CN111949041A - Elastic vibration suppression method adaptive to large uncertainty frequency - Google Patents

Elastic vibration suppression method adaptive to large uncertainty frequency Download PDF

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CN111949041A
CN111949041A CN202010787613.XA CN202010787613A CN111949041A CN 111949041 A CN111949041 A CN 111949041A CN 202010787613 A CN202010787613 A CN 202010787613A CN 111949041 A CN111949041 A CN 111949041A
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filter
frequency
elastic
frequency range
order
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CN111949041B (en
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奚勇
仲科伟
叶赛仙
陈光山
蒋虎超
郑子元
田野
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Shanghai Aerospace Control Technology Institute
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    • GPHYSICS
    • G05CONTROLLING; REGULATING
    • G05DSYSTEMS FOR CONTROLLING OR REGULATING NON-ELECTRIC VARIABLES
    • G05D1/00Control of position, course or altitude of land, water, air, or space vehicles, e.g. automatic pilot
    • G05D1/08Control of attitude, i.e. control of roll, pitch, or yaw
    • G05D1/0808Control of attitude, i.e. control of roll, pitch, or yaw specially adapted for aircraft
    • G05D1/0816Control of attitude, i.e. control of roll, pitch, or yaw specially adapted for aircraft to ensure stability
    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H21/00Adaptive networks
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02TCLIMATE CHANGE MITIGATION TECHNOLOGIES RELATED TO TRANSPORTATION
    • Y02T90/00Enabling technologies or technologies with a potential or indirect contribution to GHG emissions mitigation

Abstract

The invention discloses an elastic vibration suppression method suitable for large uncertainty frequency, which is based on the first-order elastic frequency range [ omega ] of an aircraft11ω12]Designing two filters in series, filter W11(s) and W12(s) have center frequencies of ω respectively11And ω12By adjusting the filter W11(s) and W12Parameter of(s) at [ omega ]11ω12]A required attenuation factor in the frequency range is met. Aiming at the first-order elastic frequency, the invention adopts a series connection form of double filters in the autopilot to form a notch filter with deeper filtering depth and wider width, thereby realizing stronger filtering effect on the aircraft in a larger uncertain frequency range. The invention can also be applied to the design of second-order and third-order filters of an aircraft, so as toThe effects of wider filtering frequency and larger filtering depth are obtained.

