CN111948624A - Tracking control method and system for non-road mobile pollution source detection laser radar - Google Patents

Tracking control method and system for non-road mobile pollution source detection laser radar Download PDF

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CN111948624A
CN111948624A CN202010733295.9A CN202010733295A CN111948624A CN 111948624 A CN111948624 A CN 111948624A CN 202010733295 A CN202010733295 A CN 202010733295A CN 111948624 A CN111948624 A CN 111948624A
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scanning mechanism
joint
sliding mode
angle
laser radar
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康宇
杨钰潇
卢峻森
陈才
吕文君
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University of Science and Technology of China USTC
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University of Science and Technology of China USTC
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S7/00Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/48Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S17/00
    • G01S7/481Constructional features, e.g. arrangements of optical elements
    • G01S7/4817Constructional features, e.g. arrangements of optical elements relating to scanning
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S17/00Systems using the reflection or reradiation of electromagnetic waves other than radio waves, e.g. lidar systems
    • G01S17/88Lidar systems specially adapted for specific applications
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S7/00Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/48Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S17/00

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Abstract

The invention discloses a tracking control method and a tracking control system for a non-road mobile pollution source detection laser radar, which utilize a DH modeling method and a base B0Azimuth rotary joint B1And roll rotary joint B2As joint points, respectively establishing joint coordinate systems; establishing a joint rotation angle-moment dynamics equation of the scanning mechanism according to the established joint coordinate system and the power parameters of the scanning mechanism; constructing an integral sliding mode surface by taking the difference value of the expected angle and the actual angle of the joint angle of the scanning mechanism as a tracking error; constructing a sliding mode angle controller by utilizing an integral sliding mode surface and a differentiator to adjust the actual rotating angle of the joint of the scanning mechanism to obtain the torque applied to the scanning mechanism by a motor, thereby realizing the detection of the laser mine on the pollution sourceAnd (4) achieving second-order integral sliding mode tracking control. Compared with the traditional method, the scheme has higher tracking performance and smaller energy consumption.

Description

Tracking control method and system for non-road mobile pollution source detection laser radar
Technical Field
The invention relates to the technical field of atmospheric pollution emission detection, in particular to a tracking control method and a tracking control system for a non-road mobile pollution source detection laser radar.
Background
At present, the atmospheric environment situation of China is severe, the total pollutant emission is large, and the regional atmospheric environment problem taking fine particles as characteristic pollutants is increasingly prominent. The frequently occurring problem of regional atmospheric pollution such as dust haze is closely related to the substandard emission of tail gas of urban mobile pollution sources such as motor vehicles, engineering vehicles and ships. The pollution of mobile sources has become one of the most prominent and urgent problems in the air pollution problem in China.
In the aspect of emission monitoring of non-road mobile pollution sources such as ships and the like, because an optical reflection device cannot be installed, a passive scanning observation system, namely an atmospheric pollution measurement laser radar, is adopted, and concentration information of atmospheric components is acquired by emitting laser with specific wavelength into the atmosphere and collecting and analyzing a scattering spectrum after the scattering spectrum and an atmospheric medium have physical action.
However, this monitoring and analyzing method has drawbacks in that: firstly, the measurement optical path distance is long, and the area of a monitoring area is small, so that the self-positioning of an observation target is very difficult; secondly, in the follow-up process of the observation system, the micro vibration can bring about great detection errors, and the anti-interference capability is poor.
Disclosure of Invention
The invention aims to overcome the defects in the prior art so as to improve the anti-interference capability to the external environment and quickly and stably track a target.
In order to realize the aim, the invention adopts a tracking control method of a non-road mobile pollution source detection laser radar, and a scanning mechanism of the pollution source detection laser radar comprises a base B0Azimuth rotary joint B1And roll rotary joint B2A base B0Azimuth rotary joint B1And roll rotary joint B2In turn, rotationally coupled, the method comprising:
using a DH modeling method toBase B0Azimuth rotary joint B1And roll rotary joint B2As joint points, respectively establishing joint coordinate systems;
establishing a joint rotation angle-moment dynamics equation of the scanning mechanism according to the established joint coordinate system and the power parameters of the scanning mechanism;
constructing an integral sliding mode surface by taking the difference value of the expected angle and the actual angle of the joint angle of the scanning mechanism as a tracking error;
and constructing a sliding mode angle controller by utilizing an integral sliding mode surface and a differentiator to adjust the actual rotating angle of the joint of the scanning mechanism, so as to obtain the moment applied to the scanning mechanism by the motor and realize the second-order integral sliding mode tracking control of the pollution source detection laser radar.
