnetic compensation control system based on magnetic field multi-source disturbance suppression provided by an embodiment of the present invention, including an ADC acquisition unit, a DAC output unit, a controller, a high-precision current source, a magnetic compensation coil, a magnetic field sensor, a TD-Smith lead predictor, an enhanced model-assisted extended state observer (AMESO) and a filter equivalent tuning method.
[0045] Among them, the ADC acquisition unit acquires the output signal of the magnetic field sensor. Due to the characteristics of the magnetic field sensor itself, the output signal of the ADC acquisition unit has an inertial link plus time lag characteristics; the TD-Smith lead predictor includes a Smith predictor and a TD lead device, wherein the TD lead device includes a TD tracking differentiator and a lead compensation polynomial. The signal with time lag output by the magnetic field sensor is predicted by the TD-Smith lead predictor to obtain a disturbance and a time-lag-free signal of the magnetic field, wherein the TD lead device performs lead correction on the lagging interference signal; the filter equivalent tuning method is used to adjust the model-assisted extended state observer The AMESO is adjusted to obtain the AMESO; the AMESO estimates the external magnetic field disturbance and feeds forward to the controller output to obtain the final control output (the disturbance estimation signal Zn+1 and the magnetic field estimation signal Z1, Z1 is used as feedback and the difference between it and the target value is obtained to obtain the error which enters the controller to calculate the control quantity, and Zn+1 and the control quantity are added to obtain the final control output); the final control output is given to the high-precision current source through the DAC output unit, and the control current is obtained through the high-precision current source. The control current is passed through the magnetic compensation coil to obtain the compensation magnetic field, thereby realizing the suppression of multi-source disturbances of the magnetic field including time lag, external magnetic field disturbance, power frequency interference, 1 / f noise and model mismatch.
[0046] like Figure 2 As shown, it is a control block diagram of an active magnetic compensation control system based on magnetic field multi-source disturbance suppression provided by an embodiment of the present invention; Figure 3 As shown in FIG. 1 , a flowchart of a filter equivalent tuning method for an active magnetic compensation control system based on magnetic field multi-source disturbance suppression provided by an embodiment of the present invention is shown in FIG. Figure 2 , Figure 3 A specific implementation method is described.
[0047] In the control block diagram, the reference value is 0; C(s) is the controller; G p (s) is the actual model without time delay; G0(s) is the nominal model without time delay; τ pis the time lag of the actual model; τ0 is the time lag of the nominal model; the small box dotted line is the TD advance device, TD is the tracking differentiator, T3(s) is the third-order advance compensation polynomial; the large box dotted line is the TD-Smith advance predictor; AMESO is the second-order enhanced model assisted extended state observer; β1, β2 are the observer gains; a1, a2 are the correction coefficients.
[0048] As an implementation manner of the embodiment of the present invention, the controller C(s) is a linear feedback control law controller, including but not limited to a PID controller.
[0049] As an implementation method of the present invention, the time-delay-free nominal model G0(s) is fitted as a first-order inertial link by frequency sweeping. The model includes but is not limited to a first-order inertial link.
[0050] As an implementation manner of the embodiment of the present invention, the lead compensation polynomial includes but is not limited to a third-order lead compensation polynomial T3(s).