Description

Elastic vibration suppression method adaptive to large uncertainty frequency
Technical Field
The invention relates to the field of elastic vibration suppression of aircrafts, in particular to an elastic vibration suppression method adaptive to large uncertain frequency. The invention is suitable for the aircraft with larger uncertainty of the elastic frequency.
Background
The elastic vibration suppression is an important content of the design of the automatic pilot of the aircraft, can improve the stability of the system, provides a good working environment for the subsystem and the single machine to which the automatic pilot belongs, and ensures the reliable operation of the system.
The source of autopilot high frequency noise is primarily the aircraft's own elastic vibrations. For example, in the case of missiles, the positions of the missile cable covers cause the difference of elastic frequencies in the Y direction and the Z direction, and the elastic frequencies of every missile in mass production also have the difference. This requires a control system with strong elastic vibration suppression capability over a large uncertainty frequency range.
According to the traditional filter design method, a notch filter is designed aiming at a first-order elastic frequency range, a frequency point is selected as a center frequency in a compromise mode, the elastic frequency deviates from the center frequency of the filter due to the fact that the elastic frequency has large uncertainty, and the filtering effect is obviously reduced.
According to the technical scheme, aiming at the first-order elastic frequency, a trap filter with deeper filtering depth and wider width is formed by adopting a series connection form of double filters in the autopilot, and a stronger filtering effect is achieved in a larger uncertain frequency range of the aircraft.
Disclosure of Invention
The invention aims to provide an elastic vibration suppression method suitable for large uncertainty frequency, aiming at the large uncertainty of the elastic frequency of an aircraft and achieving a strong filtering effect in a large uncertainty frequency range of the aircraft. The invention ensures stronger filtering effect in a wider frequency range by adopting a series connection form of the double filters.
In order to achieve the above object, the present invention provides an elastic vibration suppression method for large uncertainty frequency according to the first order elastic frequency range [ ω ] of the aircraft11ω12]Designing two filters in series, filter W11(s) and W12(s) have center frequencies of ω respectively11And ω12By adjusting the filter W11(s) and W12Parameter of(s) at [ omega ]11ω12]A required attenuation factor in the frequency range is met.
The elastic vibration suppression method for large uncertainty frequency is characterized in that the filter W is a filter with a frequency band of a large uncertainty11(s) and W12The formula of(s) is as follows:
Figure BDA0002622586440000021
Figure BDA0002622586440000022
in the formula, Tn11、Td11Is a deterministic structure filter W11(s) parameter of center frequency, ξn11、ξd11Is a deterministic structure filter W11(s) parameters of notch width and depth; t isn12、Td12Is a deterministic structure filter W12(s) parameter of center frequency, ξn12、ξd12Is a deterministic structure filter W12(s) parameters of notch width and depth.
The elastic vibration suppression method for large uncertainty frequency is characterized in that the filter W is a filter with a frequency band of a large uncertainty11(s) has a depth and width not greater than the filter W12(s), the filter parameters satisfy the following formula:
ξd11≤ξd12
Figure BDA0002622586440000023
the elastic vibration suppression method for large uncertainty frequency is characterized in that the filter W is adjusted11(s) and W12(s) has a parameter in [ omega ]11ω12]The required attenuation factor in the frequency range is given by the formula:
A1111)+A1211)<K
A1112)+A1212)<K
in the formula: a. the1111) Is a filter W11(s) at ω11Amplitude in dB; a. the1212) Is a filter W12(s) at ω12Amplitude in dB; k is the desired attenuation amplitude, K<0, unit: dB.
Compared with the prior art, the invention has the technical beneficial effects that:
(1) and a double-filter series connection mode is adopted, so that compared with a single notch filter mode, the filtering depth near the first-order modal frequency is improved.
(2) The method can also be applied to the design of second-order and third-order filters of the aircraft to obtain the effects of wider filtering frequency and larger filtering depth.
(3) Due to the notch filter W11The center frequency of(s) is relatively low, the influence on the stability margin is large, and the designed depth and width are not more than the filter W12And(s) depth and width to reduce the influence of the filter on the rigid stability margin and improve the system stability margin.
Drawings
The elastic vibration suppression method adapted to large uncertainty frequency of the present invention is provided by the following embodiments and the accompanying drawings.
FIG. 1 shows a filter W11(s) bode plot;
FIG. 2 shows a filter W12(s) bode plot;
FIG. 3 is a Bode plot of two filters in series;
fig. 4 is a diagram comparing the present invention with a conventional single filter scheme.
Detailed Description
An elastic vibration suppression method for large uncertainty frequency according to the present invention will be described in further detail with reference to the accompanying drawings.
The implementation steps of the method are explained by taking a certain aircraft as an example:
the first-order modal frequency of a certain aircraft is assumed as the following table, the filtering depth is required to be more than-30 dB within the range of 35 Hz-40 Hz, the filtering effect is improved as much as possible near the first-order modal frequency, and the method is suitable for the difference of various aircrafts of the same model in the production process.
TABLE 1 aircraft modal frequencies
Modal frequency First order modal frequency
In the Y direction 35Hz
In the Z direction 40Hz
(1) According to aircraft first order elastic frequency range [3540 ]]Designing two filters in series, filter W11(s) and W12The center frequencies of(s) are 35Hz and 40Hz, respectively, for example, using the following parameters, as shown in fig. 1 and 2, and the filter center frequencies are 35Hz and 40Hz, respectively.
Figure BDA0002622586440000041
Figure BDA0002622586440000042
In the formula:
Figure BDA0002622586440000043
Figure BDA0002622586440000044
Figure BDA0002622586440000045
Figure BDA0002622586440000046
(2) designing a filter W11The depth of filtering at the center frequency of(s) is about-17 dB (as in FIG. 1), design W12The depth of filtering at the center frequency of(s) is about-20 dB (as in fig. 2), and the filter parameters are as follows:
ξn11=0.1
ξd11=0.7
ξn12=0.1
ξd12=1.1
(3) filter W11(s) and W12(s) are connected in series, and the attenuation at 35Hz to 40Hz exceeds-30 dB (shown in figure 3). Compared with the conventional single filter, it can be seen that the filtering width around the first order frequency is significantly better than that of the single filter scheme (as shown in fig. 4) in the dual-filter scheme of the present invention, and the filtering effect is shown in table 2.
For example, the actual Z-direction first-order modal frequency of a certain aircraft is 45Hz, and has a difference with a design value, the filtering effect of the double-filter series connection scheme is-25.8 dB, and the filtering effect of the single-filter scheme is only 18.8 dB. The dual filter series scheme is more adaptive to modal frequency uncertainty.
TABLE 2 Filter Effect comparison
Scheme(s) The invention relates to a series connection scheme of double filters Single filter scheme
-30dB frequency range 33Hz~42Hz 35Hz~38.7Hz
-20dB frequency range 28.5Hz~49.5Hz 30.5Hz~44Hz
The invention can also be used for designing second-order and third-order filters.
Those skilled in the art will appreciate that those matters not described in detail in the present specification are well known in the art.
Although the present invention has been described with reference to the preferred embodiments, it is not intended to limit the present invention, and those skilled in the art can make variations and modifications of the present invention without departing from the spirit and scope of the present invention by using the methods and technical contents disclosed above.