Further, the integral slip form surface of the construction is:
Figure BDA0002604012940000021
wherein λ is1And λ2And a proportional coefficient and an integral coefficient diagonal matrix respectively representing the sliding mode control rate, wherein beta is a constant coefficient, e is a tracking error, sign () is a sign function, and is 1 when the sign () is greater than 0 and is-1 when the sign () is less than 0.
Further, the method includes the steps of constructing a sliding mode angle controller by using an integral sliding mode surface and a differentiator to adjust the actual rotation angle of the joint of the scanning mechanism, obtaining the moment applied to the scanning mechanism by a motor, and realizing second-order integral sliding mode tracking control of the pollution source detection laser radar, and includes the following steps:
calculating the angular velocity and the angular acceleration of the joint rotation of the scanning mechanism by using a differentiator;
and constructing a sliding mode angle controller by utilizing the integral sliding mode surface, the rotating angular speed and the angular acceleration of the joint of the scanning mechanism so as to adjust the actual rotating angle of the joint of the scanning mechanism and obtain the moment applied to the scanning mechanism by the motor.
Further, the formula for calculating the angular velocity and the angular acceleration of the joint rotation of the scanning mechanism by using the differentiator is as follows:
Figure BDA0002604012940000022
wherein Σ is a differentiator parameter and satisfies
Figure BDA0002604012940000023
The input of the differentiator is the actual angle q of the joint angle of the scanning mechanism, and the output psi of the differentiator0,ψ1,ψ2Are used to estimate the q-values respectively,
Figure BDA0002604012940000024
record as
Figure BDA0002604012940000031
Further, the sliding mode angle control rule of the sliding mode angle controller is as follows:
Figure BDA0002604012940000032
wherein the content of the first and second substances,
Figure BDA0002604012940000033
representing the first derivative of the sliding mode surface s,
Figure BDA0002604012940000034
representing said desired angle qdSecond derivative of (a)1i2i,eiRespectively represent matrices lambda12And the ith diagonal element of matrix e,
Figure BDA0002604012940000035
is the second differential of q, K1,K2Is a constant coefficient diagonal matrix, U (t-t)d) Represents tdThe moment applied to the scanning mechanism by the motor before the moment, U (t) representing time tTorque applied to the scanning mechanism by the stepper motor.
Further, the
Figure BDA0002604012940000036
β=0.6,Σ=42,
Figure BDA0002604012940000037
Further, the establishing of the joint rotation angle-moment dynamics equation of the scanning mechanism according to the established joint coordinate system and the dynamic parameters of the scanning mechanism includes:
establishing a positive kinematic equation of the laser radar scanning mechanism according to the DH parameters corresponding to the joint coordinate system;
and establishing a joint rotation angle-moment dynamics equation of the scanning mechanism according to the positive kinematics equation of the laser radar scanning mechanism and the power parameters of the laser radar scanning mechanism.
Further, the establishing of the joint rotation angle-moment dynamics equation of the scanning mechanism according to the positive kinematics equation of the lidar scanning mechanism and the dynamic parameters of the lidar scanning mechanism includes:
based on a positive kinematic equation of the laser radar scanning mechanism, performing forward iteration and backward iteration by using a Newton-Euler method to obtain a joint rotation angle-moment dynamic model of the laser radar scanning mechanism;
and substituting the dynamic parameters of the laser radar scanning mechanism into the joint rotation angle-moment dynamic model to obtain the moment-joint angle dynamic equation.
In a second aspect, a tracking control system for a non-road mobile pollution source detection laser radar is provided, which comprises a pollution source detection laser radar scanning mechanism and a controller, wherein the scanning mechanism comprises a base B0Azimuth rotary joint B1And roll rotary joint B3A base B0Azimuth rotary joint B1And roll rotary joint B2Are connected in turn in a rotating way, and the controller comprises a coordinate system establishing moduleThe system comprises a dynamic equation establishing module, an integral sliding mode surface constructing module and a second-order integral sliding mode tracking control module, wherein:
the coordinate system establishment module is used for utilizing a DH modeling method and using a base B0Azimuth rotary joint B1And roll rotary joint B2As joint points, respectively establishing joint coordinate systems;
the dynamic equation establishing module is used for establishing a joint rotation angle-moment dynamic equation of the scanning mechanism according to the established joint coordinate system and the power parameters of the scanning mechanism;
the integral sliding mode surface construction module is used for constructing an integral sliding mode surface by taking the difference value between the expected angle and the actual angle of the joint angle of the scanning mechanism as a tracking error;
and the second-order integral sliding mode tracking control module is used for constructing a sliding mode angle controller by utilizing an integral sliding mode surface and a differentiator so as to adjust the actual rotating angle of the joint of the scanning mechanism, obtain the moment applied to the scanning mechanism by the motor and realize the second-order integral sliding mode tracking control of the pollution source detection laser radar.