[0051] As an implementation method of the embodiment of the present invention, the AMESO design steps are as follows: Figure 3 As shown, the MESO design steps are as follows:
[0052] ① When time lag is ignored and the model is matched, the input-output relationship of the system is:
[0053] The inverse Laplace transform yields:
[0054] ② Order Then the system state equation is
[0055] ③ Order C=[1 0], then the state equation of the above system can be written as
[0056] ④ According to the above system state equation, MESO is obtained as Model Information It is included in the system matrix A, which can estimate the disturbance more accurately, where L0 is the observer gain matrix and the appropriate observation bandwidth ω is selected. o Setting L0 yields
[0057] As an implementation method of the embodiment of the present invention, the AMESO is further tuned by MESO using a filter equivalent tuning method, and the tuning steps are as follows:
[0058] ①Choose Chebyshev type I filter as the frequency domain equivalent filter of model-assisted extended state observer;
[0059] ② Select the appropriate passband maximum attenuation value α according to the interference level max , according to α max Calculate the passband ripple coefficient
[0060] ③ Select the filter order 2, which is the same as the order of the model-assisted extended state observer, and select the filter cutoff frequency ω b , and the observation bandwidth ω of the model-assisted extended state observer o same;
[0061] ④ Calculate the second-order Chebyshev polynomial P(ω)=cos[2arccos(ω)]=2ω 2 -1,|ω|≤1;
[0062] ⑤Find the equation The solutions S1, S2 in the left half plane and the polynomial f(S) = (S-s1)(s-S2) = s 2 The coefficient of +a1s+a2 is recorded as the correction coefficient a1,a2;
[0063] ⑥Use the correction coefficient obtained in the previous step to correct the observer gain matrix to L = [a1β1a2β2] T , complete the setting and AMESO design.
[0064] As an implementation method of an embodiment of the present invention, the system as a whole is a closed-loop structure, the reference value of the PID controller is 0, and the control law is designed using the error between it and the feedback z1 of MESO to obtain the controller output u0, and the disturbance estimation output z2 of MESO is fed forward to the controller output to obtain the final control output u.
[0065] In summary, the present invention proposes an active magnetic compensation control system based on magnetic field multi-source disturbance suppression, which uses the TD-Smith advance predictor to advance the interference correction and predict the signal, and through the enhanced model-assisted extended state observer and filter equivalent tuning method, it can estimate and compensate for the magnetic field disturbance more accurately and in real time while taking into account the bandwidth. The TD advancer can improve the robustness of Smith and reduce the requirements for model accuracy. This method can improve the stability and robustness of the system, reduce the limitations of multi-source disturbances such as time lag, power frequency interference, and circuit noise on the observer bandwidth, thereby further increasing the bandwidth and improving the response speed, significantly improving the real-time estimation accuracy and compensation suppression capability of external magnetic field disturbances, improving the magnetic field stability inside the magnetic shielding device, and providing an extremely weak magnetic environment for cardio-cerebral magnetic measurement.
[0066] Embodiment 2
[0067] Based on the same inventive concept, corresponding to any of the above-mentioned embodiments and methods, the present disclosure further provides an active magnetic compensation control method based on magnetic field multi-source disturbance suppression, and the method is applied to any of the above-mentioned systems, comprising the following steps:
[0068] The signal containing time delay output by the magnetic field sensor is collected by the ADC collection unit;
[0069] The signal with time delay output by the magnetic field sensor is estimated by the TD-Smith advance predictor, wherein the TD advance device performs advance correction on the lagging interference signal;
[0070] The model-assisted extended state observer MESO is tuned by using the filter equivalent tuning method to obtain the enhanced model-assisted extended state observer AMESO.
[0071] The external magnetic field disturbance is estimated by the enhanced model-assisted extended state observer AMESO and fed forward to the controller output to obtain the final control output;
[0072] The final control output applies current to the magnetic compensation coil after passing through the DAC output unit and the high-precision current source, thereby suppressing multi-source disturbances of the magnetic field including time lag, external magnetic field disturbance, power frequency interference, 1 / f noise and model mismatch.
[0073] In this embodiment, the TD advance device includes a TD tracking differentiator and an advance compensation polynomial, and the TD-Smith advance predictor predicts the signal containing a time delay output by the magnetic field sensor, including:
[0074] A basic Smith predictor is established based on the nominal time lag τ0 of the magnetic field sensor and the nominal model G0(s) of the system;
[0075] According to the system noise level and the model mismatch degree, the TD advancer order n and the tracking factor r are selected, and the TD tracking differentiator is used to obtain the 1st to nth order differentials of the disturbance signal with time delay.