Claims (4)

1. An elastic vibration suppression method adapting to large uncertainty frequency is characterized in that according to a first-order elastic frequency range of an aircraftEnclose [ omega ]11 ω12]Designing two filters in series, filter W11(s) and W12(s) have center frequencies of ω respectively11And ω12By adjusting the filter W11(s) and W12Parameter of(s) at [ omega ]11 ω12]A required attenuation factor in the frequency range is met.
2. The method of claim 1, wherein the filter W is adapted to suppress elastic vibrations at frequencies of large uncertainty11(s) and W12The formula of(s) is as follows:
Figure FDA0002622586430000011
Figure FDA0002622586430000012
in the formula, Tn11、Td11Is a deterministic structure filter W11(s) parameter of center frequency, ξn11、ξd11Is a deterministic structure filter W11(s) parameters of notch width and depth; t isn12、Td12Is a deterministic structure filter W12(s) parameter of center frequency, ξn12、ξd12Is a deterministic structure filter W12(s) parameters of notch width and depth.
3. The method of claim 1, wherein the filter W is adapted to suppress elastic vibrations at frequencies of large uncertainty11(s) has a depth and width not greater than the filter W12(s), the filter parameters satisfy the following formula:
ξd11≤ξd12
Figure FDA0002622586430000013
4. the method of claim 1, wherein said step of adjusting the filter W is performed by adjusting the filter W11(s) and W12(s) has a parameter in [ omega ]11ω12]The required attenuation factor in the frequency range is given by the formula:
A1111)+A1211)<K
A1112)+A1212)<K
in the formula: a. the1111) Is a filter W11(s) at ω11Amplitude in dB; a. the1212) Is a filter W12(s) at ω12Amplitude in dB; k is the desired attenuation amplitude, K<0, unit: dB.
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CN114415509A (en) * 2022-01-11 2022-04-29 西北工业大学 Servo elastic active suppression method for remote rocket projectile

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Publication number Priority date Publication date Assignee Title
CN114415509A (en) * 2022-01-11 2022-04-29 西北工业大学 Servo elastic active suppression method for remote rocket projectile
CN114415509B (en) * 2022-01-11 2023-04-28 西北工业大学 Servo elastic active inhibition method for remote rocket projectile

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