In a third aspect, there is provided a computer readable storage medium comprising a computer program for use in conjunction with a storage device, the computer program for execution by a processor, comprising:
using DH modeling method with base B0Azimuth rotary joint B1And roll rotary joint B2As joint points, respectively establishing joint coordinate systems;
establishing a joint rotation angle-moment dynamics equation of the scanning mechanism according to the established joint coordinate system and the power parameters of the scanning mechanism;
constructing an integral sliding mode surface by taking the difference value of the expected angle and the actual angle of the joint angle of the scanning mechanism as a tracking error;
and constructing a sliding mode angle controller by utilizing an integral sliding mode surface and a differentiator to adjust the actual rotating angle of the joint of the scanning mechanism, so as to obtain the moment applied to the scanning mechanism by the motor and realize the second-order integral sliding mode tracking control of the pollution source detection laser radar.
Compared with the prior art, the invention has the following technical effects: according to the invention, on the basis of a dynamic equation of the laser radar scanning mechanism, an integral terminal sliding mode surface is constructed by utilizing a difference value between an expected angle and an actual angle of each joint angle of a positioning platform, and a second-order sliding mode control rule is designed to adjust the angle of the actual joint angle according to the integral terminal sliding mode surface and a differentiator, so that a moment value is obtained, and the system state of the laser radar scanning mechanism is tracked. According to the scheme, the problems of flutter and noise sensitivity at the arrival stage are solved by adopting second-order integral sliding mode control, the uncertainty of the dynamics of a laser radar scanning system is eliminated, the robustness of the system is improved, the laser radar can track a target quickly, accurately and stably, the control cost is reduced, and the control efficiency is improved.
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The following detailed description of embodiments of the invention refers to the accompanying drawings in which:
FIG. 1 is a schematic flow diagram of a tracking control method for a non-road mobile pollution source detection lidar;
FIG. 2 is a structural diagram of a ship exhaust gas monitoring lidar provided by the embodiment;
FIG. 3 is a centroid diagram of the ship exhaust gas monitoring lidar provided by the embodiment;
FIG. 4 is a D-H link coordinate system diagram of the scanning mechanism of the laser radar for monitoring ship exhaust gas according to the present embodiment;
fig. 5 is a schematic block diagram of a second-order integral sliding mode tracking control method provided in this embodiment.
Detailed Description
To further illustrate the features of the present invention, refer to the following detailed description of the invention and the accompanying drawings. The drawings are for reference and illustration purposes only and are not intended to limit the scope of the present disclosure.
As shown in FIG. 1, the present embodiment discloses a tracking method for a non-road mobile pollution source detection lidar, the scanning of whichThe tracing mechanism comprises a base B0Azimuth rotary joint B1And roll rotary joint B2A base B0Azimuth rotary joint B1And roll rotary joint B2In turn rotatably connected, the method comprising the steps S1 to S4:
s1, using DH modeling method, using base B0Azimuth rotary joint B1And roll rotary joint B2As joint points, respectively establishing joint coordinate systems;
s2, establishing a joint rotation angle-moment dynamic equation of the scanning mechanism according to the established joint coordinate system and the power parameters of the scanning mechanism;
s3, constructing an integral sliding mode surface by taking the difference value between the expected angle and the actual angle of the joint angle of the scanning mechanism as a tracking error;
s4, constructing a sliding mode angle controller by utilizing an integral sliding mode surface and a differentiator to adjust the actual rotating angle of the scanning mechanism joint, obtaining the moment applied to the scanning mechanism by a motor, and realizing the second-order integral sliding mode tracking control of the pollution source detection laser radar.
Specifically, non-road mobile pollution source monitoring includes the emission monitoring of non-road mobile pollution sources such as boats and ships, and laser radar uses boats and ships exhaust gas monitoring laser radar to introduce as an example in this embodiment:
as shown in fig. 2 to 3, the laser radar for monitoring exhaust gas from a ship mainly includes: base B0Azimuth rotation member B1With the roll-rotating member B2Said base B0Azimuth rotation member B1With the roll-rotating member B2Are connected in turn.