[0076] The n-order lead compensation polynomial is used to combine 1-n-order differential polynomials to approximate the lead compensation of the time lag; wherein the lead compensation polynomial is in the form of:
[0077]
[0078] In the above formula, s is the Laplace operator, k is the indicator variable of the summation function, k! is the factorial of k, and k! = k×(k-1)×(k-2)×...×1. The disturbance corrected by the TD advancer and the system output estimated by Smith are added and transmitted to the enhanced model-assisted extended state observer AMESO.
[0079] In this embodiment, the filter equivalent tuning method is used to tune the model-assisted extended state observer MESO to obtain the enhanced model-assisted extended state observer AMESO, which includes:
[0080] According to the n-order nominal model G0(s), an n+1-order model-assisted extended state observer is established;
[0081] Using the bandwidth tuning method, the gain matrix of the n+1-order model-assisted extended state observer is obtained as L0=[β1 β2 …β n β n+1 ] T ;
[0082] The bandwidth tuning method is used to obtain the n+1-order model-assisted extended state observer gain matrix L0, which is defined as L0 = [β1 β2 … β n β n+1 ] T , where [β1 β2 … β n β n+1 ] T is the observer gain coefficient;
[0083] According to the design principle of low-pass filter in disturbance observer, Chebyshev type I filter is selected as the frequency domain equivalent filter of model-assisted extended state observer.
[0084] Choose the appropriate maximum passband attenuation value α max The selection principle is that if the high-frequency measurement noise is large, the maximum passband attenuation value α is increased. max If you want to improve the observer performance, reduce the maximum passband attenuation value α max ;
[0085] According to the determined α max Calculate the passband ripple coefficient
[0086] Select the filter order N+1, which is the same as the order of the model-assisted extended state observer, and select the filter cutoff frequency ω b , which is the same as the observation bandwidth of the model-assisted extended state observer;
[0087] Calculate the N+1 order Chebyshev polynomial P(ω)=cos[(N+1)arccos(ω)], |ω|≤1;
[0088] According to the transfer function of the Chebyshev filter, find the equation Where j is a complex operator, find the solution s1, s2…s in the left half plane of the equation N ,s N+1 , and calculate the polynomial f(s) = (s-s1)(s-s2)…(ssN+1 )=S N +1 +a1s N +…+a N s+a N+1 The coefficients are recorded as correction coefficients a1, a2…a N ,a N+1 ;
[0089] The obtained correction coefficient is used to correct the observer gain matrix to be L = [a1β1 a2β2 … a N β n a N+1 β n+1 ] T , the setting is completed.
[0090] The method of the above embodiment is used to be applied to a corresponding active magnetic compensation control system based on magnetic field multi-source disturbance suppression in any of the above embodiments, and has the beneficial effects of the corresponding method embodiment, which will not be repeated here.
[0091] The embodiments of the present disclosure are intended to cover all such substitutions, modifications and variations that fall within the broad scope of the appended claims. Therefore, any omissions, modifications, equivalent substitutions, improvements, etc. made within the spirit and principles of the embodiments of the present disclosure should be included in the scope of protection of the present disclosure.
Claims
1. An active magnetic compensation control system based on magnetic field multi-source disturbance suppression, characterized in that: The system comprises: an ADC acquisition unit, a DAC output unit, a controller, a high-precision current source, a magnetic compensation coil, a magnetic field sensor, a TD-Smith advance predictor, and an enhanced model-assisted extended state observer AMESO.
2. The system according to claim 1, characterized in that The overall system is a closed-loop structure. The output z1 of the enhanced model-assisted extended state observer AMESO is used for negative feedback of the closed-loop control. The reference value of the controller is 0. The error between the controller and the feedback z1 of the enhanced model-assisted extended state observer AMESO is used to design the control law to obtain the controller output. The disturbance estimation output z1 of the enhanced model-assisted extended state observer AMESO is n+1 Feedforward to the controller output to obtain the final control output.