As shown in FIG. 4, in the step S1, a D-H link coordinate system is established by the method of Denavit-Hartenberg (DH). Is a base B0Azimuth rotation member B1With the roll-rotating member B2Respectively constructing a coordinate system which is marked as a coordinate system 0, a coordinate system 1 and a coordinate system 2, and respectively marking the original points of the three coordinate systems as O0、O1And O2(ii) a Base B0Azimuth rotation member B1Hewei (Chinese character of 'Hewei')Rolling component B2Respectively, is recorded as S0、S1And S2(ii) a The azimuth angle and the roll angle of the non-road mobile pollution source monitoring laser radar are respectively recorded as theta1And theta2(ii) a Motor applied to azimuth rotary member B1And a roll rotating member B2Respectively is recorded as tau1And τ2;O0And O1Is recorded as d1;O1And O2Is recorded as d2
According to the D-H method, the DH parameter table corresponding to the D-H connecting rod coordinate system constructed in this embodiment is shown in Table 1.
TABLE 1 DH parameters table
Figure BDA0002604012940000061
Wherein the connecting rod 1 is B1And B1Upper drive B2The connecting rod 2 is B2,aiIs an axis ziAnd zi-1The length of the male perpendicular line of (a); alpha is alphaiIs an axis zi-1And ziWhen the angle between them is around the axis xiPositive when rotating anticlockwise; diIs an axis ziAnd zi-1The common vertical line and zi-1Along z of the intersection pointi-1Length of (d); thetaiIs an axis xi-1And xiWhen the angle between them is around the axis zi-1Counterclockwise rotation is positive.
In the embodiment of the present invention, the i-0, 1,2 coordinate system i is attached to the link i and moves together with the link i, but the coordinate system 0 is fixed, and when i-0, the link i can be understood as a base.
Specifically, in the above step S2, the joint rotation angle-moment dynamics equation of the scanning mechanism is established according to the established joint coordinate system and the power parameter of the scanning mechanism, and the method includes the following sub-steps S21 to S22:
and S21, establishing a positive kinematic equation of the laser radar scanning mechanism according to the DH parameters corresponding to the joint coordinate system. The method specifically comprises the following steps:
and performing kinematic analysis on the non-road mobile pollution source monitoring laser radar according to a DH parameter table corresponding to the D-H connecting rod coordinate system, and establishing a positive kinematic equation to express as follows:
Figure BDA0002604012940000071
wherein the content of the first and second substances,
Figure BDA0002604012940000072
representing a homogeneous transformation matrix from coordinate system 0 to coordinate system 1;
Figure BDA0002604012940000073
represents cos θ1、cosθ2
Figure BDA0002604012940000074
Denotes sin θ1、sinθ2
Figure BDA0002604012940000075
Representing a one-step homogeneous transformation matrix from coordinate system 0 to coordinate system 1;
Figure BDA0002604012940000077
representing a one-step homogeneous transformation matrix of coordinate system 1 to coordinate system 2.
And S22, establishing a joint rotation angle-moment dynamics equation of the scanning mechanism according to the positive kinematics equation of the laser radar scanning mechanism and the power parameters of the laser radar scanning mechanism. The method specifically comprises the following steps:
deducing a dynamic model by using the result of the step S21 to obtain a corresponding forward recursion formula and a backward recursion formula; in addition, in order to make the calculation convenient, it is necessary to order
Figure BDA0002604012940000076
These vectors or matrices are constant and therefore cannot use the ground-fixed coordinate system, but rather the individual link coordinate systems, which require rotations in positive kinematic equations in the recursion formulaThe transformation matrix transforms the calculated intermediate vector into a coordinate system, which is as follows:
according to the Newton-Euler method, the forward recursion formula is:
Figure BDA0002604012940000081
Figure BDA0002604012940000082
Figure BDA0002604012940000083
Figure BDA0002604012940000084
wherein, i is 0,1,2,
Figure BDA00026040129400000824
is represented by BiThe angular velocity of (a) of (b),
Figure BDA0002604012940000085
a unit vector representing the z-axis direction of the coordinate system i,
Figure BDA0002604012940000086
represents OiAcceleration of (O)iRepresents the origin of a coordinate system that moves with the connecting rod, but coordinate system 0 is stationary;
Figure BDA0002604012940000087
denotes SiThe acceleration of (a) is detected,
Figure BDA0002604012940000088
representing a vector
Figure BDA0002604012940000089
Indicating motorAngular acceleration of the rotor, kriIn order to reduce the gear ratio,
Figure BDA00026040129400000810
a unit vector which is the direction of the rotor rotating shaft;
Figure BDA00026040129400000811
respectively represent thetaiFirst derivative with respect to time,
Figure BDA00026040129400000812
First derivative with respect to time, thetaiSecond derivative with respect to time.
The backward recursion formula is:
Figure BDA00026040129400000813
Figure BDA00026040129400000814
Figure BDA00026040129400000815
wherein the content of the first and second substances,
Figure BDA00026040129400000816
represents the force applied by the connecting rod i-1 to the connecting rod i, miIs represented by BiThe mass of (a) of (b),
Figure BDA00026040129400000817
representing the link i-1 to the link i with respect to the origin O of the coordinate system i-1i-1The moment of force of (a) is,
Figure BDA00026040129400000818
representing a vector
Figure BDA00026040129400000819
Is represented by BiInertia tensor with respect to coordinate system iThe matrix of quantities is then used to determine,
Figure BDA00026040129400000820
representing the moment of inertia, tau, of the rotor about the axis of rotationiIs composed of
Figure BDA00026040129400000821
The component on the z-axis of the coordinate system i, i.e. the moment.
In the present embodiment, the link 0 is assumed to be the base B0Where i is also in the range of 0 to 2, and is not calculated
Figure BDA00026040129400000822
Since it has no meaning, appear
Figure BDA00026040129400000823
An intermediate quantity with an index of 3 (i.e., index i +1 when i ═ 2) is defaulted to 0.
Carrying out derivation on parameters of the laser radar scanning mechanism for monitoring the non-road mobile pollution source to obtain a matrix form of a dynamic model of the laser radar scanning mechanism:
Figure BDA0002604012940000091
wherein τ ═ (τ)1τ2)T,q=(θ1 θ2)T
Figure BDA0002604012940000092
Respectively a first derivative and a second derivative of q to time; m (q) is a generalized inertia matrix,
Figure BDA00026040129400000911
the matrix of centripetal and Coriolis forces, G (q) is gravity, G (q), and d is external disturbance.
For example, suppose the parameters of the non-road mobile pollution source monitoring lidar scanning mechanism are: m is1=100,m2=46.5,r0,1=0.18,r1,2=0.4,
Figure BDA0002604012940000093
Figure BDA0002604012940000094
The above are coordinates in the current link coordinate system; the dynamic equation of the laser radar scanning mechanism is as follows:
Figure BDA0002604012940000095
Figure BDA0002604012940000096
Figure BDA0002604012940000097
Figure BDA0002604012940000098
Figure BDA0002604012940000099
specifically, in step S3, the integral sliding mode surface of the structure is:
Figure BDA00026040129400000910
wherein λ is1And λ2And a proportional coefficient and an integral coefficient diagonal matrix respectively representing the sliding mode control rate, wherein beta is a constant coefficient, e is a tracking error, sign () is a sign function, and is 1 when the sign () is greater than 0 and is-1 when the sign () is less than 0.
Further, the above step S4: constructing a sliding mode angle controller by utilizing an integral sliding mode surface and a differentiator to adjust the actual rotation angle of the joint of the scanning mechanism to obtain the moment applied to the scanning mechanism by a motor, and realizing the second-order integral sliding mode tracking control of the pollution source detection laser radar, wherein the method comprises the following subdivision steps S41 to S42:
s41, calculating the angular speed and the angular acceleration of the joint rotation of the scanning mechanism by using a differentiator;
it should be noted that, in order to solve the problem that the angular velocity and the angular acceleration of the joint rotation of the laser radar scanning mechanism cannot be directly measured in practice, a differentiator is added to solve the problem, and the form is as follows:
Figure BDA0002604012940000101
wherein Σ is a differentiator parameter and satisfies
Figure BDA0002604012940000102
The differentiator has an input of q and an output of psi0,ψ1,ψ2Are used to estimate the q-values respectively,
Figure BDA0002604012940000103
record as
Figure BDA0002604012940000104
Then the differentiator can obtain the first and second order differentials of q within a finite time, i.e.
Figure BDA0002604012940000105
Figure BDA0002604012940000106
S42, constructing a sliding mode angle controller by using the integral sliding mode surface, the rotating angular speed and the angular acceleration of the joint of the scanning mechanism to adjust the actual rotating angle of the joint of the scanning mechanism, and obtaining the moment applied to the scanning mechanism by the motor.