3. The system according to claim 1, characterized in that The voltage control quantity output by the controller is converted into an output control current through a high-precision current source. The magnetic compensation coil is the actuator of the system and is used to convert the control current into a magnetic field. The final control output is converted into an analog voltage signal through a DAC output unit. Current is applied to the magnetic compensation coil through a high-precision current source to compensate for multi-source disturbances in the magnetic field, so that the magnetic field disturbance measured by the magnetic field sensor is close to 0, providing an extremely weak magnetic environment for cardio-cerebral magnetic measurement.
4. An active magnetic compensation control method based on magnetic field multi-source disturbance suppression, the method is applied to the system according to any one of claims 1 to 3, characterized in that: The following steps are involved: The signal containing time delay output by the magnetic field sensor is collected by the ADC collection unit; The signal with time delay output by the magnetic field sensor is estimated by the TD-Smith advance predictor, wherein the TD advance device performs advance correction on the lagging interference signal; The model-assisted extended state observer MESO is tuned by using the filter equivalent tuning method to obtain the enhanced model-assisted extended state observer AMESO. The external magnetic field disturbance is estimated by the enhanced model-assisted extended state observer AMESO and fed forward to the controller output to obtain the final control output; The final control output applies current to the magnetic compensation coil after passing through the DAC output unit and the high-precision current source, thereby suppressing multi-source disturbances of the magnetic field including time lag, external magnetic field disturbance, power frequency interference, 1 / f noise and model mismatch.
5. The method according to claim 4, characterized in that The TD advance device includes a TD tracking differentiator and an advance compensation polynomial. The TD-Smith advance predictor predicts the signal with time delay output by the magnetic field sensor and includes: A basic Smith predictor is established based on the nominal time lag τ0 of the magnetic field sensor and the nominal model G0(s) of the system; According to the system noise level and the model mismatch degree, the TD advancer order n and the tracking factor r are selected, and the TD tracking differentiator is used to obtain the 1st to nth order differentials of the disturbance signal with time delay. The n-order lead compensation polynomial is used to combine 1-n-order differential polynomials to approximate the lead compensation of the time lag; wherein the lead compensation polynomial is in the form of: Where s is the Laplace operator, k is the indicator variable of the summation function, k! is the factorial of k, k! = k×(k-1)×(k-2)×...×1; The disturbance corrected by the TD advancer and the system output estimated by Smith are added and then transmitted to the enhanced model assisted extended state observer AMESO.
6. The method according to claim 5, characterized in that Using the filter equivalent tuning method, the model-assisted extended state observer MESO is tuned to obtain the enhanced model-assisted extended state observer AMESO, which includes: According to the n-order nominal model G0(s), an n+1-order model-assisted extended state observer is established; Using the bandwidth tuning method, the gain matrix of the n+1-order model-assisted extended state observer is obtained as L0=[β1 β2 …β n β n+1 ] T ; According to the design principle of low-pass filter in disturbance observer, Chebyshev type I filter is selected as the frequency domain equivalent filter of model-assisted extended state observer. Choose the appropriate maximum passband attenuation value α max The selection principle is that if the high-frequency measurement noise is large, the maximum passband attenuation value α is increased. max If you want to improve the observer performance, reduce the maximum passband attenuation value α max ; According to the determined α max Calculate the passband ripple coefficient Select the filter order N+1, which is the same as the order of the model-assisted extended state observer, and select the filter cutoff frequency ω b , which is the same as the observation bandwidth of the model-assisted extended state observer; Calculate the N+1 order Chebyshev polynomial P(ω)=cos[(N+1)arccos(ω)], |ω|≤1; According to the transfer function of the Chebyshev filter, find the equation The solution in the left half plane is S1,s2…s N ,s N+1 , where j is a complex operator, and calculates the polynomial f(s) = (s-s1)(S-s2)…(ss N+1 )=s N+1 +α1s N +…+a N s+a N+1 The coefficients are recorded as correction coefficients a1, a2…a N ,a N+1 ; The obtained correction coefficient is used to correct the observer gain matrix to be L = [a1β1 a2β2 … a N β n a N+1 β n+1 ] T , the setting is completed.
Citation Information
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