Specifically, the sliding mode angle control law of the sliding mode angle controller is as follows:
Figure BDA0002604012940000107
wherein the content of the first and second substances,
Figure BDA0002604012940000108
representing the first derivative of the sliding mode surface s,
Figure BDA0002604012940000109
representing said desired angle qdSecond derivative of (a)1i2i,eiRespectively represent matrices lambda12And matrix e and the ith diagonal element of (1)iThe (i) th element of (a),
Figure BDA00026040129400001010
is the second differential of q, K1,K2Is a constant coefficient diagonal matrix, U (t-t)d) Represents tdThe moment applied to the scanning mechanism by the motor before the time, u (t), represents the moment applied to the scanning mechanism by the motor at the time.
As shown in fig. 5, the second-order integral sliding mode controller can obtain a moment U applied to the laser radar scanning mechanism, i.e., τ in the dynamic model equation, and then obtain a corresponding actual angle q according to calculation, so as to implement closed loop, and further control two rotating devices (azimuth rotating component B)1With the roll-rotating member B2) The method can realize the second-order integral sliding mode tracking control of the non-road mobile pollution source monitoring laser radar.
It should be noted that, in the embodiment, by adopting the second-order integral sliding mode control, the problems of flutter and noise sensitivity at the arrival stage are eliminated, the robustness of the system is improved, and the tracking speed and transient performance are improved. And due to the uncertainty of the dynamics of the laser radar scanning mechanism, t is introduced by adopting time delay estimation in the embodimentdMoment U (t-t) applied to laser radar scanning mechanism by motor before momentd) To eliminate the nonlinearity and uncertainty of system dynamics, such as parameter variation and interference, so that the sliding mode is independent of the system modeThe target can be tracked quickly, accurately and stably, and compared with the traditional method, the scheme of the embodiment has higher tracking performance and smaller energy consumption.
Preferably, in the selection of the parameters, the embodiment of the invention provides a group of better performance schemes by adjusting the parameters:
Figure BDA0002604012940000111
β=0.6,Σ=42,
Figure BDA0002604012940000112
Figure BDA0002604012940000113
when the set of parameters is selected, the system has smaller adjusting time and steady-state error under the proposed second-order integral sliding mode control method, and can realize better tracking performance of the angle of the rotating device.
It should be noted that, in this embodiment, compared with the scheme described in the chinese patent application publication No. CN110007599A, the sliding mode surfaces of the two control methods are different in selection, and the selection form of the sliding mode surface in this embodiment is to design the sign function in the integral sign, so that discontinuity of the sign function is eliminated, and the buffeting problem caused by sliding mode control is reduced, while another scheme is to introduce integral into the control law, which is simpler and clearer than the method in this embodiment.
In addition, the embodiment introduces the use of a differentiator to solve the problem that the angular velocity and the angular acceleration of the joint rotation of the laser radar scanning mechanism cannot be directly measured in practice. While in the other case the control law contains an angular velocity term (in the error derivative), it is necessary to actually measure the angular velocity of the rotating platform. However, this is not necessarily achieved in practice, and the present solution enables the turntable to be controlled well even if the angular velocity is not measurable by introducing a differentiator, and the output of the structure of the differentiator is added to the controller, which output can accurately track the value of the angular velocity over a period of time.
This exampleDiscloses a tracking control system of a non-road mobile pollution source detection laser radar, which comprises a pollution source detection laser radar scanning mechanism and a controller, wherein the scanning mechanism comprises a base B0Azimuth rotary joint B1And roll rotary joint B3A base B0Azimuth rotary joint B1And roll rotary joint B2The controller comprises a coordinate system establishing module, a dynamic equation establishing module, an integral sliding mode surface constructing module and a second-order integral sliding mode tracking control module, wherein:
the coordinate system establishment module is used for utilizing a DH modeling method and using a base B0Azimuth rotary joint B1And roll rotary joint B2As joint points, respectively establishing joint coordinate systems;
the dynamic equation establishing module is used for establishing a joint rotation angle-moment dynamic equation of the scanning mechanism according to the established joint coordinate system and the power parameters of the scanning mechanism;
the integral sliding mode surface construction module is used for constructing an integral sliding mode surface by taking the difference value between the expected angle and the actual angle of the joint angle of the scanning mechanism as a tracking error;
and the second-order integral sliding mode tracking control module is used for constructing a sliding mode angle controller by utilizing an integral sliding mode surface and a differentiator so as to adjust the actual rotating angle of the joint of the scanning mechanism, obtain the moment applied to the scanning mechanism by the motor and realize the second-order integral sliding mode tracking control of the pollution source detection laser radar.
It should be noted that the tracking control system for detecting the lidar by using the non-road mobile pollution source disclosed in this embodiment corresponds to the tracking control method for detecting the lidar by using the non-road mobile pollution source disclosed in the above embodiment, and the implementation and effect of the specific technical scheme refer to the description in the above method embodiment, which is not described herein again.
The present embodiments also disclose a computer-readable storage medium comprising a computer program for use in conjunction with a storage device, the computer program for execution by a processor, comprising:
using DH modeling method with base B0Azimuth rotary joint B1And roll rotary joint B2As joint points, respectively establishing joint coordinate systems;
establishing a joint rotation angle-moment dynamics equation of the scanning mechanism according to the established joint coordinate system and the power parameters of the scanning mechanism;
constructing an integral sliding mode surface by taking the difference value of the expected angle and the actual angle of the joint angle of the scanning mechanism as a tracking error;
and constructing a sliding mode angle controller by utilizing an integral sliding mode surface and a differentiator to adjust the actual rotating angle of the joint of the scanning mechanism, so as to obtain the moment applied to the scanning mechanism by the motor and realize the second-order integral sliding mode tracking control of the pollution source detection laser radar.
Through the above description of the embodiments, it is clear to those skilled in the art that the above embodiments can be implemented by software, and can also be implemented by software plus a necessary general hardware platform. Based on such understanding, the technical solutions of the above embodiments may be embodied in the form of a software product, which may be stored in a non-volatile storage medium (which may be a CD-ROM, a usb disk, a removable hard disk, etc.), and includes several instructions for enabling a computer device (which may be a personal computer, a server, or a network device, etc.) to execute the methods according to the embodiments of the present invention, where the foregoing storage medium includes: various media that can store program codes, such as ROM, RAM, magnetic or optical disks.
The above description is only for the purpose of illustrating the preferred embodiments of the present invention and is not to be construed as limiting the invention, and any modifications, equivalents, improvements and the like that fall within the spirit and principle of the present invention are intended to be included therein.

Claims (10)

1. The tracking control method of the laser radar for detecting the non-road mobile pollution source is characterized in that a scanning mechanism of the laser radar for detecting the non-road mobile pollution source comprises a base B0Azimuth rotary joint B1And roll rotary joint B2A base B0Azimuth rotary joint B1And roll rotary joint B2In turn, rotationally coupled, the method comprising:
using DH modeling method with base B0Azimuth rotary joint B1And roll rotary joint B2As joint points, respectively establishing joint coordinate systems;
establishing a joint rotation angle-moment dynamics equation of the scanning mechanism according to the established joint coordinate system and the power parameters of the scanning mechanism;
constructing an integral sliding mode surface by taking the difference value of the expected angle and the actual angle of the joint angle of the scanning mechanism as a tracking error;
and constructing a sliding mode angle controller by utilizing an integral sliding mode surface and a differentiator to adjust the actual rotating angle of the joint of the scanning mechanism, so as to obtain the moment applied to the scanning mechanism by the motor and realize the second-order integral sliding mode tracking control of the pollution source detection laser radar.
2. The tracking control method of the non-road mobile pollution source detection lidar according to claim 1, wherein the constructed integral sliding mode surface is:
Figure FDA0002604012930000011
wherein λ is1And λ2And a proportional coefficient and an integral coefficient diagonal matrix respectively representing the sliding mode control rate, wherein beta is a constant coefficient, e is a tracking error, sign () is a sign function, and is 1 when the sign () is greater than 0 and is-1 when the sign () is less than 0.
3. The tracking control method of the non-road mobile pollution source detection laser radar as claimed in claim 2, wherein the second-order integral sliding mode tracking control of the pollution source detection laser radar is realized by using an integral sliding mode surface and a differentiator to construct a sliding mode angle controller to adjust the actual rotation angle of the joint of the scanning mechanism so as to obtain the torque applied to the scanning mechanism by a motor, and the second-order integral sliding mode tracking control of the pollution source detection laser radar comprises the following steps:
calculating the angular velocity and the angular acceleration of the joint rotation of the scanning mechanism by using a differentiator;
and constructing a sliding mode angle controller by using the integral sliding mode surface, the rotating angular speed and the angular acceleration of the scanning mechanism joint so as to adjust the actual rotating angle of the scanning mechanism joint and obtain the moment applied to the scanning mechanism by the motor.
4. The method as claimed in claim 3, wherein the formula for calculating the angular velocity and the angular acceleration of the joint rotation of the scanning mechanism by using the differentiator is as follows:
Figure FDA0002604012930000021
wherein Σ is a differentiator parameter and satisfies
Figure FDA0002604012930000022
The input of the differentiator is the actual angle q of the joint angle of the scanning mechanism, and the output psi of the differentiator0,ψ1,ψ2Are respectively used for estimating
Figure FDA0002604012930000023
Record as
Figure FDA0002604012930000024
5. The tracking control method of the non-road mobile pollution source detection laser radar as claimed in claim 3, wherein the sliding mode angle control law of the sliding mode angle controller is as follows:
Figure FDA0002604012930000025
wherein the content of the first and second substances,
Figure FDA0002604012930000026
representing the first derivative of the sliding mode surface s,
Figure FDA0002604012930000027
representing said desired angle qdSecond derivative of (a)1i2i,eiRespectively represent matrices lambda12And matrix e and the ith diagonal element of (1)iThe (i) th element of (a),
Figure FDA0002604012930000028
is the second differential of q, K1,K2Is a constant coefficient diagonal matrix, U (t-t)d) Represents tdThe moment applied to the scanning mechanism by the motor before time, and u (t) represents the moment applied to the scanning mechanism by the motor at time t.
6. The method of claim 5, wherein the method further comprises tracking the off-road mobile pollution source detection lidar
Figure FDA0002604012930000029
Figure FDA00026040129300000210
7. The method as claimed in claim 1, wherein the step of establishing a joint rotation angle-moment dynamics equation of the scanning mechanism according to the established joint coordinate system and the dynamic parameters of the scanning mechanism comprises:
establishing a positive kinematic equation of the laser radar scanning mechanism according to the DH parameters corresponding to the joint coordinate system;
and establishing a joint rotation angle-moment dynamics equation of the scanning mechanism according to the positive kinematics equation of the laser radar scanning mechanism and the power parameters of the laser radar scanning mechanism.
8. The method as claimed in claim 1, wherein the step of establishing a joint rotation angle-moment dynamics equation of the scanning mechanism according to the positive kinematics equation of the lidar scanning mechanism and the dynamic parameters of the lidar scanning mechanism comprises:
based on a positive kinematic equation of the laser radar scanning mechanism, performing forward iteration and backward iteration by using a Newton-Euler method to obtain a joint rotation angle-moment dynamic model of the laser radar scanning mechanism;
and substituting the dynamic parameters of the laser radar scanning mechanism into the joint rotation angle-moment dynamic model to obtain the moment-joint angle dynamic equation.
9. The tracking control system for the non-road mobile pollution source detection laser radar is characterized by comprising a pollution source detection laser radar scanning mechanism and a controller, wherein the scanning mechanism comprises a base B0Azimuth rotary joint B1And roll rotary joint B3A base B0Azimuth rotary joint B1And roll rotary joint B2The controller comprises a coordinate system establishing module, a dynamic equation establishing module, an integral sliding mode surface constructing module and a second-order integral sliding mode tracking control module, wherein:
the coordinate system establishment module is used for utilizing a DH modeling method and using a base B0Azimuth rotary joint B1And roll rotary joint B2As joint points, respectively establishing joint coordinate systems;
the dynamic equation establishing module is used for establishing a joint rotation angle-moment dynamic equation of the scanning mechanism according to the established joint coordinate system and the power parameters of the scanning mechanism;
the integral sliding mode surface construction module is used for constructing an integral sliding mode surface by taking the difference value between the expected angle and the actual angle of the joint angle of the scanning mechanism as a tracking error;
and the second-order integral sliding mode tracking control module is used for constructing a sliding mode angle controller by utilizing an integral sliding mode surface and a differentiator so as to adjust the actual rotating angle of the joint of the scanning mechanism, obtain the moment applied to the scanning mechanism by the motor and realize the second-order integral sliding mode tracking control of the pollution source detection laser radar.
10. A computer-readable storage medium comprising a computer program for use in conjunction with a storage device, the computer program for execution by a processor, comprising the steps of:
using DH modeling method with base B0Azimuth rotary joint B1And roll rotary joint B2As joint points, respectively establishing joint coordinate systems;
establishing a joint rotation angle-moment dynamics equation of the scanning mechanism according to the established joint coordinate system and the power parameters of the scanning mechanism;
constructing an integral sliding mode surface by taking the difference value of the expected angle and the actual angle of the joint angle of the scanning mechanism as a tracking error;
and constructing a sliding mode angle controller by utilizing an integral sliding mode surface and a differentiator to adjust the actual rotating angle of the joint of the scanning mechanism, so as to obtain the moment applied to the scanning mechanism by the motor and realize the second-order integral sliding mode tracking control of the pollution source detection laser radar.
CN202010733295.9A 2020-07-27 2020-07-27 Tracking control method and system for non-road mobile pollution source detection laser radar Pending CN111948624A (en)

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